Sliding bias and peak limiting for optical hearing devices

Information

  • Patent Grant
  • 11259129
  • Patent Number
    11,259,129
  • Date Filed
    Tuesday, November 19, 2019
    5 years ago
  • Date Issued
    Tuesday, February 22, 2022
    2 years ago
Abstract
A processor comprises instructions to adjust a bias of an input signal in order to decrease a duty cycle of a pulse modulated optical signal. The bias can be increased, decreased, or maintained in response to one or more measured values of the signal. In many embodiments, a gain of the signal is adjusted with the bias in order to inhibit distortion. The bias can be adjusted slowly in order to inhibit audible noise, and the gain can be adjusted faster than the bias in order to inhibit clipping of the signal. In many embodiments, one or more of the bias or the gain is adjusted in response to a value of the signal traversing a threshold amount. The value may comprise a trough of the signal traversing the threshold.
Description
BACKGROUND

The field of the present invention is related to optical hearing devices.


The prior methods and apparatus for providing sound to users can be less than ideal in at least some respects. People like to communicate, and hearing is an important aspect of communication for both communication devices and prosthetic devices such as hearing aids.


Contact hearing devices that contact tissue or bone have the advantage of providing sound with decreased feedback along the ear canal to the input microphone. However, the ear is composed of several small and delicate structures such as the tympanic membrane, ossicles and cochlea. Providing compact hearing devices that fit comfortably within the ear and contact moveable structures of the ear to provide high quality sound can be challenging. Transmitting power and signals to such small devices has also proven challenging.


Recently, it has been proposed to use light based hearing devices. Light based hearing devices have the advantage of potentially being small and providing high fidelity sound. However, realization of these potential advantages has proven challenging for several reasons. Sound is transmitted with positive and negative changes in air pressure. However, the light energy transmitted from a light source only results in the generation of positive light energy, with no corresponding negative light energy being available. Although light does oscillate with electrical and magnetic fields in the Terahertz frequency range, such frequencies are too fast for most detectors to capture the oscillating positive and negative field components of light. Consequently prior methods and apparatus used to drive electrical signals associated with positive and negative sound pressure may not be well suited for use with light based systems. Also, optical components can introduce distortions to optical signals, such as non-linear behavior of the light source and detector, which can present additional challenges.


At least some of the prior electronic circuitry solutions are less than ideally suited for the transmission of light based optical signals. For example, the use of prior delta-sigma modulation with optical signals can result in more power consumption than would be ideal. Similarly, prior analog approaches to transmitting electrical signals can result in increased power consumption when used with optical systems. As hearing devices can be worn for extended amounts of time, excessive power consumption may result in less than ideal performance of the hearing device in at least some instances.


In light of the above, it would be helpful to provide improved methods and apparatus for optical hearing. Ideally such optical devices would provide decreased power consumption, low amounts of distortion, be compact, and transmit the optical signal and energy to power the transducer with decreased amounts of distortion.


SUMMARY

Embodiments of the present invention provide improved transmission of optical signals with decreased amounts of light energy and distortion. In many embodiments, circuitry is configured to bias an input signal in order to generate an optical signal with decreased power consumption and distortion. The biased input signal reduces the amount of light energy transmitted for low energy input sound, and increases the amount of light energy transmitted for higher amounts of input sound energy. The bias can be adjusted slowly in order to inhibit audible sounds from being perceived by the user when the bias is adjusted. The slowly changing bias can be combined with rapidly decreased gain in response to peaks of the signal in order to inhibit peak clipping, and the gain can be rapidly increased to restore the gain. In many embodiments, the gain both decreases and increases quickly while the bias remains substantially fixed to inhibit clipping. In many embodiments, the bias shifts the input signal in a direction corresponding to negative sound pressure in response to low amounts of negative sound pressure. A processor can be configured with a look ahead delay in order to adjust the gain in response to the signal traversing a threshold detected with the look ahead delay, such that the gain can be dynamically increased and decreased in real time in response to the detected peak in order to decrease distortion.


The biased input signal can be used with many types of circuitry, and the circuitry configured to generate the optical signal in response to the biased input signal may comprise delta sigma modulation circuitry or analog amplifier circuitry, and combinations thereof. In many embodiments, a processor is configured with instructions to adjust the bias of the input sound signal in order to decrease a duty cycle of the output optical signal.


The bias can be increased, decreased, or maintained in response to one or more measured values of the signal. In many embodiments, a gain of the signal is adjusted with the bias in order to inhibit distortion. The bias can be adjusted slowly in order to inhibit audible noise such as thumping, and the gain can be adjusted faster than the bias in order to inhibit clipping of the signal and distortion. Thumping is a user perceivable sound like a “thump” that may occur if the bias were to be adjusted too quickly. In many embodiments, one or more of the bias or the gain is adjusted in response to a value of the signal below a threshold.


In many embodiments, peak limiting with a variable change in gain is used to inhibit clipping of the biased audio signal. The processor can be configured with a look ahead delay to detect an incident peak and to adjust the gain in response to the peak detected with the look ahead delay to inhibit clipping.


In a first aspect, embodiments provide a hearing apparatus to transmit an audio signal to an ear of a user with light. The apparatus comprises an input to receive the audio signal, a light source to generate an optical signal, and an output transducer to receive the optical signal from the light source. A processor is coupled to the input and configured with instructions to receive the audio signal, determine a bias of the audio signal and a biased audio signal in response to the audio signal, and output the biased audio signal to circuitry to drive the light source with the biased signal in order to decrease light energy of the optical signal transmitted from the light source.


In many embodiments, the processor comprises instructions to adjust the bias to decrease light energy in response to decreased energy of the audio signal and to adjust the bias to increase light energy in response to increased energy of the audio signal in order to inhibit distortion. The processor may comprise instructions to adjust the bias in a direction corresponding to negative sound pressure in response to decreased amounts of negative sound pressure of the audio signal. The processor may comprise instructions to adjust the bias to decrease amounts of light energy at a first rate and to increase amounts of light energy at a second rate to inhibit distortion. The first rate may be slower than the second rate. The processor may comprise instructions to adjust the bias over a time duration of more than about 50 ms or more than about 20 ms in order to inhibit an audible thump.


In many embodiments, the processor comprises instructions for a look ahead delay to decrease the gain to inhibit clipping in response to a negative signal below a threshold amount detected with the look ahead delay. The processor may comprise instructions to adjust the biased signal to more positive values in response to the negative signal below the threshold amount and to increase the gain when the biased signal is adjusted to the more positive values. The negative signal may correspond to negative sound pressure. The threshold amount may comprise a lower end of the input range. The processor may comprise instructions to decrease the gain faster than a change in bias. The bias may remain substantially fixed when the gain is decreased in response to the signal below the threshold. The processor may comprise instructions to decrease the gain over a duration of no more than a length of the look ahead delay. The bias may remain substantially fixed to within about five percent (5%) over the length of the look ahead delay.


The processor may comprise instructions to limit the bias in response to a noise floor associated with one or more of delta sigma modulation circuitry, the circuitry to drive the light source, the light source, or the output transducer to receive the output signal.


The audio signal may comprise a fixed bias. The processor may comprise instructions to determine the biased audio signal in response to the fixed bias of the audio signal.


The circuitry to drive the light source may comprise delta sigma modulation circuitry. The delta modulation circuitry may comprise one or more of pulse width modulation circuitry, pulse density modulation circuitry, or a digital to analog converter of the processor comprising the pulse density modulation circuitry. Alternatively or in combination, the circuitry to drive the light source may comprise an analog amplifier.


In another aspect, embodiments provide a method of transmitting an audio signal to an ear of a user with light. The audio signal may be received from an input. A bias of the audio signal and a biased audio signal may be determined with a processor in response to the audio signal. The biased audio signal may be output to circuitry to drive a light source with the biased signal in order to generate an optical signal with decreased light energy transmitted from the light source. The optical signal may be received with an output transducer to vibrate the ear in response to the output optical signal.


In many embodiments, the processor comprises instructions to adjust the bias to decrease light energy in response to decreased energy of the audio signal and to adjust the bias to increase light energy in response to increased energy of the audio signal in order to inhibit distortion. The processor may comprise instructions to adjust the bias in a direction corresponding to negative sound pressure in response to decreased amounts of negative sound pressure of the audio signal. The processor may comprise instructions to adjust the bias to decrease amounts of light energy at a first rate and to increase amounts of light energy at a second rate to inhibit distortion. The first rate may be slower than the second rate. The processor may comprise instructions to adjust the bias over a time duration of more than about 50 ms or more than about 20 ms in order to inhibit an audible thump.


In many embodiments, the processor comprises instructions for a look ahead delay to decrease the gain to inhibit clipping in response to a negative signal below a threshold amount detected with the look ahead delay. The processor may comprise instructions to adjust the biased signal to more positive values in response to the negative signal below the threshold amount and to increase the gain when the biased signal is adjusted to the more positive values. The negative signal may correspond to negative sound pressure. The threshold amount may comprise a lower end of the input range. The processor may comprise instructions to decrease the gain faster than a change in bias. The bias may remain substantially fixed when the gain is decreased in response to the signal below the threshold. The processor may comprise instructions to decrease the gain over a duration of no more than a length of the look ahead delay. The bias may remain substantially fixed to within about five percent (5%) over the length of the look ahead delay.


The processor may comprise instructions to limit the bias in response to a noise floor associated with one or more of delta sigma modulation circuitry, the circuitry to drive the light source, the light source or the output transducer to receive the output signal.


The input audio signal may comprise a fixed bias. The processor may comprise instructions to determine the biased audio signal in response to the fixed bias of the audio signal.


The circuitry to drive the light source may comprise delta sigma modulation circuitry. The delta modulation circuitry may comprise one or more of pulse width modulation circuitry, pulse density modulation circuitry, or a digital to analog converter of the processor comprising the pulse density modulation circuitry. Alternatively or in combination, the circuitry to drive the light source may comprise an analog amplifier.


In another aspect, embodiments provide a method of transmitting an audio signal with light. The audio signal may be received from an input. A bias of the audio signal and a biased audio signal may be determined with a processor in response to the audio signal. The biased audio signal may be output to circuitry to drive a light source with the biased signal in order to generate an optical signal with decreased light energy transmitted from the light source.


In another aspect, embodiments provide a hearing apparatus to transmit an audio signal to an ear of a user with light. The hearing apparatus may comprise a processor coupled to an input to receive the audio signal. The processor may be configured with instructions to receive the audio signal from the input, determine a bias of the audio signal and a biased audio signal in response to the audio signal, and output the biased audio signal to circuitry to drive a light source with the biased signal in order to decrease light energy transmitted from the light source.


In another aspect, embodiments provide a hearing apparatus. The apparatus may comprise an input to receive an audio signal, a light source, an output transducer to receive an optical signal from the light source, and a processor coupled to the input. The processor may comprise instructions configured to receive the audio signal, determine a bias of the audio signal to in response to the audio signal in order to decrease power consumption of the light source, decrease a gain in response to a negative peak of the audio signal below a threshold amount, and output an optical signal to the light source in response to the determined bias and the decreased gain in response to the negative peak of the audio signal below the threshold amount.


In another aspect, embodiments provide a hearing apparatus. The hearing apparatus may comprise an input to receive an audio signal, an output transducer to receive an optical signal, and a processor coupled to the input. The processor may comprise instructions to receive the audio signal and determine a bias of the audio signal in response to the audio signal and output an optical signal in response to the bias.


The optical signal may comprise a pulse modulated optical signal. The processor may comprise instructions to output the pulse modulated optical signal. Alternatively, the optical signal may comprise an analog optical signal, and the processor may comprise instructions to output the analog optical signal.


The apparatus may further comprise a light source. The light source may comprise a laser diode. The laser diode may comprise a linear light output in response to a biased audio signal input to the laser diode.


The instructions of the processor may comprise instruction to adjust the bias in response to a value of the signal, to adjust the bias in response to a value of the signal traversing a threshold amount, or to adjust the bias and a gain of the signal in response to a value of the signal traversing a threshold amount, and combinations thereof.


The bias may be combined with the input audio signal to provide a biased audio signal. The pulse modulated signal may be determined in response to the biased audio signal. The bias may comprise a negative bias added to the input audio signal to decrease amounts of light transmitted with the pulse modulated signal. The bias may comprise a sliding bias to offset the input audio signal by a variable amount and to provide the biased audio signal with a variable bias. The bias may comprise an adjustable bias, and the instructions of the processor may be configured to adjust the bias with substantially inaudible frequencies.


The audio signal may comprise a peak. The bias may be adjusted in response to the peak of the signal. The peak may comprise a negative peak. The bias may be determined in response to the negative peak of the signal.


The audio signal may comprise a positive peak and a negative peak. The bias may be adjusted in response to the negative peak of the signal. Alternatively or in combination, the bias may be adjusted in response to the positive peak of the signal.


The processor may comprise instructions to adjust or decrease a gain of the signal in response to the value of the audio signal.


The apparatus may further comprise one or more light sources to couple to the output transducer, and drive circuitry coupled to the processor and the one or more light sources. The processor may comprise instructions to drive the one or more light sources with drive circuitry and the pulse modulated signal. The one or more light sources and the drive circuitry may be arranged to transmit power and signal to the output transducer with the pulse modulated optical signal in order to drive the output transducer assembly in response to the power and signal transmitted with the pulse modulated optical signal.


The output transducer may comprise one or more of a support, a photodiode, an electromechanical transducer, or a photostrictive material. The support may comprise one or more of a support shaped to engage a tympanic membrane of the user, a support shaped to engage an ossicle of the user, a support shaped to engage a round window of the user, a support shaped to engage an oval window of the user, or a support shaped to engage bone of the user.


The electromechanical transducer may comprise one or more of a balanced armature transducer, a coil and magnetic material, or a piezoelectric material.


In another aspect, embodiments provide a method comprising providing the apparatus as in any one of embodiments described above and herein.


In another aspect, embodiments provide a method of transmitting sound to a user. The method comprising receiving an audio signal, determining a bias of the signal in response to the signal, and providing a pulse modulated optical signal in response to the bias and the signal.





BRIEF DESCRIPTION OF THE DRAWINGS

A better understanding of the features and advantages of the present disclosure will be obtained by reference to the following detailed description that sets forth illustrative embodiments, in which the principles of the disclosure are utilized, and the accompanying drawings of which:



FIG. 1 shows a hearing aid system configured to transmit electromagnetic energy to an output transducer assembly, in accordance with embodiments;



FIGS. 2A and 2B show isometric and top views, respectively, of the output transducer assembly in accordance with embodiments;



FIG. 3 shows circuitry of the hearing aid system 10, in accordance with embodiments;



FIG. 4A shows an input signal and the input signal with bias, in accordance with embodiments;



FIG. 4B shows modulated light pulses in accordance with the adjustable bias as described herein;



FIG. 4C shows an increased amplitude input signal with the bias of FIG. 4A and peak limiting, in accordance with embodiments;



FIGS. 5A and 5B show light power curves with a fixed bias, and a sliding bias to improve sound quality and substantially decrease power consumption, in accordance with embodiments;



FIG. 5C shows an encoding of the fixed bias curve of FIG. 5A, using pulse width modulation, in accordance with embodiments;



FIG. 5D shows an encoding of the fixed bias curve of FIG. 5A, using pulse density modulation, in accordance with embodiments;



FIG. 5E shows an encoding of the sliding bias curve of FIG. 5A, using pulse width modulation, in accordance with embodiments;



FIG. 5F shows an encoding of the sliding bias curve of FIG. 5A, using pulse density modulation, in accordance with embodiments;



FIG. 6A shows amplitude of a digital input signal, adjusted with sliding bias and peak limiting to inhibit clipping, in accordance with embodiments;



FIG. 6B shows a look-ahead delay used to determine a change in gain, in accordance with embodiments;



FIG. 6C shows the adjustment of a sliding bias and gain over time, in accordance with embodiments; and



FIG. 7 shows a method of adjusting a bias and peak limiting, in accordance with embodiments.





DETAILED DESCRIPTION

A better understanding of the features and advantages of the present disclosure will be obtained by reference to the following detailed description that sets forth illustrative embodiments, in which the principles of embodiments of the present disclosure are utilized, and the accompanying drawings.


Although the detailed description contains many specifics, these should not be construed as limiting the scope of the disclosure but merely as illustrating different examples and aspects of the present disclosure. It should be appreciated that the scope of the disclosure includes other embodiments not discussed in detail above. Various other modifications, changes and variations which will be apparent to those skilled in the art may be made in the arrangement, operation and details of the method and apparatus of the present disclosure provided herein without departing from the spirit and scope of the invention as described herein.


Although specific reference is made to a hearing aid, the embodiments disclosed herein will have application with many fields, such as acoustics and listening devices, for example electronic communication devices such as cell phones.


The optical methods and apparatus disclosed herein that provide low distortion optical signals with decreased power consumption are well suited for combination with many types of commercially available electrical circuits and sound processors used to transmit electrical signals such as delta sigma modulation circuitry and class-A amplifiers for example.


The embodiments disclosed herein can be combined with implantable and non-implantable hearing devices.


The embodiments disclosed herein can be combined in one or more of many ways to provide improved sound quality with optically driven transducers.


As used herein like characters identify like elements.


As used herein light encompasses one or more of visible light, ultraviolet light, or infrared light, and combinations thereof.


As used herein electromagnetic energy encompasses light energy.


As used herein a trough encompasses a negative peak.


Examples of optical transducers that couple the transducer to structure of the ear so as to decrease occlusion are described in U.S. Pat. Nos. 7,668,325; 7,867,160; 8,396,239; 8,401,212; 8,715,153; 8,715,154; and U.S. patent application Ser. Nos. 12/820,776; 13/069,282; 61/217,801, filed Jun. 3, 2009, entitled “Balanced Armature Device and Methods for Hearing”; and PCT/US2009/057719, filed 21 Sep. 2009, entitled “Balanced Armature Device and Methods for Hearing”, published as WO 2010/033933; the full disclosures of which are incorporated herein by reference and suitable for combination in accordance with embodiments as described herein.


In many embodiments, an audio signal is transmitted using light to provide both power and signal to a transducer. Although light comprises electrical fields oscillating at terahertz frequencies, commercially available detectors do not capture the negative component of the electric field oscillation. Because the light energy applied to a transducer results in a unidirectional signal, no opposing signal is available. Therefore, a light-encoded signal can be biased in order to decrease power consumption. Power consumption increases with increasing bias, and reducing bias can extend battery life substantially. However, the bias also determines the maximum signal amplitude that can be encoded, so reducing bias constrains signal level. The embodiments disclosed herein are particularly well suited for providing a decreased bias in combination with inhibited clipping in order to provide improved sound to the user.


In many embodiments, the adjustable bias comprises a sliding bias (hereinafter “SB”). The SB algorithm monitors the signal level and may continually adjust the bias. In many embodiments, the bias is set to the minimum value that can accommodate the signal level. Power consumption can be reduced when the signal level is low, such that the tradeoff between battery life and signal range can be balanced, for example optimized.


In many embodiments, the SB algorithm sets the bias level in response to the peak levels of the signal, such as negative peaks of the signal. The peak level can be proportional to the root mean square (rms) level of signal. A factor comprising the ratio of the peak value to rms value is known as the crest factor. However, the crest factor can vary with the type of input signal and may not be well suited for use with at least some input audio signals. High crest factor signals may require high bias levels and thus increase power consumption. Therefore it may be desirable to reduce the crest factor in conjunction with applying sliding bias. There are several methods that can be used to reduce the crest factor of a signal. One method is to use a variable level peak limiting strategy, for example. Another method is to use a peak cancellation strategy. Yet another method provides a soft limiting strategy. These methods are suitable for combination in accordance with embodiments disclosed herein. In many embodiments, the peak limiting is adjustable and is not fixed, and the crest-factor limiting is dependent on the bias level.


The sliding-bias algorithm and the combined peak limiting and sliding-bias algorithms as described herein can be used alternatively or in combination as the front end to pulse-width or pulse density modulation circuitry. Alternatively, they can be used as the front end of a class-A analog system. In these embodiments, a significant savings in output power can be realized, particularly when the signal is low level.



FIG. 1 shows a hearing aid system 10 configured to transmit electromagnetic energy comprising light energy EM to an output transducer assembly 100 positioned in the ear canal EC of the user. The ear comprises an external ear, a middle ear ME and an inner ear. The external ear comprises a Pinna P and an ear canal EC and is bounded medially by an eardrum TM. Ear canal EC extends medially from pinna P to eardrum TM. Ear canal EC is at least partially defined by a skin SK disposed along the surface of the ear canal. The eardrum TM comprises an annulus TMA that extends circumferentially around a majority of the eardrum to hold the eardrum in place. The middle ear ME is disposed between eardrum TM of the ear and a cochlea CO of the ear. The middle ear ME comprises the ossicles OS to couple the eardrum TM to cochlea CO. The ossicles OS comprise an incus IN, a malleus ML and a stapes ST. The malleus ML is connected to the eardrum TM and the stapes ST is connected to an oval window OW, with the incus IN disposed between the malleus ML and stapes ST. Stapes ST is coupled to the oval window OW so as to conduct sound from the middle ear to the cochlea.


The hearing system 10 includes an input transducer assembly 20 and an output transducer assembly 100 to transmit sound to the user. Hearing system 10 may comprise a behind the ear unit BTE. Behind the ear unit BTE may comprise many components of system 10 such as a speech processor, battery, wireless transmission circuitry and input transducer assembly 10. Behind the ear unit BTE may comprise many component as described in U.S. Pat. Pub. Nos. 2007/0100197, entitled “Output transducers for hearing systems”; and 2006/0251278, entitled “Hearing system having improved high frequency response”, the full disclosures of which are incorporated herein by reference and may be suitable for combination in accordance with some embodiments of the present invention. The input transducer assembly 20 can be located at least partially behind the pinna P, although the input transducer assembly may be located at many sites. For example, the input transducer assembly may be located substantially within the ear canal, as described in U.S. Pub. No. 2006/0251278. The input transducer assembly may comprise a Bluetooth® connection to couple to a cell phone and may comprise, for example, components of the commercially available Sound ID 300, available from Sound ID of Palo Alto, Calif. The output transducer assembly 100 may comprise components to receive the light energy and vibrate the eardrum in response to light energy. An example of an output transducer assembly having components suitable for combination in accordance with embodiments as described herein is described in U.S. Pat. App. No. 61/217,801, filed Jun. 3, 2009, entitled “Balanced Armature Device and Methods for Hearing” and PCT/US2009/057719, filed 21 Sep. 2009, Balanced Armature Device and Methods for Hearing”, the full disclosure of which is incorporated herein by reference.


The input transducer assembly 20 can receive a sound input, for example an audio sound. With hearing aids for hearing impaired individuals, the input can be ambient sound. The input transducer assembly comprises at least one input transducer, for example a microphone 22. Microphone 22 can be positioned in many locations such as behind the ear, as appropriate. Microphone 22 is shown positioned to detect spatial localization cues from the ambient sound, such that the user can determine where a speaker is located based on the transmitted sound. The pinna P of the ear can diffract sound waves toward the ear canal opening such that sound localization cues can be detected with frequencies above at least about 4 kHz. The sound localization cues can be detected when the microphone is positioned within ear canal EC and also when the microphone is positioned outside the ear canal EC and within about 5 mm of the ear canal opening. The at least one input transducer may comprise a second microphone located away from the ear canal and the ear canal opening, for example positioned on the behind the ear unit BTE. The input transducer assembly can include a suitable amplifier or other electronic interface. In some embodiments, the input may comprise an electronic sound signal from a sound producing or receiving device, such as a telephone, a cellular telephone, a Bluetooth connection, a radio, a digital audio unit, and the like.


In many embodiments, at least a first microphone can be positioned in an ear canal or near an opening of the ear canal to measure high frequency sound above at least about one 4 kHz comprising spatial localization cues. A second microphone can be positioned away from the ear canal and the ear canal opening to measure at least low frequency sound below about 4 kHz. This configuration may decrease feedback to the user, as described in U.S. Pat. Pub. No. US 2009/0097681, the full disclosure of which is incorporated herein by reference and may be suitable for combination in accordance with embodiments of the present invention.


Input transducer assembly 20 includes a signal output source 12 which may comprise a light source such as an LED or a laser diode, an electromagnet, an RF source, or the like. The signal output source can produce an output based on the sound input. Output transducer assembly 100 can receive the output from input transducer assembly 20 and can produce mechanical vibrations in response. Output transducer assembly 100 comprises a sound transducer and may comprise at least one of a coil, a magnet, a magnetostrictive element, a photostrictive element, or a piezoelectric element, for example. For example, the output transducer assembly 100 can be coupled input transducer assembly 20 comprising an elongate flexible support having a coil supported thereon for insertion into the ear canal as described in U.S. Pat. Pub. No. 2009/0092271, entitled “Energy Delivery and Microphone Placement Methods for Improved Comfort in an Open Canal Hearing Aid”, the full disclosure of which is incorporated herein by reference and may be suitable for combination in accordance with some embodiments of the present invention. Alternatively or in combination, the input transducer assembly 20 may comprise a light source coupled to a fiber optic, for example as described in U.S. Pat. Pub. No. 2006/0189841 entitled, “Systems and Methods for Photo-Mechanical Hearing Transduction”, the full disclosure of which is incorporated herein by reference and may be suitable for combination in accordance with some embodiments of the present invention. The light source of the input transducer assembly 20 may also be positioned in the ear canal, and the output transducer assembly and the BTE circuitry components may be located within the ear canal so as to fit within the ear canal. When properly coupled to the subject's hearing transduction pathway, the mechanical vibrations caused by output transducer assembly 100 can induce neural impulses in the subject which can be interpreted by the subject as the original sound input.



FIGS. 2A and 2B show isometric and top views, respectively, of the output transducer assembly 100. Output transducer assembly 100 comprises a retention structure 110, a support 120, a transducer 130, at least one spring 140 and a photodetector 150. Retention structure 110 is sized to couple to the eardrum annulus TMA and at least a portion of the anterior sulcus AS of the ear canal EC. Retention structure 110 comprises an aperture 110A. Aperture 110A is sized to receive transducer 130.


The retention structure 110 can be sized to the user and may comprise one or more of an o-ring, a c-ring, a molded structure, or a structure having a shape profile so as to correspond to a mold of the ear of the user. For example retention structure 110 may comprise a polymer layer 115 coated on a positive mold of a user, such as an elastomer or other polymer. Alternatively or in combination, retention structure 110 may comprise a layer 115 of material formed with vapor deposition on a positive mold of the user, as described herein. Retention structure 110 may comprise a resilient retention structure such that the retention structure can be compressed radially inward as indicated by arrows 102 from an expanded wide profile configuration to a narrow profile configuration when passing through the ear canal and subsequently expand to the wide profile configuration when placed on one or more of the eardrum, the eardrum annulus, or the skin of the ear canal.


The retention structure 110 may comprise a shape profile corresponding to anatomical structures that define the ear canal. For example, the retention structure 110 may comprise a first end 112 corresponding to a shape profile of the anterior sulcus AS of the ear canal and the anterior portion of the eardrum annulus TMA. The first end 112 may comprise an end portion having a convex shape profile, for example a nose, so as to fit the anterior sulcus and so as to facilitate advancement of the first end 112 into the anterior sulcus. The retention structure 110 may comprise a second end 114 having a shape profile corresponding to the posterior portion of eardrum annulus TMA.


The support 120 may comprise a frame, or chassis, so as to support the components connected to support 120. Support 120 may comprise a rigid material and can be coupled to the retention structure 110, the transducer 130, the at least one spring 140 and the photodetector 150. The support 120 may comprise a biocompatible metal such as stainless steel so as to support the retention structure 110, the transducer 130, the at least one spring 140 and the photodetector 150. For example, support 120 may comprise cut sheet metal material. Alternatively, support 120 may comprise injection molded biocompatible plastic. The support 120 may comprise an elastomeric bumper structure 122 extending between the support and the retention structure, so as to couple the support to the retention structure with the elastomeric bumper. The elastomeric bumper structure 122 can also extend between the support 120 and the eardrum, such that the elastomeric bumper structure 122 contacts the eardrum TM and protects the eardrum TM from the rigid support 120. The support 120 may define an aperture 120A formed thereon. The aperture 120A can be sized so as to receive the balanced armature transducer 130, for example such that the housing of the balanced armature transducer 130 can extend at least partially through the aperture 120A when the balanced armature transducer is coupled to the eardrum TM. The support 120 may comprise an elongate dimension such that support 120 can be passed through the ear canal EC without substantial deformation when advanced along an axis corresponding to the elongate dimension, such that support 120 may comprise a substantially rigid material and thickness.


The transducer 130 comprises structures to couple to the eardrum when the retention structure 120 contacts one or more of the eardrum, the eardrum annulus, or the skin of the ear canal. The transducer 130 may comprise a balanced armature transducer having a housing and a vibratory reed 132 extending through the housing of the transducer. The vibratory reed 132 is affixed to an extension 134, for example a post, and an inner soft coupling structure 136. The soft coupling structure 136 has a convex surface that contacts the eardrum TM and vibrates the eardrum TM. The soft coupling structure 136 may comprise an elastomer such as silicone elastomer. The soft coupling structure 136 can be anatomically customized to the anatomy of the ear of the user. For example, the soft coupling structure 136 can be customized based a shape profile of the ear of the user, such as from a mold of the ear of the user as described herein.


At least one spring 140 can be connected to the support 120 and the transducer 130, so as to support the transducer 130. The at least one spring 140 may comprise a first spring 122 and a second spring 124, in which each spring is connected to opposing sides of a first end of transducer 130. The springs may comprise coil springs having a first end attached to support 120 and a second end attached to a housing of transducer 130 or a mount affixed to the housing of the transducer 130, such that the coil springs pivot the transducer about axes 140A of the coils of the coil springs and resiliently urge the transducer toward the eardrum when the retention structure contacts one or more of the eardrum, the eardrum annulus, or the skin of the ear canal. The support 120 may comprise a tube sized to receiving an end of the at least one spring 140, so as to couple the at least one spring to support 120.


A photodetector 150 can be coupled to the support 120. A bracket mount 152 can extend substantially around photodetector 150. An arm 154 extend between support 120 and bracket 152 so as to support photodetector 150 with an orientation relative to support 120 when placed in the ear canal EC. The arm 154 may comprise a ball portion so as to couple to support 120 with a ball-joint. The photodetector 150 can be coupled to transducer 130 so as to driven transducer 130 with electrical energy in response to the light energy signal from the output transducer assembly.


Resilient retention structure 110 can be resiliently deformed when inserted into the ear canal EC. The retention structure 110 can be compressed radially inward along the pivot axes 140A of the coil springs such that the retention structure 110 is compressed as indicated by arrows 102 from a wide profile configuration having a first width 110W1 to an elongate narrow profile configuration having a second width 110W2 when advanced along the ear canal EC as indicated by arrow 104 and when removed from the ear canal as indicated by arrow 106. The elongate narrow profile configuration may comprise an elongate dimension extending along an elongate axis corresponding to an elongate dimension of support 120 and aperture 120A. The elongate narrow profile configuration may comprise a shorter dimension corresponding to a width 120W of the support 120 and aperture 120A along a shorter dimension. The retention structure 110 and support 120 can be passed through the ear canal EC for placement. The reed 132 of the balanced armature transducer 130 can be aligned substantially with the ear canal EC when the assembly 100 is advanced along the ear canal EC in the elongate narrow profile configuration having second width 110W2.


The support 120 may comprise a rigidity greater than the resilient retention structure 110, such that the width 120W remains substantially fixed when the resilient retention structure is compressed from the first configuration having width 110W1 to the second configuration having width 110W2. The rigidity of support 120 greater than the resilient retention structure 110 can provide an intended amount of force to the eardrum TM when the inner soft coupling structure 136 couples to the eardrum, as the support 120 can maintain a substantially fixed shape with coupling of the at least one spring 140. In many embodiments, the outer edges of the resilient retention structure 110 can be rolled upwards toward the side of the photodetector 150 so as to compress the resilient retention structure from the first configuration having width 110W1 to the second configuration having width 110W2, such that the assembly can be easily advanced along the ear canal EC.



FIG. 3 shows circuitry of the hearing aid system 10. The circuitry of hearing system 10 may comprise one or more components of input transducer assembly 20 and output transducer assembly 100, for example.


The circuitry of the input transducer assembly 20 comprises one or more sources of an input audio signal 164, such as one or more of wireless communication circuitry 160 or microphone circuitry 162, for example. Wireless communication circuitry 160 may comprise one or more of many known wireless communication circuitry components such as circuitry compatible with Bluetooth® communication standards, for example. The microphone circuitry 162 may comprise microphone 22 and amplifiers, for example. The input audio signal 164 is received with an input of sound processor 170. Sound processor 170 can be coupled to pulse modulation circuitry 180 to generate modulated pulses, for example. Alternatively or in combination, the sound processor 170 may comprise the pulse modulation circuitry. The output of the pulse modulation circuitry 180 can be coupled to drive circuitry 190. The drive circuitry 190 can be coupled to an output light source 12, for example. The output light source 12 can provide output light energy pulses modulated in accordance with pulse modulation circuitry 190, for example.


The light output source 12 can be configured in one or more of many ways. The light output source 12 can be placed in the ear canal, or outside the ear canal such as in a BTE unit as described herein, for example. The light output source 12 may comprise one or more of many light sources such as a light emitting diode, a laser, or a laser diode, for example. In many embodiments, the output light source 12 comprises a laser diode having a linear light energy output in response to an input signal, for example. The laser diode having the substantially linear output in response to the input signal can provide a low distortion output light signal, which can be combined with an analog output or modulated output signal from the processor and drive circuitry as described herein, for example.


The circuitry of the output transducer assembly 100 can be configured in one or more of many ways to receive the pulse modulated light signal and induce vibrations of the subject's auditory pathway. In many embodiments, a photodetector 150 receives the modulated light pulses. The photodetector 150 may comprise one or more of many light sensitive materials such as a photodiode, a silicone photodiode material or a photostrictive material, for example. In many embodiments, photodetector 150 is coupled to an output transducer 130. The output transducer 130 may comprise one or more of many electromechanical actuators such as a coil, a magnetic material, a magnet, a balanced armature transducer, or a piezo electric material, for example.


The pulse modulation circuitry 180 may comprise one or more of pulse width modulation circuitry or pulse density modulation circuitry, for example. In many embodiments, the pulse modulation circuitry can be replaced or combined with one or more of many forms of circuitry. For example, the pulse modulation circuitry can be replaced with circuitry configured to output an analog optical signal, such as a class A amplifier. Alternatively, the pulse modulation circuitry can be replaced with one more of many forms of modulation circuitry such amplitude modulation, frequency modulation, or phase modulation, for example, in order to decrease the optical energy of the output signal from the light source.


The processor 170 may comprise on or more components of the input transducer assembly. The sound processor 170 may comprise one or more of: analog circuitry to amplify an analog signal from the microphone; analog to digital conversion circuitry to convert an analog input signal to a digital circuitry; digital input circuitry to receive a digital sound signal; a digital signal processor; a tangible medium embodying instructions to process a sound signal; output circuitry to output a digital signal; digital filters to adjust a sound signal in response to user preference; and combinations thereof. In many embodiments, the sound processor is configured with instructions to adjust the bias of the input signal and limit peaks as described herein.


The sound processor may comprise one or more components of a commercially available sound processor known to those of ordinary skill in the art of hearing aid design. The sound processor may comprise a tangible medium such as one or more of a computer readable memory, random access memory, read only memory, writable erasable read only memory, and a solid state hard drive. The sound processor may comprise a processor capable of executing instructions stored on the tangible medium, and may comprise gate array logic, programmable gate array logic, and combinations thereof. The processor may comprise a plurality of processors and a plurality of tangible media, for example. A person of ordinary skill in the art will recognize many configurations of processor 170 in accordance with the embodiments disclosed herein.



FIG. 4A shows an input signal 210 relative to an input reference 205 and the input signal 210 with an adjustable bias 220. The input signal 210 may comprise an audio signal as described herein. The reference level 205 may correspond to, for example, 0 volts, and the amplitude of the input signal may vary over a range of positive and negative voltages of +1 and −1, for example. The voltage scale can be arbitrary. With the initial input audio signal 210 relative to reference level 205, the input audio signal varies above and below the reference 205 which in many embodiments may correspond to, for example 0 Volts. The input signal 210 comprises a peak 217 and a trough 218. In many embodiments trough 218 comprises a negative peak. The peak 217 and trough 218 may comprise a local peak and a local trough, respectively, for example.


In some embodiments of the invention, an input signal may have a voltage range from +1 to −1 without causing clipping of the output. In embodiments of the invention where the input signal is to a range of +1 to −1 volts, a small amplitude signal (e.g. a signal ranging in amplitude from approximately +0.1 to −0.1 volts) applied to the input of the pulse modulation circuitry 180 (e.g. a pulse wave modulator or pulse density modulator) will result in a duty cycle, without the adjustable bias, of about 50%. This duty cycle of about 50% results in greater power consumption than would be ideal for the amount of variation of the input audio signal 210.


In embodiments of the invention, a bias is applied to the input signal to ensure that the output of the pulse modulation circuitry accounts for both the positive and negative going amplitude peaks. In embodiments of the invention, this bias (e.g. reference level 205) may be a fixed bias and may be illustrated in, for Example FIG. 4A as having a reference value of 0.0. As this reference level is generally chosen to ensure that the largest input signal (e.g. a signal having positive and negative peak values of +1 and −1 volts) will not encounter clipping, it is generally chosen to be larger than required to prevent clipping of smaller input signals. For a small amplitude input signal, such as signal 210 in FIG. 4A, a smaller bias 220 can be combined with the input signal 210 to provide the biased input signal 212. The biased input signal 212 decreases the duty cycle of the pulses output from the pulse modulation circuitry 180. The biased input signal 212 can be offset by an amount sufficient to substantially decrease the duty cycle of light pulses in, for example, a laser driven by the output of drive circuitry 190. In some embodiments of the invention, a reference bias 205 may be reduced by, for example, 0.7 units, as illustrated in FIG. 4A, for a period of time during which the amplitude of an input signal 210 varies between a peak of approximately 0.1 units and −0.1 units.



FIG. 4B shows pulse width modulated light pulses in a system where sliding bias has not been applied. In FIG. 4B, the instantaneous input signal value is shown from an arbitrary scale of −1 to +1. At a signal value of 0, the duty cycle of the pulse modulated signal is 50%. At signal values of −1, −0.5, +0.5 and 1, the duty cycle values are 0%, 25%, 75% and 100%, respectively. Each duty cycle comprises a period T, an on time Ton of the light source and an off time Toff of the light source. The duty cycle in percent can be defined as (Ton/T)*100. In a system such as that illustrated in FIG. 4B, a small signal, such as signal 210 from FIG. 4A would result in a duty cycle of between approximately 45% and 55%, a duty cycle which would result in the use of much more energy than would be required to actually transmit the information in signal 210. Thus, it would be advantageous to be reduce the duty cycle for signal 210 to a range of between approximately 0% and 10% to reduce the amount of energy required to transmit that signal. In some embodiments of the invention, that reduction may be accomplished through the use of a sliding bias by sensing, for example, minimum peaks of the incoming signal and modifying the amount of bias applied to reduce the duty cycle. In some embodiments of the invention, this may be done by, for example, modifying the duty cycle which is representative of the zero crossing of the incoming signal, such as, for example, reducing the duty cycle representative of a zero crossing from 50% as illustrated in FIG. 4B to approximately 10% for input signal 205 from FIG. 4A.


Although pulse width modulated signals are shown, the pulse modulated signal may comprise a pulse density modulated signal, or a pulse frequency modulated signal, for example. In many embodiments, the pulse modulated signal as described herein comprises a substantially fixed amplitude in order to inhibit effects of non-linearities of the optical sound transmission system components such one or more of the light source, the photodetector or the output transducer, for example.



FIG. 4C shows an increased amplitude of input signal 210 with the adjustable 220 bias of FIG. 4A and peak limiting. In the upper graph, Signal 210 is shown in relation to input reference 205. In this embodiment, clipping of signal 210 occurs when signal 201 exceeds an amplitude of +1.0 or −1.0, therefore, any applied bias must account for those clipping limits. It would, however, be advantageous to lower the applied bias represented by reference 205, in order to save energy. In the lower graph of FIG. 4C, bias 220, which is lower than reference bias 205 by approximately −0.7 units, is applied to signal 210 in order to provide biased signal 212. Unfortunately, as the negative peak of signal 210 is now at approximately −1.05 units, that peak will be clipped if it is not adjusted. Adjustments to the sliding bias which occur quickly (e.g. in response to changes in amplitude) may, in some embodiments, result in undesirable user perceptible noise. In some embodiments of the invention, the clipping illustrated in the lower graph of FIG. 4C may, therefore, be addressed by adjusting the gain of the system to ensure that the signal is not clipped.


The bias 220 comprises a fixed portion 222 having a substantially fixed value and a variable portion 224 comprising a gradually changing value. The gradually changing value is varied sufficiently slowly so as to inhibit user perceptible noise. However, slowly varying the bias may result in clipping of the signal until the sliding bias reaches a level at which clipping no longer occurs.


Alternatively or in combination with the adjustment to bias 220 with variable portion 224, the amplitude of signal 210 can be adjusted in order to inhibit clipping of the biased input signal 212. In many embodiments, the adjustment to the amplitude of signal 210 is provided much more rapidly than the adjustment to the bias. In embodiments of the Invention, reduction of the system gain will result in reducing or eliminating clipping of signal 210 until the bias can be adjusted to avoid such clipping, which may take several cycles of signal 210. Once the bias is adjusted sufficiently to avoid clipping, the system gain may be restored to its original value


The adjustment to the gain can be determined with a look ahead delay as described herein below with reference to FIG. 6A. Although FIG. 4C shows the change to the gain over a portion of the signal for the convenience of illustration, the change to the gain can occur over several positive and negative oscillations of the sliding bias signal as described herein.


In many embodiments, the bias adjustment comprises a steady mode in which the bias remains substantially fixed and maintained at an appropriate value to, for example, minimize energy consumption. In some embodiments of the present invention, when the system detects a signal wherein the negative going peak will exceed the system limit, the sliding bias enters an attack mode, in which the bias is increased (in some embodiments an increase in sliding bias makes it less negative). In some embodiments of the invention, where the system detects that the bias may be reduced without causing clipping, the sliding bias enters a release mode in which the bias is decreased, which, in some embodiments will result in a reduction of duty cycle in the output signal.


The gain and corresponding amplitude of the signal can be adjusted in a manner similar to the bias as described herein, and can be adjusted more quickly without substantial user perceptible artifacts, for example. In many embodiments, the adjustment to the system gain inhibits user perceptible clipping of the signal which may otherwise occur when the biased signal exceeds the lower range limit. By inhibiting the biased signal from reaching a value more negative than the negative limit of the circuitry, while reducing the sliding bias to a minimum value, improved sound quality with decreased distortion and power consumption can be provided.



FIGS. 5A and 5B show light power curves biased to substantially decrease power consumption. The system of FIGS. 5A and 5B are designed to accommodate an output signal having a maximum peak to peak amplitude of +2.0 units without clipping. The bias applied to a large amplitude signal is, therefore, approximately +1.0 units. FIG. 5A shows the power curve 250 of an input signal of medium amplitude with a bias of +1.0 units but without sliding bias applied. The fixed bias of power curve 250 provides improved signal quality and can accommodate negative voltage of an input signal such as a microphone. A sliding bias of −0.5 is shown applied to the fixed bias signal, reducing the bias applied to 0.5 units and producing a sliding biased signal 255. The sliding bias may be adjusted so that the trough (or negative peak) 256 of the signal to which the sliding bias has been applied is at or near zero power. This configuration allows the bias (and output power) to be substantially decreased when the signal to be transmitted is smaller than the maximum signal the system can transmit with clipping. In embodiments of the invention, the sliding bias is used to decrease the applied bias to a value which reduces output power consumed while preventing clipping of the output signal. FIG. 5B shows another example, in which a larger sliding bias adjustment is used to shift the bias applied to a small-amplitude signal. In this case, the power curve of signal 260 starts with a bias of +1.0. Since the peak to peak amplitude of signal 260 is approximately 0.5, −0.75 may be chosen, corresponding to the difference between the amplitude and the offset of the input signal. This results in a sliding-biased signal 256 with a bias of 0.25, so that its trough 256 is substantially decreased at or near zero power and is not clipped.


The input signal may comprise an unbiased input audio signal or a biased input audio signal. The fixed bias as described herein can be introduced to the input signal in many ways. For example an input analog audio signal from a microphone may have an input range from −1 to +1 (arbitrary), and the analog to digital converter can be configured to digitize the input analog signal such that the digitized values are positive, for example from 0 to 2 (arbitrary). Alternatively, the analog to digital converter may convert the analog values to a digital range from −1 to +1, and a fixed bias of 1.0 introduced to the digitized values with addition, for example, such that the digitized values range from 0 to 2, for example. The fixed bias may comprise a fixed bias of an input digital audio signal from an external source such as music from a digital library or a cellular phone, for example. Alternatively or in combination, the processor can be configured with instructions to provide a fixed bias to the input digital audio signal, for example.


The curves shown in FIGS. 5A and 5B can be generated with the fixed bias and sliding bias output as described herein provided to an analog amplifier such as a class B amplifier. The sliding bias can be provided in order to provide decreased power consumption as a result of a decrease in the bias during periods where a maximum bias is not required.



FIG. 5C shows an encoding of the fixed bias curve 250 of FIG. 5A, using pulse width modulation (PWM). Black bars illustrate time periods in which light is on, and white bars illustrate time periods in which light is off. In this example, a clock rate of 12.5 kHz is used, with minimum pulse width of 10 microseconds, allowing a pulse width variable from 0 to 80 microseconds in 10 microsecond increments. Higher clock rates and smaller minimum pulse widths than illustrated may be chosen to allow higher-resolution signal transmission.



FIG. 5D shows an encoding of the fixed bias curve 250 of FIG. 5A, using pulse density modulation (PDM). Black bars illustrate time periods in which light is on, and white bars illustrate time periods in which light is off. In this example, a clock rate of 100 kHz is used, corresponding to a minimum pulse width of 10 microseconds. Higher clock rates and smaller minimum pulse widths than illustrated may be chosen to allow higher-resolution signal transmission.



FIG. 5E shows an encoding of the sliding biased curve 255 of FIG. 5A, using PWM. Black bars illustrate time periods in which light is on, and white bars illustrate time periods in which light is off. In this example, a clock rate of 12.5 kHz is used, with minimum pulse width of 10 microseconds, allowing a pulse width variable from 0 to 80 microseconds in 10 microsecond increments. Higher clock rates and smaller minimum pulse widths than illustrated may be chosen to allow higher-resolution signal transmission. In comparison with FIG. 5C, the encoding of FIG. 5E has a lower duty cycle, as shown by the smaller amount of black signal, illustrating that less light power is needed to transmit the signal of sliding bias curve 255 than of fixed biased curve 250. The lower duty cycle provides substantially decreased power consumption.



FIG. 5F shows an encoding of the sliding biased curve 255 of FIG. 5A, using PDM. Black bars illustrate time periods in which light is on, and white bars illustrate time periods in which light is off. In this example, a clock rate of 100 kHz is used, corresponding to a minimum pulse width of 10 microseconds. Higher clock rates and smaller minimum pulse widths than illustrated may be chosen to allow higher-resolution signal transmission. In comparison with FIG. 5D, the encoding of FIG. 5F has a lower duty cycle, as shown by the smaller amount of black signal, illustrating that less light power is needed to transmit the signal of sliding bias curve 255 than of fixed biased curve 250. The decreased duty cycle and pulse density provides decreased power consumption.


The light source such as a laser may comprise the most significant source of power consumption with an optical hearing system, and the power drawn by the laser is often proportional to the signal offset. Therefore, applying a large sliding bias so that the signal comes close to clipping is helpful for reducing power consumption and extending battery life.


In some cases, when biasing a signal to reduce power consumption, it may be desirable, as discussed earlier, to adjust the signal gain dynamically, for example by peak limiting. Peak limiting may be useful to inhibit clipping. FIG. 6A shows amplitude of an input signal, such as a digital input signal, with sliding bias and peak limiting to inhibit clipping. An input signal 210 is shown in relation to input reference 205 corresponding to a peak-to-peak signal amplitude of 1.0 (arbitrary). The input reference 205 corresponds to a middle of the input signal range, and may correspond to an average value of a fixed bias input signal as described herein. The reference level 205 may correspond to 0 volts of an input such as a microphone as described herein, for example. The signal 210 comprises positive peaks 217 and a negative peak comprising trough 218 at signal amplitudes of about 0.5 and −0.5, respectively. Although reference is made to sine waves by wave of example, the embodiments disclosed herein are well suited with many types of input sound, including asymmetric sound having different positive and negative maximum intensities in relation to input reference 205.


As shown in FIG. 6A, a sliding bias of −0.6 units is applied to input signal 210, generating a sliding-biased signal 212 with peaks 217 at a signal levels of about −0.1 units. For a substantial of the portion of time 222, signal 212 is small enough that the sliding bias of −0.6 does not result in any clipping and the system gain may be maintained at a constant level. However, an increase in signal 212 may result in the negative peak being clipped absent a modification of the bias level and/or system gain. In the event that the increase in signal level happens faster than the bias can be increased without causing negative audio artifacts, the system gain may be dynamically adjusted, so that the trough 215 of the biased signal 212 is higher than the unadjusted trough 218. This gain adjustment ensures that clipping of the negative peaks does not occur and results in a signal 214 with a peak negative magnitude of no greater than −1.0. After reducing the system gain, the positive peak value 217 of the sliding biased curve is reduced as well, such that the sliding-biased curve has a lower peak to peak amplitude of about 0.8 units. Dynamically adjusting the biased signal in this manner inhibits negative clipping, thus decreasing distortion of the signal. Once the sliding bias is adjusted to a point where clipping no longer occurs, the system gain may be restored to its optimum value. The adjustment to the bias during time period 224 may be applied gradually, including over a period of multiple wavelengths, so that the bias remains substantially fixed when the system gain is reduced in order to inhibit user perceptible noise related to the change in bias. The processor may comprise instructions to decrease the gain over a duration no more than a length of a look ahead delay, such that bias remains substantially fixed to within about five percent (5%) over the length of the look ahead delay, for example.



FIG. 6B shows how a look-ahead delay may be employed to determine when a change in gain is needed. In FIG. 6B, a sliding-bias of approximately −0.6 units is applied to an input signal 210 to generate a sliding-biased signal 212. In the embodiment illustrated in FIG. 6B, the system has applied a look ahead delay 270 such that the output signal is delayed by a fixed period in order to modify that output in the event that the input signal changes in a manner which requires the output signal to be modified to maintain, for example, sound quality. The look-ahead delay as illustrated is about 0.5 ms, or about one quarter of a wavelength, but different look-ahead delays, including longer look-ahead delays of about 1 ms, about 2 ms, or longer than 2 ms may be chosen to provide more time to react to amplitude changes. The look-ahead delay 270 allows the generation of a prediction 216 of the value that the sliding-biased signal 212 is expected to take after the look-ahead delay. When the prediction 216 is measured to fall below a threshold value, resulting in a predicted clipping 271, a shift in signal gain is triggered. In some cases, the shift in signal gain may not immediately cause a significant change in the amplitude of the sliding-biased signal 212, but it may change the slope 272. Although the change in the sliding-biased signal may be gradual, the change in gain may cause a rapid change 273 in the predicted value 216, because the predicted value 216 reflects the accumulation of the effect of the shifted gain over the time period of the look-ahead delay 272. As a result, the sliding-biased signal 212 may be adjusted to inhibit clipping. The amount of gain adjustment can be determined in order to prevent the predicted curve 216 from clipping. The gain adjustment may be applied at different rates depending on the amount of look-ahead delay used. In some cases the gain may be adjusted gradually in response to a predicted clipping, for example in response to a growing area of predicted clipping 271. In such cases, the change 273 may be much more gradual than illustrated in FIG. 6B, and in some cases the change may be spread over much or all of the look-ahead delay 270, which may in some cases constitute one or more milliseconds, for example. This slower shift may have the benefit of inhibiting acoustic artifacts and distortions.


After a shift in gain, the amplitude of the sliding-biased signal will be reduced. To allow the amplitude to be restored without clipping, the sliding bias may be gradually adjusted. FIG. 6C shows the adjustment of a sliding bias over time. An input signal (not shown) with amplitude of about 0.5 is initially biased with a sliding bias 220 of about 0.6 in a negative direction to produce a sliding-biased curve 212. To inhibit clipping, the gain applied to sliding-biased curve 212 is reduced, resulting in an amplitude of about 0.4. In order to return to the correct value of amplitude, the sliding bias 220 is gradually adjusted from 0.6 to 0.5. During the same time, the gain is smoothly adjusted back up, increasing the amplitude of the signal along with the shift in bias. This smooth adjustment may keep the troughs of the sliding-biased curve 212 at or near a lower threshold value, allowing the signal amplitude to be increased without clipping. After the sliding bias 220 reaches about 0.5, and the gain has returned to normal, giving an amplitude 0.5, the adjustment stops and the gain and bias may remain constant until another change is appropriate as described herein. While FIG. 6C shows a linear change in bias over about 30 ms, in some cases the bias may be shifted nonlinearly and/or over shorter or longer timescales, for example to inhibit audio artifacts such as thumping.


Sliding Bias

The sliding bias as described herein applies a time-varying bias that adjusts to changes in the signal amplitude. When amplitude is low, the magnitude of the bias is increased to save power. The bias as described herein may comprise a negative number added to the signal, and the value of the bias can be decreased to save power with low energy input signals. When input sound amplitude is high, the magnitude of the bias is adjusted to inhibit clipping, for example by increasing the value of the bias to a less negative number. By dynamically varying the bias, power consumption can be significantly reduced and a high fidelity signal transmitted.


The methods and apparatus disclosed herein provide a signal processing algorithm for sliding bias that can be implemented in the digital signal processor (DSP) of an optical sound system. The processor embodies instructions of an algorithm that adjusts the bias by adding a time-varying offset to the digital signal before it is sent to the digital-to-analog converter (DAC). The digital to analog converter may comprise a digital to analog converter that converts a digital value to an output voltage. The digitally biased signal can be output from the DAC to an amplifier such as class B amplifier to drive the light sourced with an analog signal. Alternatively, the DAC may comprise delta sigma modulation circuitry. The output of the delta sigma modulation circuitry can be used to drive the light source with a digital signal, such as PWM or PDM, for example. The output of the sliding bias algorithm as disclosed herein may comprise the last element in the signal processing chain so that it provides output signal to the DAC to generate the light signal with appropriate amplification.


Signals can be represented in the DSP as fractional digital values in the range from −1 to +1, for example. The DAC comprising delta sigma modulation circuitry maps −1 to a pulse density of 0%, 0 to a pulse density of 50%, and +1 to a pulse density of 100%, for example. In many cases, the offset added by the sliding bias algorithm is in the range −1 to 0, in order to decrease power consumption.


The sliding bias algorithm as described herein is not limited to the modulation scheme that is used to represent the signal with light. The algorithm and circuitry as described herein are effective for analog, delta sigma modulation, PDM, pulse width modulation, and many other approaches, for example.


Inhibiting Sliding Bias Artifacts

The sliding bias algorithm as described herein has the advantage of significantly decreasing power consumption in order to prolong battery life. However, this advantage is preferably achieved without introducing audio artifacts. There are at least three types of artifacts which can be inhibited with the methods and apparatus as disclosed herein:


1. Clipping. If the bias is inadequate to accommodate the signal range at any moment, the signal may clip, producing potentially audible distortion which can be inhibited with adjustments to the signal gain.


2. Thumping. The time varying bias as described herein is a signal that is added to the input signal, and this signal is introduced in a manner that is substantially inaudible. If the bias is shifted too rapidly, it approaches a step function and may become audible. This rapid change in bias can be referred to as “thumping”. Because a step function comprises a predominantly low-frequency signal, the user can perceive a rapid change in bias as a thump. Work in relation to embodiments suggests that the low-frequency rolloff of the output transducer assembly that receives transmitted optical power and signal, such as the tympanic membrane transducer assembly, may help to reduce the audibility of the bias shift. A person of ordinary skill in the art can conduct experiments to determine times over which the bias can be adjusted in order to inhibit user perceptible thumping in accordance with embodiments disclosed herein.


3. Noise. Due to nonlinearities of one or more of the DAC, laser driver circuitry, laser, or other components, user perceptible noise could potentially be introduced. The sliding bias as disclosed herein can be configured to inhibit noise that might otherwise be present with a low amplitude signal. For example, the noise may rise slightly as sliding bias approaches the lower end of the input range, for example below about −0.9. The algorithm can optionally limit the sliding bias values to a predetermined minimum amount, for example no lower than about −0.9. Work in relation to embodiments suggests that suitable delta sigma modulation circuitry can be provided that does not introduce distortion with low amplitude signals, and limiting of the sliding bias as described herein may not be helpful in at least some embodiments.


Peak Limiting

The circuitry as disclosed herein can be configured to inhibit clipping without producing audible thumping. Peak limiting as disclosed herein can be used to inhibit clipping with adjustments to the gain.


Clipping may occur if a high-amplitude signal arrives when the bias is low. In order to inhibit clipping, a look ahead delay can be provided in order to shift the bias up in advance of the arrival of the high-amplitude signal. However, the look ahead delay may not provide sufficient time to adjust the bias for a rapidly decreasing signal, and peak limiting can be provided to inhibit clipping of rapidly decreasing signals.


With a rapidly changing signal, the length of the look ahead delay may not be sufficient to allow the bias to change slowly in order to inhibit a user perceptible thump. Work in relation to embodiments suggests that a full-range bias shift applied over a duration of less than about 20-50 ms may produce an audible thump. Therefore, peak limiting can be employed to inhibit clipping while allowing the bias to be changed sufficiently slowly to inhibit thumping.


Limitations of the look ahead delay can be overcome by providing peak limiting with the sliding bias algorithm. An approach to peak limiting is to apply a rapid gain reduction just before the peak and to restore the gain just after the peak, for example as shown above with reference FIGS. 4C and 6. The advantages of combining peak limiting and sliding bias are that a rapid gain change is less likely to create a user perceivable artifact, and peak limiting allows a shorter look ahead delay to be used with the sliding bias.


The sliding bias and peak limiting algorithms can be combined in many ways. A short look ahead delay of a few milliseconds can used to identify a peak that would otherwise be clipped by the low bias and initiate the rapid gain reduction that is helpful to limit the peak sufficiently to inhibit clipping. At about the same time, a slow bias increase can be initiated to accommodate higher positive and negative peaks of the input signal. The gain may then be slowly increased as the bias increases, until full gain is restored. Alternatively or in combination, the gain may be rapidly restored in response to a negative signal rising above a threshold as described herein, depending on the amplitude of the input signal and how rapidly the input signal changes.


Although peak limiting may be considered a form of artifact, peak limiting combined with the sliding is likely to less likely to be apparent to the user than clipping. The digital peak limiting on the lower peak, has the advantage of being less perceivable and can produce less artifact than rapidly increasing the bias, for example.


Implementation of the Algorithm
Bias Calculation and Updating

In many implementations, the sliding bias algorithm operates by tracking the negative-going peak of the signal and applying a bias that is as negative as possible without causing the negative-going signal peak to drop below the clipping level of −1. If the negative-going signal peak is M, the most negative bias that can be applied is −1−M.


Several additional constraints may be imposed on the bias value:






    • An extra margin against clipping may be imposed. This is an algorithm parameter ε, referred to as the “bias margin”. With the margin imposed, the most negative bias is ε−1−M rather than −1−M. Work in relation to embodiments suggests that a bias margin within a range from about 0.05 to about 0.15, for example 0.1, can be useful for decreasing distortion. A bias margin can be similarly employed with analog systems and delta sigma modulation systems, for example.

    • A lower boundary may be imposed on the range of the bias value. This lower bound is an algorithm parameter Bmin, referred to as the “most negative allowed bias”. The most negative allowed bias can be used to avoid bias values that unacceptably elevate the noise floor.

    • An upper bound at the middle of the input signal range, such as 0, can be imposed on the range of the bias value, in order to prevent the bias margin from pushing the bias into positive territory.





In many implementations, the algorithm uses a linear trajectory to shift the bias, although non-linear trajectories can be used. The term “attack” refers to shifting the bias up to prevent clipping when the signal amplitude rises, and the term “release” refers to shifting the bias down to save power when the signal amplitude falls. The slopes of the linear trajectories can be determined by algorithm parameters SBSA (sliding bias attack slope) and SBSR (sliding bias release slope), both specified in units of samples−1.


In many implementations, the algorithm has three bias-related state variables:

    • The “current bias” (BC) is the bias value that is being applied at any instant.
    • The “target bias” (BT) is the endpoint of the bias-shifting trajectory.
    • The “sliding bias mode” (SBMode) is the mode of operation, which may be Attack, Release, or Steady. In Attack mode, the bias is shifting up. In Release mode, the bias is shifting down. In Steady mode, the bias is held steady for a period of time while the negative-going peak of the signal is monitored. The duration of Steady mode is an algorithm parameter D, referred to as the “steady duration”, in samples.


The algorithm can be initialized as follows:

    • BC=0
    • BT=−1
    • SBMode=Steady


While in Steady mode, the algorithm monitors the signal and sets BT=ε−1−M, where M is the most negative observed signal value. BT is constrained to the range from Bmin to 0.


Steady mode is exited if either of the following conditions occur:

    • If the steady duration D is exhausted, Release mode is entered.
    • If BT>BC, Attack mode is entered.


While in Attack mode, BC is incremented by SBSA until it reaches BT, at which point Steady mode is entered. During this process, BT is updated if a signal value is observed that requires BT to be set to a higher value.


While in Release mode, BC is decremented by SBSR until it reaches BT, at which point Steady mode is entered. During this process, if a signal value is observed that requires BT>BC, Attack mode is entered.


Peak Limiting

The peak limiting algorithm may begin by calculating a peak limiting threshold, which is the largest negative-going peak signal magnitude in dB in relation to full-scale that can be accommodated by the current bias value BC without clipping. The peak limiting threshold is defined as T=20 log10(BC+1). The integration between the sliding bias and peak limiting algorithms is configured such that the peak limiting threshold depends on the current bias value.


Next, the algorithm calculates the amount in dB by which the negative-going peak signal magnitude exceeds the peak limiting threshold. If M is the negative-going signal peak, then the exceedance may be calculated as E=20 log10(−M)−T. E is set to 0 if M≥0, and E is constrained to be ≥0 to prevent negative exceedance.


Finally, the algorithm applies a time-varying gain as required to compensate for exceedance and prevent clipping. When exceedance occurs (i.e., E>0), the gain is gradually reduced to −E dB before the peak and gradually restored. A look ahead delay is employed to detect exceedance in advance so that the gain change can be initiated in time to prevent clipping. The look ahead delay is an algorithm parameter Δ (also referred to herein as “look ahead time delay”), in samples.


The gain change trajectory may be linear in dB. Within the peak limiting algorithm, the term “attack” refers to reducing the gain and “release” refers to increasing the gain. The slopes of the gain trajectories can be determined by algorithm parameters PLSA (peak limiting attack slope) and PLSR (peak limiting release slope), both specified in units of dB/sample.


The algorithm has three peak-limiting-related state variables:

    • The “current gain” (GC) is the gain value that is being applied at any instant.
    • The “target gain” (GT) is the endpoint of the gain-shifting trajectory.
    • The “peak limiting mode” (PLMode) is the mode of operation, which may be Attack, Release, or Steady. In Attack mode, the gain is falling. In Release mode, the gain is rising. In Steady mode, the gain is held steady for a period of time while the exceedance is monitored. The duration of Steady mode is the look ahead delay Δ.


The algorithm is initialized as follows:

    • GC=0
    • GT=0
    • PLMode=Steady


While in Steady mode, the algorithm monitors the exceedance E and sets GT=−E. Steady mode is exited if either of the following conditions occurs:

    • If the time spent in Steady mode exceeds the look ahead delay Δ, Release mode is entered.
    • If GT<GC, Attack mode is entered.


While in Attack mode, GC is decremented by PLSA until it reaches GT, at which point Steady mode is entered. During this process, GT is updated if an exceedance is observed that requires GT to be set to a lower value.


While in Release mode, GC is incremented by PLSR until it reaches GT, at which point Steady mode is entered. During this process, if an exceedance is observed that requires GT<GC, Attack mode is entered.


Parameter Selection

While the parameters can be selected in many ways and may comprise many values, this section provides non-limiting examples of considerations for selecting values of the algorithm parameters.


In the following, R represents the system sampling rate, in Hz.


The algorithm parameters are summarized in the following table.

















Parameter
Symbol
Units









Bias margin
ε
unitless



Most negative allowed bias
Bmin
unitless



Sliding bias steady mode duration
D
samples



Sliding bias attack slope
SBSA
samples−1



Sliding bias release slope
SBSR
samples−1



Peak limiting attack slope
PLSA
dB/sample



Peak limiting release slope
PLSR
dB/sample



Look ahead delay
Δ
samples










Ideally, ε should be set to 0 to substantially decrease power consumption. However, setting the bias so low that negative-going peaks are at the digital rail can produce distortion, possibly related to the noise floor and associated circuitry as disclosed herein. The value for ε should be set to the minimum value that prevents such distortion. Work in relation to embodiments suggests that ε with in a range from about 0.05 to about 0.2, for example equal to 0.1 can provide acceptable results. A distortion analysis can be performed by a person of ordinary skill in the art in order to choose an appropriate value.


Bmin can be set as negative as possible, to substantially decrease power consumption, but high enough to substantially avoid bias values that unacceptably elevate noise. A system noise analysis can be performed by a person of ordinary skill in the art in order to choose an appropriate value.


The parameter D can be chosen to provide an acceptable tradeoff between power consumption and artifacts. Smaller values of D reduce power consumption by allowing the bias to shift down more quickly in response to a drop in signal amplitude. Larger values of D reduce the rate of occurrence of clipping and/or peak-limiting artifacts, because the bias will be shifted down after the signal amplitude has been low for a longer duration, which reduces the likelihood of incorrectly concluding that the signal amplitude has actually decreased. Suitable values are in the range from 1 to 10 seconds, which corresponds to a range from R to 10R samples.


SBSR should be set fast enough to substantially decrease power consumption and slow enough to substantially inhibit user perceptible thumping. A suitable value is 1/(0.5R) samples−1, which implements a full-range bias shift over the course of 500 ms, for example.


Choosing SBSA can result a tradeoff between different types of artifacts. Faster values of SBSA allow a faster response to signal amplitude increase, which substantially decreases clipping and peak-limiting artifacts, but slower values of SBSA decrease thumping. A suitable value is 1/(0.05R) samples−1, which implements a full-range bias shift over the course of 50 ms, for example.


The peak-limiting slopes PLSA and PLSR can be chosen with a tradeoff between different types of artifacts. Fast slopes substantially decrease envelope distortion by making the gain change more time-limited, but excessively fast slopes may introduce spectral distortion. In addition, there is an interaction among PLSA, Bmin, and Δ. To inhibit clipping, the following relationship can be considered:

PLSA≥−20 log10(Bmin+1)/α


This constraint can allow the attack slope to increase fast enough to respond to the worst-case exceedance condition within the look ahead delay. If the system noise analysis yields a choice of Bmin=−0.5, and a look ahead delay of 2 ms is acceptable, an attack slope of at least 3 dB/ms=3000/R dB/sample can be provided to inhibit clipping. The release slope is not critical for preventing clipping, so the release slope can be slower to inhibit spectral distortion. A suitable value might be 1 dB/ms=1000/R dB/sample, for example.


Additional Description of the Algorithm

The algorithm can be block-oriented for efficiency and for compatibility with the block-based architecture of commercially available DSP systems. L is the block length, in samples. The look ahead delay is constrained to be an integral number of blocks. The symbol K can be used to represent the look ahead delay in blocks; hence α=KL.


The algorithm receives a block of input samples, x[i:i+L−1], and produces a block of output samples, y[i:i+L−1], where i is the starting sample number of the current block. The algorithm proceeds in three sections:

    • 1. The pre block loop section analyzes the input block, sets the sliding bias mode and target bias, and sets the peak limiting mode and target gain. The pre-block-loop section is described in further detail below with reference to method 300 and method 400 of FIG. 7.
    • 2. The block loop applies the time-varying bias and gain to the input block to produce the output block. The block loop is described in further detail below with reference to method 500 and method 600 of FIG. 7.
    • 3. The post block loop section checks for termination of the bias and gain trajectories and resets state variables accordingly. The post block loop section is described in further detail below with reference to method 700 and 800 of FIG. 7


The following table shows the state variables used in the algorithm and their initial values.















Parameter
Symbol
Units
Initial Value







Sliding bias mode
SBMode
Steady, Attack,
Steady




or Release


Peak limiting mode
PLMode
Steady, Attack,
Steady




or Release


Sliding bias steady counter
SBCtr
samples
D


Peak limiting steady counter
PLCtr
samples
KL


Target bias
BT
unitless
−1


Current bias
BC
unitless
0


Target peak limiting gain
GT
dB
0


Current peak limiting gain
GC
dB
0










FIG. 7 shows a method 900 of implementing an adjustable bias and peak limiting, in accordance with embodiments. The method 900 may comprise one or more of a plurality of methods, such as one or more of a method 300, a method 400, a method 500, a method 600, a method 700 or a method 800, for example.


The method 900 may comprise one or more of the following parameters:


Signals:

    • x[i]=input at sample i, range [−1, +1]
    • y[i]=output at sample i, range [−1, +1]


Parameters:

    • L=input/output block length, samples
    • K=look ahead delay, blocks
    • D=sliding bias steady mode duration, samples
    • SBSA=sliding bias attack slope, samples−1
    • SBSR=sliding bias release slope, samples−1
    • PLSA=peak limiting attack slope, dB/sample
    • PLSR=peak limiting release slope, dB/sample
    • ε=bias margin (unitless)
    • Bmin=most negative allowed bias (unitless)


State Variables:

    • SBMode=sliding bias mode (Steady, Attack, or Release)
    • PLMode=peak limiting mode (Steady, Attack, or Release)
    • SBCtr=sliding bias steady counter, samples
    • PLCtr=peak limiting steady counter, samples
    • BT=target bias (unitless)
    • BC=current bias (unitless)
    • GT=target peak limiting gain, dB
    • GC=current peak limiting gain, dB
    • i=starting sample number of current block


Initialization of State Variables:

    • SBMode=Steady
    • PLMode=Steady
    • SBCtr=D
    • PLCtr=K×L
    • BT=−1
    • BC=0
    • GT=0
    • GC=0
    • i=0


Method 300 comprises analyzing input signals of a system to determine whether a signal bias can be shifted and clipping inhibited, in accordance with embodiments.


At a step 302, a block of incoming signal is provided. The signal block may comprise signal from one or more auditory inputs as described herein.


At a step 304, the minimum value, M, of the incoming signal of the block is determined.


At a step 306, the most negative bias, B, that can be applied to the block without clipping any troughs of the input is determined.


At a step 308, the values of B and a target bias, BT, are compared.


At a step 310, if the value of BT is less than the value of B, then the value of BT is set to equal the value of B.


At a step 311, the value of BT is compared to the value of BC.


At a step 312, if the value of BT is greater than BC, then a signal bias mode (hereinafter “SBMode”), is set to “Attack.”


Steps 308, 310, 311, and 312 disclose a method of setting the SBMode to “attack” when the bias should be increased in order to account for deeper troughs in the signal, so as to inhibit clipping.


At a step 314, the value of SBMode is compared to “steady.”


At a step 316, if the value of SBMode is equal to “steady,” a counter with a defined interval or cycle is decremented.


At a step 317, the value of the counter is compared to zero.


At a step 318, if the counter is less than or equal to zero, then the SBMode is set to “release.”


Steps 314, 316, 317, and 318 disclose a method of setting SBMode to “release” when, after a defined period as determined by the counter, no peaks were clipped.


A method 400 comprises analyzing input signals of a system to determine whether or not the gain should be adjusted to limit peaks in order to inhibit clipping, in accordance with embodiments.


At a step 402, a threshold T for the peak limiting algorithm disclosed herein is determined, comprising a formula that includes the value of BC from method 300.


At a step 403, the value of M, the minimum value of the incoming signal of the block of step 302, is compared to 0.


At a step 404, if M is less than 0, then an exceedance E is determined, representing the number of decibels a signal trough goes below the threshold, if at all.


At a step 406, if M is not less than 0, then E is set to equal 0.


At a step 407, the value of −1 multiplied by E is compared to a target peak limiting gain, GT.


At a step 408, if −1 multiplied by E is less than GT, then GT is set to equal −1 multiplied by E.


At a step 409, the value of GT is compared to the value of the current gain of the system, GC.


At a step 410, if GT is less than GC, the peak limiting mode (hereinafter “PLMode”), is set to “attack.”


Steps 407, 408, 409, and 410 disclose a method of setting the peak limiting mode to “attack” in order to adjust for troughs that may be clipped.


At a step 412, the value of PLMode is compared to “steady.”


At a step 414, if the value of PLMode is equal to “steady,” a counter with a defined interval or cycle is decremented.


At a step 415, the value of the counter is compared to 0.


At a step 416, once the counter has been exhausted, PLMode is set to “release.”


At a step 418, the PLMode and the SBMode of method 300 is passed on to a subsequent block loop method.


Steps 412, 414, 415, and 416 disclose a method of setting the peak limiting mode to “release” when, after a given period as determined by the counter, no peaks have been clipped.


Method 500 comprises changing the signal bias and inhibiting clipping, in accordance with embodiments. Method 500 comprises a block loop method that may accept outputs from method 300.


At a step 502, a loop is initiated.


At a step 503, the state of SBmode is determined. At step 503, the state variable SBMode comprises an input from the outputs of method 300, for example. The SBMode may comprise states “attack” and “release”, for example.


At a step 504, if SBMode is set to “attack,” then BC will be set to the smaller value of either BC plus a sliding bias attack mode slope, or BT.


At a step 505, the state of SBMode is determined.


At a step 506, if SBMode is set to “release,” then BC will be set to the larger value of either BC minus a sliding bias release mode slope, or BT.


At a step 508, the loop executes until any loop conditions are satisfied. For example, such loop conditions may comprise exhaustion of a counter.


Method 600 comprises changing the gain of a system in order to inhibit clipping, in accordance with embodiments. Method comprises a block loop method that may accept outputs from method 400.


At a step 602, a loop is initiated.


At step 603, the state of PLMode is determined. At step 603, the state variable PLMode comprises an input from the outputs of embodiments such as those of method 400. For example, PLMode may comprise states “attack” and “release.”


At a step 604, if PLMode is set to “attack,” then GC will be set to the larger value of either GC minus a peak limiting attack mode slope, or GT.


At a step 605, the state of PLMode is determined.


At a step 606, if PLMode is set to “release,” then GC will be set to the smaller value of either GC minus a peak limiting release mode slope, or GT.


At a step 608, an output sample—comprising an equation comprising variables such as GC, a look ahead time delay, and a current bias—is determined.


At a step 610, the loop executes until any loop conditions are satisfied. For example, such loop conditions may comprise exhaustion of a counter.


A method 700 comprises updating the sliding bias mode as appropriate, in accordance with embodiments. Method 700 comprises accepting outputs from methods such as method 500.


At a step 701, the value of BC is compared to the value of BT, and the value of SBMode is determined.


At a step 702, if BC is equal to BT and SBMode is not set to “steady, then SBMode will be set to “steady” for a defined amount of time. State variables, such as BT, are also initialized.


At a step 704, the method terminates.


A method 800 comprises updating the peak limiting mode as appropriate, in accordance with embodiments. Method 800 comprises accepting outputs from methods such as method 600.


At a step 801, the value of GC is compared to the value of GT, and the value of PLMode is determined.


At a step 802, if GC is equal to GT, and PLMode is not set to “steady, then PLMode will be set to “steady” for a given amount of time. State variables, such as GT, are also initialized.


At a step 804, the algorithm terminates.


The method 900 discloses a method of adjusting a bias and limiting peaks, in accordance with embodiments. A person of ordinary skill in the art will recognize many variations and modifications based on the disclosure provided herein. For example, some steps may be added or removed. The steps can be combined, or the order changed. Some of the methods may comprise sub-methods. Some of the steps may comprise sub-steps, and many of the steps can be repeated.


The values of method 900 can be determined with one or more of calculations, look up tables, fuzzy logic, or neural networks, for example.


The method 900 can be embodied with instructions stored on a tangible medium of processor 170. The processor can be coupled to components of the system in order to perform one or more steps of method 900.


Examples of ranges of parameters suitable for use with method 900 may comprise one or more of the following, where R is the sampling rate of the system:

    • K (look ahead delay), within a range from about 0.0001R/L to about 0.01R/L
    • D (sliding bias steady mode duration), within a range from about 0.5R to about 2R
    • SBSA (sliding bias attack slope), within a range from about 1/(0.01R) to about 1/(0.9R)
    • SBSR (sliding bias release slope), within a range from about 1/(0.1R) to about 1/(0.9R)
    • PLSA (peak limiting attack slope), within a range from about 1000/R to about 9000/R
    • PLSR (peak limiting release slope), within a range from about 100/R to about 10000/R
    • ε (bias margin), within a range from about 0.05 to about 0.3
    • Bmin (most negative allowed bias), within a range from about −0.5 to about −1.0


While preferred embodiments of the present disclosure have been shown and described herein, it will be obvious to those skilled in the art that such embodiments are provided by way of example only. Numerous variations, changes, and substitutions will be apparent to those skilled in the art without departing from the scope of the present disclosure. It should be understood that various alternatives to the embodiments of the present disclosure described herein may be employed without departing from the scope of the present invention. Therefore, the scope of the present invention shall be defined solely by the scope of the appended claims and the equivalents thereof.

Claims
  • 1. A hearing apparatus to transmit an audio signal to an ear of a user, the apparatus comprising: an input to receive the audio signal;a source of electromagnetic energy to generate an electromagnetic signal;an output transducer to receive the electromagnetic signal from the source of electromagnetic energy; anda processor coupled to the input, the processor configured with instructions to receive the audio signal,determine a bias of the audio signal and a biased audio signal in response to the audio signal, andoutput the biased audio signal to circuitry to drive the source of electromagnetic energy with the biased signal in order to decrease energy of the electromagnetic signal transmitted from the source of electromagnetic energy,wherein the processor comprises instructions for a look ahead delay to decrease the gain to inhibit clipping in response to a negative signal below a threshold amount detected with the look ahead delay.
  • 2. An apparatus as in claim 1, wherein the processor comprises instructions to adjust the bias to decrease the energy of the electromagnetic signal in response to decreased energy of the audio signal and to adjust the bias to increase the energy of the electromagnetic signal in response to increased energy of the audio signal in order to inhibit distortion.
  • 3. An apparatus as in claim 2, wherein the processor comprises instructions to adjust the bias in a direction corresponding to negative sound pressure in response to decreased amounts of negative sound pressure of the audio signal.
  • 4. An apparatus as in claim 2, wherein the processor comprises instructions to adjust the bias to decrease amounts of the energy of the electromagnetic signal at a first rate and to increase amounts of the energy of the electromagnetic signal at a second rate to inhibit distortion, the first rate slower than the second rate.
  • 5. An apparatus as in claim 2, wherein the processor comprises instructions to adjust the bias over a time duration of more than about 50 ms in order to inhibit an audible thump.
  • 6. An apparatus as in claim 2, wherein the processor comprises instructions to adjust the bias over a time duration of more than about 20 ms in order to inhibit an audible thump.
  • 7. An apparatus as in claim 1, wherein the processor comprises instructions to adjust the biased signal to more positive values in response to the negative signal below the threshold amount and to increase the gain when the biased signal is adjusted to the more positive values.
  • 8. An apparatus as in claim 1, wherein the negative signal corresponds to negative sound pressure and the threshold amount comprises a lower end of the input range.
  • 9. An apparatus as in claim 8, wherein the processor comprises instructions to decrease the gain faster than a change in bias and wherein the bias remains substantially fixed when the gain is decreased in response to the signal below the threshold.
  • 10. An apparatus as in claim 9, wherein the processor comprises instructions to decrease the gain over a duration no more than a length of the look ahead delay and wherein the bias remains substantially fixed to within about five percent (5%) over the length of the look ahead delay.
  • 11. An apparatus as in claim 1, wherein the processor comprises instructions to limit the bias in response to a noise floor associated with one or more of delta sigma modulation circuitry, the circuitry to drive the source of electromagnetic energy, the source of the electromagnetic energy, or the output transducer to receive the output signal.
  • 12. An apparatus as in claim 1, wherein the audio signal comprises a fixed bias and the processor comprises instructions to determine the biased audio signal in response to the fixed bias of the audio signal.
  • 13. An apparatus as in claim 1, wherein the circuitry to drive the source of electromagnetic energy comprises delta sigma modulation circuitry.
  • 14. An apparatus as in claim 13, wherein the delta modulation circuitry comprises one or more of pulse width modulation circuitry, pulse density modulation circuitry, or a digital to analog converter of the processor comprising the pulse density modulation circuitry.
  • 15. An apparatus as in claim 1, wherein the circuitry to drive the source of electromagnetic energy comprises an analog amplifier.
  • 16. A hearing apparatus to transmit an audio signal to an ear of a user, the apparatus comprising: an input to receive the audio signal;a source of electromagnetic energy to generate an electromagnetic signal;an output transducer to receive the electromagnetic signal from the source of electromagnetic energy; anda processor coupled to the input, the processor configured with instructions to receive the audio signal,determine a bias of the audio signal and a biased audio signal in response to the audio signal, andoutput the biased audio signal to circuitry to drive the source of electromagnetic energy with the biased signal in order to decrease electromagnetic energy of the electromagnetic signal transmitted from the source of electromagnetic energy,wherein the processor comprises instructions to limit the bias in response to a noise floor associated with one or more of delta sigma modulation circuitry, the circuitry to drive the source of electromagnetic energy, the source of electromagnetic energy or the output transducer to receive the output signal.
  • 17. An apparatus as in claim 16, wherein the processor comprises instructions to adjust the bias to decrease electromagnetic energy in response to decreased energy of the audio signal and to adjust the bias to increase electromagnetic energy in response to increased energy of the audio signal in order to inhibit distortion.
  • 18. An apparatus as in claim 17, wherein the processor comprises instructions to adjust the bias in a direction corresponding to negative sound pressure in response to decreased amounts of negative sound pressure of the audio signal.
  • 19. An apparatus as in claim 17, wherein the processor comprises instructions to adjust the bias to decrease amounts of electromagnetic energy at a first rate and to increase amounts of electromagnetic energy at a second rate to inhibit distortion, the first rate slower than the second rate.
  • 20. An apparatus as in claim 17, wherein the processor comprises instructions to adjust the bias over a time duration of more than about 50 ms in order to inhibit an audible thump.
  • 21. An apparatus as in claim 17, wherein the processor comprises instructions to adjust the bias over a time duration of more than about 20 ms in order to inhibit an audible thump.
  • 22. An apparatus as in claim 16, wherein the processor comprises instructions for a look ahead delay to decrease the gain to inhibit clipping in response to a negative signal below a threshold amount detected with the look ahead delay.
  • 23. An apparatus as in claim 22, wherein the processor comprises instructions to adjust the biased signal to more positive values in response to the negative signal below the threshold amount and to increase the gain when the biased signal is adjusted to the more positive values.
  • 24. An apparatus as in claim 22, wherein the negative signal corresponds to negative sound pressure and the threshold amount comprises a lower end of the input range.
  • 25. An apparatus as in claim 24, wherein the processor comprises instructions to decrease the gain faster than a change in bias and wherein the bias remains substantially fixed when the gain is decreased in response to the signal below the threshold.
  • 26. An apparatus as in claim 25, wherein the processor comprises instructions to decrease the gain over a duration no more than a length of the look ahead delay and wherein the bias remains substantially fixed to within about five percent (5%) over the length of the look ahead delay.
  • 27. An apparatus as in claim 16, wherein the audio signal comprises a fixed bias and the processor comprises instructions to determine the biased audio signal in response to the fixed bias of the audio signal.
  • 28. An apparatus as in claim 16, wherein the circuitry to drive the source of electromagnetic energy comprises delta sigma modulation circuitry.
  • 29. An apparatus as in claim 28, wherein the delta modulation circuitry comprises one or more of pulse width modulation circuitry, pulse density modulation circuitry, or a digital to analog converter of the processor comprising the pulse density modulation circuitry.
  • 30. An apparatus as in claim 16, wherein the circuitry to drive the source of electromagnetic energy comprises an analog amplifier.
  • 31. A hearing apparatus to transmit an audio signal to an ear of a user, the apparatus comprising: an input to receive the audio signal;a source of electromagnetic energy to generate an electromagnetic signal;an output transducer to receive the electromagnetic signal from the source of electromagnetic energy; anda processor coupled to the input, the processor configured with instructions to receive the audio signal,determine a bias of the audio signal and a biased audio signal in response to the audio signal, andoutput the biased audio signal to circuitry to drive the source of electromagnetic energy with the biased signal in order to decrease electromagnetic energy of the electromagnetic signal transmitted from the electromagnetic source,wherein the audio signal comprises a fixed bias and the processor comprises instructions to determine the biased audio signal in response to the fixed bias of the audio signal.
  • 32. An apparatus as in claim 31, wherein the processor comprises instructions to adjust the bias to decrease electromagnetic energy in response to decreased energy of the audio signal and to adjust the bias to increase electromagnetic energy in response to increased energy of the audio signal in order to inhibit distortion.
  • 33. An apparatus as in claim 32, wherein the processor comprises instructions to adjust the bias in a direction corresponding to negative sound pressure in response to decreased amounts of negative sound pressure of the audio signal.
  • 34. An apparatus as in claim 32, wherein the processor comprises instructions to adjust the bias to decrease amounts of electromagnetic energy at a first rate and to increase amounts of electromagnetic energy at a second rate to inhibit distortion, the first rate slower than the second rate.
  • 35. An apparatus as in claim 32, wherein the processor comprises instructions to adjust the bias over a time duration of more than about 50 ms in order to inhibit an audible thump.
  • 36. An apparatus as in claim 32, wherein the processor comprises instructions to adjust the bias over a time duration of more than about 20 ms in order to inhibit an audible thump.
  • 37. An apparatus as in claim 31, wherein the processor comprises instructions for a look ahead delay to decrease the gain to inhibit clipping in response to a negative signal below a threshold amount detected with the look ahead delay.
  • 38. An apparatus as in claim 37, wherein the processor comprises instructions to adjust the biased signal to more positive values in response to the negative signal below the threshold amount and to increase the gain when the biased signal is adjusted to the more positive values.
  • 39. An apparatus as in claim 37, wherein the negative signal corresponds to negative sound pressure and the threshold amount comprises a lower end of the input range.
  • 40. An apparatus as in claim 39, wherein the processor comprises instructions to decrease the gain faster than a change in bias and wherein the bias remains substantially fixed when the gain is decreased in response to the signal below the threshold.
  • 41. An apparatus as in claim 40, wherein the processor comprises instructions to decrease the gain over a duration no more than a length of the look ahead delay and wherein the bias remains substantially fixed to within about five percent (5%) over the length of the look ahead delay.
  • 42. An apparatus as in claim 31, wherein the processor comprises instructions to limit the bias in response to a noise floor associated with one or more of delta sigma modulation circuitry, the circuitry to drive the source of electromagnetic energy, the source of electromagnetic energy or the output transducer to receive the output signal.
  • 43. An apparatus as in claim 31, wherein the circuitry to drive the source of electromagnetic energy comprises delta sigma modulation circuitry.
  • 44. An apparatus as in claim 43, wherein the delta modulation circuitry comprises one or more of pulse width modulation circuitry, pulse density modulation circuitry, or a digital to analog converter of the processor comprising the pulse density modulation circuitry.
  • 45. An apparatus as in claim 31, wherein the circuitry to drive the source of electromagnetic energy comprises an analog amplifier.
CROSS-REFERENCE

The present patent application is a continuation of U.S. Patent Application No. 15,890,185, filed Feb. 6, 2018, now U.S. Pat. No. 10,531,206; which is a continuation of U.S. patent application Ser. No. 14/813,301, filed Jul. 30, 2015, now U.S. Pat. No. 9,930,458; which is a continuation of PCT Application No. PCT/US15/40397, filed Jul. 14, 2015; which claims priority to U.S. Provisional Patent Application No. 62/024,275, filed Jul. 14, 2014; the entire disclosures of which are incorporated herein by reference.

US Referenced Citations (713)
Number Name Date Kind
2763334 Starkey Sep 1956 A
3209082 McCarrell et al. Sep 1965 A
3229049 Goldberg Jan 1966 A
3440314 Frisch Apr 1969 A
3449768 Doyle Jun 1969 A
3526949 Genovese Sep 1970 A
3549818 Turner Dec 1970 A
3585416 Mellen Jun 1971 A
3594514 Wingrove Jul 1971 A
3710399 Hurst Jan 1973 A
3712962 Epley Jan 1973 A
3764748 Branch et al. Oct 1973 A
3808179 Gaylord Apr 1974 A
3870832 Fredrickson Mar 1975 A
3882285 Nunley et al. May 1975 A
3965430 Brandt Jun 1976 A
3985977 Beaty et al. Oct 1976 A
4002897 Kleinman et al. Jan 1977 A
4031318 Pitre Jun 1977 A
4061972 Burgess Dec 1977 A
4075042 Das Feb 1978 A
4098277 Mendell Jul 1978 A
4109116 Victoreen Aug 1978 A
4120570 Gaylord Oct 1978 A
4207441 Chouard et al. Jun 1980 A
4248899 Lyon et al. Feb 1981 A
4252440 Frosch et al. Feb 1981 A
4281419 Treace Aug 1981 A
4303772 Novicky Dec 1981 A
4319359 Wolf Mar 1982 A
4334315 Ono et al. Jun 1982 A
4334321 Edelman Jun 1982 A
4338929 Lundin et al. Jul 1982 A
4339954 Anson et al. Jul 1982 A
4357497 Hochmair et al. Nov 1982 A
4375016 Harada Feb 1983 A
4380689 Giannetti Apr 1983 A
4428377 Zollner et al. Jan 1984 A
4524294 Brody Jun 1985 A
4540761 Kawamura et al. Sep 1985 A
4556122 Goode Dec 1985 A
4592087 Killion May 1986 A
4606329 Hough Aug 1986 A
4611598 Hortmann et al. Sep 1986 A
4628907 Epley Dec 1986 A
4641377 Rush et al. Feb 1987 A
4652414 Schlaegel Mar 1987 A
4654554 Kishi Mar 1987 A
4689819 Killion Aug 1987 A
4696287 Hortmann et al. Sep 1987 A
4729366 Schaefer Mar 1988 A
4741339 Harrison et al. May 1988 A
4742499 Butler May 1988 A
4756312 Epley Jul 1988 A
4759070 Voroba et al. Jul 1988 A
4766607 Feldman Aug 1988 A
4774933 Hough et al. Oct 1988 A
4776322 Hough et al. Oct 1988 A
4782818 Mori Nov 1988 A
4800884 Heide et al. Jan 1989 A
4800982 Carlson Jan 1989 A
4817607 Tatge Apr 1989 A
4840178 Heide et al. Jun 1989 A
4845755 Busch et al. Jul 1989 A
4865035 Mori Sep 1989 A
4870688 Voroba et al. Sep 1989 A
4918745 Hutchison Apr 1990 A
4932405 Peeters et al. Jun 1990 A
4936305 Ashtiani et al. Jun 1990 A
4944301 Widin et al. Jul 1990 A
4948855 Novicky Aug 1990 A
4957478 Maniglia et al. Sep 1990 A
4963963 Dorman Oct 1990 A
4982434 Lenhardt et al. Jan 1991 A
4999819 Newnham et al. Mar 1991 A
5003608 Carlson Mar 1991 A
5012520 Steeger Apr 1991 A
5015224 Maniglia May 1991 A
5015225 Hough et al. May 1991 A
5031219 Ward et al. Jul 1991 A
5061282 Jacobs Oct 1991 A
5066091 Stoy et al. Nov 1991 A
5068902 Ward Nov 1991 A
5094108 Kim et al. Mar 1992 A
5117461 Moseley May 1992 A
5142186 Cross et al. Aug 1992 A
5163957 Sade et al. Nov 1992 A
5167235 Seacord et al. Dec 1992 A
5201007 Ward et al. Apr 1993 A
5220612 Tibbei et al. Jun 1993 A
5259032 Perkins et al. Nov 1993 A
5272757 Scofield et al. Dec 1993 A
5276910 Buchele Jan 1994 A
5277694 Leysieffer et al. Jan 1994 A
5282858 Bisch et al. Feb 1994 A
5296797 Bartlett Mar 1994 A
5298692 Ikeda et al. Mar 1994 A
5338287 Miller et al. Aug 1994 A
5360388 Spindel et al. Nov 1994 A
5378933 Pfannenmueller et al. Jan 1995 A
5402496 Soli et al. Mar 1995 A
5411467 Hortmann et al. May 1995 A
5424698 Dydyk et al. Jun 1995 A
5425104 Shennib et al. Jun 1995 A
5440082 Claes Aug 1995 A
5440237 Brown et al. Aug 1995 A
5455994 Termeer et al. Oct 1995 A
5456654 Ball Oct 1995 A
5531787 Lesinski et al. Jul 1996 A
5531954 Heide et al. Jul 1996 A
5535282 Luca Jul 1996 A
5554096 Ball Sep 1996 A
5558618 Maniglia Sep 1996 A
5571148 Loeb et al. Nov 1996 A
5572594 Devoe et al. Nov 1996 A
5606621 Reiter et al. Feb 1997 A
5624376 Ball et al. Apr 1997 A
5654530 Sauer et al. Aug 1997 A
5692059 Kruger Nov 1997 A
5699809 Combs et al. Dec 1997 A
5701348 Shennib et al. Dec 1997 A
5707338 Adams et al. Jan 1998 A
5715321 Andrea et al. Feb 1998 A
5721783 Anderson Feb 1998 A
5722411 Suzuki et al. Mar 1998 A
5729077 Newnham et al. Mar 1998 A
5740258 Goodwin-Johansson Apr 1998 A
5742692 Garcia et al. Apr 1998 A
5749912 Zhang et al. May 1998 A
5762583 Adams et al. Jun 1998 A
5772575 Lesinski et al. Jun 1998 A
5774259 Saitoh et al. Jun 1998 A
5782744 Money Jul 1998 A
5788711 Lehner et al. Aug 1998 A
5795287 Ball et al. Aug 1998 A
5797834 Goode Aug 1998 A
5800336 Ball et al. Sep 1998 A
5804109 Perkins Sep 1998 A
5804907 Park et al. Sep 1998 A
5814095 Mueller et al. Sep 1998 A
5824022 Zilberman et al. Oct 1998 A
5825122 Givargizov et al. Oct 1998 A
5836863 Bushek et al. Nov 1998 A
5842967 Kroll Dec 1998 A
5851199 Peerless et al. Dec 1998 A
5857958 Ball et al. Jan 1999 A
5859916 Ball et al. Jan 1999 A
5868682 Combs et al. Feb 1999 A
5879283 Adams et al. Mar 1999 A
5888187 Jaeger et al. Mar 1999 A
5897486 Ball et al. Apr 1999 A
5899847 Adams et al. May 1999 A
5900274 Chatterjee et al. May 1999 A
5906635 Maniglia May 1999 A
5913815 Ball et al. Jun 1999 A
5922017 Bredberg et al. Jul 1999 A
5922077 Espy et al. Jul 1999 A
5935170 Haakansson et al. Aug 1999 A
5940519 Kuo Aug 1999 A
5949895 Ball et al. Sep 1999 A
5951601 Lesinski et al. Sep 1999 A
5984859 Lesinski Nov 1999 A
5987146 Pluvinage et al. Nov 1999 A
6001129 Bushek et al. Dec 1999 A
6005955 Kroll et al. Dec 1999 A
6011984 Van Antwerp et al. Jan 2000 A
6024717 Ball et al. Feb 2000 A
6038480 Hrdlicka et al. Mar 2000 A
6045528 Arenberg et al. Apr 2000 A
6050933 Bushek et al. Apr 2000 A
6067474 Schulman et al. May 2000 A
6068589 Neukermans May 2000 A
6068590 Brisken May 2000 A
6072884 Kates Jun 2000 A
6084975 Perkins Jul 2000 A
6093144 Jaeger et al. Jul 2000 A
6135612 Clore Oct 2000 A
6137889 Shennib et al. Oct 2000 A
6139488 Ball Oct 2000 A
6153966 Neukermans Nov 2000 A
6168948 Anderson et al. Jan 2001 B1
6174278 Jaeger et al. Jan 2001 B1
6175637 Fujihira et al. Jan 2001 B1
6181801 Puthuff et al. Jan 2001 B1
6190305 Ball et al. Feb 2001 B1
6190306 Kennedy Feb 2001 B1
6208445 Reime Mar 2001 B1
6216040 Harrison Apr 2001 B1
6217508 Ball et al. Apr 2001 B1
6219427 Kates et al. Apr 2001 B1
6222302 Imada et al. Apr 2001 B1
6222927 Feng et al. Apr 2001 B1
6240192 Brennan et al. May 2001 B1
6241767 Stennert et al. Jun 2001 B1
6259951 Kuzma et al. Jul 2001 B1
6261224 Adams et al. Jul 2001 B1
6264603 Kennedy Jul 2001 B1
6277148 Dormer Aug 2001 B1
6312959 Datskos Nov 2001 B1
6339648 McIntosh Jan 2002 B1
6342035 Kroll et al. Jan 2002 B1
6354990 Juneau et al. Mar 2002 B1
6359993 Brimhall Mar 2002 B2
6366863 Bye et al. Apr 2002 B1
6374143 Berrang et al. Apr 2002 B1
6385363 Rajic et al. May 2002 B1
6387039 Moses May 2002 B1
6390971 Adams et al. May 2002 B1
6393130 Stonikas et al. May 2002 B1
6422991 Jaeger Jul 2002 B1
6432248 Popp et al. Aug 2002 B1
6434246 Kates et al. Aug 2002 B1
6434247 Kates et al. Aug 2002 B1
6436028 Dormer Aug 2002 B1
6438244 Juneau et al. Aug 2002 B1
6445799 Taenzer et al. Sep 2002 B1
6473512 Juneau et al. Oct 2002 B1
6475134 Ball et al. Nov 2002 B1
6491622 Kasic, II et al. Dec 2002 B1
6491644 Vujanic et al. Dec 2002 B1
6491722 Kroll et al. Dec 2002 B1
6493453 Glendon Dec 2002 B1
6493454 Loi et al. Dec 2002 B1
6498858 Kates Dec 2002 B2
6507758 Greenberg et al. Jan 2003 B1
6519376 Biagi et al. Feb 2003 B2
6523985 Hamanaka et al. Feb 2003 B2
6536530 Schultz et al. Mar 2003 B2
6537200 Leysieffer et al. Mar 2003 B2
6547715 Mueller et al. Apr 2003 B1
6549633 Westermann Apr 2003 B1
6549635 Gebert Apr 2003 B1
6554761 Puria et al. Apr 2003 B1
6575894 Leysieffer et al. Jun 2003 B2
6592513 Kroll et al. Jul 2003 B1
6603860 Taenzer et al. Aug 2003 B1
6620110 Schmid Sep 2003 B2
6626822 Jaeger et al. Sep 2003 B1
6629922 Puria et al. Oct 2003 B1
6631196 Taenzer et al. Oct 2003 B1
6643378 Schumaier Nov 2003 B2
6663575 Leysieffer Dec 2003 B2
6668062 Luo et al. Dec 2003 B1
6676592 Ball et al. Jan 2004 B2
6681022 Puthuff et al. Jan 2004 B1
6695943 Juneau et al. Feb 2004 B2
6697674 Leysieffer Feb 2004 B2
6724902 Shennib et al. Apr 2004 B1
6726618 Miller Apr 2004 B2
6726718 Carlyle et al. Apr 2004 B1
6727789 Tibbetts et al. Apr 2004 B2
6728024 Ribak Apr 2004 B2
6735318 Cho May 2004 B2
6754358 Boesen et al. Jun 2004 B1
6754359 Svean et al. Jun 2004 B1
6754537 Harrison et al. Jun 2004 B1
6785394 Olsen et al. Aug 2004 B1
6792114 Kates et al. Sep 2004 B1
6801629 Brimhall et al. Oct 2004 B2
6829363 Sacha Dec 2004 B2
6831986 Kates Dec 2004 B2
6837857 Stirnemann Jan 2005 B2
6842647 Griffith et al. Jan 2005 B1
6888949 Vanden et al. May 2005 B1
6900926 Ribak May 2005 B2
6912289 Vonlanthen et al. Jun 2005 B2
6920340 Laderman Jul 2005 B2
6931231 Griffin Aug 2005 B1
6940988 Shennib et al. Sep 2005 B1
6940989 Shennib et al. Sep 2005 B1
D512979 Corcoran et al. Dec 2005 S
6975402 Bisson et al. Dec 2005 B2
6978159 Feng et al. Dec 2005 B2
7020297 Fang et al. Mar 2006 B2
7024010 Saunders et al. Apr 2006 B2
7043037 Lichtblau et al. May 2006 B2
7050675 Zhou et al. May 2006 B2
7050876 Fu et al. May 2006 B1
7057256 Mazur et al. Jun 2006 B2
7058182 Kates Jun 2006 B2
7058188 Allred Jun 2006 B1
7072475 Denap et al. Jul 2006 B1
7076076 Bauman Jul 2006 B2
7095981 Voroba et al. Aug 2006 B1
7167572 Harrison et al. Jan 2007 B1
7174026 Niederdrank et al. Feb 2007 B2
7179238 Hissong Feb 2007 B2
7181034 Armstrong Feb 2007 B2
7203331 Boesen Apr 2007 B2
7239069 Cho Jul 2007 B2
7245732 Jorgensen et al. Jul 2007 B2
7255457 Ducharme et al. Aug 2007 B2
7266208 Charvin et al. Sep 2007 B2
7289639 Abel et al. Oct 2007 B2
7313245 Shennib Dec 2007 B1
7315211 Lee et al. Jan 2008 B1
7322930 Jaeger et al. Jan 2008 B2
7349741 Maltan et al. Mar 2008 B2
7354792 Mazur et al. Apr 2008 B2
7376563 Leysieffer et al. May 2008 B2
7390689 Mazur et al. Jun 2008 B2
7394909 Widmer et al. Jul 2008 B1
7421087 Perkins et al. Sep 2008 B2
7424122 Ryan Sep 2008 B2
7444877 Li et al. Nov 2008 B2
7547275 Cho et al. Jun 2009 B2
7630646 Anderson et al. Dec 2009 B2
7645877 Gmeiner et al. Jan 2010 B2
7668325 Puria et al. Feb 2010 B2
7747295 Choi Jun 2010 B2
7778434 Juneau et al. Aug 2010 B2
7809150 Natarajan et al. Oct 2010 B2
7822215 Carazo et al. Oct 2010 B2
7826632 Von Buol et al. Nov 2010 B2
7853033 Maltan et al. Dec 2010 B2
7867160 Pluvinage et al. Jan 2011 B2
7883535 Cantin et al. Feb 2011 B2
7885359 Meltzer Feb 2011 B2
7983435 Moses Jul 2011 B2
8090134 Takigawa et al. Jan 2012 B2
8099169 Karunasiri Jan 2012 B1
8116494 Rass Feb 2012 B2
8128551 Jolly Mar 2012 B2
8157730 Leboeuf et al. Apr 2012 B2
8197461 Arenberg et al. Jun 2012 B1
8204786 Leboeuf et al. Jun 2012 B2
8233651 Haller Jul 2012 B1
8251903 Leboeuf et al. Aug 2012 B2
8284970 Sacha Oct 2012 B2
8295505 Weinans et al. Oct 2012 B2
8295523 Fay et al. Oct 2012 B2
8320601 Takigawa et al. Nov 2012 B2
8320982 Leboeuf et al. Nov 2012 B2
8340310 Ambrose et al. Dec 2012 B2
8340335 Shennib Dec 2012 B1
8391527 Feucht et al. Mar 2013 B2
8396235 Gebhardt et al. Mar 2013 B2
8396239 Fay et al. Mar 2013 B2
8401212 Puria et al. Mar 2013 B2
8401214 Perkins et al. Mar 2013 B2
8506473 Puria Aug 2013 B2
8512242 Leboeuf et al. Aug 2013 B2
8526651 Van Hal et al. Sep 2013 B2
8526652 Ambrose et al. Sep 2013 B2
8526971 Giniger et al. Sep 2013 B2
8545383 Wenzel, I et al. Oct 2013 B2
8600089 Wenzel et al. Dec 2013 B2
8647270 Leboeuf et al. Feb 2014 B2
8652040 Leboeuf et al. Feb 2014 B2
8684922 Tran Apr 2014 B2
8696054 Crum Apr 2014 B2
8696541 Pluvinage et al. Apr 2014 B2
8700111 Leboeuf et al. Apr 2014 B2
8702607 Leboeuf et al. Apr 2014 B2
8715152 Puria et al. May 2014 B2
8715153 Puria et al. May 2014 B2
8715154 Perkins et al. May 2014 B2
8761423 Wagner et al. Jun 2014 B2
8787609 Perkins et al. Jul 2014 B2
8788002 Leboeuf et al. Jul 2014 B2
8817998 Inoue Aug 2014 B2
8824715 Fay et al. Sep 2014 B2
8837758 Knudsen Sep 2014 B2
8845705 Perkins et al. Sep 2014 B2
8855323 Kroman Oct 2014 B2
8858419 Puria et al. Oct 2014 B2
8885860 Djalilian et al. Nov 2014 B2
8886269 Leboeuf et al. Nov 2014 B2
8888701 Leboeuf et al. Nov 2014 B2
8923941 Leboeuf et al. Dec 2014 B2
8929965 Leboeuf et al. Jan 2015 B2
8929966 Leboeuf et al. Jan 2015 B2
8934952 Leboeuf et al. Jan 2015 B2
8942776 Leboeuf et al. Jan 2015 B2
8961415 Leboeuf et al. Feb 2015 B2
8986187 Perkins et al. Mar 2015 B2
8989830 Leboeuf et al. Mar 2015 B2
9044180 Leboeuf et al. Jun 2015 B2
9049528 Fay et al. Jun 2015 B2
9055379 Puria et al. Jun 2015 B2
9131312 Leboeuf et al. Sep 2015 B2
9154891 Puria et al. Oct 2015 B2
9211069 Larsen et al. Dec 2015 B2
9226083 Puria et al. Dec 2015 B2
9277335 Perkins et al. Mar 2016 B2
9289135 Leboeuf et al. Mar 2016 B2
9289175 Leboeuf et al. Mar 2016 B2
9301696 Leboeuf et al. Apr 2016 B2
9314167 Leboeuf et al. Apr 2016 B2
9392377 Olsen et al. Jul 2016 B2
9427191 Leboeuf et al. Aug 2016 B2
9497556 Kaltenbacher et al. Nov 2016 B2
9521962 Leboeuf Dec 2016 B2
9524092 Ren et al. Dec 2016 B2
9538921 Leboeuf et al. Jan 2017 B2
9544700 Puria et al. Jan 2017 B2
9564862 Hoyerby Feb 2017 B2
9591409 Puria et al. Mar 2017 B2
9749758 Puria et al. Aug 2017 B2
9750462 Leboeuf et al. Sep 2017 B2
9788785 Leboeuf Oct 2017 B2
9788794 Leboeuf et al. Oct 2017 B2
9794653 Aumer et al. Oct 2017 B2
9794688 You Oct 2017 B2
9801552 Romesburg et al. Oct 2017 B2
9808204 Leboeuf et al. Nov 2017 B2
9924276 Wenzel Mar 2018 B2
9930458 Freed et al. Mar 2018 B2
9949035 Rucker et al. Apr 2018 B2
9949039 Puria et al. Apr 2018 B2
9949045 Kure et al. Apr 2018 B2
9961454 Puria et al. May 2018 B2
9964672 Phair et al. May 2018 B2
10003888 Stephanou et al. Jun 2018 B2
10034103 Puria et al. Jul 2018 B2
10154352 Perkins et al. Dec 2018 B2
10178483 Teran et al. Jan 2019 B2
10206045 Kaltenbacher et al. Feb 2019 B2
10237663 Puria et al. Mar 2019 B2
10284964 Olsen et al. May 2019 B2
10286215 Perkins et al. May 2019 B2
10292601 Facteau et al. May 2019 B2
10306381 Sandhu et al. May 2019 B2
10492010 Rucker et al. Nov 2019 B2
10511913 Puria et al. Dec 2019 B2
10516946 Puria et al. Dec 2019 B2
10516949 Puria et al. Dec 2019 B2
10516950 Perkins et al. Dec 2019 B2
10516951 Wenzel Dec 2019 B2
10531206 Freed et al. Jan 2020 B2
10609492 Olsen et al. Mar 2020 B2
10743110 Puria et al. Aug 2020 B2
10779094 Rucker et al. Sep 2020 B2
10863286 Perkins et al. Dec 2020 B2
11057714 Puria et al. Jul 2021 B2
11058305 Perkins et al. Jul 2021 B2
11070927 Rucker et al. Jul 2021 B2
11102594 Shaquer et al. Aug 2021 B2
11166114 Perkins et al. Nov 2021 B2
20010003788 Ball et al. Jun 2001 A1
20010007050 Adelman Jul 2001 A1
20010024507 Boesen Sep 2001 A1
20010027342 Dormer Oct 2001 A1
20010029313 Kennedy Oct 2001 A1
20010043708 Brimhall Nov 2001 A1
20010053871 Zilberman et al. Dec 2001 A1
20010055405 Cho Dec 2001 A1
20020012438 Leysieffer et al. Jan 2002 A1
20020025055 Stonikas et al. Feb 2002 A1
20020029070 Leysieffer et al. Mar 2002 A1
20020030871 Anderson et al. Mar 2002 A1
20020035309 Leysieffer Mar 2002 A1
20020048374 Soli et al. Apr 2002 A1
20020085728 Shennib et al. Jul 2002 A1
20020086715 Sahagen Jul 2002 A1
20020172350 Edwards et al. Nov 2002 A1
20020183587 Dormer Dec 2002 A1
20030021903 Shlenker et al. Jan 2003 A1
20030055311 Neukermans et al. Mar 2003 A1
20030064746 Rader et al. Apr 2003 A1
20030081803 Petilli et al. May 2003 A1
20030097178 Roberson et al. May 2003 A1
20030125602 Sokolich et al. Jul 2003 A1
20030142841 Wiegand Jul 2003 A1
20030208099 Ball Nov 2003 A1
20030208888 Fearing et al. Nov 2003 A1
20030220536 Hissong Nov 2003 A1
20040019294 Stirnemann Jan 2004 A1
20040093040 Boylston et al. May 2004 A1
20040121291 Knapp et al. Jun 2004 A1
20040158157 Jensen et al. Aug 2004 A1
20040165742 Shennib et al. Aug 2004 A1
20040166495 Greinwald et al. Aug 2004 A1
20040167377 Schafer et al. Aug 2004 A1
20040184732 Zhou et al. Sep 2004 A1
20040190734 Kates Sep 2004 A1
20040202339 O'Brien et al. Oct 2004 A1
20040202340 Armstrong et al. Oct 2004 A1
20040208333 Cheung et al. Oct 2004 A1
20040234089 Rembrand et al. Nov 2004 A1
20040234092 Wada et al. Nov 2004 A1
20040236416 Falotico Nov 2004 A1
20040240691 Grafenberg Dec 2004 A1
20050018859 Buchholz Jan 2005 A1
20050020873 Berrang et al. Jan 2005 A1
20050036639 Bachler et al. Feb 2005 A1
20050038498 Dubrow et al. Feb 2005 A1
20050088435 Geng Apr 2005 A1
20050101830 Easter et al. May 2005 A1
20050111683 Chabries et al. May 2005 A1
20050117765 Meyer et al. Jun 2005 A1
20050163333 Abel et al. Jul 2005 A1
20050190939 Fretz et al. Sep 2005 A1
20050196005 Shennib et al. Sep 2005 A1
20050222823 Brumback et al. Oct 2005 A1
20050226446 Luo et al. Oct 2005 A1
20050267549 Della et al. Dec 2005 A1
20050271870 Jackson Dec 2005 A1
20050288739 Hassler et al. Dec 2005 A1
20060015155 Charvin et al. Jan 2006 A1
20060023908 Perkins et al. Feb 2006 A1
20060058573 Neisz et al. Mar 2006 A1
20060062420 Araki Mar 2006 A1
20060074159 Lu et al. Apr 2006 A1
20060075175 Jensen et al. Apr 2006 A1
20060107744 Li et al. May 2006 A1
20060129210 Cantin et al. Jun 2006 A1
20060161227 Walsh, Jr. et al. Jul 2006 A1
20060161255 Zarowski et al. Jul 2006 A1
20060177079 Baekgaard et al. Aug 2006 A1
20060177082 Solomito, Jr. et al. Aug 2006 A1
20060183965 Kasic et al. Aug 2006 A1
20060189841 Pluvinage et al. Aug 2006 A1
20060231914 Carey, III Oct 2006 A1
20060233398 Husung Oct 2006 A1
20060237126 Guffrey et al. Oct 2006 A1
20060247735 Honert et al. Nov 2006 A1
20060251278 Puria et al. Nov 2006 A1
20060256989 Olsen et al. Nov 2006 A1
20060278245 Gan Dec 2006 A1
20070030990 Fischer Feb 2007 A1
20070036377 Stirnemann Feb 2007 A1
20070076913 Schanz Apr 2007 A1
20070083078 Easter et al. Apr 2007 A1
20070100197 Perkins et al. May 2007 A1
20070127748 Carlile et al. Jun 2007 A1
20070127752 Armstrong Jun 2007 A1
20070127766 Combest Jun 2007 A1
20070135870 Shanks et al. Jun 2007 A1
20070161848 Dalton et al. Jul 2007 A1
20070191673 Ball et al. Aug 2007 A1
20070201713 Fang et al. Aug 2007 A1
20070206825 Thomasson Sep 2007 A1
20070223755 Salvetti et al. Sep 2007 A1
20070225776 Fritsch et al. Sep 2007 A1
20070236704 Carr et al. Oct 2007 A1
20070250119 Tyler et al. Oct 2007 A1
20070251082 Milojevic et al. Nov 2007 A1
20070258507 Lee et al. Nov 2007 A1
20070286429 Grafenberg et al. Dec 2007 A1
20080021518 Hochmair et al. Jan 2008 A1
20080051623 Schneider et al. Feb 2008 A1
20080054509 Berman et al. Mar 2008 A1
20080063228 Mejia et al. Mar 2008 A1
20080063231 Juneau et al. Mar 2008 A1
20080064918 Jolly Mar 2008 A1
20080077198 Webb et al. Mar 2008 A1
20080089292 Kitazoe et al. Apr 2008 A1
20080107292 Kornagel May 2008 A1
20080123866 Rule et al. May 2008 A1
20080130927 Theverapperuma et al. Jun 2008 A1
20080188707 Bernard et al. Aug 2008 A1
20080298600 Poe et al. Dec 2008 A1
20080300703 Widmer et al. Dec 2008 A1
20090016553 Ho et al. Jan 2009 A1
20090023976 Cho et al. Jan 2009 A1
20090043149 Abel et al. Feb 2009 A1
20090076581 Gibson Mar 2009 A1
20090092271 Fay et al. Apr 2009 A1
20090097681 Puria et al. Apr 2009 A1
20090131742 Cho et al. May 2009 A1
20090141919 Spitaels et al. Jun 2009 A1
20090149697 Steinhardt et al. Jun 2009 A1
20090157143 Edler et al. Jun 2009 A1
20090175474 Salvetti et al. Jul 2009 A1
20090246627 Park Oct 2009 A1
20090253951 Ball et al. Oct 2009 A1
20090262966 Vestergaard et al. Oct 2009 A1
20090281367 Cho et al. Nov 2009 A1
20090310805 Petroff Dec 2009 A1
20090316922 Merks et al. Dec 2009 A1
20100034409 Fay et al. Feb 2010 A1
20100036488 De, Jr. et al. Feb 2010 A1
20100048982 Puria Feb 2010 A1
20100085176 Flick Apr 2010 A1
20100103404 Remke et al. Apr 2010 A1
20100111315 Kroman May 2010 A1
20100114190 Bendett et al. May 2010 A1
20100145135 Ball et al. Jun 2010 A1
20100152527 Puria Jun 2010 A1
20100171369 Baarman et al. Jul 2010 A1
20100172507 Merks Jul 2010 A1
20100177918 Keady et al. Jul 2010 A1
20100202645 Puria et al. Aug 2010 A1
20100222639 Purcell et al. Sep 2010 A1
20100260364 Merks Oct 2010 A1
20100272299 Van Schuylenbergh et al. Oct 2010 A1
20100290653 Wiggins et al. Nov 2010 A1
20100312040 Puria et al. Dec 2010 A1
20110062793 Azancot et al. Mar 2011 A1
20110069852 Arndt et al. Mar 2011 A1
20110077453 Pluvinage et al. Mar 2011 A1
20110084654 Julstrom et al. Apr 2011 A1
20110112462 Parker et al. May 2011 A1
20110116666 Dittberner et al. May 2011 A1
20110125222 Perkins et al. May 2011 A1
20110130622 Ilberg et al. Jun 2011 A1
20110142274 Perkins et al. Jun 2011 A1
20110144414 Spearman et al. Jun 2011 A1
20110152601 Puria et al. Jun 2011 A1
20110152602 Perkins et al. Jun 2011 A1
20110152603 Perkins et al. Jun 2011 A1
20110152976 Perkins et al. Jun 2011 A1
20110164771 Jensen et al. Jul 2011 A1
20110182453 Van Hal et al. Jul 2011 A1
20110196460 Weiss Aug 2011 A1
20110221391 Won et al. Sep 2011 A1
20110249845 Kates Oct 2011 A1
20110249847 Salvetti et al. Oct 2011 A1
20110257290 Zeller et al. Oct 2011 A1
20110258839 Probst Oct 2011 A1
20110271965 Parkins et al. Nov 2011 A1
20120008807 Gran Jan 2012 A1
20120014546 Puria et al. Jan 2012 A1
20120038881 Amirparviz et al. Feb 2012 A1
20120039493 Rucker et al. Feb 2012 A1
20120092461 Fisker et al. Apr 2012 A1
20120114157 Arndt et al. May 2012 A1
20120140967 Aubert et al. Jun 2012 A1
20120217087 Ambrose et al. Aug 2012 A1
20120236524 Pugh et al. Sep 2012 A1
20120263339 Funahashi Oct 2012 A1
20130004004 Zhao et al. Jan 2013 A1
20130034258 Lin Feb 2013 A1
20130083938 Bakalos et al. Apr 2013 A1
20130089227 Kates Apr 2013 A1
20130195300 Larsen et al. Aug 2013 A1
20130230204 Monahan et al. Sep 2013 A1
20130287239 Fay et al. Oct 2013 A1
20130303835 Koskowich Nov 2013 A1
20130308782 Dittberner et al. Nov 2013 A1
20130308807 Burns Nov 2013 A1
20130315428 Perkins et al. Nov 2013 A1
20130343584 Bennett et al. Dec 2013 A1
20130343585 Bennett et al. Dec 2013 A1
20130343587 Naylor et al. Dec 2013 A1
20140003640 Puria et al. Jan 2014 A1
20140056453 Olsen et al. Feb 2014 A1
20140084698 Asanuma et al. Mar 2014 A1
20140107423 Yaacobi Apr 2014 A1
20140153761 Shennib et al. Jun 2014 A1
20140169603 Sacha et al. Jun 2014 A1
20140177863 Parkins Jun 2014 A1
20140194891 Shahoian Jul 2014 A1
20140254856 Blick et al. Sep 2014 A1
20140275734 Perkins et al. Sep 2014 A1
20140286514 Pluvinage et al. Sep 2014 A1
20140288356 Van Vlem Sep 2014 A1
20140288358 Puria et al. Sep 2014 A1
20140296620 Puria et al. Oct 2014 A1
20140321657 Stirnemann Oct 2014 A1
20140379874 Starr et al. Dec 2014 A1
20150021568 Gong et al. Jan 2015 A1
20150023540 Fay et al. Jan 2015 A1
20150031941 Perkins et al. Jan 2015 A1
20150049889 Bern Feb 2015 A1
20150117689 Bergs et al. Apr 2015 A1
20150124985 Kim et al. May 2015 A1
20150201269 Dahl et al. Jul 2015 A1
20150222978 Murozaki et al. Aug 2015 A1
20150245131 Facteau et al. Aug 2015 A1
20150358743 Killion Dec 2015 A1
20160008176 Goldstein Jan 2016 A1
20160029132 Freed et al. Jan 2016 A1
20160064814 Jang et al. Mar 2016 A1
20160087687 Kesler et al. Mar 2016 A1
20160094043 Hao et al. Mar 2016 A1
20160150331 Wenzel May 2016 A1
20160277854 Puria et al. Sep 2016 A1
20160309265 Pluvinage et al. Oct 2016 A1
20160309266 Olsen et al. Oct 2016 A1
20160330555 Vonlanthen et al. Nov 2016 A1
20170040012 Goldstein Feb 2017 A1
20170095202 Facteau et al. Apr 2017 A1
20170150275 Puria et al. May 2017 A1
20170195801 Rucker et al. Jul 2017 A1
20170195806 Atamaniuk et al. Jul 2017 A1
20170195809 Teran et al. Jul 2017 A1
20170257710 Parker Sep 2017 A1
20180014128 Puria et al. Jan 2018 A1
20180020291 Puria et al. Jan 2018 A1
20180020296 Wenzel Jan 2018 A1
20180077503 Shaquer et al. Mar 2018 A1
20180077504 Shaquer et al. Mar 2018 A1
20180167750 Freed et al. Jun 2018 A1
20180213331 Rucker et al. Jul 2018 A1
20180213335 Puria et al. Jul 2018 A1
20180262846 Perkins et al. Sep 2018 A1
20180317026 Puria Nov 2018 A1
20180376255 Parker Dec 2018 A1
20190069097 Perkins et al. Feb 2019 A1
20190166438 Perkins et al. May 2019 A1
20190230449 Puria Jul 2019 A1
20190239005 Sandhu et al. Aug 2019 A1
20190253811 Unno et al. Aug 2019 A1
20190253815 Atamaniuk et al. Aug 2019 A1
20200037082 Perkins et al. Jan 2020 A1
20200068323 Perkins et al. Feb 2020 A1
20200084551 Puria et al. Mar 2020 A1
20200092662 Wenzel Mar 2020 A1
20200128338 Shaquer et al. Apr 2020 A1
20200186941 Olsen et al. Jun 2020 A1
20200186942 Flaherty et al. Jun 2020 A1
20200304927 Shaquer et al. Sep 2020 A1
20200396551 Dy et al. Dec 2020 A1
20210029451 Fitz et al. Jan 2021 A1
20210029474 Larkin et al. Jan 2021 A1
20210186343 Perkins et al. Jun 2021 A1
20210266686 Puria et al. Aug 2021 A1
20210274293 Perkins et al. Sep 2021 A1
20210289301 Atamaniuk et al. Sep 2021 A1
20210306777 Rucker et al. Sep 2021 A1
20210314712 Shaquer et al. Oct 2021 A1
Foreign Referenced Citations (117)
Number Date Country
2004301961 Feb 2005 AU
2242545 Sep 2009 CA
1176731 Mar 1998 CN
101459868 Jun 2009 CN
101489171 Jul 2009 CN
102301747 Dec 2011 CN
105491496 Apr 2016 CN
2044870 Mar 1972 DE
3243850 May 1984 DE
3508830 Sep 1986 DE
102013114771 Jun 2015 DE
0092822 Nov 1983 EP
0242038 Oct 1987 EP
0291325 Nov 1988 EP
0296092 Dec 1988 EP
0242038 May 1989 EP
0296092 Aug 1989 EP
0352954 Jan 1990 EP
0291325 Jun 1990 EP
0352954 Aug 1991 EP
1035753 Sep 2000 EP
1435757 Jul 2004 EP
1845919 Oct 2007 EP
1955407 Aug 2008 EP
1845919 Sep 2010 EP
2272520 Jan 2011 EP
2301262 Mar 2011 EP
2752030 Jul 2014 EP
3101519 Dec 2016 EP
2425502 Jan 2017 EP
2907294 May 2017 EP
3183814 Jun 2017 EP
3094067 Oct 2017 EP
3006079 Mar 2019 EP
2455820 Nov 1980 FR
2085694 Apr 1982 GB
S60154800 Aug 1985 JP
S621726 Jan 1987 JP
S63252174 Oct 1988 JP
S6443252 Feb 1989 JP
H09327098 Dec 1997 JP
2000504913 Apr 2000 JP
2004187953 Jul 2004 JP
2004193908 Jul 2004 JP
2005516505 Jun 2005 JP
2006060833 Mar 2006 JP
100624445 Sep 2006 KR
WO-9209181 May 1992 WO
WO-9501678 Jan 1995 WO
WO-9621334 Jul 1996 WO
WO-9736457 Oct 1997 WO
WO-9745074 Dec 1997 WO
WO-9806236 Feb 1998 WO
WO-9903146 Jan 1999 WO
WO-9915111 Apr 1999 WO
WO-0022875 Apr 2000 WO
WO-0022875 Jul 2000 WO
WO-0150815 Jul 2001 WO
WO-0158206 Aug 2001 WO
WO-0176059 Oct 2001 WO
WO-0158206 Feb 2002 WO
WO-0239874 May 2002 WO
WO-0239874 Feb 2003 WO
WO-03030772 Apr 2003 WO
WO-03063542 Jul 2003 WO
WO-03063542 Jan 2004 WO
WO-2004010733 Jan 2004 WO
WO-2005015952 Feb 2005 WO
WO-2005107320 Nov 2005 WO
WO-2006014915 Feb 2006 WO
WO-2006037156 Apr 2006 WO
WO-2006039146 Apr 2006 WO
WO-2006042298 Apr 2006 WO
WO-2006071210 Jul 2006 WO
WO-2006075169 Jul 2006 WO
WO-2006075175 Jul 2006 WO
WO-2006118819 Nov 2006 WO
WO-2006042298 Dec 2006 WO
WO-2007023164 Mar 2007 WO
WO-2009046329 Apr 2009 WO
WO-2009047370 Apr 2009 WO
WO-2009049320 Apr 2009 WO
WO-2009056167 May 2009 WO
WO-2009062142 May 2009 WO
WO-2009047370 Jul 2009 WO
WO-2009125903 Oct 2009 WO
WO-2009145842 Dec 2009 WO
WO-2009146151 Dec 2009 WO
WO-2009155358 Dec 2009 WO
WO-2009155361 Dec 2009 WO
WO-2009155385 Dec 2009 WO
WO-2010033932 Mar 2010 WO
WO-2010033933 Mar 2010 WO
WO-2010077781 Jul 2010 WO
WO-2010147935 Dec 2010 WO
WO-2010148345 Dec 2010 WO
WO-2011005500 Jan 2011 WO
WO-2012088187 Jun 2012 WO
WO-2012149970 Nov 2012 WO
WO-2013016336 Jan 2013 WO
WO-2016011044 Jan 2016 WO
WO-2016045709 Mar 2016 WO
WO-2016146487 Sep 2016 WO
WO-2017045700 Mar 2017 WO
WO-2017059218 Apr 2017 WO
WO-2017059240 Apr 2017 WO
WO-2017116791 Jul 2017 WO
WO-2017116865 Jul 2017 WO
WO-2018048794 Mar 2018 WO
WO-2018081121 May 2018 WO
WO-2018093733 May 2018 WO
WO-2019055308 Mar 2019 WO
WO-2019173470 Sep 2019 WO
WO-2019199680 Oct 2019 WO
WO-2019199683 Oct 2019 WO
WO-2020176086 Sep 2020 WO
WO-2021003087 Jan 2021 WO
Non-Patent Literature Citations (153)
Entry
“International search report and written opinion dated Oct. 15, 2015 for PCT/US2015/040397.”
“Office Action date Aug. 29, 2018 for U.S. Appl. No. 15/890,185.”
Asbeck, et al. Scaling Hard Vertical Surfaces with Compliant Microspine Arrays, The International Journal of Robotics Research 2006; 25; 1165-79.
ATASOY [Paper] Opto-acoustic Imaging. for BYM504E Biomedical Imaging Systems class at ITU, downloaded from the Internet www2.itu.edu.td—cilesiz/courses/BYM504- 2005-OA504041413.pdf, 14 pages.
Athanassiou, et al. Laser controlled photomechanical actuation of photochromic polymers Microsystems. Rev. Adv. Mater. Sci. 2003; 5:245- 251.
Autumn, et al. Dynamics of geckos running vertically, The Journal of Experimental Biology 209, 260-272, (2006).
Autumn, et al., Evidence for van der Waals adhesion in gecko setae, www.pnas.orgycgiydoiyl0.1073ypnas.192252799 (2002).
Ayatollahi, et al. Design and Modeling of Micromachined Condenser MEMS Loudspeaker using Permanent Magnet Neodymium-Iron-Boron (Nd—Fe—B). IEEE International Conference on Semiconductor Electronics, 2006. ICSE '06, Oct. 29, 2006-Dec. 1, 2006; 160-166.
Baer, et al. Effects of Low Pass Filtering on the Intelligibility of Speech in Noise for People With and Without Dead Regions at High Frequencies. J. Acost. Soc. Am 112 (3), pt. 1, (Sep. 2002), pp. 1133-1144.
Best, et al. The influence of high frequencies on speech localization. Abstract 981 (Feb. 24, 2003) from www.aro.org/abstracts/abstracts.html.
Birch, et al. Microengineered systems for the hearing impaired. IEE Colloquium on Medical Applications of Microengineering, Jan. 31, 1996; pp. 2/1-2/5.
Boedts. Tympanic epithelial migration, Clinical Otolaryngology 1978, 3, 249-253.
Burkhard, et al. Anthropometric Manikin for Acoustic Research. J. Acoust. Soc. Am., vol. 58, No. 1, (Jul. 1975), pp. 214-222.
Camacho-Lopez, et al. Fast Liquid Crystal Elastomer Swims Into the Dark, Electronic Liquid Crystal Communications. Nov. 26, 2003; 9 pages total.
Carlile, et al. Frequency bandwidth and multi-talker environments. Audio Engineering Society Convention 120. Audio Engineering Society, May 20-23, 2006. Paris, France. 118: 8 pages.
Carlile, et al. Spatialisation of talkers and the segregation of concurrent speech. Abstract 1264 (Feb. 24, 2004) from www.aro.org/abstracts/abstracts.html.
Cheng, et al. A Silicon Microspeaker for Hearing Instruments. Journal of Micromechanics and Microengineering 2004; 14(7):859-866.
Cheng; et al., “A silicon microspeaker for hearing instruments. Journal of Micromechanics and Microengineering 14, No. 7 (2004): 859-866.”
Dictionary.com's (via American Heritage Medical Dictionary) online dictionary definition of‘percutaneous’. Accessed on Jun. 3, 2013. 2 pages.
Merriam-Webster's online dictionary definition of ‘percutaneous’. Accessed on Jun. 3, 2013. 3 pages.
Datskos, et al. Photoinduced and thermal stress in silicon microcantilevers. Applied Physics Letters. Oct. 19, 1998; 73(16):2319-2321.
Decraemer, et al. A method for determining three-dimensional vibration in the ear. Hearing Res., 77:19-37 (1994).
Dundas et al. The Earlens Light-Driven Hearing Aid: Top 10 questions and answers. Hearing Review. 2018;25(2):36-39.
Ear. Downloaded from the Internet. Accessed Jun. 17, 2008. 4 pages. URL:<http://wwwmgs.bionet.nsc.ru/mgs/gnw/trrd/thesaurus/Se/ear.html>.
Edinger, J.R. High-Quality Audio Amplifier With Automatic Bias Control. Audio Engineering; Jun. 1947; pp. 7-9.
Fay, et al. Cat eardrum response mechanics. Mechanics and Computation Division. Department of Mechanical Engineering. Standford University. 2002; 10 pages total.
Fay, et al. Preliminary evaluation of a light-based contact hearing device for the hearing impaired. Otol Neurotol. Jul. 2013;34(5):912-21. doi: 10.1097/MAO.0b013e31827de4b1.
Fay, et al. The discordant eardrum, PNAS, Dec. 26, 2006, vol. 103, No. 52, p. 19743-19748.
Fay. Cat eardrum mechanics. Ph.D. thesis. Disseration submitted to Department of Aeronautics and Astronautics. Standford University. May 2001; 210 pages total.
Fletcher. Effects of Distortion on the Individual Speech Sounds. Chapter 18, ASA Edition of Speech and Hearing in Communication, Acoust Soc.of Am. (republished in 1995) pp. 415-423.
Freyman, et al. Spatial Release from Informational Masking in Speech Recognition. J. Acost. Soc. Am., vol. 109, No. 5, pt. 1, (May 2001); 2112-2122.
Freyman, et al. The Role of Perceived Spatial Separation in the Unmasking of Speech. J. Acoust. Soc. Am., vol. 106, No. 6, (Dec. 1999); 3578-3588.
Fritsch, et al. EarLens transducer behavior in high-field strength MRI scanners. Otolaryngol Head Neck Surg. Mar. 2009;140(3):426-8. doi: 10.1016/j.otohns.2008.10.016.
Galbraith et al. A wide-band efficient inductive transdermal power and data link with coupling insensitive gain IEEE Trans Biomed Eng. Apr. 1987;34(4):265-75.
Gantz, et al. Broad Spectrum Amplification with a Light Driven Hearing System. Combined Otolaryngology Spring Meetings, 2016 (Chicago).
Gantz, et al. Light Driven Hearing Aid: A Multi-Center Clinical Study. Association for Research in Otolaryngology Annual Meeting, 2016 (San Diego).
Gantz, et al. Light-Driven Contact Hearing Aid for Broad Spectrum Amplification: Safety and Effectiveness Pivotal Study. Otology & Neurotology Journal, 2016 (in review).
Gantz, et al. Light-Driven Contact Hearing Aid for Broad-Spectrum Amplification: Safety and Effectiveness Pivotal Study. Otology & Neurotology. Copyright 2016. 7 pages.
Ge, et al., Carbon nanotube-based synthetic gecko tapes, p. 10792-10795, PNAS, Jun. 26, 2007, vol. 104, No. 26.
Gennum, GA3280 Preliminary Data Sheet: Voyageur TD Open Platform DSP System for Ultra Low Audio Processing, downloaded from the Internet:<<http://www.sounddesigntechnologies.com/products/pdf/37601DOC.pdf>>, Oct. 2006; 17 pages.
Gobin, et al. Comments on the physical basis of the active materials concept. Proc. SPIE 2003; 4512:84-92.
Gorb, et al. Structural Design and Biomechanics of Friction-Based Releasable Attachment Devices in Insects, Integr. Comp_ Biol., 42:1127-1139 (2002).
Hakansson, et al. Percutaneous vs. transcutaneous transducers for hearing by direct bone conduction (Abstract). Otolaryngol Head Neck Surg. Apr. 1990;102(4):339-44.
Hato, et al. Three-dimensional stapes footplate motion in human temporal bones. Audiol. Neurootol., 8:140-152 (Jan. 30, 2003).
Headphones. Wikipedia Entry. Downloaded from the Internet. Accessed Oct. 27, 2008. 7 pages. URL: http://en.wikipedia.org/wiki/Headphones>.
Hofman, et al. Relearning Sound Localization With New Ears. Nature Neuroscience, vol. 1, No. 5, (Sep. 1998); 417-421.
Izzo, et al. Laser Stimulation of Auditory Neurons: Effect of Shorter Pulse Duration and Penetration Depth. Biophys J. Apr. 15, 2008;94(8):3159-3166.
Izzo, et al. Laser Stimulation of the Auditory Nerve. Lasers Surg Med. Sep. 2006;38(8):745-753.
Izzo, et al. Selectivity of Neural Stimulation in the Auditory System: A Comparison of Optic and Electric Stimuli. J Biomed Opt. Mar.-Apr. 2007;12(2):021008.
Jian, et al. A 0.6 V, 1.66 mW energy harvester and audio driver for tympanic membrane transducer with wirelessly optical signal and power transfer. InCircuits and Systems (ISCAS), 2014 IEEE International Symposium on Jun. 1, 2014. 874-7. IEEE.
Jin, et al. Speech Localization. J. Audio Eng. Soc. convention paper, presented at the AES 112th Convention, Munich, Germany, May 10-13, 2002, 13 pages total.
Khaleghi et al. Attenuating the feedback pressure of a light-activated hearing device to allows microphone placement at the ear canal entrance. IHCON 2016, International Hearing Aid Research Conference, Tahoe City, CA, Aug. 2016.
Khaleghi et al. Mechano-Electro-Magnetic Finite Element Model of a Balanced Armature Transducer for a Contact Hearing Aid. Proc. MoH 2017, Mechanics of Hearing workshop, Brock University, Jun. 2017.
Khaleghi et al. Multiphysics Finite Element Model of a Balanced Armature Transducer used in a Contact Hearing Device. ARO 2017, 40th ARO MidWinter Meeting, Baltimore, MD, Feb. 2017.
Khaleghi, et al. Attenuating the ear canal feedback pressure of a laser-driven hearing aid. J Acoust Soc Am. Mar. 2017;141(3):1683.
Khaleghi, et al. Characterization of Ear-Canal Feedback Pressure due to Umbo-Drive Forces: Finite-Element vs. Circuit Models. ARO Midwinter Meeting 2016, (San Diego).
Kiessling, et al. Occlusion Effect of Earmolds with Different Venting Systems. J Am Acad Audiol. Apr. 2005;16(4):237-49.
Killion, et al. The case of the missing dots: AI and SNR loss. The Hearing Journal, 1998. 51(5), 32-47.
Killion. Myths About Hearing Noise and Directional Microphones. The Hearing Review. Feb. 2004; 11(2):14, 16, 18, 19, 72 & 73.
Killion. SNR loss: I can hear what people say but I can't understand them. The Hearing Review, 1997; 4(12):8-14.
Lee, et al. A Novel Opto-Electromagnetic Actuator Coupled to the tympanic Membrane. J Biomech. Dec. 5, 2008;41 (16):3515-8. Epub Nov. 7, 2008.
Lee, et al. The optimal magnetic force for a novel actuator coupled to the tympanic membrane: a finite element analysis. Biomedical engineering: applications, basis and communications. 2007; 19(3):171-177.
Levy et al. Light-driven contact hearing aid: a removable direct-drive hearing device option for mild to severe sensorineural hearing impairment. Conference on Implantable Auditory Prostheses, Tahoe City, CA, Jul. 2017. 4 pages.
Levy, et al. Characterization of the available feedback gain margin at two device microphone locations, in the fossa triangularis and Behind the Ear, for the light-based contact hearing device. Acoustical Society of America (ASA) meeting, 2013 (San Francisco).
Levy, et al. Extended High-Frequency Bandwidth Improves Speech Reception in the Presence of Spatially Separated Masking Speech. Ear Hear. Sep.-Oct. 2015;36(5):e214-24. doi: 10.1097/AUD.0000000000000161.
LEZAL. Chalcogenide glasses - survey and progress. Journal of Optoelectronics and Advanced Materials. Mar. 2003; 5(1):23-34.
Mah. Fundamentals of photovoltaic materials. National Solar Power Research Institute. Dec. 21, 1998, 3-9.
Makino, et al. Epithelial migration in the healing process of tympanic membrane perforations. Eur Arch Otorhinolaryngol. 1990; 247: 352-355.
Makino, et al., Epithelial migration on the tympanic membrane and external canal, Arch Otorhinolaryngol (1986) 243:39-42.
Markoff. Intuition + Money: An Aha Moment. New York Times Oct. 11, 2008, p. BU4, 3 pages total.
Martin, et al. Utility of Monaural Spectral Cues is Enhanced in the Presence of Cues to Sound-Source Lateral Angle. JARO. 2004; 5:80-89.
McElveen et al. Overcoming High-Frequency Limitations of Air Conduction Hearing Devices Using a LIGHT-DRIVEN Contact Hearing Aid. Poster presentation at The Triological Society, 120th Annual Meeting at COSM, Apr. 28, 2017; San Diego, CA.
Michaels, et al., Auditory Epithelial Migration on the Human Tympanic Membrane: II. The Existence of Two Discrete Migratory Pathways and Their Embryologic Correlates, The American Journal of Anatomy 189:189-200 (1990).
Moore, et al. Perceived naturalness of spectrally distorted speech and music. J Acoust Soc Am. Jul. 2003;114(1):408-19.
Moore, et al. Spectro-temporal characteristics of speech at high frequencies, and the potential for restoration of audibility to people with mild-to-moderate hearing loss. Ear Hear. Dec. 2008;29(6):907-22. doi: 10.1097/AUD.0b013e31818246f6.
Moore. Loudness perception and intensity resolution. Cochlear Hearing Loss, Chapter 4, pp. 90-115, Whurr Publishers Ltd., London (1998).
Murphy M, Aksak B, Sitti M. Adhesion and anisotropic friction enhancements of angled heterogeneous micro-fiber arrays with spherical and spatula tips. J Adhesion Sci Technol, vol. 21, No. 12-13, p. 1281-1296, 2007.
Murugasu, et al. Malleus-to-footplate versus malleus-to-stapes-head ossicular reconstruction prostheses: temporal bone pressure gain measurements and clinical audiological data. Otol Neurotol. Jul. 2005; 2694):572-582.
Musicant, et al. Direction-Dependent Spectral Properties of Cat External Ear: New Data and Cross-Species Comparisons. J. Acostic. Soc. Am, May 10-13, 2002, vol. 87, No. 2, (Feb. 1990), pp. 757-781.
National Semiconductor, LM4673 Boomer: Filterless, 2.65W, Mono, Class D Audio Power Amplifier, [Data Sheet] downloaded from the Internet:<<http://www.national.com/ds/LM/LM4673.pdf>>; Nov. 1, 2007; 24 pages.
Nishihara, et al. Effect of changes in mass on middle ear function. Otolaryngol Head Neck Surg. Nov. 1993;109(5):889-910.
Notice of Allowance dated Sep. 29, 2017 for U.S. Appl. No. 14/813,301.
Notice of Allowance dated Nov. 7, 2017 forU.S. Appl. No. 14/813,301.
O'Connor, et al. Middle ear Cavity and Ear Canal Pressure-Driven Stapes Velocity Responses in Human Cadaveric Temporal Bones. J Acoust Soc Am. Sep. 2006;120(3):1517-28.
Office Action dated Sep. 29, 2016 for U.S. Appl. No. 14/813,301.
Park, et al. Design and analysis of a microelectromagnetic vibration transducer used as an implantable middle ear hearing aid. J. Micromech. Microeng. Vol. 12 (2002), pp. 505-511.
Perkins, et al. Light-based Contact Hearing Device: Characterization of available Feedback Gain Margin at two device microphone locations. Presented at AAO-HNSF Annual Meeting, 2013 (Vancouver).
Perkins, et al. The EarLens Photonic Transducer: Extended bandwidth. Presented at AAO-HNSF Annual Meeting, 2011 (San Francisco).
Perkins, et al. The EarLens System: New sound transduction methods. Hear Res. Feb. 2, 2010; 10 pages total.
Perkins, R. Earlens tympanic contact transducer: a new method of sound transduction to the human ear. Otolaryngol Head Neck Surg. Jun. 1996;114(6):720-8.
Poosanaas, et al. Influence of sample thickness on the performance of photostrictive ceramics, J. App. Phys. Aug. 1, 1998; 84(3):1508-1512.
Puria et al. A gear in the middle ear. ARO Denver CO, 2007b.
Puria, et al. Cues above 4 kilohertz can improve spatially separated speech recognition. The Journal of the Acoustical Society of America, 2011, 129, 2384.
Puria, et al. Extending bandwidth above 4 kHz improves speech understanding in the presence of masking speech. Association for Research in Otolaryngology Annual Meeting, 2012 (San Diego).
Puria, et al. Extending bandwidth provides the brain what it needs to improve hearing in noise. First international conference on cognitive hearing science for communication, 2011 (Linkoping, Sweden).
Puria, et al. Hearing Restoration: Improved Multi-talker Speech Understanding. 5th International Symposium on Middle Ear Mechanics In Research and Otology (MEMRO), Jun. 2009 (Stanford University).
Puria, et al. Imaging, Physiology and Biomechanics of the middle ear: Towards understating the functional consequences of anatomy. Stanford Mechanics and Computation Symposium, 2005, ed Fong J.
Puria, et al. Malleus-to-footplate ossicular reconstruction prosthesis positioning: cochleovestibular pressure optimization. Otol Nerotol. May 2005; 2693):368-379.
Puria, et al. Measurements and model of the cat middle ear: Evidence of tympanic membrane acoustic delay. J. Acoust. Soc. Am., 104(6):3463-3481 (Dec. 1998).
Puria, et al. Middle Ear Morphometry From Cadaveric Temporal Bone MicroCT Imaging. Proceedings of the 4th International Symposium, Zurich, Switzerland, Jul. 27-30, 2006, Middle Ear Mechanics in Research and Otology, pp. 259-268.
Puria, et al. Sound-Pressure Measurements In The Cochlear Vestibule of Human-Cadaver Ears. Journal of the Acoustical Society of America. 1997; 101 (5-1): 2754-2770.
Puria, et al. Temporal-Bone Measurements of the Maximum Equivalent Pressure Output and Maximum Stable Gain of a Light-Driven Hearing System That Mechanically Stimulates the Umbo. Otol Neurotol. Feb. 2016;37(2):160-6. doi: 10.1097/MAO.0000000000000941.
Puria, et al. The EarLens Photonic Hearing Aid. Association for Research in Otolaryngology Annual Meeting, 2012 (San Diego).
Puria, et al. The Effects of bandwidth and microphone location on understanding of masked speech by normal-hearing and hearing-impaired listeners. International Conference for Hearing Aid Research (IHCON) meeting, 2012 (Tahoe City).
Puria, et al. Tympanic-membrane and malleus-incus-complex co-adaptations for high-frequency hearing in mammals. Hear Res. May 2010;263(1-2):183-90. doi: 10.1016/j.heares.2009.10.013. Epub Oct. 28, 2009.
Puria, et al., Mechano-Acoustical Transformations in A. Basbaum et al., eds., The Senses: A Comprehensive Reference, v3, p. 165-202, Academic Press (2008).
Puria, S. Middle Ear Hearing Devices. Chapter 10. Part of the series Springer Handbook of Auditory Research pp. 273-308. Date: Feb. 9, 2013.
Puria. Measurements of human middle ear forward and reverse acoustics: implications for otoacoustic emissions. J Acoust Soc Am. May 2003;113(5):2773-89.
Qu, et al. Carbon Nanotube Arrays with Strong Shear Binding-On and Easy Normal Lifting-Off, Oct. 10, 2008 vol. 322 Science. 238-242.
R.P. Jackson, C. Chlebicki, T.B. Krasieva, R. Zalpuri, W.J. Triffo, S. Puria, “Multiphoton and Transmission Electron Microscopy of Collagen in Ex Vivo Tympanic Membranes,” Biomedeal Computation at STandford, Oct. 2008.
Robles, et al. Mechanics of the mammalian cochlea. Physiol Rev. Jul. 2001;81(3):1305-52.
Roush. SiOnyx Brings “Black Silicon” into the Light; Material Could Upend Solar, Imaging Industries. Xconomy, Oct. 12, 2008, retrieved from the Internet: www.xconomy.com/boston/2008/10/12/sionyx-brings-black-silicon-into-the-light¬material-could-upend-solar-imaging-industries> 4 pages total.
Rubinstein. How Cochlear Implants Encode Speech, CurrOpin Otolaryngol Head Neck Surg. Oct. 2004;12(5):444-8; retrieved from the Internet: www.ohsu.edu/nod/documents/week3/Rubenstein.pdf.
School of Physics Sydney, Australia. Acoustic Compliance, Inertance and Impedance. 1-6. (2018). http://www.animations.physics.unsw.edu.au/jw/compliance-inertance-impedance.htm.
Sekaric, et al. Nanomechanical resonant structures as tunable passive modulators. App. Phys. Lett. Nov. 2003; 80(19):3617-3619.
Shaw. Transformation of Sound Pressure Level From the Free Field to the Eardrum in the Horizontal Plane. J. Acoust. Soc. Am., vol. 56, No. 6, (Dec. 1974), 1848-1861.
Shih. Shape and displacement control of beams with various boundary conditions via photostrictive optical actuators. Proc. IMECE. Nov. 2003; 1-10.
Song, et al. The development of a non-surgical direct drive hearing device with a wireless actuator coupled to the tympanic membrane. Applied Acoustics. Dec. 31, 2013;74(12):1511-8.
Sound Design Technologies, —Voyager TDTM Open Platform DSP System for Ultra Low Power Audio Processing—GA3280 Data Sheet. Oct. 2007; retrieved from the Internet:<<http://www.sounddes.com/pdf/37601DOC.pdf>>, 15 page total.
Spolenak, et al. Effects of contact shape on the scaling of biological attachments. Proc. R. Soc. A. 2005;461:305-319.
Stenfelt, et al. Bone-Conducted Sound: Physiological and Clinical Aspects. Otology & Neurotology, Nov. 2005; 26 (6):1245-1261.
Struck, et al. Comparison of Real-world Bandwidth in Hearing Aids vs Earlens Light-driven Hearing Aid System. The Hearing Review. TechTopic: EarLens. Hearingreview.com. Mar. 14, 2017. pp. 24-28.
Stuchlik, et al. Micro-Nano Actuators Driven by Polarized Light. IEEE Proc. Sci. Meas. Techn. Mar. 2004; 151 (2):131-136.
Suski, et al. Optically activated ZnO/Si02/Si cantilever beams. Sensors and Actuators A (Physical), 0 (nr: 24). 2003; 221-225.
Takagi, et al. Mechanochemical Synthesis of Piezoelectric PLZT Powder. KONA. 2003; 51(21):234-241.
Thakoor, et al. Optical microactuation in piezoceramics. Proc. SPIE. Jul. 1998; 3328:376-391.
The Scientist and Engineers Guide to Digital Signal Processing, copyright 01997-1998 by Steven W. Smith, available online at www.DSPguide.com.
Thompson. Tutorial on microphone technologies for directional hearing aids. Hearing Journal. Nov. 2003; 56(11):14-16, 18, 20-21.
Tzou, et al. Smart Materials, Precision Sensors/Actuators, Smart Structures, and Structronic Systems. Mechanics of Advanced Materials and Structures. 2004; 11:367-393.
U.S. Appl. No. 15/890,185 Notice of Allowance dated May 14, 2019.
Uchino, et al. Photostricitve actuators. Ferroelectrics. 2001; 258:147-158.
Vickers, et al. Effects of Low-Pass Filtering on the Intelligibility of Speech in Quiet for People With and Without Dead Regions at High Frequencies. J. Acoust. Soc. Am. Aug. 2001; 110(2):1164-1175.
Vinge. Wireless Energy Transfer by Resonant Inductive Coupling. Master of Science Thesis. Chalmers University of Technology. 1-83 (2015).
Vinikman-Pinhasi, et al. Piezoelectric and Piezooptic Effects in Porous Silicon. Applied Physics Letters, Mar. 2006; 88(11): 11905-111906.
Wang, et al. Preliminary Assessment of Remote Photoelectric Excitation of an Actuator for a Hearing Implant. Proceeding of the 2005 IEEE, Engineering in Medicine and Biology 27th nnual Conference, Shanghai, China. Sep. 1-4, 2005; 6233-6234.
Web Books Publishing, “The Ear,” accessed online Jan. 22, 2013, available online Nov. 2, 2007 at http://www.web-books.com/eLibrary/Medicine/Physiology/Ear/Ear.htm.
Wiener, et al. On the Sound Pressure Transformation by the Head and Auditory Meatus of the Cat. Acta Otolaryngol. Mar. 1966; 61(3):255-269.
Wightman, et al. Monaural Sound Localization Revisited. J Acoust Soc Am. Feb. 1997;101(2):1050-1063.
Wiki. Sliding Bias Variant 1, Dynamic Hearing (2015).
Wikipedia. Inductive Coupling. 1-2 (Jan. 11, 2018). https://en.wikipedia.org/wiki/Inductive_coupling.
Wikipedia. Pulse-density Coupling. 1-4 (Apr. 6, 2017). https://en.wikipedia.org/wiki/Pulse-density_modulation.
Wikipedia. Resonant Inductive Coupling. 1-11 (Jan. 12, 2018). https://en.wikipedia.org/wiki/Resonant_inductive_coupling#cite_note-13.
Yao, et al. Adhesion and sliding response of a biologically inspired fibrillar surface: experimental observations, J. R. Soc. Interface (2008) 5, 723-733 doi:10.1098/rsif.2007.1225 Published online Oct. 30, 2007.
Yao, et al. Maximum strength for intermolecular adhesion of nanospheres at an optimal size. J. R. Soc. Interface doi:10.10981 rsif.2008.0066 Published online 2008.
Yi, et al. Piezoelectric Microspeaker with Compressive Nitride Diaphragm. The Fifteenth IEEE International Conference on Micro Electro Mechanical Systems, 2002; 260-263.
Yu, et al. Photomechanics: Directed bending of a polymer film by light. Nature. Sep. 2003; 425:145.
Co-pending U.S. Appl. No. 17/356,217, inventors Imatani; Kyle et al., filed Jun. 23, 2021.
European search report and opinion dated May 4, 2018 for EP Application No. 15821719.0.
Folkeard, et al. Detection, Speech Recognition, Loudness, and Preference Outcomes With a Direct Drive Hearing Aid: Effects of Bandwidth. Trends Hear. Jan.-Dec. 2021; 25: 1-17. doi: 10.1177/2331216521999139.
Knight, D. Diode detectors for RF measurement. Paper. Jan. 1, 2016. [Retrieved from 1-16 online] (retrieved Feb. 11, 2020) abstract, p. 1; section 1, p. 6; section 1.3, p. 9; section 3 voltage-double rectifier, p. 21; section 5, p. 27. URL: g3ynh.info/circuits/Diode_det.pdf.
Notice of Allowance dated Jul. 19, 2019 for U.S. Appl. No. 15/890,185.
Notice of Allowance dated Aug. 29, 2019 for U.S. Appl. No. 15/890,185.
Co-pending U.S. Appl. No. 17/412,850, inventors Flaherty; Bryan et al., filed on Aug. 26, 2021.
Related Publications (1)
Number Date Country
20200092664 A1 Mar 2020 US
Provisional Applications (1)
Number Date Country
62024275 Jul 2014 US
Continuations (3)
Number Date Country
Parent 15890185 Feb 2018 US
Child 16688774 US
Parent 14813301 Jul 2015 US
Child 15890185 US
Parent PCT/US2015/040397 Jul 2015 US
Child 14813301 US