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Maximum Entropy Models from Phase Harmonic Covariances

arXiv 1911.10017 ↗First posted 22 Nov 2019eess.SP cs.IT cs.LGcited by 13

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Abstract (arXiv)

The covariance of a stationary process X is diagonalized by a Fourier transform. It does not take into account the complex Fourier phase and defines Gaussian maximum entropy models. We introduce a general family of phase harmonic covariance moments, which rely on complex phases to capture non-Gaussian properties. They are defined as the covariance of hatH (L X), where L is a complex linear operator and hatH is a non-linear phase harmonic operator which multiplies the phase of each complex coefficient by integers. The operator hatH (L X) can also be calculated from rectifiers, which relates hatH (L X) to neural network coefficients. If L is a Fourier transform then the covariance is a sparse matrix whose non-zero off-diagonal coefficients capture dependencies between frequencies. These coefficients have similarities with high order moment, but smaller statistical variabilities because hatH (L X) is Lipschitz. If L is a complex wavelet transform then off-diagonal coefficients reveal dependencies across scales, which specify the geometry of local coherent structures. We introduce maximum entropy models conditioned by these wavelet phase harmonic covariances. The precision of these models is numerically evaluated to synthesize images of turbulent flows and other stationary processes.

Key facts. Cited by 13 papers in the map (data through 7 Oct 2026). First posted on arXiv 22 Nov 2019.

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Citing papers per year: 2021: 1; 2022: 5; 2023: 4; 2024: 3.

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