# This is a makehrtf HRIR definition file.  It is used to define the layout
# and source data to be processed into an OpenAL Soft compatible HRTF.
#
# This definition is used to transform the left ear HRIRs from the full set
# of KEMAR HRIRs provided by Bill Gardner <billg@media.mit.edu> and Keith
# Martin <kdm@media.mit.edu> of MIT Media Laboratory.
#
# The data (full.tar.Z or full.zip) is available from:
#
#  http://sound.media.mit.edu/resources/KEMAR.html
#
# It is copyright 1994 by MIT Media Laboratory, and provided free of charge
# with no restrictions on use so long as the authors (above) are cited.
#
# This definition is used to generate the internal HRTF table used by OpenAL
# Soft.

# The following are the dataset metrics.  They must always be specified at
# start of a definition file, but their order is not important.

# Sampling rate of the HRIR data (in hertz).
rate     = 44100

# The number of points to use from the HRIR data.  This should be a
# sufficiently large value (to encompass the entire impulse response).  It
# cannot be smaller than the truncation size (default is 32) specified on the
# command line.
points   = 512

# A list of the number of azimuths measured for each elevation.  There must
# be at least 5 elevations covering the 180 degrees for the dataset to be
# viable.
azimuths = 1, 12, 24, 36, 45, 56, 60, 72, 72, 72, 72, 72, 60, 56, 45, 36, 24, 12, 1

# The approximate radius (measured ear-to-ear) of the listener's head (in
# meters).  This does not have to match the dataset, since makehrtf uses a
# spherical model to reconstruct the propagation delay.
radius   = 0.09

# The distance between the source and the listener (in meters).  This does
# have to match the dataset, but it's effect is minimal at the moment due to
# the coupled nature of OpenAL Soft's HRTF model.
distance = 1.4

# Following the metrics is the list of source HRIRs for each elevation and
# azimuth pair.  They don't have to be specified in order, but the final
# composition must not be sparse.  They can however begin above a number of
# elevations (as typical for HRIR measurements).
#
# The elevation and azimuth indices are used to determine the resulting polar
# coordinates following OpenAL Soft's convention (-90 degree elevation
# increasing counter-clockwise from the bottom; 0 degree azimuth increasing
# clockwise from the front).
#
# More than one HRIR can be used per source, in which case the average
# magnitude response of all references for that source is used.
#
# Source specification is of the form (~BNF):
#
#  source = '[' ev_index ',' az_index ']' '=' source_ref [ '+' source_ref ]*
#
#  ev_index   = unsigned_integer
#  az_index   = unsigned_integer
#  source_ref = ref_spec ':' filename
#
#  ref_spec = ( wave_fmt  '(' wave_parms ')' [ '@' start_sample   ] ) |
#             ( bin_fmt   '(' bini_parms ')' [ '@' start_bytes    ] ) |
#             ( bin_fmt   '(' binf_parms ')' [ '@' start_bytes    ] ) |
#             ( ascii_fmt '(' asci_parms ')' [ '@' start_elements ] ) |
#             ( ascii_fmt '(' ascf_parms ')' [ '@' start_elements ] )
#  filename = double_quoted_string
#
#  wave_fmt       = 'wave'
#  wave_parms     = channel
#  bin_fmt        = 'bin_le' | 'bin_be'
#  bini_parms     = 'int' ',' byte_size [ ',' bin_sig_bits ] [ ';' skip_bytes ]
#  binf_parms     = 'fp'  ',' byte_size                      [ ';' skip_bytes ]
#  ascii_fmt      = 'ascii'
#  asci_parms     = 'int' ',' sig_bits  [ ';' skip_elements ]
#  ascf_parms     = 'fp'                [ ';' skip_elements ]
#  start_sample   = unsigned_integer
#  start_bytes    = unsigned_integer
#  start_elements = unsigned_integer
#
#  channel       = unsigned_integer
#  byte_size     = unsigned_integer
#  bin_sig_bits  = signed_integer
#  skip_bytes    = unsigned_integer
#  sig_bits      = unsigned_integer
#  skip_elements = unsigned_integer
#
# For bin_sig_bits, positive values mean the significant bits start at the
# MSB (padding toward the LSB) while negative values mean they start at the
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