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@ -1,5 +1,5 @@
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import numpy as np
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__all__ = ['dct', 'idct']
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__all__ = ['dct', 'idct', 'dctn', 'idctn']
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def dct(x, n=None):
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"""
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Discrete Cosine Transform
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@ -105,3 +105,258 @@ def idct(x, n=None):
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return y.real
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else:
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return y
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def dctn(y, axis=None, w=None):
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'''
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DCTN N-D discrete cosine transform.
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Y = DCTN(X) returns the discrete cosine transform of X. The array Y is
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the same size as X and contains the discrete cosine transform
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coefficients. This transform can be inverted using IDCTN.
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DCTN(X,axis) applies the DCTN operation across the dimension axis.
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Class Support
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-------------
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Input array can be numeric or logical. The returned array is of class
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double.
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Reference
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---------
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Narasimha M. et al, On the computation of the discrete cosine
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transform, IEEE Trans Comm, 26, 6, 1978, pp 934-936.
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Example
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-------
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RGB = imread('autumn.tif');
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I = rgb2gray(RGB);
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J = dctn(I);
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imshow(log(abs(J)),[]), colormap(jet), colorbar
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The commands below set values less than magnitude 10 in the DCT matrix
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to zero, then reconstruct the image using the inverse DCT.
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J(abs(J)<10) = 0;
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K = idctn(J);
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figure, imshow(I)
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figure, imshow(K,[0 255])
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See also
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--------
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idctn, dct, idct
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'''
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y = np.atleast_1d(y)
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shape0 = y.shape
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if axis is None:
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y = y.squeeze() # Working across singleton dimensions is useless
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dimy = y.ndim
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if dimy==1:
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y = np.atleast_2d(y)
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y = y.T
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# Some modifications are required if Y is a vector
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# if isvector(y):
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# if y.shape[0]==1:
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# if axis==0:
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# return y, None
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# elif axis==1:
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# axis=0
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# y = y.T
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# elif axis==1:
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# return y, None
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if w is None:
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w = [0,] * dimy
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for dim in range(dimy):
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if axis is not None and dim!=axis:
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continue
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n = (dimy==1)*y.size + (dimy>1)*shape0[dim]
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#w{dim} = exp(1i*(0:n-1)'*pi/2/n);
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w[dim] = np.exp(1j * np.arange(n) * np.pi / (2 * n))
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# --- DCT algorithm ---
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if np.iscomplex(y).any():
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y = np.complex(dctn(np.real(y),axis,w),dctn(np.imag(y),axis,w))
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else:
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for dim in range(dimy):
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y = shiftdim(y,1)
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if axis is not None and dim!=axis:
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y = shiftdim(y, 1)
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continue
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siz = y.shape
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n = siz[-1]
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y = y[...,np.r_[0:n:2, 2*int(n//2)-1:0:-2]]
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y = y.reshape((-1,n))
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y = y*np.sqrt(2*n);
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y = (np.fft.ifft(y, n=n, axis=1) * w[dim]).real
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y[:,0] = y[:,0]/np.sqrt(2)
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y = y.reshape(siz)
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#end
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#end
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return y.reshape(shape0), w
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def idctn(y, axis=None, w=None):
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'''
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IDCTN N-D inverse discrete cosine transform.
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X = IDCTN(Y) inverts the N-D DCT transform, returning the original
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array if Y was obtained using Y = DCTN(X).
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IDCTN(X,DIM) applies the IDCTN operation across the dimension DIM.
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Class Support
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-------------
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Input array can be numeric or logical. The returned array is of class
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double.
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Reference
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---------
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Narasimha M. et al, On the computation of the discrete cosine
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transform, IEEE Trans Comm, 26, 6, 1978, pp 934-936.
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Example
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-------
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RGB = imread('autumn.tif');
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I = rgb2gray(RGB);
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J = dctn(I);
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imshow(log(abs(J)),[]), colormap(jet), colorbar
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The commands below set values less than magnitude 10 in the DCT matrix
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to zero, then reconstruct the image using the inverse DCT.
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J(abs(J)<10) = 0;
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K = idctn(J);
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figure, imshow(I)
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figure, imshow(K,[0 255])
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See also
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--------
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dctn, idct, dct
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-- Damien Garcia -- 2009/04, revised 2009/11
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website: <a
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href="matlab:web('http://www.biomecardio.com')">www.BiomeCardio.com</a>
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----------
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[Y,W] = IDCTN(X,DIM,W) uses and returns the weights which are used by
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the program. If IDCTN is required for several large arrays of same
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size, the weights can be reused to make the algorithm faster. A typical
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syntax is the following:
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w = [];
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for k = 1:10
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[y{k},w] = idctn(x{k},[],w);
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end
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The weights (w) are calculated during the first call of IDCTN then
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reused in the next calls.
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'''
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y = np.atleast_1d(y)
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shape0 = y.shape
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if axis is None:
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y = y.squeeze() # Working across singleton dimensions is useless
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dimy = y.ndim
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if dimy==1:
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y = np.atleast_2d(y)
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y = y.T
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# Some modifications are required if Y is a vector
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# if isvector(y):
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# if y.shape[0]==1:
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# if axis==0:
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# return y, None
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# elif axis==1:
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# axis=0
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# y = y.T
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# elif axis==1:
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# return y, None
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#
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if w is None:
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w = [0,] * dimy
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for dim in range(dimy):
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if axis is not None and dim!=axis:
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continue
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n = (dimy==1)*y.size + (dimy>1)*shape0[dim]
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#w{dim} = exp(1i*(0:n-1)'*pi/2/n);
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w[dim] = np.exp(1j * np.arange(n) * np.pi / (2 * n))
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# --- IDCT algorithm ---
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if np.iscomplex(y).any():
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y = np.complex(idctn(np.real(y),axis,w),idctn(np.imag(y),axis,w))
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else:
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for dim in range(dimy):
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y = shiftdim(y,1)
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if axis is not None and dim!=axis:
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#y = shiftdim(y, 1)
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continue
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siz = y.shape
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n = siz[-1]
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y = y.reshape((-1,n)) * w[dim]
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y[:,0] = y[:,0]/np.sqrt(2)
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y = (np.fft.ifft(y, n=n, axis=1)).real
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y = y * np.sqrt(2*n)
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I = np.empty(n,dtype=int)
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I.put(np.r_[0:n:2],np.r_[0:int(n//2)+np.remainder(n,2)])
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I.put(np.r_[1:n:2],np.r_[n-1:int(n//2)-1:-1])
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y = y[:,I]
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y = y.reshape(siz)
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y = y.reshape(shape0);
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return y, w
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def no_leading_ones(x):
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first = 0
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for i, xi in enumerate(x):
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if xi != 1:
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first = i
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break
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return x[first:]
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def shiftdim(x, n=None):
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if n is None:
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# returns the array B with the same number of
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# elements as X but with any leading singleton
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# dimensions removed.
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return x.reshape(no_leading_ones(x.shape))
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elif n>=0:
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# When n is positive, shiftdim shifts the dimensions
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# to the left and wraps the n leading dimensions to the end.
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return x.transpose(np.roll(range(x.ndim), -n))
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else:
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# When n is negative, shiftdim shifts the dimensions
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# to the right and pads with singletons.
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return x.reshape((1,)*-n+x.shape)
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def test_dctn():
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a = np.arange(12).reshape((3,-1))
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#y = dct(a)
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#x = idct(y)
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#print(y)
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#print(x)
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print(a)
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yn = dctn(a)[0]
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xn = idctn(yn)[0]
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print(yn)
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print(xn)
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def test_docstrings():
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import doctest
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doctest.testmod()
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if __name__ == '__main__':
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#test_docstrings()
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test_dctn()
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