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pytensor
Commits
aae090b5
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aae090b5
authored
2月 10, 2010
作者:
James Bergstra
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added Fourier.py to sandbox
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fourier.py
theano/sandbox/fourier.py
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theano/sandbox/fourier.py
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aae090b5
"""Provides Ops for FFT and DCT.
"""
from
theano.gof
import
Op
,
Apply
,
generic
from
theano
import
tensor
import
numpy.fft
import
numpy
class
GradTodo
(
Op
):
def
make_node
(
self
,
x
):
return
Apply
(
self
,
[
x
],
[
x
.
type
()])
def
perform
(
self
,
node
,
inputs
,
outputs
):
raise
NotImplementedError
(
'TODO'
)
grad_todo
=
GradTodo
()
class
FFT
(
Op
):
"""Fast Fourier Transform
.. TODO:
The current implementation just works for matrix inputs, and permits taking a 1D FFT over
either rows or columns. Add support for N-D FFTs as provided by either numpy or FFTW
directly.
.. TODO:
Give the C code that uses FFTW.
.. TODO:
unit tests.
"""
default_output
=
0
# don't return the plan object in the 'buf' output
half
=
False
"""Only return the first half (positive-valued) of the frequency components"""
def
__init__
(
self
,
half
=
False
,
inverse
=
False
):
self
.
half
=
half
self
.
inverse
=
inverse
def
__eq__
(
self
,
other
):
return
type
(
self
)
==
type
(
other
)
and
(
self
.
half
==
other
.
half
)
and
(
self
.
inverse
==
other
.
inverse
)
def
__hash__
(
self
):
return
hash
(
type
(
self
))
^
hash
(
self
.
half
)
^
9828743
^
(
self
.
inverse
)
def
__ne__
(
self
,
other
):
return
not
(
self
==
other
)
def
make_node
(
self
,
frames
,
n
,
axis
):
""" compute an n-point fft of frames along given axis """
_frames
=
tensor
.
as_tensor
(
frames
,
ndim
=
2
)
_n
=
tensor
.
as_tensor
(
n
,
ndim
=
0
)
_axis
=
tensor
.
as_tensor
(
axis
,
ndim
=
0
)
if
self
.
half
and
_frames
.
type
.
dtype
.
startswith
(
'complex'
):
raise
TypeError
(
'Argument to HalfFFT must not be complex'
,
frames
)
spectrogram
=
tensor
.
zmatrix
()
buf
=
generic
()
# The `buf` output is present for future work
# when we call FFTW directly and re-use the 'plan' that FFTW creates.
# In that case, buf would store a CObject encapsulating the plan.
rval
=
Apply
(
self
,
[
_frames
,
_n
,
_axis
],
[
spectrogram
,
buf
])
return
rval
def
perform
(
self
,
node
,
(
frames
,
n
,
axis
),
(
spectrogram
,
buf
)):
if
self
.
inverse
:
fft_fn
=
numpy
.
fft
.
ifft
else
:
fft_fn
=
numpy
.
fft
.
fft
fft
=
fft_fn
(
frames
,
int
(
n
),
int
(
axis
))
if
self
.
half
:
M
,
N
=
fft
.
shape
if
axis
==
0
:
if
(
M
%
2
):
raise
ValueError
(
'halfFFT on odd-length vectors is undefined'
)
spectrogram
[
0
]
=
fft
[
0
:
M
/
2
,
:]
elif
axis
==
1
:
if
(
N
%
2
):
raise
ValueError
(
'halfFFT on odd-length vectors is undefined'
)
spectrogram
[
0
]
=
fft
[:,
0
:
N
/
2
]
else
:
raise
NotImplementedError
()
else
:
spectrogram
[
0
]
=
fft
def
grad
(
self
,
(
frames
,
n
,
axis
),
(
g_spectrogram
,
g_buf
)):
return
[
grad_todo
(
frames
),
None
,
None
]
fft
=
FFT
(
half
=
False
,
inverse
=
False
)
half_fft
=
FFT
(
half
=
True
,
inverse
=
False
)
ifft
=
FFT
(
half
=
False
,
inverse
=
True
)
half_ifft
=
FFT
(
half
=
True
,
inverse
=
True
)
def
dct_matrix
(
rows
,
cols
,
unitary
=
True
):
"""
Return a (rows x cols) matrix implementing a discrete cosine transform.
This algorithm is adapted from Dan Ellis' Rastmat
spec2cep.m, lines 15 - 20.
"""
rval
=
numpy
.
zeros
((
rows
,
cols
))
col_range
=
numpy
.
arange
(
cols
)
scale
=
numpy
.
sqrt
(
2.0
/
cols
)
for
i
in
xrange
(
rows
):
rval
[
i
]
=
numpy
.
cos
(
i
*
(
col_range
*
2
+
1
)
/
(
2.0
*
cols
)
*
numpy
.
pi
)
*
scale
if
unitary
:
rval
[
0
]
*=
numpy
.
sqrt
(
0.5
)
return
rval
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