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28 nips-2005-Analyzing Auditory Neurons by Learning Distance Functions


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Author: Inna Weiner, Tomer Hertz, Israel Nelken, Daphna Weinshall

Abstract: We present a novel approach to the characterization of complex sensory neurons. One of the main goals of characterizing sensory neurons is to characterize dimensions in stimulus space to which the neurons are highly sensitive (causing large gradients in the neural responses) or alternatively dimensions in stimulus space to which the neuronal response are invariant (defining iso-response manifolds). We formulate this problem as that of learning a geometry on stimulus space that is compatible with the neural responses: the distance between stimuli should be large when the responses they evoke are very different, and small when the responses they evoke are similar. Here we show how to successfully train such distance functions using rather limited amount of information. The data consisted of the responses of neurons in primary auditory cortex (A1) of anesthetized cats to 32 stimuli derived from natural sounds. For each neuron, a subset of all pairs of stimuli was selected such that the responses of the two stimuli in a pair were either very similar or very dissimilar. The distance function was trained to fit these constraints. The resulting distance functions generalized to predict the distances between the responses of a test stimulus and the trained stimuli. 1

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Summary: the most important sentenses genereted by tfidf model

sentIndex sentText sentNum sentScore

1 We formulate this problem as that of learning a geometry on stimulus space that is compatible with the neural responses: the distance between stimuli should be large when the responses they evoke are very different, and small when the responses they evoke are similar. [sent-9, score-1.616]

2 Here we show how to successfully train such distance functions using rather limited amount of information. [sent-10, score-0.223]

3 The data consisted of the responses of neurons in primary auditory cortex (A1) of anesthetized cats to 32 stimuli derived from natural sounds. [sent-11, score-1.358]

4 For each neuron, a subset of all pairs of stimuli was selected such that the responses of the two stimuli in a pair were either very similar or very dissimilar. [sent-12, score-1.306]

5 The resulting distance functions generalized to predict the distances between the responses of a test stimulus and the trained stimuli. [sent-14, score-0.895]

6 1 Introduction A major challenge in auditory neuroscience is to understand how cortical neurons represent the acoustic environment. [sent-15, score-0.637]

7 Neural responses to complex sounds are idiosyncratic, and small perturbations in the stimuli may give rise to large changes in the responses. [sent-16, score-0.877]

8 The dominant approach to the functional characterization of sensory neurons attempts to predict the response of the cortical neuron to a novel stimulus. [sent-18, score-0.506]

9 Prediction is usually estimated from a set of known responses of a given neuron to a set of stimuli (sounds). [sent-19, score-0.861]

10 The most popular approach computes the spectrotemporal receptive field (STRF) of each neuron, and uses this linear model to predict neuronal responses. [sent-20, score-0.253]

11 In this paper we take a different approach to the characterization of auditory cortical neurons. [sent-22, score-0.472]

12 Our approach attempts to learn the non-linear warping of stimulus space that is in- duced by the neuronal responses. [sent-23, score-0.351]

13 This approach is motivated by our previous observations [3] that different neurons impose different partitions of the stimulus space, which are not necessarily simply related to the spectro-temporal structure of the stimuli. [sent-24, score-0.405]

14 More specifically, we characterize a neuron by learning a pairwise distance function over the stimulus domain that will be consistent with the similarities between the responses to different stimuli, see Section 2. [sent-25, score-0.845]

15 Intuitively a good distance function would assign small values to pairs of stimuli that elicit a similar neuronal response, and large values to pairs of stimuli that elicit different neuronal responses. [sent-26, score-1.551]

16 Second, unlike most functional characterizations that are limited to linear or weakly non-linear models, distance learning can approximate functions that are highly non-linear. [sent-28, score-0.25]

17 Finally, we explicitly learn a distance function on stimulus space; by examining the properties of such a function, it may be possible to determine the stimulus features that most strongly influence the responses of a cortical neuron. [sent-29, score-1.081]

18 In this paper we therefore focus on two questions: (1) Can we learn distance functions over the stimulus domain for single cells using information extracted from their neuronal responses? [sent-31, score-0.713]

19 and (2) What is the predictive power of these cell specific distance functions when presented with novel stimuli? [sent-33, score-0.495]

20 In order to address these questions we used extracellular recordings from 22 cells in the auditory cortex of cats in response to natural bird chirps and some modified versions of these chirps [1]. [sent-34, score-0.793]

21 To estimate the distance between responses, we used a normalized distance measure between the peri-stimulus time histograms of the responses to the different stimuli. [sent-35, score-0.73]

22 Our results, described in Section 4, show that we can learn compatible distance functions on the stimulus domain with relatively low training errors. [sent-36, score-0.452]

23 This result is interesting by itself as a possible characterization of cortical auditory neurons, a goal which eluded many previous studies [3]. [sent-37, score-0.472]

24 Using cross validation, we measure the test error (or predictive power) of our method, and report generalization power which is significantly higher than previously reported for natural stimuli [10]. [sent-38, score-0.586]

25 We then show that performance can be further improved by learning a distance function using information from pairs of related neurons. [sent-39, score-0.259]

26 Finally, we show better generalization performance for wide-band stimuli as compared to narrow-band stimuli. [sent-40, score-0.433]

27 These latter two contributions may have some interesting biological implications regarding the nature of the computations done by auditory cortical neurons. [sent-41, score-0.419]

28 Related work Recently, considerable attention has been focused on spectrotemporal receptive fields (STRFs) as characterizations of the function of auditory cortical neurons [8, 4, 2, 11, 16]. [sent-42, score-0.76]

29 It can be interpreted both as providing the neuron’s most efficient stimulus (in the time-frequency domain), and also as the spectro-temporal impulse response of the neuron [10, 12]. [sent-44, score-0.367]

30 Furthermore, when STRFs are used to predict neuronal responses to natural stimuli they often fail to predict the correct responses [10, 6]. [sent-47, score-1.284]

31 Similar results were also reported in [14], who found that STRF models account for only 18 − 40% (on average) of the stimulus related power in auditory cortical neural responses to dynamic random chord stimuli. [sent-50, score-1.018]

32 Various other studies have shown that there are significant and relevant non-linearities in auditory cortical responses to natural stimuli [13, 1, 9, 10]. [sent-51, score-1.237]

33 al [1] have shown that auditory neurons are extremely sensitive to small perturbations in the (natural) acoustic context. [sent-53, score-0.531]

34 2 Formalizing the problem as a distance learning problem Our approach is based on the idea of learning a cell-specific distance function over the space of all possible stimuli, relying on partial information extracted from the neuronal responses of the cell. [sent-55, score-0.812]

35 The initial data consists of stimuli and the resulting neural responses. [sent-56, score-0.433]

36 We use the neuronal responses to identify pairs of stimuli to which the neuron responded similarly and pairs to which the neuron responded very differently. [sent-57, score-1.341]

37 These pairs can be formally described by equivalence constraints. [sent-58, score-0.227]

38 Equivalence constraints are relations between pairs of datapoints, which indicate whether the points in the pair belong to the same category or not. [sent-59, score-0.196]

39 In this setting the goal of the algorithm is to learn a distance function that attempts to comply with the equivalence constraints. [sent-61, score-0.286]

40 Specifically, we combine equivalence constraints gathered from pairs of cells which have similar responses, and train a single distance function for both cells. [sent-63, score-0.661]

41 Our results demonstrate that this approach improves prediction results of the “weaker” cell, and almost always improves the result of the “stronger” cell in each pair. [sent-64, score-0.333]

42 Another interesting result of this formalism is the ability to classify stimuli based on the responses of the total recorded cortical cell ensemble. [sent-65, score-1.22]

43 For some stimuli, the predictive performance based on the learned inter-stimuli distance was very good, whereas for other stimuli it was rather poor. [sent-66, score-0.621]

44 These differences were correlated with the acoustic structure of the stimuli, partitioning them into narrowband and wideband stimuli. [sent-67, score-0.358]

45 3 Methods Experimental setup Extracellular recordings were made in primary auditory cortex of nine halothane-anesthetized cats. [sent-68, score-0.356]

46 Single neurons were recorded using metal microelectrodes and an online spike sorter (MSD, alpha-omega). [sent-72, score-0.193]

47 Four stimuli, each of length 60-100 ms, consisted of a main tonal component with frequency and amplitude modulation and of a background noise consisting of echoes and unrelated components. [sent-77, score-0.192]

48 Each of these stimuli was further modified by separating the main tonal component from the noise, and by further separating the noise into echoes and background. [sent-78, score-0.529]

49 In total, 8 versions of each stimulus were used, and therefore each neuron had a dataset consisting of 32 datapoints. [sent-80, score-0.313]

50 Each stimulus was represented using the first d real Cepstral coefficients. [sent-84, score-0.225]

51 Neuronal responses were represented by creating PeriStimulus Time Histograms (PSTHs) using 20 repetitions recorded for each stimuli. [sent-87, score-0.382]

52 Obtaining equivalence constraints over stimuli pairs The distances between responses were measured using a normalized χ2 distance measure. [sent-89, score-1.356]

53 All responses to both stimuli (40 responses in total) were superimposed to generate a single high-resolution PSTH. [sent-90, score-1.113]

54 The same bins were then used to generate the PSTHs of the responses to the two stimuli separately. [sent-92, score-0.773]

55 The (r i −r i )2 N i i distance between pairs of histograms is given by: χ2 (r1 , r2 ) = i=1 (ri1+ri2)/2 /(N − 1). [sent-95, score-0.331]

56 1 2 In order to identify pairs (or small groups) of similar responses, we computed the normalized χ2 distance matrix over all pairs of responses, and used the complete-linkage algorithm to cluster the responses into 8 − 12 clusters. [sent-96, score-0.735]

57 In order to obtain negative equivalence constraints, for each cluster ci we used the 2−3 furthest clusters from it to define negative constraints. [sent-98, score-0.247]

58 Distance learning method In this paper, we use the DistBoost algorithm [7], which is a semi-supervised boosting learning algorithm that learns a distance function using unlabeled datapoints and equivalence constraints. [sent-100, score-0.347]

59 Evaluation methods In order to evaluate the quality of the learned distance function, we measured the correlation between the distances computed by our distance learning algorithm to those induced by the χ2 distance over the responses. [sent-103, score-0.704]

60 For each stimulus we measured the distances to all other stimuli using the learnt distance function. [sent-104, score-0.981]

61 We then computed the rank-order (Spearman) correlation coefficient between these learnt distances in the stimulus domain and the χ2 distances between the appropriate responses. [sent-105, score-0.583]

62 This procedure produced a single correlation coefficient for each of the 32 stimuli, and the average correlation coefficient across all stimuli was used as the overall performance measure. [sent-106, score-0.631]

63 The optimal cell specific parameters were determined using this approach. [sent-111, score-0.273]

64 , xn ), xk ∈ X A set of equivalence constraints: (xi1 , xi2 , yi ), where yi ∈ {−1, 1} Unlabeled pairs of points: (xi1 , xi2 , yi = ∗), implicitly defined by all unconstrained pairs of points 1 • Initialize Wi1 i2 = 1/(n2 ) i1 , i2 = 1, . [sent-115, score-0.432]

65 Generate a weak “ hypothesis ht :” X × X → [−1, 1] and define a weak distance function as 1 ˜ ht (xi , xj ) = 2 1 − ht (xi , xj ) ∈ [0, 1] 3. [sent-126, score-0.519]

66 In each run, we removed a single stimulus from the dataset, trained our algorithm on the remaining 31 stimuli, and then tested its performance on the datapoint that was left out (see Fig. [sent-140, score-0.298]

67 As can be seen, on some cells our algorithm obtains correlations that are as high as 0. [sent-143, score-0.227]

68 41, while for other cells the average test correlation is less then 0. [sent-144, score-0.286]

69 Boosting the performance of weak cells In order to boost the performance of cells with low average correlations, we constructed the following experiment: We clustered the responses of each cell, using the complete-linkage algorithm over the χ2 distances with 4 1 clusters. [sent-156, score-0.791]

70 This measure was used to identify pairs of cells whose partition of the stimuli was most similar to each other. [sent-159, score-0.675]

71 In our experiment we took the four cells with the lowest Cell 13 All cells Cell 18 30 30 25 25 20 20 15 15 10 10 5 −1 −0. [sent-160, score-0.284]

72 The Mean Test Rank−Order Correlation rank-order correlations were computed between the learnt distances and the distances between the recorded responses for each single stimulus (N = 22 ∗ 32). [sent-167, score-0.918]

73 The distribution of train and test correlations is displayed as histograms on the top and on the right respectively. [sent-191, score-0.266]

74 Right: Test rankorder correlations when training using constraints extracted from each cell separately, and when using the intersection of the constraints extracted from a pair of cells. [sent-192, score-0.589]

75 This procedure always improves the performance of the weaker cell, and usually also improves the performance of the stronger cell 1 performance (right column of Fig 3), and for each of them used the F 2 score to retrieve the most similar cell. [sent-193, score-0.369]

76 For each of these pairs, we trained our algorithm once more, using the constraints obtained by intersecting the constraints derived from the two cells in the pair, in the LOU paradigm. [sent-194, score-0.34]

77 Interestingly and counter-intuitively, when training the better performing cell in each pair using the intersection of its constraints with those from the poorly performing cell, results deteriorated only for one of the four better performing cells. [sent-197, score-0.379]

78 Stimulus classification The cross-validation results induced a partition of the stimulus space into narrowband and wideband stimuli. [sent-198, score-0.516]

79 We measured the predictability of each stimulus by averaging the LOU test results obtained for the stimulus across all cells (see Fig. [sent-199, score-0.754]

80 Our analysis shows that wideband stimuli are more predictable than narrowband stimuli, despite the fact that the neuronal responses to these two groups are not different as a whole. [sent-201, score-1.19]

81 5 Discussion In the standard approach to auditory modeling, a linear or weakly non-linear model is fitted to the data, and neuronal properties are read from the resulting model. [sent-203, score-0.468]

82 The usefulness of this approach is limited however by the weak predictability of A1 responses when using such models. [sent-204, score-0.496]

83 5 1 1 Figure 3: Histograms of cell specific test rank-order correlations for the 22 cells in the dataset. [sent-251, score-0.545]

84 The rank-order correlations compare the predicted distances to the distances between the recorded responses, measured on a single stimulus which was left out during the training stage. [sent-252, score-0.612]

85 For visualization purposes, cells are ordered (columns) by their average test correlation per stimulus in descending order. [sent-253, score-0.511]

86 We use the neural data as a guide for training a highly non-linear distance function on stimulus space, which is compatible with the neural responses. [sent-256, score-0.419]

87 First, we demonstrated that we can improve the test performance of a distance function by using constraints on the similarity or dissimilarity between stimuli derived from the responses of multiple neurons. [sent-259, score-1.046]

88 Thus, it is possible that intersecting constraints derived from multiple neurons uncover regularities that are hard to extract from individual neurons. [sent-261, score-0.278]

89 Second, it turned out that some stimuli consistently behaved better than others across the neuronal population. [sent-262, score-0.559]

90 This difference was correlated with the acoustic structure of the stimuli: those stimuli that contained the weak background component (wideband stimuli) were generally predicted better. [sent-263, score-0.64]

91 This result is surprising both because background component is substantially weaker than the other acoustic components in the stimuli (by as much as 35-40 dB). [sent-264, score-0.567]

92 It may mean that the relationships between physical structure (as characterized by the Cepstral parameters) and the neuronal responses becomes simpler in the presence of the background component, but is much more idiosyncratic when this component is absent. [sent-265, score-0.539]

93 This result underscores the importance of interactions between narrow and wideband stimuli for understanding the complexity of cortical processing. [sent-266, score-0.767]

94 One major problem during an experiment is that of stimulus selection: choosing the best set of stimuli for characterizing the responses of a neuron. [sent-269, score-0.998]

95 The predictability of wideband stimuli is clearly better than that of the narrowband stimuli. [sent-287, score-0.808]

96 find surprising stimuli: either stimuli that are very different in terms of physical structure but that would result in responses that are similar to those already measured, or stimuli that are very similar to already tested stimuli but that are predicted to give rise to very different responses. [sent-288, score-1.676]

97 Group redundancy measures reveal redundancy reduction in the auditory pathway. [sent-313, score-0.287]

98 Analysis of dynamic spectra in ferret primary auditory cortex. [sent-357, score-0.365]

99 Processing of complex stimuli and natural scenes in the auditory cortex. [sent-394, score-0.765]

100 Relating cluster and population responses to natural sounds and tonal stimuli in cat primary auditory cortex. [sent-400, score-1.323]


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V+ V- II+ V+ V- II+ V+ V- II+ V+ V- II+ V+ V- II+ V+ V- II+ Figure 3: The first-order all-pass delay circuit (left) and the second-order all-pass delay (right). The differential output of the delay circuits is converted into a current which is multiplied by a variable gain implemented as shown in Figure 4. The gain cell includes a differential pair with source degeneration via transistors N4 and N5. The source degeneration improves the linearity of the current. The three gain cells implemented on the aVLSI have default gains of 2, 3 and 0.91 which are set by holding the default input high and appropriately ratioing the bias currents through the value of vbiasp. To correct any on-chip mismatches and/or explore other gain configurations a current splitter cell [7] (p-splitter, figure 4) allows the gain to be programmed by digital means post fabrication. 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Figure 5 shows the basic building blocks for the filters – the Tau Cell [8] and the multiplier cell – and block diagrams showing how these blocks were connected to create the necessary filtering blocks. The Tau Cell is a log-domain filter which has the firstorder response: I out 1 , = I in sτ + 1 where τ = nC aVT Ia and n = the slope factor, VT = thermal voltage, Ca = capacitance, and Ia = bias current. In figure 5, the input currents to the Tau Cell, Imult and A*Ia, are only used when building a second-order filter. The multiplier cell is simply a translinear loop where: I out1 ∗ I mult = I out 2 ∗ AI a or Imult = AIaIout2/Iout1. The configurations of the Tau Cell to get particular responses are covered in [8] along with the corresponding equations. The high frequency filter of Figure 2 is implemented by the high-pass filter in Figure 5 with a corner frequency of 17kHz. The low frequency filter, however, is divided into two parts since the biological filter’s response (see for example Figure 3A in [9]) separates well into a narrow second-order band-pass filter with a 10kHz resonant frequency and a wide band-pass filter made from a first-order high-pass filter with a 3kHz corner frequency followed by a first-order low-pass filter with a 12kHz corner frequency. These filters are then added together to reproduce the biological filter. The filters’ responses can be adjusted post fabrication via their bias currents. This allows for compensation due to processing and matching errors. Figure 4: The Gain Cell above is used to convert the differential voltage input from the delay cells into a single-ended current output. The gain of each cell is controllable via a programmable current cell (p_splitter). An on-chip bias generator [7] was used to create all the necessary current biases on the chip. 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After that, recordings were taken of the directional frequency responses. Sounds were generated by computer for each chip input to simulate moving the forelegs by delaying the sound by the appropriate amount of time; this was a much simpler solution than using microphones and moving them using motors. 4 Results The aVLSI chip was tested to measure its gains and delays, which were successfully tuned to the appropriate values. The chip was then compared with the simulation to check that it was faithfully modelling the system. A result of this test at 4kHz (approximately the cricket calling-song frequency) is shown in Figure 6. Apart from a drop in amplitude of the signal, the response of the circuit was very similar to that of the simulator. The differences were expected because the aVLSI circuit has to deal with real-world noise, whereas the simulated version has perfect signals. Examples of the gain versus frequency response of the two log-domain band-pass filters are shown in Figure 7. Note that the narrow-band filter peaks at 6kHz, which is significantly above the mating song frequency of the cricket which is around 4.5kHz. This is not a mistake, but is observed in real crickets as well. As stated in the introduction, a range of further testing results with both the circuit and the simulator are being published in [6]. 5 D i s c u s s i on The aVLSI auditory sensor in this research models the hearing of the field cricket Gryllus bimaculatus. It is a more faithful model of the cricket auditory system than was previously built in [4], reproducing all the acoustic inputs, as well as the responses to frequencies of both the co specific calling song and bat echolocation chirps. It also generates outputs corresponding to the two sets of behaviourally relevant auditory receptor fibres. Results showed that it matched the biological data well, though there were some inconsistencies due to an error in the specification that will be addressed in a future iteration of the design. A more complete implementation across all frequencies was impractical because of complexity and size issues as well as serving no clear behavioural purpose. Figure 6: Vibration amplitude of the left (dotted) and right (solid) virtual tympana measured in decibels in response to a 4kHz tone in simulation (left) and on the aVLSI chip (right). The plot shows the amplitude of the tympanal responses as the sound source is rotated around the cricket. Figure 7: Frequency-Gain curves for the narrow-band and wide-band bandpass filters. The long-term aim of this work is to better understand simple sensorimotor control loops in crickets and other insects. The next step is to mount this circuitry on a robot to carry out behavioural experiments, which we will compare with existing and new behavioural data (such as that in [10]). This will allow us to refine our models of the neural circuitry involved. Modelling the sensory afferent neurons in hardware is necessary in order to reduce processor load on our robot, so the next revision will include these either onboard, or on a companion chip as we have done before [11]. We will also move both sides of the auditory system onto a single chip to conserve space on the robot. It is our belief and experience that, as a result of this intelligent pre-processing carried out at the sensor level, the neural circuits necessary to accurately model the behaviour will remain simple. Acknowledgments The authors thank the Institute of Neuromorphic Engineering and the UK Biotechnology and Biological Sciences Research Council for funding the research in this paper. References [1] R. Wehner. Matched filters – neural models of the external world. J Comp Physiol A, 161: 511–531, 1987. [2] A. Michelsen, A. V. Popov, and B. Lewis. Physics of directional hearing in the cricket Gryllus bimaculatus. Journal of Comparative Physiology A, 175:153–164, 1994. [3] A. Michelsen. The tuned cricket. News Physiol. Sci., 13:32–38, 1998. [4] H. H. Lund, B. Webb, and J. Hallam. A robot attracted to the cricket species Gryllus bimaculatus. In P. Husbands and I. Harvey, editors, Proceedings of 4th European Conference on Artificial Life, pages 246–255. MIT Press/Bradford Books, MA., 1997. [5] R Reeve and B. Webb. New neural circuits for robot phonotaxis. Phil. Trans. R. Soc. Lond. A, 361:2245–2266, August 2003. [6] R. Reeve, A. van Schaik, C. Jin, T. Hamilton, B. Torben-Nielsen and B. Webb Directional hearing in a silicon cricket. Biosystems, (in revision), 2005b [7] T. 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The current splitter takes an input current (Ibias, figure 4) and divides it into branches which recursively halve the current, i.e., the first branch gives ½ Ibias, the second branch ¼ Ibias, the third branch 1/8 Ibias and so on. These currents can be used together with digitally controlled switches as a Digital-to-Analogue converter. By holding default low and setting C5:C0 appropriately, any gain – from 4 to 0.125 – can be set. To save on output pins the program bits (C5:C0) for each of the three gain cells are set via a single 18-bit shift register in bit-serial fashion. Summing the output of the three gain circuits in the current domain simply involves connecting three wires together. Therefore, a natural option for the filters that follow is to use current domain filters. In our case we have chosen to implement log-domain filters using MOS transistors operating in weak inversion. Figure 5 shows the basic building blocks for the filters – the Tau Cell [8] and the multiplier cell – and block diagrams showing how these blocks were connected to create the necessary filtering blocks. The Tau Cell is a log-domain filter which has the firstorder response: I out 1 , = I in sτ + 1 where τ = nC aVT Ia and n = the slope factor, VT = thermal voltage, Ca = capacitance, and Ia = bias current. In figure 5, the input currents to the Tau Cell, Imult and A*Ia, are only used when building a second-order filter. The multiplier cell is simply a translinear loop where: I out1 ∗ I mult = I out 2 ∗ AI a or Imult = AIaIout2/Iout1. The configurations of the Tau Cell to get particular responses are covered in [8] along with the corresponding equations. The high frequency filter of Figure 2 is implemented by the high-pass filter in Figure 5 with a corner frequency of 17kHz. 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After that, recordings were taken of the directional frequency responses. Sounds were generated by computer for each chip input to simulate moving the forelegs by delaying the sound by the appropriate amount of time; this was a much simpler solution than using microphones and moving them using motors. 4 Results The aVLSI chip was tested to measure its gains and delays, which were successfully tuned to the appropriate values. The chip was then compared with the simulation to check that it was faithfully modelling the system. A result of this test at 4kHz (approximately the cricket calling-song frequency) is shown in Figure 6. Apart from a drop in amplitude of the signal, the response of the circuit was very similar to that of the simulator. The differences were expected because the aVLSI circuit has to deal with real-world noise, whereas the simulated version has perfect signals. 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Results showed that it matched the biological data well, though there were some inconsistencies due to an error in the specification that will be addressed in a future iteration of the design. A more complete implementation across all frequencies was impractical because of complexity and size issues as well as serving no clear behavioural purpose. Figure 6: Vibration amplitude of the left (dotted) and right (solid) virtual tympana measured in decibels in response to a 4kHz tone in simulation (left) and on the aVLSI chip (right). The plot shows the amplitude of the tympanal responses as the sound source is rotated around the cricket. Figure 7: Frequency-Gain curves for the narrow-band and wide-band bandpass filters. The long-term aim of this work is to better understand simple sensorimotor control loops in crickets and other insects. The next step is to mount this circuitry on a robot to carry out behavioural experiments, which we will compare with existing and new behavioural data (such as that in [10]). This will allow us to refine our models of the neural circuitry involved. Modelling the sensory afferent neurons in hardware is necessary in order to reduce processor load on our robot, so the next revision will include these either onboard, or on a companion chip as we have done before [11]. We will also move both sides of the auditory system onto a single chip to conserve space on the robot. It is our belief and experience that, as a result of this intelligent pre-processing carried out at the sensor level, the neural circuits necessary to accurately model the behaviour will remain simple. Acknowledgments The authors thank the Institute of Neuromorphic Engineering and the UK Biotechnology and Biological Sciences Research Council for funding the research in this paper. References [1] R. Wehner. Matched filters – neural models of the external world. J Comp Physiol A, 161: 511–531, 1987. [2] A. Michelsen, A. V. Popov, and B. Lewis. Physics of directional hearing in the cricket Gryllus bimaculatus. Journal of Comparative Physiology A, 175:153–164, 1994. [3] A. Michelsen. The tuned cricket. News Physiol. Sci., 13:32–38, 1998. [4] H. H. Lund, B. Webb, and J. Hallam. A robot attracted to the cricket species Gryllus bimaculatus. In P. Husbands and I. Harvey, editors, Proceedings of 4th European Conference on Artificial Life, pages 246–255. MIT Press/Bradford Books, MA., 1997. [5] R Reeve and B. Webb. New neural circuits for robot phonotaxis. Phil. Trans. R. Soc. Lond. A, 361:2245–2266, August 2003. [6] R. Reeve, A. van Schaik, C. Jin, T. Hamilton, B. Torben-Nielsen and B. Webb Directional hearing in a silicon cricket. Biosystems, (in revision), 2005b [7] T. 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