Photonics Research, Volume. 12, Issue 8, 1828(2024)
Integrated photonic fractional convolution accelerator
[1] A. V. Oppenheim, A. S. Willsky, S. H. Nawab. Signals and Systems, 2(1997).
[2] I. Goodfellow, Y. Bengio, A. Courville. Deep Learning(2016).
[10] J. W. Goodman. Introduction to Fourier Optics(2005).
[34] F. Olver, D. Lozier, R. Boisvert. NIST Handbook of Mathematical Functions(2010).
[38] [38] This depends on the definition of the DFrFT operator, and the cyclic index identity α=4 is also used in the literature.
[41] A. F. Nikiforov, V. B. Uvarov. Special Functions of Mathematical Physics(1988).
[42] [42] Oscillations in the discrete case are defined by their zero crossings. That is, a discrete function f has a zero-crossing at n if fnfn−1 ≤ 0.
[43] [43] For maximum pooling, the N = 2m-dimensional output is decomposed into m sub-groups, each of dimension two, where only the maximum number within each sub-group is preserved.
[45] J. W. Woods. Image Enhancement and Analysis, 223-256(2012).
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Kevin Zelaya, Mohammed-Ali Miri, "Integrated photonic fractional convolution accelerator," Photonics Res. 12, 1828 (2024)
Category: Silicon Photonics
Received: Jan. 3, 2024
Accepted: May. 21, 2024
Published Online: Aug. 2, 2024
The Author Email: Kevin Zelaya (kevin.zelaya@cinvestav.mx)