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+# 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 <[email protected]> and Keith
+# Martin <[email protected]> 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
+# LSB.
+
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