Ripples in the Anterior Auditory Field and Inferior Colliculus of the Ferret

Similar documents
Neuronal correlates of pitch in the Inferior Colliculus

Spectro-Temporal Methods in Primary Auditory Cortex David Klein Didier Depireux Jonathan Simon Shihab Shamma

Spectro-Temporal Processing of Dynamic Broadband Sounds In Auditory Cortex

0.18 μm CMOS Fully Differential CTIA for a 32x16 ROIC for 3D Ladar Imaging Systems

Durable Aircraft. February 7, 2011

David Siegel Masters Student University of Cincinnati. IAB 17, May 5 7, 2009 Ford & UM

Investigation of a Forward Looking Conformal Broadband Antenna for Airborne Wide Area Surveillance

Frequency Stabilization Using Matched Fabry-Perots as References

COM DEV AIS Initiative. TEXAS II Meeting September 03, 2008 Ian D Souza

PSEUDO-RANDOM CODE CORRELATOR TIMING ERRORS DUE TO MULTIPLE REFLECTIONS IN TRANSMISSION LINES

Radar Detection of Marine Mammals

Loop-Dipole Antenna Modeling using the FEKO code

Remote Sediment Property From Chirp Data Collected During ASIAEX

August 9, Attached please find the progress report for ONR Contract N C-0230 for the period of January 20, 2015 to April 19, 2015.

Active Denial Array. Directed Energy. Technology, Modeling, and Assessment

Presentation to TEXAS II

Strategic Technical Baselines for UK Nuclear Clean-up Programmes. Presented by Brian Ensor Strategy and Engineering Manager NDA

U.S. Army Training and Doctrine Command (TRADOC) Virtual World Project

Coherent distributed radar for highresolution

Technology Maturation Planning for the Autonomous Approach and Landing Capability (AALC) Program

REPORT DOCUMENTATION PAGE

IREAP. MURI 2001 Review. John Rodgers, T. M. Firestone,V. L. Granatstein, M. Walter

Report Documentation Page

Report Documentation Page

A RENEWED SPIRIT OF DISCOVERY

SA Joint USN/USMC Spectrum Conference. Gerry Fitzgerald. Organization: G036 Project: 0710V250-A1

N C-0002 P13003-BBN. $475,359 (Base) $440,469 $277,858

Innovative 3D Visualization of Electro-optic Data for MCM

Modeling of Ionospheric Refraction of UHF Radar Signals at High Latitudes

Development of a charged-particle accumulator using an RF confinement method FA

Robotics and Artificial Intelligence. Rodney Brooks Director, MIT Computer Science and Artificial Intelligence Laboratory CTO, irobot Corp

Mathematics, Information, and Life Sciences

REPORT DOCUMENTATION PAGE

ULTRASTABLE OSCILLATORS FOR SPACE APPLICATIONS

REPORT DOCUMENTATION PAGE. Thermal transport and measurement of specific heat in artificially sculpted nanostructures. Dr. Mandar Madhokar Deshmukh

A HIGH-PRECISION COUNTER USING THE DSP TECHNIQUE

Wavelength Division Multiplexing (WDM) Technology for Naval Air Applications

Signal Processing Architectures for Ultra-Wideband Wide-Angle Synthetic Aperture Radar Applications

SYSTEMATIC EFFECTS IN GPS AND WAAS TIME TRANSFERS

Drexel Object Occlusion Repository (DOOR) Trip Denton, John Novatnack and Ali Shokoufandeh

Hybrid QR Factorization Algorithm for High Performance Computing Architectures. Peter Vouras Naval Research Laboratory Radar Division

Student Independent Research Project : Evaluation of Thermal Voltage Converters Low-Frequency Errors

Rump Session: Advanced Silicon Technology Foundry Access Options for DoD Research. Prof. Ken Shepard. Columbia University

Acoustic Change Detection Using Sources of Opportunity

NEURAL NETWORKS IN ANTENNA ENGINEERING BEYOND BLACK-BOX MODELING

Synthetic Behavior for Small Unit Infantry: Basic Situational Awareness Infrastructure

Non-Data Aided Doppler Shift Estimation for Underwater Acoustic Communication

Ground Based GPS Phase Measurements for Atmospheric Sounding

Solar Radar Experiments

A Multi-Use Low-Cost, Integrated, Conductivity/Temperature Sensor

INFRASOUND SENSOR MODELS AND EVALUATION. Richard P. Kromer and Timothy S. McDonald Sandia National Laboratories

EFFECTS OF ELECTROMAGNETIC PULSES ON A MULTILAYERED SYSTEM

Experimental Studies of Vulnerabilities in Devices and On-Chip Protection

REPORT DOCUMENTATION PAGE

Joint Milli-Arcsecond Pathfinder Survey (JMAPS): Overview and Application to NWO Mission

HIGH TEMPERATURE (250 C) SIC POWER MODULE FOR MILITARY HYBRID ELECTRICAL VEHICLE APPLICATIONS

Underwater Intelligent Sensor Protection System

INTEGRATIVE MIGRATORY BIRD MANAGEMENT ON MILITARY BASES: THE ROLE OF RADAR ORNITHOLOGY

CFDTD Solution For Large Waveguide Slot Arrays

Evanescent Acoustic Wave Scattering by Targets and Diffraction by Ripples

SILICON CARBIDE FOR NEXT GENERATION VEHICULAR POWER CONVERTERS. John Kajs SAIC August UNCLASSIFIED: Dist A. Approved for public release

Reduced Power Laser Designation Systems

Acoustic Horizontal Coherence and Beamwidth Variability Observed in ASIAEX (SCS)

North Pacific Acoustic Laboratory (NPAL) Towed Array Measurements

Range-Depth Tracking of Sounds from a Single-Point Deployment by Exploiting the Deep-Water Sound Speed Minimum

Automatic Payload Deployment System (APDS)

Two-Way Time Transfer Modem

Department of Defense Partners in Flight

14. Model Based Systems Engineering: Issues of application to Soft Systems

RECENT TIMING ACTIVITIES AT THE U.S. NAVAL RESEARCH LABORATORY

FAST DIRECT-P(Y) GPS SIGNAL ACQUISITION USING A SPECIAL PORTABLE CLOCK

VHF/UHF Imagery of Targets, Decoys, and Trees

UNCLASSIFIED UNCLASSIFIED 1

LONG TERM GOALS OBJECTIVES

AUVFEST 05 Quick Look Report of NPS Activities

MATLAB Algorithms for Rapid Detection and Embedding of Palindrome and Emordnilap Electronic Watermarks in Simulated Chemical and Biological Image Data

Acoustic Measurements of Tiny Optically Active Bubbles in the Upper Ocean

USAARL NUH-60FS Acoustic Characterization

THE DET CURVE IN ASSESSMENT OF DETECTION TASK PERFORMANCE

Ocean Acoustics and Signal Processing for Robust Detection and Estimation

Ship echo discrimination in HF radar sea-clutter

MONITORING RUBBLE-MOUND COASTAL STRUCTURES WITH PHOTOGRAMMETRY

Army Acoustics Needs

Diver-Operated Instruments for In-Situ Measurement of Optical Properties

REPORT DOCUMENTATION PAGE. 1. REPORT DATE (DD-MM-YYYY) 2. REPORT TYPE 3. DATES COVERED (From - To) Monthly IMay-Jun 2008

Frequency Dependent Harmonic Powers in a Modified Uni-Traveling Carrier (MUTC) Photodetector

Investigation of Modulated Laser Techniques for Improved Underwater Imaging

THE NATIONAL SHIPBUILDING RESEARCH PROGRAM

Marine Mammal Acoustic Tracking from Adapting HARP Technologies

A Comparison of Two Computational Technologies for Digital Pulse Compression

DARPA TRUST in IC s Effort. Dr. Dean Collins Deputy Director, MTO 7 March 2007

Digital Radiography and X-ray Computed Tomography Slice Inspection of an Aluminum Truss Section

ARL-TN-0835 July US Army Research Laboratory

Pressure vs. decibel modulation in spectrotemporal representations: How nonlinear are auditory cortical stimuli?

Experimental Observation of RF Radiation Generated by an Explosively Driven Voltage Generator

Fall 2014 SEI Research Review Aligning Acquisition Strategy and Software Architecture

Sea Surface Backscatter Distortions of Scanning Radar Altimeter Ocean Wave Measurements

DoDTechipedia. Technology Awareness. Technology and the Modern World

Measurement of Ocean Spatial Coherence by Spaceborne Synthetic Aperture Radar

Wavelet Shrinkage and Denoising. Brian Dadson & Lynette Obiero Summer 2009 Undergraduate Research Supported by NSF through MAA

Transcription:

Ripples in the Anterior Auditory Field and Inferior Colliculus of the Ferret Didier Depireux Nina Kowalski Shihab Shamma Tony Owens Huib Versnel Amitai Kohn University of Maryland College Park Supported in part by the Air Force Office of Scientific Research, the Office of Naval Research, the National Science Foundation Grant CD-88312 and the National Institutes of Health.

Report Documentation Page Form Approved OMB No. 7-188 Public reporting burden for the collection of information is estimated to average 1 hour per response, including the time for reviewing instructions, searching existing data sources, gathering and maintaining the data needed, and completing and reviewing the collection of information. Send comments regarding this burden estimate or any other aspect of this collection of information, including suggestions for reducing this burden, to Washington Headquarters Services, Directorate for Information Operations and Reports, 1215 Jefferson Davis Highway, Suite 12, Arlington VA 2222-32. Respondents should be aware that notwithstanding any other provision of law, no person shall be subject to a penalty for failing to comply with a collection of information if it does not display a currently valid OMB control number. 1. REPORT DATE 1996 2. REPORT TYPE 3. DATES COVERED --1996 to --1996. TITLE AND SUBTITLE Ripples in the Anterior Auditory Field and Inferior Colliculus of the Ferret 5a. CONTRACT NUMBER 5b. GRANT NUMBER 5c. PROGRAM ELEMENT NUMBER 6. AUTHOR(S) 5d. PROJECT NUMBER 5e. TASK NUMBER 5f. WORK UNIT NUMBER 7. PERFORMING ORGANIZATION NAME(S) AND ADDRESS(ES) Office of Naval Research,One Liberty Center,875 North Randolph Street Suite 125,Arlington,VA,2223-1995 8. PERFORMING ORGANIZATION REPORT NUMBER 9. SPONSORING/MONITORING AGENCY NAME(S) AND ADDRESS(ES) 1. SPONSOR/MONITOR S ACRONYM(S) 12. DISTRIBUTION/AVAILABILITY STATEMENT Approved for public release; distribution unlimited 13. SUPPLEMENTARY NOTES The original document contains color images. 1. ABSTRACT see report 15. SUBJECT TERMS 11. SPONSOR/MONITOR S REPORT NUMBER(S) 16. SECURITY CLASSIFICATION OF: 17. LIMITATION OF ABSTRACT a. REPORT unclassified b. ABSTRACT unclassified c. THIS PAGE unclassified 18. NUMBER OF PAGES 26 19a. NAME OF RESPONSIBLE PERSON Standard Form 298 (Rev. 8-98) Prescribed by ANSI Std Z39-18

Methods! Responses of single units in AI, anterior field (AAF), and Inferior Colliculus (IC) in the barbiturate-anaesthetized ferret were recorded with single tungsten electrodes. Data were collected from a total of 7, 5 and 11 (resp.) ferrets, each weighing between 1.5-2.1 kg.! Surgery and Animal Preparation: The techniques involved in the surgery and preparation for recording are described in detail in Shamma et al. (1993). The ferrets were anesthetized with pentobarbital sodium ( mg/kg IP) and maintained in an areflexic state using a continuous IV infusion of pentobarbital (~ 5 mg/kg/hr) diluted with dextrose-electrolyte solution for metabolic stability. Data collection typically lasted 6-7 hours.! Recording Procedures: Single-unit action potentials were recorded using glassinsulated tungsten microelectrodes with 5 to 6 MΩ impedances. The recorded signals were led through amplifiers and filters. Depending on the paradigm, a stimulus was presented every few seconds, and raster plots with 1ms time resolution were produced.! In AI, recordings were typically made at depths of 3-6 µm (layers III and IV). In AAF, electrode penetrations were made parallel to the depth of the suprasylvian sulcus (SSS), approximately.5 mm caudal of the sulcus so that cortical layers III and/or IV were reached. IC was exposed by removal of (visual) cortex, and electrodes were lowered until ICC was reached, following standard criteria.

Change in Ripple Phase 2 1 Ω = 1. cyc/oct 1 1 2 3 5-1 1 2 3 5 2 Tonotopic Axis Amplitude -2 9 18 27 Phase (degrees) 36

2 1 Measuring the Ripple Transfer Function 1. cyc/oct. cyc/oct. cyc/oct 1 1 2 3 5-1 1 2 3 5 Tonotopic Axis 1 1 18 Phase.5 Amplitude 72 36..8 1.2 1.6 2..8 1.2 1.6 Ripple Frequency (cyc/oct) 2

.8 cycles/octave at 8 different phases Stimulus onset: 1 ms Stimulus offset: 15 ms phase ripple at 6 different ripple freq.

Tuning as a function of Ripple Frequency and Phase 9 18 27 5 135 225 315 Ripple phase (degrees) Amplitude 3 2 1.5 1 1.5 2 Phase (radians) Ripple Frequency (cyc/oct) 1-1 -2.5 1 1.5 2

Response fields of varying bandwidth Τ(Ω) Φ (Ω) RF A Spike 8 Ωo=.6..8 1.6 2. 3.2. φ (radians) 2π -2π -π -6π -8π φ o = 1..8 1.6 2. 3.2. Spike 1.5 -.5-1 BF RF = 5.2 khz 157/1a B Spike 8 6 2 Ωo= 2. φ (radians) 2π -2π -π -6π -8π φ o = - 11 Spike.5 BF RF = 5.9 khz 152/6d..8 1.6 2. 3.2. Ω (cycles/octave) -1π..8 1.6 2. 3.2. Ω (cycles/octave) -.5 1 2 8 162 Frequency (khz)

Response Fields with varying asymmetries Τ(Ω) Φ (Ω) RF A Spike B Spike.5 1 1.5 Ω ο =.8..8 1.6 2. 3.2. Ω ο =.8..8 1.6 2. 3.2. Ω (cycles/octave) φ (radians) φ (radians) 2π -2π -π -6π -8π 2π -2π -π -6π -8π φ o = 16..8 1.6 2. 3.2. φ o = 2..8 1.6 2. 3.2. Ω (cycles/octave) Spike Spike 1.5.5 -.5 -.15 1.5.5 -.5 -.15 BF RF = 9. khz BF RF = 7.6 khz 1 2 8 162 Frequency (khz) 15/6e 157/3d

. The Anterior Cortical Field M SSS R H L L H H L H AAF AI Area of magnification AAF L AI

BF s and latencies are similar 2 N = 17 AAF 3 2 N = 168 AI 1.25.5 1 2 8 16 BF(kHz) N = 139 6.25.5 1 2 8 BF (khz) N = 165 AI 16 2 AAF 2 5 1 15 2 25 3 35 Latency (ms) 5 1 15 2 25 3 35 Latency (ms)

Bandwidths (BW2) are larger in AAF 3 2 1 N = 128 AAF 2 N =151 AI 1 2 3 5 6 BW2 (octaves) 1 2 3 5 6 BW 2 (octaves) Bandwidth (Octaves) 6 2 AAF.1 1 1 BF (khz) Bandwidth (Octaves) 6 2 AI.1 1 1 BF (khz)

Tuning to Ripples tends to be lower in AAF 2 1 N = 9 AAF Ω = Best Stationary Ripple Frequency (cyc/oct) 6 2 N = 155 AI 12 8..8 1.2 1.6 2 2. 2.8 Ω (cyc/oct) Single Unit Cluster 2..8 1.2 1.6 2 2. Ω (cyc/oct) RF s asymmetries are evenly distributed N = 5 AAF N = 155 AI 2.8-18 -12-6 6 12 18 Phi -18-12 -6 6 12 18 Phi

Predictions Using Stationary Ripples Response Field of Cell 1 2 8 16 32 BF khz 16/6a Spectral Profile of stimulus 1 2 8 16 32 khz BF Response of Cell to Profile Spike count 1 2 Measured Response Predicted Response Response to flat spectrum shift, δ (octaves)

The Inferior Colliculus Cer SC IC R L IC

. Of BF s and Latencies 2 1 N = 138 IC 3 2 N = 168 AI 1.25.5 1 2 8 16 BF (khz) Single Unit Cluster.25.5 1 2 8 BF (khz) 16 2 N = 1 IC 6 2 N = 165 AI 5 1 15 2 25 3 35 Latency (ms) 5 1 15 2 25 3 35 Latency (ms)

Bandwidths 3 2 N = 138 IC N = 151 AI 1 2 1 2 3 5 6 BW 2 (octaves) 1 2 3 5 6 BW 2 (octaves) 5 IC 5 Bandwidth (Octaves) 3 2 1.25.5 1 2 8 16 BF (khz) Bandwidth (Octaves) 3 2 1.25.5 1 2 8 16 BF (khz)

. Best Ripple Frequency 6 N = 155 8 N=1 2 AI 6 2 IC..8 1.2 1.6 2 2. Ω (cyc/oct) 2.8 Single Unit Cluster.2..6.8 1 1.2 1. 1.6 Ω (cyc/oct) 12 N = 53 8 Ω = Best Ripple Frequency.2..6.8 1 Tuning at.2 (c/)/ Tuning at best ripple

RF s are more symmetrical in IC 3 2 N = 138 IC 2 N = 155 AI 1-18 -12-6 6 12 18 Phi Single Unit Cluster -18-12 -6 6 12 18 Phi

Temporal properties: Moving Ripples ω = Hz A t = ms t = 62.5 ms.5 1. 2.. 8. 16. Tonotopic Axis Response Field of Cell t = 125 ms.5 16 Tonotopic Axis (khz) t = 187.5 ms τ d τ m Expected Response Ω = ripple frequency in cycle/octaves ω = temporal frequency in Hz t

Responses to Moving Ripples Temporal Frequency (Hz) 8 12 16 2 2 28 32 Ripple Frequency is. cycles/oct 175/12c Ω =. cyc/oct ω = to 32 Hz Time (ms) 3 sweeps per ω

. Step 1. From Spike to Period Histogram ω (Hz) 8 12 16 2 2 Step 2. Magnitude and Phase of Best Fit Spike 2 T Ωο (ω) ω ο = best temporal frequency 8 16 2 32 ω (Hz) 2 IR(t) Radians 8π 6π π 2π 2π Φ (ω) Ω ο Φ Ωο (ω) Φ Ωο () 8 16 2 ω (Hz) F -1 28 32 6 Time (ms) 18 2 Spike 1-1.5.1.15.2.25 Time (sec) Impulse Response Function

.. Linearity of responses in the Auditory Cortex AI and AAF display similar characteristics Anterior Field: (A) Stimulus Spectrogram,S(x,t) (B)RF (x) (C) Σ RF (x) S(x,t) x (D) IR(t) (E) Predicted Response 2. 1.6 1.2.8. Frequency (khz) khz 8 2 1.5.25.5 1 Time (sec) 181/21d 12 8 8 -.2..6.8 1 Time (sec) * -.1.2.3..5 Time (sec) 6 2-2 -.2..6.8 1 Time (sec)

. Predicting the Response to a Complex Stimulus Primary Auditory Cortex: (A) Stimulus Spectrogram,S(x,t) (B)RF (x) (C) Σ RF (x) S(x,t) x (D) IR(t) (E) Predicted Response +8 Hz at. cyc/ oct 8 2 1 6 ρ =.7 2 2. 1.6 1.2.8. +8+12+16 Hz at 1.2 cyc/ oct 17/3a -2 8-1 -2.1.2.25.1.2.25 Time (sec) Time (sec) 2-2 - ρ =.9.1.2.25 Time (sec) 1 2.5 1. Time (sec) 17/3a -.1.2 Time (sec).25-1 -2.1.2.25 Time (sec) -2.1.2.25 Time (sec) Predicted response Measured response

Inferior Colliculus Responses Temporal Frequency (Hz) 12 Ripple Frequency is.2 cyc/oct 2 189IC/2a Time (ms) 8 2 56 189IC/2a Ω =.2 cyc/oct ω = to 6 Hz Time (ms) 15 sweeps per ω

Summary! Stationary and traveling ripples can be used to extract spectral and temporal properties of auditory cortical neurons.! Linearity: Responses to a broad-band complex stimuli, decomposed into a linear combination of ripples, can be predicted by summing the neuronal responses to the individual ripples.! Only Cortical neurons are selective to ripple frequencies; Collicular neurons are low-pass with respect to ripple frequencies.! Therefore, AI and AAF neurons could perform a multi-scale analysis of spectral shape: the spectral profile is analyzed at different degrees of resolution by neurons with receptive fields of different best frequencies, bandwidths and asymmetries.

References! DeValois R. and DeValois K. (1988) Spatial Vision. New York: Oxford U. Press! Shamma S.A., Versnel H. and Kowalski N. (1995) Ripple analysis in ferret primary auditory cortex I. Response characteristics of single units to sinusoidally rippled spectra. Auditory Neuroscience 1(3), pp. 233-25.! Shamma S.A. and Versnel H. (1995) Ripple analysis in ferret primary auditory cortex. II. Prediction of unit responses to arbitrary spectral profiles. Auditory Neuroscience 1(3), pp. 255-27.! Versnel H., Kowalski N. and Shamma S.A. (1995) Ripple analysis in ferret primary auditory cortex.iii. Topographic distribution of ripple response parameters. Auditory Neuroscience 1(3), pp. 271-285.! Schreiner C.E. and Calhoun B.M. (1995) Spectral envelope coding in cat primary auditory cortex: properties of ripple transfer functions. Auditory Neuroscience 1(1): 23 pages.! Kowalski N., Versnel H. and Shamma S.A. (1995) Comparison of responses in the anterior and primary auditory fields of the ferret cortex. J. Neurophys. 73(), pp.1513-1523.! Owens A. and Shamma S. Surface evoked potentials reveal selectivity to spectral shape features. ARO 96.! Kowalski N., D.A.D. and Shamma S.A. (1995) Analysis of dynamic spectra in ferret primary auditory cortex: I. Response characteristics of single units to moving rippled spectra.! Kowalski N., D.A.D. and Shamma S.A. (1995) Analysis of dynamic spectra in ferret primary auditory cortex: II. Prediction of unit responses to arbitrary dynamic spectra.