The invention relates to audio processing and in particular to an apparatus for capturing audio information from a target location. Moreover, the application relates to spatially selective sound acquisition by acoustic triangulation.
Spatial sound acquisition aims at capturing an entire sound field which is present at a recording room or just certain desired components of the sound field that are of interest for the application at hand. As an example, in a situation where several people in a room have a conversation, it may be of interest to either capture the entire sound field (including its spatial characteristics) or just a signal that a certain talker produces. The latter enables to isolate the sound and apply specific processing to it, such as amplification, filtering etc.
There are a number of methods known for spatially selectively capturing certain sound components. These methods often employ microphones with a high directionality or microphone arrays. Most methods have in common that the microphone or the microphone array is arranged in a fixed known geometry. The spacing between the microphones is as small as possible for coincident microphone techniques, whereas it is normally a few centimeters for the other methods. In the following, we refer to any apparatus for the directionally selective acquisition of the spatial sound (e.g., directional microphones, microphone arrays, etc.) as a beamformer.
Traditionally, directional (spatial) selectivity in sound capture, i.e., a spatially selective sound acquisition, can be achieved in several ways:
One possible way is to employ directional microphones (e.g., cardioid, super cardioid, or shot gun microphones). There, all microphones capture the sound differently depending on the direction-of-arrival (DOA) relative to the microphone. In some microphones, this effect is minor, as they capture sound almost independently of the direction. These microphones are called omnidirectional microphones. Typically in such microphones, a circular diaphragm is attached to a small airtight enclosure, see, for example,
If the diaphragm is not attached to the enclosure and sound reaches it equally from each side, its directional pattern has two lobes of equal magnitude. It captures sound with equal level from both front and back of the diaphragm, however, with inversed polarities. This microphone does not capture sound coming from the directions parallel to the plane of the diaphragm. This directional pattern is called dipole or figure-of-eight. If the enclosure of omnidirectional microphone is not airtight, but a special construction is made, which allows the sound waves to propagate through the enclosure and reach the diaphragm, the directional pattern is somewhere between omnidirectional and dipole (see [Ea01]). The patterns may have two lobes; however, the lobes may have different magnitudes. The patterns may also have a single lobe; the most important example is the cardioid pattern, where the directional function D can be expressed as D=0.5(1+cos(θ)), where θ is the direction of arrival of sound (see [Ea01]). This function quantifies the relative magnitude of the captured sound level of a plane wave at the angle θ with respect to the angle with the highest sensitivity. Omnidirectional microphones are called zeroth-order microphones and other patterns mentioned in the previous, such as dipole and cardioid patterns, are known as first-order patterns. These kinds of microphones do not allow arbitrary shaping of the pattern since their directivity pattern is almost entirely determined by their mechanical construction.
Some special acoustical structures also exist which can be used to create narrower directional patterns to microphones than first-order ones. For example, if a tube which has holes in it is attached to an omnidirectional microphone, a microphone with a very narrow directional pattern can be created. Such microphones are called shotgun or rifle microphones (see [Ea01]). They typically do not have flat frequency responses and their directivity cannot be controlled after recording.
Another method to construct a microphone with directional characteristics is to record sound with an array of omnidirectional or directional microphones and to apply signal processing afterwards, see, for example,
There exist a variety of methods for this. In simplest form, when sound is recorded with two omnidirectional microphones close to each other and subtracted from each other, a virtual microphone signal with a dipole characteristic is formed. See, e.g.
The microphone signals can also be delayed or filtered before summing to each other. In beamforming, a signal corresponding to a narrow beam is formed by filtering each microphone signal with a specially designed filter and then adding them together. This “filter-and-sum beamforming” is explained in
These techniques are blind to the signal itself, e.g., they are not aware of the direction of arrival of sound. Instead, estimation of the “direction of arrival” (DOA) is a task of its own, see, for example,
In principle, many different directional characteristics can be formed with these techniques. For forming arbitrary spatially very selective sensitivity patterns, however, a large number of microphones may be used. In general, all these techniques rely on distances of adjacent microphones which are small compared to the wavelength of interest.
Another way for realizing directional selectivity in sound capture is parametric spatial filtering. Standard beamformer designs, which may, for example, be based on a limited number of microphones and which possess time-invariant filters in their filter-and-sum structure (see [BS01]) usually exhibit only limited spatial selectivity. To increase the spatial selectivity, recently parametric spatial filtering techniques have been proposed which apply (time-variant) spectral gain functions to the input signal spectrum. The gain functions are designed based on parameters, which are related to the human perception of spatial sound. One spatial filtering approach is presented in
In DirAC, the sound field is analyzed in one location at which the active intensity vector as well as the sound pressure is measured. These physical quantities are used to extract the three DirAC parameters: sound pressure, direction-of-arrival (DOA) and diffuseness of sound. DirAC makes use of the assumption that the human auditory system can only process one direction per time- and frequency-tile. This assumption is also exploited by other spatial audio coding techniques like MPEG Surround, see, for example:
The spatial filtering approach, as described in [DiFi2009], allows for an almost free choice of spatial selectivity.
A further technique makes use of comparable spatial parameters. This technique is explained in
In contrast to the technique described in [DiFi2009], in which a spectral gain function is applied to an omnidirectional microphone signal, the approach in [Fa108] makes use of two cardioid microphones.
The two mentioned parametric spatial filtering techniques rely on microphone spacings, which are small compared to the wavelength of interest. Ideally, the techniques described in [DiFi2009] and [Fa108] are based on coincident directional microphones.
Another way of realizing directional selectivity in sound capture is a filtering of microphone signals based on the coherence between microphone signals. In
A major limitation of traditional approaches for spatially selective sound acquisition is that the recorded sound is invariably related to the location of the beamformer. In many applications it is, however, not possible (or feasible) to place a beamformer in the desired position, e.g., at a desired angle relative to the sound source of interest.
Traditional beamformers, may, for example, employ microphone arrays and can form a directional pattern (“beam”) to capture sound from one direction—and reject sound from other directions. Consequently, there is no possibility to restrict the region of sound capture regarding its distance from the capturing microphone array.
It would be extremely desirable to have a capturing device which can selectively capture sound originating not only from one direction, but directly restricted to originating from one place (spot), similar to the way a close-up spot microphone at the desired place would perform.
According to an embodiment, an apparatus for capturing audio information from a target location may have: a first beamformer being arranged in a recording environment and having a first recording characteristic, a second beamformer being arranged in the recording environment and having a second recording characteristic, and a signal generator, wherein the first beamformer is configured for recording a first beamformer audio signal when the first beamformer is directed towards the target location with respect to the first recording characteristic, and wherein the second beamformer is configured for recording a second beamformer audio signal when the second beamformer is directed towards the target location with respect to the second recording characteristic, wherein the first beamformer and the second beamformer are arranged such that a first virtual straight line, being defined to pass through the first beamformer and the target location, and a second virtual straight line, being defined to pass through the second beamformer and the target location, are not parallel with respect to each other, and wherein the signal generator is configured to generate an audio output signal based on the first beamformer audio signal and on the second beamformer audio signal, so that the audio output signal has relatively more audio information from the target location compared to the audio information from the target location in the first and the second beamformer audio signal, wherein the signal generator has an intersection calculator for generating the audio output signal in the spectral domain based on the first and second beamformer audio signal, and wherein the intersection calculator is configured to compute the audio output signal in the spectral domain by calculating a cross-spectral density of the first and the second beamformer audio signal, and by calculating a power spectral density of the first or the second beamformer audio signal.
According to another embodiment, a method for computing audio information from a target location may have the steps of recording a first beamformer audio signal by a first beamformer being arranged in a recording environment and having a first recording characteristic when the first beamformer is directed towards the target location with respect to the first recording characteristic, recording a second beamformer audio signal by a second beamformer being arranged in the recording environment and having a second recording characteristic when the second beamformer is directed towards the target location with respect to the second recording characteristic, generating an audio output signal based on the first beamformer audio signal and on the second beamformer audio signal so that the audio output signal has relatively more audio information from the target location compared to the audio information from the target location in the first and the second beamformer audio signal, wherein the first beamformer and the second beamformer are arranged such that a first virtual straight line, being defined to pass through the first beamformer and the target location and a second virtual straight line, being defined to pass through the second beamformer and the target location, are not parallel with respect to each other, wherein the audio output signal is generated in the spectral domain by calculating the first and second beamformer audio signal, and wherein the audio output signal is computed in the spectral domain by calculating a cross-spectral density of the first and the second beamformer audio signal, and by calculating a power spectral density of the first or the second beamformer audio signal.
Another embodiment may have a computer program for implementing the method for computing audio information from a target location, may have the steps of: recording a first beamformer audio signal by a first beamformer being arranged in a recording environment and having a first recording characteristic when the first beamformer is directed towards the target location with respect to the first recording characteristic, recording a second beamformer audio signal by a second beamformer being arranged in the recording environment and having a second recording characteristic when the second beamformer is directed towards the target location with respect to the second recording characteristic, generating an audio output signal based on the first beamformer audio signal and on the second beamformer audio signal so that the audio output signal has relatively more audio information from the target location compared to the audio information from the target location in the first and the second beamformer audio signal, wherein the first beamformer and the second beamformer are arranged such that a first virtual straight line, being defined to pass through the first beamformer and the target location and a second virtual straight line, being defined to pass through the second beamformer and the target location, are not parallel with respect to each other, wherein the audio output signal is generated in the spectral domain by calculating the first and second beamformer audio signal, and wherein the audio output signal is computed in the spectral domain by calculating a cross-spectral density of the first and the second beamformer audio signal, and by calculating a power spectral density of the first or the second beamformer audio signal, when the computer program is executed by a computer or processor.
An apparatus for capturing audio information from a target location is provided. The apparatus comprises a first beamformer being arranged in a recording environment and having a first recording characteristic, a second beamformer being arranged in the recording environment and having a second recording characteristic and a signal generator. The first beamformer is configured for recording a first beamformer audio signal and the second beamformer is configured for recording a second beamformer audio signal when the first beamformer and the second beamformer are directed towards the target location with respect to the first and second recording characteristic. The first beamformer and the second beamformer are arranged such that a first virtual straight line, being defined to pass through the first beamformer and the target location, and a second virtual straight line, being defined to pass through the second beamformer and the target location, are not parallel with respect to each other. The signal generator is configured to generate an audio output signal based on the first beamformer audio signal and on the second beamformer audio signal so that the audio output signal reflects relatively more audio information from the target location compared to the audio information from the target location in the first and second beamformer audio signal. With respect to a three-dimensional environment, advantageously, the first virtual straight line and the second virtual straight line intersect and define a plane that can be arbitrarily oriented.
By this, means to capture sound in a spatially selective way are provided, i.e., pick up sound originating from a specific target location just as if a close-up “spot microphone” had been installed at this location. Instead of really installing this spot microphone, however, its output signal can be simulated by using two beamformers placed at different distant positions.
These two beamformers are not positioned closely to each other but they are located such that each of them performs an independent directional sound acquisition. Their “beams” overlap at a desired spot and their individual outputs are subsequently combined to form a final output signal. In contrast to other possible approaches, the combination of the two individual outputs does not require any information or knowledge about the position of the two beamformers in a common coordinate system. Thus, the entire setup for virtual spot microphone acquisition comprises two beamformers that operate independently, plus a signal processor which combines both individual output signals into the signal of the remote “spot microphone”.
In an embodiment, the apparatus comprises a first and a second beamformer, e.g., two spatial microphones and a signal generator, e.g., a combination unit, e.g. a processor, for realizing “acoustic intersection”. Each spatial microphone has a clear directional selectivity, i.e., it attenuates sound originating from locations outside its beam as compared to sound originating from a location inside its beam. The spatial microphones operate independently from each other. The location of the two spatial microphones, also flexible by nature, is chosen such that the target spatial location is located in the geometric intersection of the two beams. In an advantageous embodiment, the two spatial microphones form an angle of around 90 degrees with respect to the target location. The combination unit, e.g. the processor, may be unaware of the geometric location of the two spatial microphones or the location of the target source.
According to an embodiment, the first beamformer and the second beamformer are arranged with respect to the target location such that the first virtual straight line and the second virtual straight line cross each other, and such that they intersect in the target location with an angle of intersection between 30 degrees and 150 degrees. In a further embodiment, the angle of intersection is between 60 degrees and 120 degrees. In an advantageous embodiment, the angle of intersection is about 90 degrees.
In an embodiment, the signal generator comprises an adaptive filter having a plurality of filter coefficients. The adaptive filter is arranged to receive the first beamformer audio signal. The filter is adapted to modify the first beamformer audio signal depending on the filter coefficients to obtain a filtered first beamformer audio signal. The signal generator is configured to adjust the filter coefficients of the filter depending on the second beamformer audio signal. The signal generator may be configured to adjust the filter coefficients such that the difference between the filtered first beamformer audio signal and the second beamformer second audio signal is minimized.
In an embodiment, the signal generator comprises an intersection calculator for generating the audio output signal in the spectral domain based on the first and second beamformer audio signal. According to an embodiment, the signal generator may further comprise an analysis filterbank for transforming the first and the second beamformer audio signal from a time domain to a spectral domain, and a synthesis filterbank for transforming the audio output signal from a spectral domain to a time domain. The intersection calculator may be configured to calculate the audio output signal in the spectral domain based on the first beamformer audio signal being represented in the spectral domain and on the second beamformer audio signal being represented in the spectral domain.
In a further embodiment, the intersection calculator is configured to compute the audio output signal in the spectral domain based on a cross-spectral density of the first and the second beamformer audio signal, and based on a power spectral density of the first or the second beamformer audio signal.
According to an embodiment, the intersection calculator is configured to compute the audio output signal in the spectral domain by employing the formula
wherein Y1(k, n) is the audio output signal in the spectral domain, wherein S1(k, n) is the first beamformer audio signal, wherein C12(k, n) is a cross-spectral density of the first and the second beamformer audio signal, and wherein P1(k, n) is a power spectral density of the first beamformer audio signal, or
by employing the formula
wherein Y2(k, n) is the audio output signal in the spectral domain, wherein S2(k, n) is the second beamformer audio signal, wherein C12(k, n) is a cross-spectral density of the first and the second beamformer audio signal, and wherein P2(k, n) is a power spectral density of the second beamformer audio signal.
In another embodiment, the intersection calculator is adapted to calculate both the signal Y1(k, n) and Y2(k, n) and to select the smaller of both signals as the audio output signal.
In another embodiment, the intersection calculator is configured to compute the audio output signal in the spectral domain by employing the formula
wherein Y3(k, n) is the audio output signal in the spectral domain, wherein S1 is the first beamformer audio signal, wherein C12(k, n) is a cross-spectral density of the first beamformer audio signal, wherein P1(k, n) is a power spectral density of the first beamformer audio signal, and wherein P2(k, n) is a power spectral density of the second beamformer audio signal, or by employing the formula
wherein Y4(k, n) is the audio output signal in the spectral domain, wherein S2 is the second beamformer audio signal, wherein C12(k, n) is a cross-spectral density of the first and the second beamformer audio signal, wherein P1(k, n) is a power spectral density of the first beamformer audio signal, and wherein P2(k, n) is a power spectral density of the second beamformer audio signal.
In another embodiment, the intersection calculator may be adapted to calculate both the signal Y3(k, n) and Y4(k, n) and to select the smaller of both signals as the audio output signal.
According to another embodiment, the signal generator may be adapted to generate the audio output signal by combining the first and the second beamformer audio signal to obtain a combined signal and by weighting the combined signal by a gain factor. The combined signal may, for example, be weighted in a time domain, in a subband domain or in a Fast Fourier Transform domain.
In a further embodiment, the signal generator is adapted to generate the audio output signal by generating a combined signal such that the power spectral density value of the combined signal is equal to the minimum of the power spectral density value of the first and the second beamformer audio signal for each considered time-frequency tile.
Embodiments of the present invention will be detailed subsequently referring to the appended drawings, in which:
a illustrates a beamformer and a beam of the beamformer being directed towards a target location,
b illustrates a beamformer and a beam of the beamformer showing further details,
a illustrates a geometric setup of two beamformers with respect to a target location according to an embodiment,
b depicts the geometric setup of the two beamformers of
c illustrates the geometric setup of the two beamformers of
a illustrates a beamformer 310. The beamformer 310 of the embodiment of
a illustrates a curved line 316 that encloses a beam 315. All points on the curved line 316 that defines the beam 315 are characterized in that a predefined sound pressure level originating from a point on the curved line results in the same signal level output of the microphone for all points on the curved line.
Moreover,
b illustrates this in more detail. The points 325, 326 and 327 have equal distance d from the beamformer 310. A sound with a predefined sound pressure level originating from the point 325 on the major axis 320 results in a first signal level output in the beamformer that is greater than or equal to a second signal level output of the beamformer resulting from a sound with the predefined sound pressure level originating from, for example, point 326 or point 327, which have the same distance d from the beamformer 310 as the point 325 on the major axis. In the three-dimensional case, this means, that the major axis indicates the point on a virtual ball with the beamformer located in the center of the ball, which generates the greatest signal level output in the beamformer when a predefined sound pressure level originates from the point compared with any other point on the virtual ball.
Returning to
The beamformer 310 has a recording characteristic that indicates the ability of the beamformer to record sound depending on the direction the sound originates from. The recording characteristic of the beamformer 310 comprises the direction of the major axis 320 in space, the direction, form and properties of the beam 315, etc.
a illustrates a geometric setup of two beamformers, a first beamformer 410 and a second beamformer 420, with respect to a target location 430. A first beam 415 of the first beamformer 410 and a second beam 425 of the second beamformer 420 are illustrated. Moreover,
The first beam 415 of the first beamformer 410 and the second beam 425 of the second beamformer 420 intersect in the target location 430, where a target source that outputs sound is located. An angle of intersection of the first major axis 418 of the first beamformer 410 and the second major axis 428 of the second beamformer 420 is denoted as α. Optimally, the angle of intersection α is 90 degrees. In other embodiments, the angle of intersection is between 30 degrees and 150 degrees.
In a three-dimensional environment, advantageously, the first major axis and the second virtual major axis intersect and define a plane that can be arbitrarily oriented.
b depicts the geometric setup of the two beamformers of
In the embodiment of
According to the embodiment of
c illustrates this in more detail. According to an embodiment, the first beamformer 410 captures sound from a first direction. The second beamformer 420, which is located quite distantly from the first beamformer 410, captures sound from a second direction.
The first and the second beamformer 410, 420 are arranged such that they are directed to the target location 430. In advantageous embodiments, the beamformers 410, 420, e.g. two microphone arrays, are distant from each other and face the target spot from different directions. This is different to traditional microphone array processing, where only a single array is used and its different sensors are placed in close proximity of each other. The first major axis 418 of the first beamformer 410 and the second major axis 428 of the second beamformer 420 form two straight lines which are not arranged in parallel, but which instead intersect with an angle of intersection a. The second beamformer 420 would be optimally positioned with respect to the first beamformer, when the angle of intersection is 90 degrees. In embodiments, the angle of intersection is at least 60 degrees.
The target spot or target area for sound capture is the intersection of both beams 415, 425. The signal from this area is derived by processing the output signals of the two beamformers 410, 420, such that an “acoustic intersection” is computed. This intersection can be considered as the signal part that is common/coherent between the two individual beamformer output signals.
Such a concept exploits both the individual directionality of the beamformers and the coherence between the beamformer output signals. This is different to common microphone array processing, where only a single array is used and its different sensors are placed in close proximity of each other.
By this, emitted sound is captured/acquired from a specific target location. This is in contrast to approaches which use distributed microphones for estimating the position of sound sources, but which do not aim at an enhanced recording of the localized sound sources by considering the output of distant microphone arrays as proposed according to embodiments.
Besides using highly directional microphones, the concepts according to embodiments can be implemented with both classical beamformers and parametric spatial filters. If the beamformer introduces frequency-dependent amplitude and phase distortions, this should be known and taken into account for the computation of the “acoustic intersection”.
In an embodiment, a device, e.g. a signal generator, computes an “acoustic intersection” component. An ideal device for computing the intersection would deliver full output, if a signal is present in both beamformer audio signals (e.g. the audio signals recorded by the first and the second beamformer) and it would deliver zero output, if a signal is present only in one or none of the two beamformer audio signals. A good suppression characteristics that also ensures a good performance of the device may, for example, be achieved, by determining the transfer gain of a signal only present in one beamformer audio signal and by setting it into relation to the transfer gain for a signal present in both beamformer audio signals.
The two beamformer audio signals s1 and s2 may be considered as a superposition of a filtered, delayed and/or scaled common target signal s and individual noise/interferer signals, n1 and n2, such that
s
1
=f
1(s)+n1
and
s
2
=f
2(s)+n2
where f1(x) and f2(x) are the individual filtering, delay and/or scaling functions present for the two signals. Thus, the task is to estimate s from s1=f1(s)+n1 and s2=f2(s)+n2. To avoid ambiguities, f2(x) can be set to identity without loss in generality.
The “intersection component” may be implemented, in different ways.
According to an embodiment, the common part between the two signals is computed using filters, e.g. classic adaptive LMS (Least Mean Square) filters, as they are common for acoustic echo cancellation.
The signal generator of
The signal generator of
The signal generator is adapted to adjust the filter coefficients of the adaptive filter 510 such that the difference between the filtered version of s1 (=s) and s2 is minimized. Thus, the signal s, i.e. the filtered version of s1, can be considered as representing the desired coherent output signal. Thus, the signal s, i.e. the filtered version of s1 represents the desired coherent output signal.
In another embodiment, the common part between the two signals is extracted based on a coherence metric between the two signals, see, for example, the coherence metrics described in
See also, the coherence metrics described in [Fa06] and [Her08].
A coherent part of two signals can be extracted from signals being represented in a time domain, but also, and advantageously, from signals being represented in a spectral domain, e.g. a time/frequency domain.
Moreover, the signal generator comprises an intersection calculator 620 for generating an audio output signal in the spectral domain.
Furthermore, the signal generator comprises a synthesis filterbank 630 for transforming the generated audio output signal from a spectral domain to a time domain. The synthesis filterbank 630 may, for example, comprise Short-Time Fourier Transform (STFT) synthesis filterbanks, polyphase synthesis filterbanks, Quadrature Mirror Filter (QMF) synthesis filterbanks, but also synthesis filterbanks like Discrete Fourier Transform (DFT), Discrete Cosine Transform (DCT) and the Modified Discrete Cosine Transform (MDCT) synthesis filterbanks.
In the following, possible ways of computing the audio output signal, e.g. by extracting a coherence, are explained. The intersection calculator 620 of
The coherence, as extracted is a measure of the common coherent content while compensating for scaling and phase shift operations. See, for example:
One possibility to generate an estimate of the coherent signal part of the first and the second beamformer audio signal is to apply the cross-factors to one of the two signals. The cross-factors may be time-averaged. Here, it is assumed, that the relative delay between the first and the second beamformer audio signal is limited, such that it is substantially smaller than the filterbank window size.
In the following, embodiments of calculating the audio output signal in the spectral domain by extracting the common signal part and by employing the correlation based approach based on an explicit calculation of a measure of coherence is explained in detail.
The signals S1(k,n) and S2(k,n) denote spectral-domain representations of the beamformer audio signals where k is a frequency index and n is a time index. For each particular time-frequency tile (k,n) specified by a particular frequency index k and a particular time index n, a coefficient exists for each of the signals S1(k,n) and S2(k,n). From the two spectral-domain beamformer audio signals S1(k,n), S2(k,n), the intersection component energy is computed. This intersection component energy may be computed by e.g., determining the magnitude of the cross-spectral density (CSD) C12(k,n) of S1(k,n) and S2(k,n):
C
12(k,n)=|E{S1(k,n)·S*2(k,n)}|
Here, the superscript * denotes the conjugate of a complex number and E{ } represents mathematical expectation. In practice, the expectation operator is replaced, e.g., by temporal or frequency smoothing of the term S1(k,n)·S*2(k,n), depending on the time/frequency resolution of the filterbank employed.
The power spectral density (PSD) P1(k,n) of the first beamformer audio signal S1(k,n) and the power spectral density P2(k,n) of the second beamformer audio signal S2(k,n) may be computed according to the formulae:
P
1(k,n)=E{|S1(k,n)|2}
P
2(k,n)=E{|S2(k,n)|2}.
In the following, embodiments for practical implementations of the computation of the acoustic intersection Y(k,n) from the two beamformer audio signals are presented.
A first way to obtain an output signal is based on modifying the first beamformer audio signal S1(k,n):
Similarly, an alternative output signal can be derived from the second beamformer audio signal S2(k,n):
For determining the output signal, it may be useful to limit the maximum value of the gain functions G1(k,n) and G2(k,n) to a certain threshold value, e.g. to one.
In step 710 a cross-spectral density C12(k, n) of the first and the second beamformer audio signal is computed. For example, the above-described formula C12(k,n)=|E{S1(k,n)·S*2(k,n)}| may be applied.
In step 720, the power spectral density P1(k, n) of the first beamformer audio signal is computed. Alternatively, the power spectral density of the second beamformer audio signal may be used as well.
Subsequently, in step 730, a gain function G1(k, n) is computed based on the cross-spectral density calculated in step 710 and the power spectral density calculated in step 720.
Finally, in step 740, the first beamformer audio signal S1(k, n) is modified to obtain desired the audio output signal Y1(k, n). If the power spectral density of the second beamformer audio signal has been calculated in step 720, then, the second beamformer audio signal s2(k, n) may be modified to obtain the desired audio output signal.
Since both implementations have a single energy term in the denominator, which can become small depending on the location of the active sound source with respect to the two beams, it is advantageous to use a gain that represents the ratio between the sound energy corresponding to the acoustic intersection and the overall or mean sound energy picked up by the beamformers. An output signal may be obtained by applying the formula
or by applying the formula:
In both examples described above, the gain functions will take small values in case the recorded sound in the beamformer audio signals does not comprise signal components of the acoustic intersection. On the other hand, gain values close to one are obtained if the beamformer audio signals correspond to the desired acoustic intersection.
Furthermore, in order to make sure that only components appear in the audio output signal that correspond to the acoustic intersection (despite of the limited directivity of the used beamformers) it may be advisable to compute the final output signal as the smaller signal (by energy) of Y1 and Y2 (or Y3 and Y4), respectively. In an embodiment, the signal Y1 or Y2 of the two signals Y1, Y2 is considered as the smaller signal, that has the smaller average energy. In another embodiment, the signal Y3 or Y4 is considered as the smaller signal of both signals Y3, Y4, that has the smaller average energy.
Also, other ways of calculating audio output signals exist that, unlike described with respect to the previous embodiments, make use of both the first and the second beamformer audio signals SI and S2 (as opposed to only using their powers) by combining them into a single signal which is subsequently weighted using one of the described gain functions. For example, the first and the second beamformer audio signal S1 and S2 may be added and the resulting sum signal may subsequently be weighted using one of the above-described gain functions.
The spectral-domain audio output signal S may be converted back from a time/frequency representation to a time signal by using a synthesis (inverse) filterbank.
In another embodiment, the common part between the two signals is extracted by processing the magnitude spectra of a combined signal (e.g. a sum signal), for example, such that it has the intersection (e.g. minimum) PSD (Power Spectral Density) of both (normalized) beamformer signals. The input signals may be analyzed in a time/frequency selective fashion, as described before, and an idealized assumption is made that the two noise signals are sparse and disjoint, i.e. do not appear at the same time/frequency tile. In this case, a simple solution would be to limit the Power Spectral Density (PSD) value of one of the signals to the value of the other signal after some suitable re-normalization/alignment procedure. It may be assumed that the relative delay between the two signals is limited such that it is substantially smaller than the filterbank window size.
Although some aspects have been described in the context of an apparatus, it is clear that these aspects also represent a description of the corresponding method, where a block or device corresponds to a method step or a feature of a method step. Analogously, aspects described in the context of a method step also represent a description of a corresponding block or item or feature of a corresponding apparatus.
A signal generated according to the above-described embodiments can be stored on a digital storage medium or can be transmitted on a transmission medium such as a wireless transmission medium or a wired transmission medium such as the Internet.
Depending on certain implementation requirements, embodiments of the invention can be implemented in hardware or in software. The implementation can be performed using a digital storage medium, for example a floppy disk, a DVD, a CD, a ROM, a PROM, an EPROM, an EEPROM or a FLASH memory, having electronically readable control signals stored thereon, which cooperate (or are capable of cooperating) with a programmable computer system such that the respective method is performed.
Some embodiments according to the invention comprise a non-transitory data carrier having electronically readable control signals, which are capable of cooperating with a programmable computer system, such that one of the methods described herein is performed.
Generally, embodiments of the present invention can be implemented as a computer program product with a program code, the program code being operative for performing one of the methods when the computer program product runs on a computer. The program code may for example be stored on a machine readable carrier.
Other embodiments comprise the computer program for performing one of the methods described herein, stored on a machine readable carrier.
In other words, an embodiment of the inventive method is, therefore, a computer program having a program code for performing one of the methods described herein, when the computer program runs on a computer.
A further embodiment of the inventive methods is, therefore, a data carrier (or a digital storage medium, or a computer-readable medium) comprising, recorded thereon, the computer program for performing one of the methods described herein.
A further embodiment of the inventive method is, therefore, a data stream or a sequence of signals representing the computer program for performing one of the methods described herein. The data stream or the sequence of signals may for example be configured to be transferred via a data communication connection, for example via the Internet.
A further embodiment comprises a processing means, for example a computer, or a programmable logic device, configured to or adapted to perform one of the methods described herein.
A further embodiment comprises a computer having installed thereon the computer program for performing one of the methods described herein.
In some embodiments, a programmable logic device (for example a field programmable gate array) may be used to perform some or all of the functionalities of the methods described herein. In some embodiments, a field programmable gate array may cooperate with a microprocessor in order to perform one of the methods described herein. Generally, the methods are advantageously performed by any hardware apparatus.
While this invention has been described in terms of several embodiments, there are alterations, permutations, and equivalents which fall within the scope of this invention. It should also be noted that there are many alternative ways of implementing the methods and compositions of the present invention. It is therefore intended that the following appended claims be interpreted as including all such alterations, permutations and equivalents as fall within the true spirit and scope of the present invention.
This application is a continuation of copending International Application No. PCT/EP2011/071600, filed Dec. 2, 2011, which is incorporated herein by reference in its entirety, and additionally claims priority from U.S. Application No. 61/419,720, filed Dec. 3, 2010, which is also incorporated herein by reference in its entirety.
Number | Date | Country | |
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61419720 | Dec 2010 | US |
Number | Date | Country | |
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Parent | PCT/EP2011/071600 | Dec 2011 | US |
Child | 13904857 | US |