Control circuit for a light source in an optical measurement system by applying voltage with a first polarity to start an emission of a light pulse and applying voltage with a second polarity to stop the emission of the light pulse

Information

  • Patent Grant
  • 11864867
  • Patent Number
    11,864,867
  • Date Filed
    Tuesday, March 16, 2021
    3 years ago
  • Date Issued
    Tuesday, January 9, 2024
    3 months ago
Abstract
An exemplary system includes a light source and a control circuit configured to apply voltage having a first polarity to the light source for a first time period to provide a threshold charge for the light source to start an emission of a light pulse that is directed at a target within a body. The control circuit is further configured to apply voltage having a second polarity opposite the first polarity to the light source for a second time period subsequent to the first time period to discharge the light source to stop the emission of the light pulse.
Description
BACKGROUND INFORMATION

Detecting neural activity in the brain (or any other turbid medium) is useful for medical diagnostics, imaging, neuroengineering, brain-computer interfacing, and a variety of other diagnostic and consumer-related applications. For example, it may be desirable to detect neural activity in the brain of a user to determine if a particular region of the brain has been impacted by reduced blood irrigation, a hemorrhage, or any other type of damage. As another example, it may be desirable to detect neural activity in the brain of a user and computationally decode the detected neural activity into commands that can be used to control various types of consumer electronics (e.g., by controlling a cursor on a computer screen, changing channels on a television, turning lights on, etc.).


Neural activity and other attributes of the brain may be determined or inferred by measuring responses of tissue within the brain to light pulses. Light pulses may be provided by light sources such as lasers that are controlled by control circuits of an optical measurement system.


A photodetector capable of detecting a single photon (i.e., a single particle of optical energy) is an example of a non-invasive detector that can be used in the optical measurement system to detect neural activity within the brain. An exemplary photodetector is implemented by a semiconductor-based single-photon avalanche diode (SPAD), which is capable of capturing individual photons with very high time-of-arrival resolution (a few tens of picoseconds).





BRIEF DESCRIPTION OF THE DRAWINGS

The accompanying drawings illustrate various embodiments and are a part of the specification. The illustrated embodiments are merely examples and do not limit the scope of the disclosure. Throughout the drawings, identical or similar reference numbers designate identical or similar elements.



FIG. 1 shows an exemplary optical measurement system.



FIG. 2 illustrates an exemplary detector architecture.



FIG. 3 illustrates an exemplary timing diagram for performing an optical measurement operation using an optical measurement system.



FIG. 4 illustrates a graph of an exemplary temporal point spread function that may be generated by an optical measurement system in response to a light pulse.



FIG. 5 shows an exemplary non-invasive wearable brain interface system.



FIG. 6 shows an exemplary wearable module assembly.



FIGS. 7-8 show exemplary control circuits for a laser diode.



FIG. 9 shows an exemplary timing diagram for the control circuit.



FIGS. 10-11 show exemplary control circuits for a laser diode.



FIGS. 12-17 illustrate embodiments of a wearable device that includes elements of the optical measurement systems described herein.



FIG. 18 illustrates an exemplary computing device.



FIG. 19 illustrates an exemplary method.





DETAILED DESCRIPTION

Systems, circuits, and methods controlling a light source (e.g., a laser diode) in an optical measurement system are described herein. For example, the systems, circuits, and methods described herein may be configured to control (e.g., drive) a laser diode to emit light pulses. The systems, circuits, and methods may control precise starting and stopping of the emission of the light pulses by controlling slew rates of current applied to the laser diode. The slew rates may be controlled by applying voltage having a first polarity to the laser diode and then applying voltage having a second polarity opposite the first polarity to the laser diode. In some examples, the voltage having the second polarity may be applied such that the current applied to the laser diode drops to a negative current, which may discharge the laser more rapidly than simply ceasing to apply the current. The slew rates may be further controlled by additional components of the control circuit, such as voltage levels provided by one or more voltage sources, inductors, capacitors, etc.


Such precise control of light pulse timing may provide light pulses that may enable accurate detection of neural activity. Additionally, calibrating the light pulses to a current profile or other characteristic of the laser diode may result in increased power efficiency. Further, elements and components of the circuits and systems described herein may provide for additional efficiencies in resources.


These and other advantages and benefits of the present systems, circuits, and methods are described more fully herein.



FIG. 1 shows an exemplary optical measurement system 100 configured to perform an optical measurement operation with respect to a body 102. Optical measurement system 100 may, in some examples, be portable and/or wearable by a user. Optical measurement systems that may be used in connection with the embodiments described herein are described more fully in U.S. patent application Ser. No. 17/176,315, filed Feb. 16, 2021; U.S. patent application Ser. No. 17/176,309, filed Feb. 16, 2021; U.S. patent application Ser. No. 17/176,460, filed Feb. 16, 2021; U.S. patent application Ser. No. 17/176,470, filed Feb. 16, 2021; U.S. patent application Ser. No. 17/176,487, filed Feb. 16, 2021; U.S. patent application Ser. No. 17/176,539, filed Feb. 16, 2021; U.S. patent application Ser. No. 17/176,560, filed Feb. 16, 2021; and U.S. patent application Ser. No. 17/176,466, filed Feb. 16, 2021, which applications are incorporated herein by reference in their entirety.


In some examples, optical measurement operations performed by optical measurement system 100 are associated with a time domain-based optical measurement technique. Example time domain-based optical measurement techniques include, but are not limited to, time-correlated single-photon counting (TCSPC), time domain near infrared spectroscopy (TD-NIRS), time domain diffusive correlation spectroscopy (TD-DCS), and time domain Digital Optical Tomography (TD-DOT). For example, TCSPC detects single photons and measures a time of arrival of the photons with respect to a reference signal (e.g., a light source). By repeating the light pulses, TCSPC may accumulate a sufficient number of photon events to statistically determine a histogram representing the distribution of detected photons. Based on the histogram of photon distribution, the response of tissue to light pulses may be determined in order to study the detected neural activity and/or other attributes of the brain.


As shown, optical measurement system 100 includes a detector 104 that includes a plurality of individual photodetectors (e.g., photodetector 106), a processor 108 coupled to detector 104, a light source 110, a controller 112, and optical conduits 114 and 116 (e.g., light pipes). However, one or more of these components may not, in certain embodiments, be considered to be a part of optical measurement system 100. For example, in implementations where optical measurement system 100 is wearable by a user, processor 108 and/or controller 112 may in some embodiments be separate from optical measurement system 100 and not configured to be worn by the user.


Detector 104 may include any number of photodetectors 106 as may serve a particular implementation, such as 2n photodetectors (e.g., 256, 512, . . . , 16384, etc.), where n is an integer greater than or equal to one (e.g., 4, 5, 8, 10, 11, 14, etc.). Photodetectors 106 may be arranged in any suitable manner.


Photodetectors 106 may each be implemented by any suitable circuit configured to detect individual photons of light incident upon photodetectors 106. For example, each photodetector 106 may be implemented by a single photon avalanche diode (SPAD) circuit and/or other circuitry as may serve a particular implementation.


Processor 108 may be implemented by one or more physical processing (e.g., computing) devices. In some examples, processor 108 may execute instructions (e.g., software) configured to perform one or more of the operations described herein.


Light source 110 may be implemented by any suitable component configured to generate and emit light. For example, light source 110 may be implemented by one or more laser diodes. In some examples, the light emitted by light source 110 is high coherence light (e.g., light that has a coherence length of at least 5 centimeters) at a predetermined center wavelength.


Light source 110 is controlled by controller 112, which may be implemented by any suitable computing device (e.g., processor 108), integrated circuit, and/or combination of hardware and/or software as may serve a particular implementation. In some examples, controller 112 is configured to control light source 110 by turning light source 110 on and off and/or setting an intensity of light generated by light source 110. Controller 112 may be manually operated by a user, or may be programmed to control light source 110 automatically.


Light emitted by light source 110 may travel via an optical conduit 114 (e.g., a light pipe, a light guide, a waveguide, a single-mode optical fiber, and/or or a multi-mode optical fiber) to body 102 of a subject. In cases where optical conduit 114 is implemented by a light guide, the light guide may be spring loaded and/or have a cantilever mechanism to allow for conformably pressing the light guide firmly against body 102.


Body 102 may include any suitable turbid medium. For example, in some implementations, body 102 is a head or any other body part of a human or other animal. Alternatively, body 102 may be a non-living object. For illustrative purposes, it will be assumed in the examples provided herein that body 102 is a human head.


As indicated by arrow 120, the light emitted by light source 110 enters body 102 at a first location 122 on body 102. Accordingly, a distal end of optical conduit 114 may be positioned at (e.g., right above or physically attached to) first location 122 (e.g., to a scalp of the subject). In some examples, the light may emerge from optical conduit 114 and spread out to a certain spot size on body 102 to fall under a predetermined safety limit.


As used herein, “distal” means nearer, along the optical path of the light emitted by light source 110 or the light received by detector 104, to the target (e.g., within body 102) than to light source 110 or detector 104. Thus, the distal end of optical conduit 114 is nearer to body 102 than to light source 110, and the distal end of optical conduit 116 is nearer to body 102 than to detector 104. Additionally, as used herein, “proximal” means nearer, along the optical path of the light emitted by light source 110 or the light received by detector 104, to light source 110 or detector 104 than to body 102. Thus, the proximal end of optical conduit 114 is nearer to light source 110 than to body 102, and the proximal end of optical conduit 116 is nearer to detector 104 than to body 102.


As shown, the distal end of optical conduit 116 (e.g., a light pipe, a single-mode optical fiber, and/or or a multi-mode optical fiber) is positioned at (e.g., right above or physically attached to) output location 126 on body 102. In this manner, optical conduit 116 may collect light 124 as it exits body 102 at location 126 and carry the light to detector 104. The light may pass through one or more lenses and/or other optical elements (not shown) that direct the light onto each of the photodetectors 106 included in detector 104.


Photodetectors 106 may be connected in parallel in detector 104. An output of each of photodetectors 106 may be accumulated to generate an accumulated output of detector 104. Processor 108 may receive the accumulated output and determine, based on the accumulated output, a temporal distribution of photons detected by photodetectors 106. Processor 108 may then generate, based on the temporal distribution, a histogram representing a light pulse response of a target (e.g., brain tissue, blood flow, etc.) in body 102. Example embodiments of accumulated outputs are described herein.



FIG. 2 illustrates an exemplary detector architecture 200 that may be used in accordance with the systems and methods described herein. As shown, architecture 200 includes a SPAD circuit 202 that implements photodetector 106, a control circuit 204, a time-to-digital converter (TDC) 206, and a signal processing circuit 208. Architecture 200 may include additional or alternative components as may serve a particular implementation.


In some examples, SPAD circuit 202 includes a SPAD and a fast gating circuit configured to operate together to detect a photon incident upon the SPAD. As described herein, SPAD circuit 202 may generate an output when SPAD circuit 202 detects a photon.


The fast gating circuit included in SPAD circuit 202 may be implemented in any suitable manner. For example, the fast gating circuit may include a capacitor that is pre-charged with a bias voltage before a command is provided to arm the SPAD. Gating the SPAD with a capacitor instead of with an active voltage source, such as is done in some conventional SPAD architectures, has a number of advantages and benefits. For example, a SPAD that is gated with a capacitor may be armed practically instantaneously compared to a SPAD that is gated with an active voltage source. This is because the capacitor is already charged with the bias voltage when a command is provided to arm the SPAD. This is described more fully in U.S. Pat. Nos. 10,158,038 and 10,424,683, which are incorporated herein by reference in their entireties.


In some alternative configurations, SPAD circuit 202 does not include a fast gating circuit. In these configurations, the SPAD included in SPAD circuit 202 may be gated in any suitable manner or be configured to operate in a free running mode with passive quenching.


Control circuit 204 may be implemented by an application specific integrated circuit (ASIC) or any other suitable circuit configured to control an operation of various components within SPAD circuit 202. For example, control circuit 204 may output control logic that puts the SPAD included in SPAD circuit 202 in either an armed or a disarmed state.


In some examples, control circuit 204 may control a gate delay, which specifies a predetermined amount of time control circuit 204 is to wait after an occurrence of a light pulse (e.g., a laser pulse) to put the SPAD in the armed state. To this end, control circuit 204 may receive light pulse timing information, which indicates a time at which a light pulse occurs (e.g., a time at which the light pulse is applied to body 102). Control circuit 204 may also control a programmable gate width, which specifies how long the SPAD is kept in the armed state before being disarmed.


Control circuit 204 is further configured to control signal processing circuit 208. For example, control circuit 204 may provide histogram parameters (e.g., time bins, number of light pulses, type of histogram, etc.) to signal processing circuit 208. Signal processing circuit 208 may generate histogram data in accordance with the histogram parameters. In some examples, control circuit 204 is at least partially implemented by controller 112.


TDC 206 is configured to measure a time difference between an occurrence of an output pulse generated by SPAD circuit 202 and an occurrence of a light pulse. To this end, TDC 206 may also receive the same light pulse timing information that control circuit 204 receives. TDC 206 may be implemented by any suitable circuitry as may serve a particular implementation.


Signal processing circuit 208 is configured to perform one or more signal processing operations on data output by TDC 206. For example, signal processing circuit 208 may generate histogram data based on the data output by TDC 206 and in accordance with histogram parameters provided by control circuit 204. To illustrate, signal processing circuit 208 may generate, store, transmit, compress, analyze, decode, and/or otherwise process histograms based on the data output by TDC 206. In some examples, signal processing circuit 208 may provide processed data to control circuit 204, which may use the processed data in any suitable manner. In some examples, signal processing circuit 208 is at least partially implemented by processor 108.


In some examples, each photodetector 106 (e.g., SPAD circuit 202) may have a dedicated TDC 206 associated therewith. For example, for an array of N photodetectors 106, there may be a corresponding array of N TDCs 206. Alternatively, a single TDC 206 may be associated with multiple photodetectors 106. Likewise, a single control circuit 204 and a single signal processing circuit 208 may be provided for a one or more photodetectors 106 and/or TDCs 206.



FIG. 3 illustrates an exemplary timing diagram 300 for performing an optical measurement operation using optical measurement system 100. Optical measurement system 100 may be configured to perform the optical measurement operation by directing light pulses (e.g., laser pulses) toward a target within a body (e.g., body 102). The light pulses may be short (e.g., 10-2000 picoseconds (ps)) and repeated at a high frequency (e.g., between 100,000 hertz (Hz) and 100 megahertz (MHz)). The light pulses may be scattered by the target and then detected by optical measurement system 100. Optical measurement system 100 may measure a time relative to the light pulse for each detected photon. By counting the number of photons detected at each time relative to each light pulse repeated over a plurality of light pulses, optical measurement system 100 may generate a histogram that represents a light pulse response of the target (e.g., a temporal point spread function (TPSF)). The terms histogram and TPSF are used interchangeably herein to refer to a light pulse response of a target.


For example, timing diagram 300 shows a sequence of light pulses 302 (e.g., light pulses 302-1 and 302-2) that may be applied to the target (e.g., tissue within a brain of a user, blood flow, a fluorescent material used as a probe in a body of a user, etc.). Timing diagram 300 also shows a pulse wave 304 representing predetermined gated time windows (also referred as gated time periods) during which photodetectors 106 are gated ON to detect photons. Referring to light pulse 302-1, light pulse 302-1 is applied at a time to. At a time t1, a first instance of the predetermined gated time window begins. Photodetectors 106 may be armed at time t1, enabling photodetectors 106 to detect photons scattered by the target during the predetermined gated time window. In this example, time t1 is set to be at a certain time after time to, which may minimize photons detected directly from the laser pulse, before the laser pulse reaches the target. However, in some alternative examples, time t1 is set to be equal to time to.


At a time t2, the predetermined gated time window ends. In some examples, photodetectors 106 may be disarmed at time t2. In other examples, photodetectors 106 may be reset (e.g., disarmed and re-armed) at time t2 or at a time subsequent to time t2. During the predetermined gated time window, photodetectors 106 may detect photons scattered by the target. Photodetectors 106 may be configured to remain armed during the predetermined gated time window such that photodetectors 106 maintain an output upon detecting a photon during the predetermined gated time window. For example, a photodetector 106 may detect a photon at a time t3, which is during the predetermined gated time window between times t1 and t2. The photodetector 106 may be configured to provide an output indicating that the photodetector 106 has detected a photon. The photodetector 106 may be configured to continue providing the output until time t2, when the photodetector may be disarmed and/or reset. Optical measurement system 100 may generate an accumulated output from the plurality of photodetectors. Optical measurement system 100 may sample the accumulated output to determine times at which photons are detected by photodetectors 106 to generate a TPSF.


As mentioned, in some alternative examples, photodetector 106 may be configured to operate in a free-running mode such that photodetector 106 is not actively armed and disarmed (e.g., at the end of each predetermined gated time window represented by pulse wave 304). In contrast, while operating in the free-running mode, photodetector 106 may be configured to reset within a configurable time period after an occurrence of a photon detection event (i.e., after photodetector 106 detects a photon) and immediately begin detecting new photons. However, only photons detected within a desired time window (e.g., during each gated time window represented by pulse wave 304) may be included in the TPSF.



FIG. 4 illustrates a graph 400 of an exemplary TPSF 402 that may be generated by optical measurement system 100 in response to a light pulse 404 (which, in practice, represents a plurality of light pulses). Graph 400 shows a normalized count of photons on a y-axis and time bins on an x-axis. As shown, TPSF 402 is delayed with respect to a temporal occurrence of light pulse 404. In some examples, the number of photons detected in each time bin subsequent to each occurrence of light pulse 404 may be aggregated (e.g., integrated) to generate TPSF 402. TPSF 402 may be analyzed and/or processed in any suitable manner to determine or infer detected neural activity.


Optical measurement system 100 may be implemented by or included in any suitable device. For example, optical measurement system 100 may be included, in whole or in part, in a non-invasive wearable device (e.g., a headpiece) that a user may wear to perform one or more diagnostic, imaging, analytical, and/or consumer-related operations. The non-invasive wearable device may be placed on a user's head or other part of the user to detect neural activity. In some examples, such neural activity may be used to make behavioral and mental state analysis, awareness and predictions for the user.


Mental state described herein refers to the measured neural activity related to physiological brain states and/or mental brain states, e.g., joy, excitement, relaxation, surprise, fear, stress, anxiety, sadness, anger, disgust, contempt, contentment, calmness, focus, attention, approval, creativity, positive or negative reflections/attitude on experiences or the use of objects, etc. Further details on the methods and systems related to a predicted brain state, behavior, preferences, or attitude of the user, and the creation, training, and use of neuromes can be found in U.S. Provisional Patent Application No. 63/047,991, filed Jul. 3, 2020. Exemplary measurement systems and methods using biofeedback for awareness and modulation of mental state are described in more detail in U.S. patent application Ser. No. 16/364,338, filed Mar. 26, 2019, published as US2020/0196932A1. Exemplary measurement systems and methods used for detecting and modulating the mental state of a user using entertainment selections, e.g., music, film/video, are described in more detail in U.S. patent application Ser. No. 16/835,972, filed Mar. 31, 2020, published as US2020/0315510A1. Exemplary measurement systems and methods used for detecting and modulating the mental state of a user using product formulation from, e.g., beverages, food, selective food/drink ingredients, fragrances, and assessment based on product-elicited brain state measurements are described in more detail in U.S. patent application Ser. No. 16/853,614, filed Apr. 20, 2020, published as US2020/0337624A1. Exemplary measurement systems and methods used for detecting and modulating the mental state of a user through awareness of priming effects are described in more detail in U.S. patent application Ser. No. 16/885,596, filed May 28, 2020, published as US2020/0390358A1. These applications and corresponding U.S. publications are incorporated herein by reference in their entirety.



FIG. 5 shows an exemplary non-invasive wearable brain interface system 500 (“brain interface system 500”) that implements optical measurement system 100 (shown in FIG. 1). As shown, brain interface system 500 includes a head-mountable component 502 configured to be attached to a user's head. Head-mountable component 502 may be implemented by a cap shape that is worn on a head of a user. Alternative implementations of head-mountable component 502 include helmets, beanies, headbands, other hat shapes, or other forms conformable to be worn on a user's head, etc. Head-mountable component 502 may be made out of any suitable cloth, soft polymer, plastic, hard shell, and/or any other suitable material as may serve a particular implementation. Examples of headgears used with wearable brain interface systems are described more fully in U.S. Pat. No. 10,340,408, incorporated herein by reference in its entirety.


Head-mountable component 502 includes a plurality of detectors 504, which may implement or be similar to detector 104, and a plurality of light sources 506, which may be implemented by or be similar to light source 110. It will be recognized that in some alternative embodiments, head-mountable component 502 may include a single detector 504 and/or a single light source 506.


Brain interface system 500 may be used for controlling an optical path to the brain and for transforming photodetector measurements into an intensity value that represents an optical property of a target within the brain. Brain interface system 500 allows optical detection of deep anatomical locations beyond skin and bone (e.g., skull) by extracting data from photons originating from light source 506 and emitted to a target location within the user's brain, in contrast to conventional imaging systems and methods (e.g., optical coherence tomography (OCT)), which only image superficial tissue structures or through optically transparent structures.


Brain interface system 500 may further include a processor 508 configured to communicate with (e.g., control and/or receive signals from) detectors 504 and light sources 506 by way of a communication link 510. Communication link 510 may include any suitable wired and/or wireless communication link. Processor 508 may include any suitable housing and may be located on the user's scalp, neck, shoulders, chest, or arm, as may be desirable. In some variations, processor 508 may be integrated in the same assembly housing as detectors 504 and light sources 506.


As shown, brain interface system 500 may optionally include a remote processor 512 in communication with processor 508. For example, remote processor 512 may store measured data from detectors 504 and/or processor 508 from previous detection sessions and/or from multiple brain interface systems (not shown). Power for detectors 504, light sources 506, and/or processor 508 may be provided via a wearable battery (not shown). In some examples, processor 508 and the battery may be enclosed in a single housing, and wires carrying power signals from processor 508 and the battery may extend to detectors 504 and light sources 506. Alternatively, power may be provided wirelessly (e.g., by induction).


In some alternative embodiments, head mountable component 502 does not include individual light sources. Instead, a light source configured to generate the light that is detected by detector 504 may be included elsewhere in brain interface system 500. For example, a light source may be included in processor 508 and coupled to head mountable component 502 through optical connections.


Each of the light sources described herein may be implemented by any suitable device. For example, a light source as used herein may be, for example, a distributed feedback (DFB) laser, a super luminescent diode (SLD), a light emitting diode (LED), a diode-pumped solid-state (DPSS) laser, a laser diode (LD), a super luminescent light emitting diode (sLED), a vertical-cavity surface-emitting laser (VCSEL), a titanium sapphire laser, a micro light emitting diode (mLED), and/or any other suitable laser or light source.


Optical measurement system 100 may alternatively be included in a non-wearable device (e.g., a medical device and/or consumer device that is placed near the head or other body part of a user to perform one or more diagnostic, imaging, and/or consumer-related operations). Optical measurement system 100 may alternatively be included in a sub-assembly enclosure of a wearable invasive device (e.g., an implantable medical device for brain recording and imaging).


Optical measurement system 100 may be modular in that one or more components of optical measurement system 100 may be removed, changed out, or otherwise modified as may serve a particular implementation. Additionally or alternatively, optical measurement system 100 may be modular such that one or more components of optical measurement system 100 may be housed in a separate housing (e.g., module) and/or may be movable relative to other components. Exemplary modular multimodal measurement systems are described in more detail in U.S. patent application Ser. No. 17/176,460, filed Feb. 16, 2021, U.S. patent application Ser. No. 17/176,470, filed Feb. 16, 2021, U.S. patent application Ser. No. 17/176,487, filed Feb. 16, 2021, U.S. Provisional Patent Application No. 63/038,481, filed Jun. 12, 2020, and U.S. patent application Ser. No. 17/176,560, filed Feb. 16, 2021, which applications are incorporated herein by reference in their respective entireties.


To illustrate, FIG. 6 shows an exemplary wearable module assembly 600 (“assembly 600”) that implements one or more of the optical measurement features described herein. Assembly 600 may be worn on the head or any other suitable body part of the user. As shown, assembly 600 may include a plurality of modules 602 (e.g., modules 602-1 through 602-3). While three modules 602 are shown to be included in assembly 600 in FIG. 6, in alternative configurations, any number of modules 602 (e.g., a single module up to sixteen or more modules) may be included in assembly 600. Moreover, while modules 602 are shown to be adjacent to and touching one another, modules 602 may alternatively be spaced apart from one another (e.g., in implementations where modules 602 are configured to be inserted into individual slots or cutouts of the headgear).


The wearable module assembly 600 may also conform to three-dimensional surface geometries, such as a user's head. Exemplary wearable module assemblies comprising a plurality of wearable modules are described in more detail in U.S. Provisional Patent Application No. 62/992,550, filed Mar. 20, 2020, which application is incorporated herein by reference in its entirety.


Each module 602 includes a source 604 and a plurality of detectors 606 (e.g., detectors 606-1 through 606-6). Source 604 may be implemented by one or more light sources similar to light source 110. Each detector 606 may implement or be similar to detector 104 and may include a plurality of photodetectors (e.g., SPADs) as well as other circuitry (e.g., TDCs). As shown, detectors 606 are arranged around and substantially equidistant from source 604. In other words, the spacing between a light source (i.e., a distal end portion of a light source optical conduit) and the detectors (i.e., distal end portions of optical conduits for each detector) are maintained at the same fixed distance on each module to ensure homogeneous coverage over specific areas and to facilitate processing of the detected signals. The fixed spacing also provides consistent spatial (lateral and depth) resolution across the target area of interest, e.g., brain tissue. Moreover, maintaining a known distance between the light emitter and the detector allows subsequent processing of the detected signals to infer spatial (e.g., depth localization, inverse modeling) information about the detected signals. Detectors 606 may be alternatively disposed as may serve a particular implementation.



FIG. 7 shows an exemplary control circuit 700 coupled to a laser diode 702. Laser diode 702 may be an implementation of light source 110 of optical measurement system 100 (shown in FIG. 1). Control circuit 700 may be implemented by controller 112 or a portion of controller 112 (shown in FIG. 1). While the light source in FIG. 7 is shown as a laser diode, the light source may be any suitable light source that may be controlled by control circuits as described herein.


Control circuit 700 includes a charging voltage source 704, a discharging voltage source 706, and a switching circuit 708 (e.g., switching circuit 708-1 and 708-2). Control circuit 700 may include additional or alternative components as may serve a particular implementation.


Charging voltage source 704 and discharging voltage source 706 may be implemented by any suitable component and/or circuit that provides a voltage. Switching circuit 708 may be configured to selectively couple charging voltage source 704 and discharging voltage source 706 to laser diode 702 to charge and discharge laser diode 702.


Laser diode 702 may be configured to emit light once a current applied to laser diode 702 meets a threshold current and supplies a threshold charge to laser diode 702. While the current applied to laser diode 702 supplies at least the threshold charge, laser diode 702 may be configured to continue to emit light. Once the current applied to laser diode 702 is reduced and laser diode 702 is discharged to below the threshold charge, laser diode 702 may stop emitting light. Thus, by controlling the current applied to laser diode 702, control circuit 700 may cause laser diode 702 to emit a light pulse.


Control circuit 700 may be configured to control the current applied to laser diode 702 by applying a voltage having a first polarity to laser diode 702 to increase the current applied to laser diode 702 for a first period of time so that the current applied to laser diode 702 will provide a threshold charge to start emission of a light pulse. Subsequently, control circuit 700 may be configured to apply a voltage having an opposite polarity to laser diode 702 to reduce the current applied to laser diode 702 to discharge laser diode 702 and stop the emission of the light pulse.


For example, charging voltage source 704 may be configured to apply the voltage having the first polarity to laser diode 702. Switching circuit 708 may be configured to couple charging voltage source 704 to laser diode 702 during the first time period. Discharging voltage source 706 may be configured to apply the voltage having the opposite polarity to laser diode 702. Switching circuit 708 may be configured to couple discharging voltage source 706 to laser diode 702 during the second time period. Examples of switching circuit 708 are described herein.


For instance, FIG. 8 shows an exemplary configuration 800 of control circuit 700. Configuration 800 includes laser diode 702, charging voltage source 704, and discharging voltage source 706. Configuration 800 further includes an implementation of switching circuit 708 that includes a first set of transistors 802 (e.g., transistor 802-1 and transistor 802-2) and a second set of transistors 804 (e.g., transistor 804-1 and transistor 804-2). Configuration 800 further includes a reverse diode 806. Reverse diode 806 may be coupled antiparallel to laser diode 702 to protect laser diode 702 against a reverse voltage applied accidentally or induced by stray inductances in control circuit 700. In some alternative implementations, control circuit 700 does not include reverse diode 806.


Transistors 802 are controlled by a control signal 808, while transistors 804 are controlled by a control signal 810. Transistors 802 may be configured such that control signal 808 may turn off one of transistors 802 while turning on the other of transistors 802 and vice versa. Transistors 804 may be configured to be similarly controlled by control signal 810. For example, in configuration 800, transistor 802-1 and transistor 804-1 are P-channel metal-oxide-semiconductor field-effect transistors (MOSFETs). Transistor 802-2 and transistor 804-2 are N-channel MOSFETs. Thus, a high signal provided as control signal 808 may turn off transistor 802-1 and turn on transistor 802-2, while a low signal provided as control signal 808 may turn on transistor 802-1 and turn off transistor 802-2. Similarly, a high signal provided as control signal 810 may turn off transistor 804-1 and turn on transistor 804-2, while a low signal provided as control signal 810 may turn on transistor 804-1 and turn off transistor 804-2. Based on timings of control signal 808 and control signal 810, voltages of opposite polarities may be applied to laser diode 702 to control a current applied to laser diode 702 and consequently, a light pulse emitted by laser diode 702.



FIG. 9 shows an exemplary timing diagram 900 for a control circuit such as configuration 800. Timing diagram 900 includes a graph 902-1 showing timing of control signal 808, a graph 902-2 showing timing of control signal 810, and a graph 902-3 showing timing of a resulting current applied to laser diode 702.


Graph 902-1 includes an x-axis 904-1 representing time (in nanoseconds (ns)) and a y-axis 906-1 representing voltage (in volts (V)) provided as control signal 808. Graph 902-1 further includes a line 908-1 that shows control signal 808 output over time. Similarly, graph 902-2 includes an x-axis 904-2 representing a same timeline as x-axis 904-1 of graph 902-1 and a y-axis 906-2 representing voltage (V) provided as control signal 810. Graph 902-2 further includes a line 908-2 that shows control signal 810 over time. Graph 902-3 includes an x-axis 904-3 representing the same timeline as x-axis 904-1 and a y-axis 906-3 representing a current (in amperes (A)) applied to laser diode 702. Graph 902-3 further includes a line 908-3 that shows the current over time.


In this example, for a first time period from time 0 ns to 2 ns, line 908-1 shows the voltage of control signal 808 is 0 V, thus providing a low signal to transistors 802. As a result, transistor 802-1 is on and transistor 802-2 is off. During the same first time period, line 908-2 shows the voltage of control signal 810 is at 20 V, which may be a voltage level provided by discharging voltage source 706. Thus, control signal 810 provides a high signal to transistors 804, turning off transistor 804-1 and turning on transistor 804-2. Consequently, charging voltage source 704 is coupled to laser diode 702 through transistor 802-1 and then to ground through transistor 804-2, allowing the current applied to laser diode 702 to increase, as shown by line 908-3, from 0 A to 0.8 A. Stray inductances in control circuit 700 may affect a slew rate of the current increase, and as a result, a duration of the first time period.


By 2 ns, laser diode 702 may be sufficiently charged to begin emitting a light pulse. At this time, the current applied to laser diode 702 may be reduced so that the emission of the light pulse is stopped to provide a light pulse with a short duration without oscillation. As shown, from 2 ns to 2.5 ns may be a second time period during which line 908-1 shows the voltage of control signal 808 is set to 5 V, which may be a voltage level provided by charging voltage source 704. Thus, control signal 808 provides a high signal to transistors 802, turning off transistor 802-1 and turning on transistor 802-2. Meanwhile, line 908-2 shows the voltage of control signal 810 is set to 0 V, providing a low signal to transistors 804. As a result, transistor 804-1 turns on and transistor 804-2 turns off. Consequently, discharging voltage source 706 is coupled to laser diode 702 through transistor 804-1 and then to ground through transistor 802-2, which reverses a polarity of the voltage applied to laser diode 702. As a result, the current applied to laser diode 702 drops, as shown by line 908-3, from 0.8 A to −0.2 A. Such a drop in the current applied to laser diode 702 may rapidly discharge laser diode 702 to stop the emission of the light pulse.


Once the light pulse emission is stopped at 2.5 ns, control signal 808 may remain high while control signal 810 is also set to high, as shown by lines 908-1 and 908-2, respectively. Having both control signals 808 and 810 set to high results in transistors 802-1 and 804-1 turning off and transistors 802-2 and 804-2 turning on. Thus, laser diode 702 is disconnected from both charging voltage source 704 and discharging voltage source 706 and the current applied to laser diode 702 decays to 0 A, as shown by line 908-3.


In this manner, control circuit 700 may drive laser diode 702 to emit a light pulse of any suitable duration. For instance, a charging slew rate of the increasing current applied to laser diode 702 during the first time period may be controlled based on a voltage level output by charging voltage source 704. By increasing the output voltage from 5 V to a higher voltage level, the charging slew rate may be increased so that the first time period during which the current applied to laser diode 702 increases is shortened. Conversely, decreasing the output voltage may decrease the charging slew rate and lengthen the first time period. Likewise, a discharging slew rate of the decreasing current applied to laser diode 702 during the second time period may be controlled based on a voltage level output by discharging voltage source 706. The output voltage levels for either or both of charging voltage source 704 and discharging voltage source 706 may be calibrated based on a current profile or any other suitable characteristic of laser diode 702 and/or driving conditions (e.g., temperature or any other suitable condition) of laser diode 702. Such calibration may result in a reduction of power dissipation of an overall circuit including control circuit 700 and laser diode 702. Additionally or alternatively, charging voltage source 704 and/or discharging voltage source 706 may be adjustable voltage sources that are included in a closed-loop system. The closed-loop system may include one or more photodetectors (e.g., SPADs) that provide output regarding the light pulses generated by laser diode 702 as feedback to control circuit 700. Based on the feedback, charging voltage source 704 and/or discharging voltage source 706 may be adjusted to adjust the charging and/or discharging slew rates.



FIG. 10 shows another exemplary configuration 1000 of control circuit 700. Configuration 1000 includes laser diode 702, charging voltage source 704, and discharging voltage source 706. Configuration 1000 also includes transistors 802 controlled by control signal 808, transistors 804 controlled by control signal 810, and reverse diode 806. Configuration further includes a capacitor 1002, which may be configured to provide direct current (DC) decoupling and provide a safety barrier in case one or more of transistors 802 and transistors 804 may fail. Capacitor 1002 may also be configured to provide a charge to laser diode 702, which may allow for a margin of error in timing accuracy of control signal 808 and/or control signal 810.


For example, capacitor 1002 may be charged through reverse diode 806 from discharging voltage source 706 by turning on transistor 804-1 and transistor 802-2 and turning off transistor 802-1 and transistor 804-2. Subsequently, transistor 804-2 may be turned on and transistor 804-1 may be turned off. As a result, capacitor 1002 may discharge to laser diode 702. Additionally, transistor 802-1 may be turned on and transistor 802-2 turned off so that charging voltage source 704 may also be coupled to laser diode 702 to apply additional voltage.



FIG. 11 shows another exemplary control circuit 1100 coupled to laser diode 702. Control circuit 1100 may be configured to control laser diode 702 in a manner similar to control circuit 700, reversing a polarity of a voltage applied to laser diode 702 to control slew rates of a current applied to laser diode 702. In contrast to control circuit 700, however, control circuit 1100 includes one voltage source 1102. Voltage source 1102 is selectively coupled to laser diode 702 via switching circuits 1104 and 1106. Control circuit 1100 further includes inductors 1108 and 1110.


Switching circuits 1104 and 1106 may be implemented by any suitable component or components configured to allow laser diode 702 to selectively couple to a cathode of voltage source 1102, an anode of voltage source 1102, or neither. Switching circuits 1104 and 1106 may be controlled in a manner similar to control circuit 700 (e.g., as described with configuration 800) to apply voltage having a first polarity to laser diode 702 to provide a threshold charge for laser diode 702 to start an emission of a light pulse and then apply voltage having a second polarity opposite the first polarity to laser diode 702 to discharge laser diode 702 to stop the emission of the light pulse. For example, switching circuit 1104 may couple the cathode of voltage source 1102 to laser diode 702 while switching circuit 1106 couples the anode of voltage source 1102 to laser diode 702. Thus, voltage having the first polarity is applied to laser diode 702 to provide the threshold charge for laser diode 702. Subsequently, switching circuit 1104 may couple the anode of voltage source 1102 to laser diode 702 while switching circuit 1106 couples the cathode of voltage source 1102 to laser diode 702 to apply voltage having the second polarity to laser diode 702 to discharge laser diode 702. Once laser diode 702 is discharged, switching circuits 1104 and 1106 may couple laser diode 702 to neither the cathode nor the anode of voltage source 1102, allowing current applied to laser diode 702 to decay to zero.


Inductor 1108 may be configured to control a charging slew rate of the current applied to laser diode 702 as the current increases to start the emission of the light pulse. Similarly, inductor 1110 may be configured to control a discharging slew rate of the current applied to laser diode 702 as the current decreases to stop the emission of the light pulse. In alternative examples, inductor 1108 and/or inductor 1110 may be not included. Additionally, a similar inductor or inductors may be included in configuration 800 or configuration 1000 to further control the charging slew rate or the discharging slew rate.


As mentioned, optical measurement system 100 may be at least partially wearable by a user. For example, optical measurement system 100 may be implemented by a wearable device configured to be worn by a user (e.g., a head-mountable component configured to be worn on a head of the user). The wearable device may include one or more photodetectors and/or any of the other components described herein. In some examples, one or more components (e.g., processor 108, controller 112, etc.) may not be included in the wearable device and/or included in a separate wearable device than the wearable device in which the one or more photodetectors are included. In these examples, one or more communication interfaces (e.g., cables, wireless interfaces, etc.) may be used to facilitate communication between the various components.



FIGS. 12-17 illustrate embodiments of a wearable device 1200 that includes elements of the optical detection systems described herein. In particular, the wearable devices 1200 include a plurality of modules 1202, similar to the modules shown in FIG. 6 as described herein. For example, each module 1202 includes a source 604 and a plurality of detectors 606 (e.g., detectors 606-1 through 606-6). Source 604 may be implemented by one or more light sources similar to light source 110. Each detector 606 may implement or be similar to detector 104 and may include a plurality of photodetectors. The wearable devices 1200 may each also include a controller (e.g., controller 112) and a processor (e.g., processor 108) and/or be communicatively connected to a controller and processor. In general, wearable device 1200 may be implemented by any suitable headgear and/or clothing article configured to be worn by a user. The headgear and/or clothing article may include batteries, cables, and/or other peripherals for the components of the optical measurement systems described herein.



FIG. 12 illustrates an embodiment of a wearable device 1200 in the form of a helmet with a handle 1204. A cable 1206 extends from the wearable device 1200 for attachment to a battery or hub (with components such as a processor or the like). FIG. 13 illustrates another embodiment of a wearable device 1200 in the form of a helmet showing a back view. FIG. 14 illustrates a third embodiment of a wearable device 1200 in the form of a helmet with the cable 1206 leading to a wearable garment 1208 (such as a vest or partial vest) that can include a battery or a hub. Alternatively or additionally, the wearable device 1200 can include a crest 1210 or other protrusion for placement of the hub or battery.



FIG. 15 illustrates another embodiment of a wearable device 1200 in the form of a cap with a wearable garment 1208 in the form of a scarf that may contain or conceal a cable, battery, and/or hub. FIG. 16 illustrates additional embodiments of a wearable device 1200 in the form of a helmet with a one-piece scarf 1208 or two-piece scarf 1208-1. FIG. 17 illustrates an embodiment of a wearable device 1200 that includes a hood 1210 and a beanie 1212 which contains the modules 1202, as well as a wearable garment 1208 that may contain a battery or hub.


In some examples, a non-transitory computer-readable medium storing computer-readable instructions may be provided in accordance with the principles described herein. The instructions, when executed by a processor of a computing device, may direct the processor and/or computing device to perform one or more operations, including one or more of the operations described herein. Such instructions may be stored and/or transmitted using any of a variety of known computer-readable media.


A non-transitory computer-readable medium as referred to herein may include any non-transitory storage medium that participates in providing data (e.g., instructions) that may be read and/or executed by a computing device (e.g., by a processor of a computing device). For example, a non-transitory computer-readable medium may include, but is not limited to, any combination of non-volatile storage media and/or volatile storage media. Exemplary non-volatile storage media include, but are not limited to, read-only memory, flash memory, a solid-state drive, a magnetic storage device (e.g. a hard disk, a floppy disk, magnetic tape, etc.), ferroelectric random-access memory (“RAM”), and an optical disc (e.g., a compact disc, a digital video disc, a Blu-ray disc, etc.). Exemplary volatile storage media include, but are not limited to, RAM (e.g., dynamic RAM).



FIG. 18 illustrates an exemplary computing device 1800 that may be specifically configured to perform one or more of the processes described herein. Any of the systems, units, computing devices, and/or other components described herein may be implemented by computing device 1800.


As shown in FIG. 18, computing device 1800 may include a communication interface 1802, a processor 1804, a storage device 1806, and an input/output (“I/O”) module 1808 communicatively connected one to another via a communication infrastructure 1810. While an exemplary computing device 1800 is shown in FIG. 18, the components illustrated in FIG. 18 are not intended to be limiting. Additional or alternative components may be used in other embodiments. Components of computing device 1800 shown in FIG. 18 will now be described in additional detail.


Communication interface 1802 may be configured to communicate with one or more computing devices. Examples of communication interface 1802 include, without limitation, a wired network interface (such as a network interface card), a wireless network interface (such as a wireless network interface card), a modem, an audio/video connection, and any other suitable interface.


Processor 1804 generally represents any type or form of processing unit capable of processing data and/or interpreting, executing, and/or directing execution of one or more of the instructions, processes, and/or operations described herein. Processor 1804 may perform operations by executing computer-executable instructions 1812 (e.g., an application, software, code, and/or other executable data instance) stored in storage device 1806.


Storage device 1806 may include one or more data storage media, devices, or configurations and may employ any type, form, and combination of data storage media and/or device. For example, storage device 1806 may include, but is not limited to, any combination of the non-volatile media and/or volatile media described herein. Electronic data, including data described herein, may be temporarily and/or permanently stored in storage device 1806. For example, data representative of computer-executable instructions 1812 configured to direct processor 1804 to perform any of the operations described herein may be stored within storage device 1806. In some examples, data may be arranged in one or more databases residing within storage device 1806.


I/O module 1808 may include one or more I/O modules configured to receive user input and provide user output. I/O module 1808 may include any hardware, firmware, software, or combination thereof supportive of input and output capabilities. For example, I/O module 1808 may include hardware and/or software for capturing user input, including, but not limited to, a keyboard or keypad, a touchscreen component (e.g., touchscreen display), a receiver (e.g., an RF or infrared receiver), motion sensors, and/or one or more input buttons.


I/O module 1808 may include one or more devices for presenting output to a user, including, but not limited to, a graphics engine, a display (e.g., a display screen), one or more output drivers (e.g., display drivers), one or more audio speakers, and one or more audio drivers. In certain embodiments, I/O module 1808 is configured to provide graphical data to a display for presentation to a user. The graphical data may be representative of one or more graphical user interfaces and/or any other graphical content as may serve a particular implementation.



FIG. 19 illustrates an exemplary method 1900 that may be performed by control circuit 700 and/or any implementation thereof. While FIG. 19 illustrates exemplary operations according to one embodiment, other embodiments may omit, add to, reorder, and/or modify any of the operations shown in FIG. 19.


In operation 1902, a control circuit applies voltage having a first polarity to a light source for a first time period to provide a threshold charge for the light source to start an emission of a light pulse. Operation 1902 may be performed in any of the ways described herein.


In operation 1904, the control circuit applies voltage having a second polarity opposite the first polarity to the light source for a second time period subsequent to the first time period to discharge the light source to stop the emission of the light pulse. Operation 1904 may be performed in any of the ways described herein.


An exemplary optical measurement system described herein includes a light source and a control circuit. The control circuit is configured to apply voltage having a first polarity to the light source for a first time period to provide a threshold charge for the light source to start an emission of a light pulse that is directed at a target within a body. The control circuit is further configured to apply voltage having a second polarity opposite the first polarity to the light source for a second time period subsequent to the first time period to discharge the light source to stop the emission of the light pulse.


An exemplary system described herein includes a single photon avalanche diode (SPAD) configured to detect a photon from a light pulse after the light pulse reflects off a target within a body, a fast gating circuit configured to arm and disarm the SPAD, a light source, and a control circuit. The control circuit is configured to apply voltage having a first polarity to the light source for a first time period to provide a threshold charge for the light source to start an emission of the light pulse. The control circuit is further configured to apply voltage having a second polarity opposite the first polarity to the light source for a second time period subsequent to the first time period to discharge the light source to stop the emission of the light pulse.


An exemplary wearable system for use by a user described herein includes a head-mountable component configured to be attached to a head of the user, a light source, and a control circuit. The head-mountable component includes a photodetector configured to detect a photon from a light pulse after the light pulse reflects off a target within the head. The control circuit is configured to apply voltage having a first polarity to the light source for a first time period to provide a threshold charge for the light source to start an emission of a light pulse. The control circuit is further configured to apply voltage having a second polarity opposite the first polarity to the light source for a second time period subsequent to the first time period to discharge the light source to stop the emission of the light pulse.


An exemplary method described herein includes applying, by a control circuit, voltage having a first polarity to a light source for a first time period to provide a threshold charge for the light source to start an emission of a light pulse. The method further includes applying, by the control circuit, voltage having a second polarity opposite the first polarity to the light source for a second time period subsequent to the first time period to discharge the light source to stop the emission of the light pulse.


In the preceding description, various exemplary embodiments have been described with reference to the accompanying drawings. It will, however, be evident that various modifications and changes may be made thereto, and additional embodiments may be implemented, without departing from the scope of the invention as set forth in the claims that follow. For example, certain features of one embodiment described herein may be combined with or substituted for features of another embodiment described herein. The description and drawings are accordingly to be regarded in an illustrative rather than a restrictive sense.

Claims
  • 1. An optical measurement system comprising: a light source; anda control circuit configured to: apply voltage having a first polarity to the light source for a first time period to provide a threshold charge for the light source to start an emission of a light pulse, andapply voltage having a second polarity opposite the first polarity to the light source for a second time period subsequent to the first time period to discharge the light source to stop the emission of the light pulse.
  • 2. The optical measurement system of claim 1, wherein the second time period is at least of a duration such that a negative current is applied to the light source.
  • 3. The optical measurement system of claim 1, wherein the control circuit comprises: a first voltage source configured to apply the voltage having the first polarity;a second voltage source configured to apply the voltage having the second polarity; anda switching circuit configured to selectively couple the first voltage source to the light source and the second voltage source to the light source.
  • 4. The optical measurement system of claim 3, wherein: the switching circuit includes: a first transistor and a second transistor coupled to the first voltage source and the light source, anda third transistor and a fourth transistor coupled to the second voltage source and the light source;the first transistor and the fourth transistor are on and the second transistor and the third are off during the first time period; andthe second transistor and the third transistor are on and the first transistor and the fourth transistor are off during the second time period.
  • 5. The optical measurement system of claim 3, wherein: the first voltage source is adjustable to control a charging slew rate of a current applied to the light source that increases to start the emission of the light pulse; andand the second voltage source is adjustable to control a discharging slew rate of the current applied to the light source that decreases to stop the emission of the light pulse.
  • 6. The optical measurement system of claim 1, wherein the control circuit comprises an inductor coupled to the light source to control a slew rate of at least one of: increasing a current applied to the light source; anddecreasing the current applied to the light source.
  • 7. The optical measurement system of claim 1, wherein at least one of a duration of the first time period and a duration of the second time period are configured based on a characteristic of the light source.
  • 8. The optical measurement system of claim 1, wherein the control circuit comprises: a voltage source;a first inductor coupled to the voltage source;a first switching circuit coupled to the first inductor and the light source;a second inductor coupled to the voltage source; anda second switching circuit coupled to the second inductor and the light source, wherein: the first switching circuit and the second switching circuit are configured to selectively couple the voltage source to the light source through the first inductor or the second inductor,the first inductor is configured to control a charging slew rate of a current applied to the light source that increases to start the emission of the light pulse, andthe second inductor is configured to control a discharging slew rate of the current applied to the light source that decreases to stop the emission of the light pulse.
  • 9. The optical measurement system of claim 1, further comprising a photodetector configured to detect a photon from the light pulse after the light pulse reflects off a target within a body.
  • 10. The optical measurement system of claim 9, wherein the control circuit further comprises: a first adjustable voltage source configured to apply the voltage having the first polarity and configured to control a charging slew rate of a current applied to the light source that increases to start the emission of the light pulse;a second adjustable voltage source configured to apply the voltage having the second polarity and configured to control a discharging slew rate of the current applied to the light source that decreases to stop the emission of the light pulse; andwherein at least one of the charging slew rate and the discharging slew rate is specified based on an output of the photodetector.
  • 11. The optical measurement system of claim 9, further comprising: an array of photodetectors including the photodetector; anda signal processing circuit that generates a histogram based on times that the array of photodetectors detect photons from the light pulse after the light pulse reflects off the target.
  • 12. The optical measurement system of claim 9, wherein the photodetector comprises: a single photon avalanche diode (SPAD); anda fast gating circuit configured to arm and disarm the SPAD.
  • 13. The optical measurement system of claim 9, wherein the photodetector is included in a wearable device configured to be worn by a user.
  • 14. The optical measurement system of claim 13, wherein the wearable device includes a head-mountable component configured to be worn on a head of the user.
  • 15. The optical measurement system of claim 1, wherein the light source includes a laser diode.
  • 16. A system comprising: a single photon avalanche diode (SPAD) configured to detect a photon from a light pulse after the light pulse reflects off a target within a body;a fast gating circuit configured to arm and disarm the SPAD;a light source; anda control circuit configured to: apply voltage having a first polarity to the light source for a first time period to provide a threshold charge for the light source to start an emission of the light pulse, andapply voltage having a second polarity opposite the first polarity to the light source for a second time period subsequent to the first time period to discharge the light source to stop the emission of the light pulse.
  • 17. The system of claim 16, wherein the second time period is at least of a duration such that a negative current is applied to the light source.
  • 18. The system of claim 16, wherein the control circuit comprises: a first voltage source configured to apply the voltage having the first polarity;a second voltage source configured to apply the voltage having the second polarity; anda switching circuit configured to selectively couple the first voltage source to the light source and the second voltage source to the light source.
  • 19. The system of claim 18, wherein: the switching circuit includes: a first transistor and a second transistor coupled to the first voltage source and the light source, anda third transistor and a fourth transistor coupled to the second voltage source and the light source;the first transistor and the fourth transistor are on and the second transistor and the third are off during the first time period; andthe second transistor and the third transistor are on and the first transistor and the fourth transistor are off during the second time period.
  • 20. The system of claim 18, wherein: the first voltage source is adjustable to control a charging slew rate of a current applied to the light source that increases to start the emission of the light pulse; andand the second voltage source is adjustable to control a discharging slew rate of the current applied to the light source that decreases to stop the emission of the light pulse.
  • 21. The system of claim 16, wherein the control circuit comprises an inductor coupled to the light source to control a slew rate of at least one of: increasing a current applied to the light source; anddecreasing the current applied to the light source.
  • 22. The system of claim 16, wherein at least one of a duration of the first time period and a duration of the second time period are configured based on a characteristic of the light source.
  • 23. The system of claim 16, wherein the control circuit comprises: a voltage source;a first inductor coupled to the voltage source;a first switching circuit coupled to the first inductor and the light source;a second inductor coupled to the voltage source; anda second switching circuit coupled to the second inductor and the light source, wherein: the first switching circuit and the second switching circuit are configured to selectively couple the voltage source to the light source through the first inductor or the second inductor,the first inductor is configured to control a charging slew rate of a current applied to the light source that increases to start the emission of the light pulse, andthe second inductor is configured to control a discharging slew rate of the current applied to the light source that decreases to stop the emission of the light pulse.
  • 24. The system of claim 16, wherein the control circuit further comprises: a first adjustable voltage source configured to apply the voltage having the first polarity and configured to control a charging slew rate of a current applied to the light source that increases to start the emission of the light pulse;a second adjustable voltage source configured to apply the voltage having the second polarity and configured to control a discharging slew rate of the current applied to the light source that decreases to stop the emission of the light pulse; andwherein at least one of the charging slew rate and the discharging slew rate is specified based on an output of the SPAD.
  • 25. The system of claim 16, further comprising: an array of SPADs including the SPAD; anda signal processing circuit that generates a histogram based on times that the array of SPADs detect photons from the light pulse after the light pulse reflects off the target.
  • 26. The system of claim 16, wherein the SPAD is included in a wearable device configured to be worn by a user.
  • 27. The system of claim 26, wherein the wearable device includes a head-mountable component configured to be worn on a head of the user.
  • 28. The system of claim 16, wherein the light source includes a laser diode.
RELATED APPLICATIONS

The present application claims priority under 35 U.S.C. § 119(e) to U.S. Provisional Patent Application No. 62/992,486, filed on Mar. 20, 2020, and to U.S. Provisional Patent Application No. 63/038,485, filed on Jun. 12, 2020. These applications are incorporated herein by reference in their respective entireties.

US Referenced Citations (341)
Number Name Date Kind
4018534 Thorn et al. Apr 1977 A
4207892 Binder Jun 1980 A
4281645 Jobsis Aug 1981 A
4321930 Jobsis Mar 1982 A
4515165 Carroll May 1985 A
4655225 Dahne et al. Apr 1987 A
4928248 Takahashi et al. May 1990 A
4963727 Cova Oct 1990 A
4995044 Blazo Feb 1991 A
5088493 Giannini Feb 1992 A
5090415 Yamashita Feb 1992 A
5309458 Carl May 1994 A
5386827 Chance et al. Feb 1995 A
5528365 Gonatas et al. Jun 1996 A
5625458 Alfano et al. Apr 1997 A
5761230 Pono et al. Jun 1998 A
5853370 Chance et al. Dec 1998 A
5895984 Renz Apr 1999 A
5929982 Anderson Jul 1999 A
5983120 Groner et al. Nov 1999 A
5987045 Albares et al. Nov 1999 A
6163715 Larsen et al. Dec 2000 A
6240309 Yamashita et al. May 2001 B1
6384663 Cova et al. May 2002 B2
6541752 Zappa et al. Apr 2003 B2
6618614 Chance Sep 2003 B1
6640133 Yamashita Oct 2003 B2
6683294 Herbert et al. Jan 2004 B1
6748254 O'Neil Jun 2004 B2
6992772 Block Jan 2006 B2
7095491 Forstner et al. Aug 2006 B2
7356365 Schurman Apr 2008 B2
7507596 Yaung et al. Mar 2009 B2
7547872 Niclass et al. Jun 2009 B2
7613504 Rowe Nov 2009 B2
7667400 Goushcha Feb 2010 B1
7705284 Inoue et al. Apr 2010 B2
7714292 Agarwal et al. May 2010 B2
7774047 Yamashita et al. Aug 2010 B2
7899506 Xu et al. Mar 2011 B2
8026471 Itzler Sep 2011 B2
8078250 Chen et al. Dec 2011 B2
8082015 Yodh et al. Dec 2011 B2
8115170 Stellari et al. Feb 2012 B2
8168934 Niclass et al. May 2012 B2
8352012 Besio Jan 2013 B2
8633431 Kim Jan 2014 B2
8637875 Finkelstein et al. Jan 2014 B2
8754378 Prescher et al. Jun 2014 B2
8817257 Herve Aug 2014 B2
8937509 Xu et al. Jan 2015 B2
8986207 Li Mar 2015 B2
9012860 Nyman et al. Apr 2015 B2
9041136 Chia May 2015 B2
9058081 Baxter Jun 2015 B2
9076707 Harmon Jul 2015 B2
9101279 Ritchey et al. Aug 2015 B2
9131861 Ince et al. Sep 2015 B2
9157858 Claps Oct 2015 B2
9160949 Zhang et al. Oct 2015 B2
9176241 Frach Nov 2015 B2
9178100 Webster et al. Nov 2015 B2
9190552 Brunel et al. Nov 2015 B2
9201138 Eisele et al. Dec 2015 B2
9209320 Webster Dec 2015 B1
9257523 Schneider et al. Feb 2016 B2
9257589 Niclass et al. Feb 2016 B2
9299732 Webster et al. Mar 2016 B2
9299873 Mazzillo et al. Mar 2016 B2
9312401 Webster Apr 2016 B2
9316735 Baxter Apr 2016 B2
9331116 Webster May 2016 B2
9368487 Su et al. Jun 2016 B1
9401448 Bienfang et al. Jul 2016 B2
9407796 Dinten et al. Aug 2016 B2
9419635 Kumar et al. Aug 2016 B2
9431439 Soga et al. Aug 2016 B2
9442201 Schmand et al. Sep 2016 B2
9449377 Sarkar et al. Sep 2016 B2
9450007 Motta et al. Sep 2016 B1
9466631 Fallica et al. Oct 2016 B2
9476979 Drader et al. Oct 2016 B2
9478579 Dai et al. Oct 2016 B2
9529079 Droz Dec 2016 B1
9535157 Caley et al. Jan 2017 B2
9574936 Heinonen Feb 2017 B2
9625580 Kotelnikov et al. Apr 2017 B2
9627569 Harmon Apr 2017 B2
9634826 Park Apr 2017 B1
9639063 Dutton et al. May 2017 B2
9640704 Frey et al. May 2017 B2
9658158 Renna et al. May 2017 B2
9659980 McGarvey et al. May 2017 B2
9671284 Dandin Jun 2017 B1
9681844 Xu et al. Jun 2017 B2
9685576 Webster Jun 2017 B2
9702758 Nouri Jul 2017 B2
9728659 Hirigoyen et al. Aug 2017 B2
9741879 Frey et al. Aug 2017 B2
9753351 Eldada Sep 2017 B2
9767246 Dolinsky et al. Sep 2017 B2
9768211 Harmon Sep 2017 B2
9773930 Motta et al. Sep 2017 B2
9804092 Zeng et al. Oct 2017 B2
9812438 Schneider et al. Nov 2017 B2
9831283 Shepard et al. Nov 2017 B2
9851302 Mattioli Della Rocca et al. Dec 2017 B2
9867250 Powers et al. Jan 2018 B1
9869753 Eldada Jan 2018 B2
9881963 Chen et al. Jan 2018 B1
9882003 Aharoni Jan 2018 B1
9886095 Pothier Feb 2018 B2
9899544 Mazzillo et al. Feb 2018 B1
9899557 Muscara' et al. Feb 2018 B2
9939316 Scott et al. Apr 2018 B2
9939536 O'Neill et al. Apr 2018 B2
9946344 Ayaz et al. Apr 2018 B2
D817553 Aaskov et al. May 2018 S
9983670 Coleman May 2018 B2
9997551 Mandai et al. Jun 2018 B2
10016137 Yang et al. Jul 2018 B1
D825112 Saez Aug 2018 S
10056415 Na et al. Aug 2018 B2
10103513 Zhang et al. Oct 2018 B1
10141458 Zhang et al. Nov 2018 B2
10157954 Na et al. Dec 2018 B2
10158038 Do Valle et al. Dec 2018 B1
10219700 Yang et al. Mar 2019 B1
10256264 Na et al. Apr 2019 B2
10340408 Katnani Jul 2019 B1
10424683 Do Valle Sep 2019 B1
10483125 Inoue Nov 2019 B2
10515993 Field et al. Dec 2019 B2
10533893 Leonardo Jan 2020 B2
10558171 Kondo Feb 2020 B2
10594306 Dandin Mar 2020 B2
10627460 Alford et al. Apr 2020 B2
10697829 Delic Jun 2020 B2
10772561 Donaldson Sep 2020 B2
10809796 Armstrong-Muntner Oct 2020 B2
10825847 Furukawa Nov 2020 B2
10912504 Nakaji Feb 2021 B2
10976386 Alford Apr 2021 B2
10983177 Jiménez-Martínez Apr 2021 B2
10996293 Mohseni May 2021 B2
11006876 Johnson May 2021 B2
11006878 Johnson May 2021 B2
20020195545 Nishimura Dec 2002 A1
20040057478 Saito Mar 2004 A1
20040078216 Toto Apr 2004 A1
20040160996 Giorgi et al. Aug 2004 A1
20050038344 Chance Feb 2005 A1
20050061986 Kardynal et al. Mar 2005 A1
20050124863 Cook Jun 2005 A1
20050228291 Chance Oct 2005 A1
20060171845 Martin Aug 2006 A1
20060197452 Zhang Sep 2006 A1
20070038116 Yamanaka Feb 2007 A1
20070083097 Fujiwara Apr 2007 A1
20080021341 Harris et al. Jan 2008 A1
20090012402 Mintz Jan 2009 A1
20090054789 Kiguchi et al. Feb 2009 A1
20090163775 Barrett Jun 2009 A1
20090313048 Kahn et al. Dec 2009 A1
20100210952 Taira et al. Aug 2010 A1
20100249557 Besko et al. Sep 2010 A1
20100301194 Patel Dec 2010 A1
20110208675 Shoureshi et al. Aug 2011 A1
20110248175 Frach Oct 2011 A1
20120016635 Brodsky et al. Jan 2012 A1
20120029304 Medina et al. Feb 2012 A1
20120083673 Al-Ali et al. Apr 2012 A1
20120101838 Lingard et al. Apr 2012 A1
20130015331 Birk Jan 2013 A1
20130030267 Lisogurski Jan 2013 A1
20130030270 Chiou et al. Jan 2013 A1
20130032713 Barbi et al. Feb 2013 A1
20130090541 MacFarlane et al. Apr 2013 A1
20130144644 Simpson Jun 2013 A1
20130221221 Bouzid et al. Aug 2013 A1
20130225953 Oliviero et al. Aug 2013 A1
20130342835 Blacksberg Dec 2013 A1
20140027607 Mordarski et al. Jan 2014 A1
20140028211 Imam Jan 2014 A1
20140055181 Chavpas Feb 2014 A1
20140066783 Kiani Mar 2014 A1
20140171757 Kawato et al. Jun 2014 A1
20140185643 McComb et al. Jul 2014 A1
20140191115 Webster et al. Jul 2014 A1
20140211194 Pacala et al. Jul 2014 A1
20140217264 Shepard Aug 2014 A1
20140275891 Muehlemann et al. Sep 2014 A1
20140289001 Shelton Sep 2014 A1
20140291481 Zhang et al. Oct 2014 A1
20150038811 Asaka Feb 2015 A1
20150038812 Ayaz et al. Feb 2015 A1
20150041625 Dutton Feb 2015 A1
20150041627 Webster Feb 2015 A1
20150054111 Niclass et al. Feb 2015 A1
20150057511 Basu Feb 2015 A1
20150077279 Song Mar 2015 A1
20150094552 Golda Apr 2015 A1
20150150505 Kaskoun et al. Jun 2015 A1
20150157262 Schuessler Jun 2015 A1
20150157435 Chasins et al. Jun 2015 A1
20150182136 Durduran et al. Jul 2015 A1
20150192677 Yu et al. Jul 2015 A1
20150200222 Webster Jul 2015 A1
20150293224 Eldada et al. Oct 2015 A1
20150327777 Kostic et al. Nov 2015 A1
20150333095 Fallica et al. Nov 2015 A1
20150364635 Bodlovic et al. Dec 2015 A1
20160049765 Eldada Feb 2016 A1
20160099371 Webster Apr 2016 A1
20160119983 Moore Apr 2016 A1
20160150963 Roukes et al. Jun 2016 A1
20160161600 Eldada et al. Jun 2016 A1
20160181302 McGarvey et al. Jun 2016 A1
20160182902 Guo Jun 2016 A1
20160218236 Dhulla et al. Jul 2016 A1
20160247301 Fang Aug 2016 A1
20160278715 Yu et al. Sep 2016 A1
20160287107 Szabados Oct 2016 A1
20160296168 Abreu Oct 2016 A1
20160341656 Liu et al. Nov 2016 A1
20160345880 Nakaji et al. Dec 2016 A1
20160356718 Yoon et al. Dec 2016 A1
20160357260 Raynor et al. Dec 2016 A1
20170030769 Clemens et al. Feb 2017 A1
20170047372 McGarvey et al. Feb 2017 A1
20170052065 Sharma et al. Feb 2017 A1
20170085547 De Aguiar et al. Mar 2017 A1
20170118423 Zhou et al. Apr 2017 A1
20170124713 Jurgenson et al. May 2017 A1
20170131143 Andreou et al. May 2017 A1
20170139041 Drader et al. May 2017 A1
20170141100 Tseng et al. May 2017 A1
20170164857 Soulet De Brugiere Jun 2017 A1
20170176579 Niclass et al. Jun 2017 A1
20170176596 Shpunt et al. Jun 2017 A1
20170179173 Mandai et al. Jun 2017 A1
20170186798 Yang et al. Jun 2017 A1
20170202518 Furman et al. Jul 2017 A1
20170265822 Du Sep 2017 A1
20170276545 Henriksson Sep 2017 A1
20170281086 Donaldson Oct 2017 A1
20170299700 Pacala et al. Oct 2017 A1
20170303789 Tichauer et al. Oct 2017 A1
20170314989 Mazzillo et al. Nov 2017 A1
20170363467 Clemens et al. Dec 2017 A1
20170367650 Wallois Dec 2017 A1
20180003821 Imai Jan 2018 A1
20180014741 Chou Jan 2018 A1
20180019268 Zhang et al. Jan 2018 A1
20180020960 Sarussi Jan 2018 A1
20180026147 Zhang et al. Jan 2018 A1
20180027196 Yang et al. Jan 2018 A1
20180033895 Mazzillo et al. Feb 2018 A1
20180039053 Kremer et al. Feb 2018 A1
20180045816 Jarosinski et al. Feb 2018 A1
20180062345 Bills et al. Mar 2018 A1
20180066986 Kasai et al. Mar 2018 A1
20180069043 Pan et al. Mar 2018 A1
20180070830 Sutin et al. Mar 2018 A1
20180070831 Sutin et al. Mar 2018 A1
20180081061 Mandai et al. Mar 2018 A1
20180089531 Geva et al. Mar 2018 A1
20180089848 Yang et al. Mar 2018 A1
20180090526 Mandai et al. Mar 2018 A1
20180090536 Mandai et al. Mar 2018 A1
20180102442 Wang et al. Apr 2018 A1
20180103528 Moore Apr 2018 A1
20180103861 Sutin et al. Apr 2018 A1
20180117331 Kuzniecky May 2018 A1
20180120152 Leonardo May 2018 A1
20180122560 Okuda May 2018 A1
20180156660 Turgeon Jun 2018 A1
20180167606 Cazaux et al. Jun 2018 A1
20180175230 Droz et al. Jun 2018 A1
20180180473 Clemens et al. Jun 2018 A1
20180185667 Huang Jul 2018 A1
20180217261 Wang Aug 2018 A1
20180296094 Nakamura Oct 2018 A1
20180366342 Inoue et al. Dec 2018 A1
20190006399 Otake et al. Jan 2019 A1
20190025406 Krelboim Jan 2019 A1
20190026849 Demeyer Jan 2019 A1
20190088697 Furukawa et al. Mar 2019 A1
20190091483 Deckert Mar 2019 A1
20190113385 Fukuchi Apr 2019 A1
20190120975 Ouvrier-Buffet Apr 2019 A1
20190167211 Everman et al. Jun 2019 A1
20190175068 Everdell Jun 2019 A1
20190200888 Poltorak Jul 2019 A1
20190209012 Yoshimoto et al. Jul 2019 A1
20190261869 Franceschini Aug 2019 A1
20190298158 Dhaliwal Oct 2019 A1
20190343395 Cussac Nov 2019 A1
20190355773 Field et al. Nov 2019 A1
20190355861 Katnani Nov 2019 A1
20190363210 Do Valle Nov 2019 A1
20190378869 Field et al. Dec 2019 A1
20190388018 Horstmeyer Dec 2019 A1
20190391213 Alford Dec 2019 A1
20200022581 Vanegas Jan 2020 A1
20200041727 Yamamoto Feb 2020 A1
20200044098 Azuma Feb 2020 A1
20200056263 Bhattacharyya Feb 2020 A1
20200057115 Jiménez-Martínez Feb 2020 A1
20200057116 Zorzos et al. Feb 2020 A1
20200060542 Alford Feb 2020 A1
20200088811 Mohseni Mar 2020 A1
20200109481 Sobek Apr 2020 A1
20200123416 Bhattacharyya Apr 2020 A1
20200136632 Lin Apr 2020 A1
20200182692 Lilic Jun 2020 A1
20200188030 Kopper et al. Jun 2020 A1
20200191883 Bhattacharyya Jun 2020 A1
20200196932 Johnson et al. Jun 2020 A1
20200241094 Alford Jul 2020 A1
20200253479 Nurmikko Aug 2020 A1
20200256929 Ledbetter et al. Aug 2020 A1
20200309873 Ledbetter et al. Oct 2020 A1
20200315510 Johnson Oct 2020 A1
20200334559 Anderson Oct 2020 A1
20200337624 Johnson Oct 2020 A1
20200341081 Mohseni et al. Oct 2020 A1
20200348368 Garber et al. Nov 2020 A1
20200381128 Pratt Dec 2020 A1
20200390358 Johnson Dec 2020 A1
20200393902 Mann et al. Dec 2020 A1
20200400763 Pratt Dec 2020 A1
20210015385 Katnani Jan 2021 A1
20210011094 Bednarke Feb 2021 A1
20210041512 Pratt Feb 2021 A1
20210063510 Ledbetter Mar 2021 A1
20210013974 Seidman May 2021 A1
20210139742 Seidman May 2021 A1
20210265512 Ayel Aug 2021 A1
20210290064 Do Valle Sep 2021 A1
20210294996 Field Sep 2021 A1
Foreign Referenced Citations (26)
Number Date Country
200950235 Sep 2007 CN
107865635 Apr 2018 CN
0656536 Apr 2004 EP
2294973 Mar 2011 EP
3419168 Dec 2018 EP
3487072 May 2019 EP
20170087639 Jul 2017 KR
8804034 Jun 1988 WO
1999053577 Oct 1999 WO
2008144831 Dec 2008 WO
2011083563 Jul 2011 WO
2012135068 Oct 2012 WO
2013034770 Mar 2013 WO
2013066959 May 2013 WO
2015052523 Apr 2015 WO
2015109005 Jul 2015 WO
2016166002 Oct 2016 WO
2017004663 Jan 2017 WO
2017083826 May 2017 WO
2017130682 Aug 2017 WO
2017150146 Sep 2017 WO
2017203936 Nov 2017 WO
2018007829 Jan 2018 WO
2018033751 Feb 2018 WO
2018122560 Jul 2018 WO
2019221784 Nov 2019 WO
Non-Patent Literature Citations (76)
Entry
International Search Report and Written Opinion received in International Application No. PCT/2020/027537, dated Sep. 7, 2020.
International Search Report and Written Opinion received in International Application No. PCT/2020/028820, dated Aug. 26, 2020.
International Search Report and Written Opinion received in International Application No. PCT/US20/34062, dated Aug. 26, 2020.
International Search Report and Written Opinion received in International Application No. PCT/US2018/058580, dated Feb. 12, 2019.
International Search Report and Written Opinion received in International Application No. PCT/US2018/062777, dated Feb. 13, 2019.
International Search Report and Written Opinion received in International Application No. PCT/US2019/019317, dated May 28, 2019.
Non-Final Office Action received in U.S. Appl. No. 16/177,351, dated Apr. 1, 2019.
Non-Final Office Action received in U.S. Appl. No. 16/283,730, dated May 16, 2019.
Non-Final Office Action received in U.S. Appl. No. 16/370,991, dated Feb. 10, 2020.
Non-Final Office Action received in U.S. Appl. No. 16/537,360, dated Feb. 25, 2020.
Non-Final Office Action received in U.S. Appl. No. 16/544,850, dated Jun. 25, 2020.
Non-Final Office Action received in U.S. Appl. No. 16/856,524, dated Dec. 1, 2020.
Partial Search Report received in International Application No. PCT/2020/028820, dated Jul. 1, 2020.
Partial Search Report received in International Application No. PCT/US2020/027537, dated Jul. 17, 2020.
Alayed, et al.,“Characterization of a Time-Resolved Diffuse Optical Spectroscopy Prototype Using Low-Cost, Compact Single Photon Avalanche Detectors for Tissue Optics Applications,” Sensors 2018, 18, 3680; doi:10.3390/s18113680, Oct. 29, 2018.
Bellis, et al.,“Photon counting imaging: the DigitalAPD,” Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series, Feb. 2006, vol. 6068, pp. 111-120.
Blutman, et al.,“A 0.1 pJ Freeze Vernier Time-to-Digital Converter in 65nm CMOS,” 2014 International Symposium on Circuits and Systems (ISCAS), Melbourne, Australia, Jun. 1-5, 2014.
Cambie, et al.,“Every photon counts: understanding and optimizing photon paths in luminescent solar concentrator-based photomicroreactors (LSC-PMs),” React. Chem. Eng., 2017, 2, 561-566.
Contini, et al.,“Photon migration through a turbid slab described by a model based on diffusion approximation. I. Theory,” Appl. Opt. 36(19), 4587 (1997).
Dalla Mora, et al., “Fast-Gated Single-Photon Avalanche Diode for Wide Dynamic Range Near Infrared Spectroscopy,” IEEE Journal of Selected Topics in Quantum Electronics, vol. 16, No. 4, Jul./Aug. 2010.
Dalla Mora, et al., “Memory effect in silicon time-gated single-photon avalanche diodes,” http://dx.doi.org/10.1063/1.4915332, Journal of Applied Physics 117, 114501, 2015.
De Heyn, et al.,“A fast start-up 3GHz-10GHz digitally controlled oscillator for UWB impulse radio in 90nm CMOS,” 2007 European Solid-State Circuits Conference—(ESSCIRC), Munich, Germany, pp. 484-487 Sep. 11-13, 2007.
Di Sieno, et al.,“Probe-hosted large area silicon photomultiplier and high-throughput timing electronics for enhanced performance time-domain functional near-infrared spectroscopy,” Biomed. Opt. Express 11(11), 6389 (2020).
Dutton, et al.,“A Time-Correlated Single-Photon-Counting Sensor with 14GS/s Histogramming Time-to-Digital Converter,” 2015 IEEE International Solid-State Circuits Conference ISSCC 2015 / SESSION 11 / Sensors and Imagers for Life Sciences / 11.5, Feb. 22-26, 2015.
Fishburn, et al., “Temporal Derivative Distribution Repair (TDDR): A motion correction method for fNIRS,” Neuroimage. Jan. 1, 2019; 184: 171-179. doi:10.1016/j.neuroimage.2018.09.025.
Fisher, et al., “A Reconfigurable Single-Photon-Counting Integrating Receiver for Optical Communications,” IEEE Journal of Solid-State Circuits, vol. 48, No. 7, Jul. 2013, https://www.researchgate.net/publication/260626902.
Gallivanoni, et al., “Progress in Quenching Circuits for Single Photon Avalanche Diodes,” IEEE Transactions on Nuclear Science, vol. 57, No. 6, Dec. 2010.
Gnecchi, et al.,“A 1x16 SiPM Array for Automotive 3D Imaging LIDAR Systems.”, Proceedings of the 2017 International Image Sensor Workshop (IISW), Hiroshima, Japan, (2017).
Harmon, et al.,“Compound Semiconductor SPAD Arrays,” LightSpin Technologies, http://www.lightspintech.com/publications.html (2013).
Henderson, et al., “A 192 × 128 Time Correlated SPAD Image Sensor in 40-nm CMOS Technology,” IEEE Journal of Solid-State Circuits, 2019.
Henderson, et al.,“A 256×256 40nm/90nm CMOS 3D-Stacked 120dB Dynamic-Range Reconfigurable Time-Resolved SPAD Imager,” 2019 IEEE International Solid- State Circuits Conference—(ISSCC), San Francisco, CA, USA, 2019, pp. 106-108. doi: 10.1109/ISSCC.2019.8662355.
Huikari, et al., “High-Energy Picosecond Pulse Generation by Gain Switching in Asymmetric Waveguide Structure Multiple Quantum Well Lasers,” IEEE Journal of Selected Topics in Quantum Electronics, vol. 21, No. 6, Nov. / Dec. 2015.
Huppert, et al.,“HomER: a review of time-series analysis methods for near-infrared spectroscopy of the brain,” Appl. Opt. 48(10), D280 (2009).
Kienle, et al.,“Improved solutions of the steady-state and the time-resolved diffusion equations for reflectance from a semi-infinite turbid medium,” J. Opt. Soc. Am. A 14(1), 246 (1997).
Konugolu, et al., “Broadband (600-1350 nm) Time-Resolved Diffuse Optical Spectrometer for Clinical Use,” IEEE Journal of Selected Topics in Quantum Electronics, vol. 22, No. 3, May/Jun. 2016.
Lacerenza, et al., “Wearable and wireless time-domain near-infrared spectroscopy system for brain and muscle hemodynamic monitoring,” Biomed. Opt. Express 11(10), 5934 (2020).
Lange, et al.,“Clinical Brain Monitoring with Time Domain NIRS: A Review and Future Perspectives,” Applied Sciences 9(8), 1612 (2019).
Lange, et al., “MAESTROS: A Multiwavelength Time-Domain NIRS System to Monitor Changes in Oxygenation and Oxidation State of Cytochrome-C-Oxidase,” IEEE J. Select. Topics Quantum Electron. 25(1), 1-12 (2019).
Lee, et al.,“High-Performance Back-Illuminated Three-Dimensional Stacked Single-Photon Avalanche Diode Implemented in 45-nm CMOS Technology,” IEEE Journal of Selected Topics in Quantum Electronics 6, 1-9 (2018).
Li, et al.,“Step-Puise Modulation of Gain-Switched Semiconductor Pulsed Laser,” Appl. Sci. 2019, 9, 602; doi:10.3390/app9030602.
Mandai, et al., “A 4 X 4 X 416 digital SiPM array with 192 TDCs for multiple high-resolution timestamp acquisition,” 2013 JINST 8 PO5024, May 31, 2013.
Martelli, et al.,“Optimal estimation reconstruction of the optical properties of a two-layered tissue phantom from time-resolved single-distance measurements,” Journal of Biomedical Optics 20(11), 115001 (Nov. 2015).
Maruyama, et al.,“A 1024 x 8, 700-ps Time-Gated SPAD Line Sensor for Planetary Surface Exploration With Laser Raman Spectroscopy and LIBS,” IEEE Journal of Solid-State Circuits, vol. 49, No. 1, Jan. 2014.
Mita, et al., “High-Speed and Compact Quenching Circuit for Single-Photon Avalanche Diodes,” IEEE Transactions on Instrumentation and Measurement, vol. 57, No. 3, Mar. 2008. pp. 543-547.
Mora, et al., “Fast silicon photomultiplier improves signal harvesting and reduces complexity in time-domain diffuse optics,” Opt. Express 23(11), 13937 (2015).
Mora, et al., “Fast-Gated Single-Photon Avalanche Diode for Wide Dynamic Range Near Infrared Spectroscopy,” IEEE Journal of Selected Topics in Quantum Electronics, vol. 16, No. 4, pp. 1023-1030, Jul./Aug. 2010.
Parmesan, et al.,“A 256 x 256 SPAD array with in-pixel Time to Amplitude Conversion for Fluorescence Lifetime Imaging Microscopy,” Memory 900.M4, 2015.
Pifferi, et al., “Performance assessment of photon migration instruments: the MEDPHOT protocol,” Applied Optics, 44(11), 2104-2114 (2005).
Prahl, et al., “Optical Absorption of Hemoglobin,” http://omic.ogi.edu/spectra/hemoglobin/index.html (1999).
Puszka, et al.,“Time-resolved diffuse optical tomography using fast-gated single-photon avalanche diodes,” Biomedical optics express, 2013, vol. 4, No. 8, pp. 1351-1365 (Year: 2013).
Re, et al.,“Multi-channel medical device for time domain functional near infrared spectroscopy based on wavelength space multiplexing,” Biomed. Opt. Express 4(10), 2231 (2013).
Renna, et al.,“Eight-Wavelength, Dual Detection Channel Instrument for Near-Infrared Time-Resolved Diffuse Optical Spectroscopy,” IEEE J. Select. Topics Quantum Electron. 25(1), 1-11 (2019).
Richardson, et al.,“A 32x32 50ps resolution 10 bit time to digital converter array in 130nm CMOS for time correlated imaging,” CICC 2009 Proceedings of the IEEE 2009 Custom Integrated Circuits Conference. IEEE Society, San Jose, U.S.A., pp. 77-80, CICC 2009, San Jose, U.S.A., Sep. 13, 2009. https://doi.org/doi:10.1109/CICC.2009.5280890.
Takai, et al.,“Single-Photon Avalanche Diode with Enhanced NIR-Sensitivity for Automotive LIDAR Systems,” Sensors, 2016, 16(4): 459, pp. 1-9 (Year: 2016).
Torricelli, et al., “Time domain functional NIRS imaging for human brain mapping,” Neurolmage 85, 28-50 (2014).
Wabnitz, et al., “Depth-selective data analysis for time-domain fNIRS: moments vs. time windows,” Biomed. Opt. Express 11(8), 4224 (2020).
Wabnitz, et al., “Performance assessment of time-domain optical brain imagers, part 1: basic instrumental performance protocol,” Journal of Biomedical Optics 19(8), 086010 (Aug. 2014).
Wabnitz, et al., “Performance assessment of time-domain optical brain imagers, part 2: nEUROPt protocol,” Journal of Biomedical Optics 19(8), 086012 (Aug. 2014).
Wojtkiewicz, et al., “Self-calibrating time-resolved near infrared spectroscopy,” Biomed. Opt. Express 10(5), 2657 (2019).
Zhang, et al.,“A CMOS SPAD Imager with Collision Detection and 128 Dynamically Reallocating TDCs for Single- Photon Counting and 3D Time-of-Flight Imaging,” Sensors (Basel, Switzerland), 18(11), 4016. doi:10.3390/s18114016 Nov. 17, 2018.
Zucchelli, et al.,“Method for the discrimination of superficial and deep absorption variations by time domain fNIRS,” 2013 OSA Dec. 1, 2013 | vol. 4. No. 12 | DOI:10.1364/BOE.4.002893 | Biomedical Optics Express 2893.
Chen, et al., “A PVT Insensitive Field Programmable Gate Array Time-to-digital Converter”, 2013 IEEE Nordic-Mediterranean Workshop on Time-to-Digital Converters. Oct. 3, 2013.
Field, et al., “A 100-fps, Time-Correlated Single-PhotonCounting-Based Fluorescence-Lifetime Imager in 130-nm CMOS”, IEEE Journal of Solid-State Circuits, vol. 49, No. 4, Apr. 2014.
Lebid, et al., “Multi-Timescale Measurements of Brain Responses in Visual Cortex During Functional Stimulation Using Time-Resolved Spectroscopy”, SPIE vol. 5826. Dec. 31, 2005. p. 609, last paragraph—p. 610, paragraph 1.
Zheng, et al., “An Integrated Bias Voltage Control Method for SPAD Arrays”, Oct. 1, 2018, IEEE Service Center.
“emojipedia.org”, https://emojipedia.org (accessed May 27, 2021).
“International Search Report and Written Opinion received in International Application No. PCT/2021/018188”.
“International Search Report and Written Opinion received in International Application No. PCT/US2021/018155”.
“International Search Report and Written Opinion received in International Application No. PCT/US2021/018187”.
“International Search Report and Written Opinion received in International Application No. PCT/US2021/018190”.
“scienceofpeople.com/emojis”, https://www.scienceofpeople.com/emojis/ (accessed May 27, 2021).
Hebert, et al.,“Spatiotemporal image correlation spectroscopy (STICS) theory, verification, and application to protein velocity mapping in living CHO cells”, Biophysical journal 88, No. 5 (2005): 3601-3614.
Kheng, et al.,“Image Processing”, https://www.comp.nus.edu.sg/˜cs4243/lecture/imageproc.pdf, Mar. 9, 2014.
Sneha, et al.,“Understanding Correlation”, https://www.allaboutcircuits.com/technical-articles/understanding-correlation/, Jan. 4, 2017.
Xu, et al.,“A 655 μW Silicon Photomultiplier-Based NIRS/EEG/EIT Monitoring ASIC for Wearable Functional Brain Imaging”, IEEE Transactions on Biomedical Circuits and Systems, IEEE, US, vol. 12, No. 6, Dec. 1, 2018.
Zucconi, et al.,“The Autocorrelation Function”, https://www.alanzucconi.com/2016/06/06/autocorrelation-function/, Jun. 6, 2016.
Related Publications (1)
Number Date Country
20210290067 A1 Sep 2021 US
Provisional Applications (2)
Number Date Country
63038485 Jun 2020 US
62992486 Mar 2020 US