Photonics Research, Volume. 12, Issue 8, 1828(2024)

Integrated photonic fractional convolution accelerator

Kevin Zelaya1、* and Mohammed-Ali Miri1,2,3
Author Affiliations
  • 1Department of Physics, Queens College of the City University of New York, Queens, New York 11367, USA
  • 2Physics Program, The Graduate Center of the City University of New York, New York, New York 10016, USA
  • 3e-mail: mmirilab@gmail.com
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    References(48)

    [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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    Paper Information

    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)

    DOI:10.1364/PRJ.517491

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