Lines Matching refs:varname
166 \varname{[residue_begin]} and
167 \varname{[residue_end]} select the specific sub-portion of
170 \varname{[residue_begin]} and ends at
171 \varname{[residue_end]}. Preceding and following values in
173 values as well as \varname{[residue_partition_size]}apply to
175 \varname{[residue_partition_size]} is as explained above,
176 \varname{[residue_classifications]} is the number of possible
178 \varname{[residue_classbook]} is the codebook number used to
180 \varname{[residue_classbook]} determines how many
183 \varname{[residue_classbook]}, along with
184 \varname{[residue_classifications]}, overdetermines to
186 If \varname{[residue_classifications]}\^{}\varname{[residue_classbook]}.dimensions
187 exceeds \varname{[residue_classbook]}.entries, the
255 Depending on the values of \varname{[residue_begin]} and
256 \varname{[residue_end]}, it is obvious that the encoded
260 set \varname{[residue_begin]} and
261 \varname{[residue_end]} to specify a range partially or
263 decode, limit \varname{[residue_begin]} and
264 \varname{[residue_end]} to the maximum possible vector size
266 \varname{[ch]} is provided by the higher level decoding
357 \item \varname{[n]} is the value in \varname{[residue_partition_size]}
358 \item \varname{[v]} is the residue vector
359 \item \varname{[offset]} is the beginning read offset in [v]
391 \item \varname{[n]} is the value in
392 \varname{[residue_partition_size]}
393 \item \varname{[v]} is the residue vector
394 \item \varname{[offset]} is the beginning read offset in [v]
429 \item If all vectors 0 through \emph{ch}-1 are marked 'do not decode', allocate and clear a single vector \varname{[v]}of length \emph{ch*n} and skip step 2 below; proceed directly to the post-decode step.
430 \item Rather than performing format 1 decode to produce \emph{ch} vectors of length \emph{n} each, call format 1 decode to produce a single vector \varname{[v]} of length \emph{ch*n}.
431 \item Post decode: Deinterleave the single vector \varname{[v]} returned by format 1 decode as described above into \emph{ch} independent vectors, one for each outputchannel, according to: