Asseverate
发表于 2025-3-28 16:36:42
a set . in the Marchenko class. We discuss the nonuniqueness arising in the inverse scattering problem if the scattering matrix is defined one way with the Dirichlet boundary condition and in a different way with a non-Dirichlet boundary condition, as usually done in the standard literature. We pres
GNAW
发表于 2025-3-28 22:06:23
ly from the transistor-level netlist, placed globally, optimized locally, and then finally committed each to a specific shape-level form while concurrently optimizing for both density and routability. .The essential flaw in prior efforts is an over-reliance on geometric assumptions from large-scale
支柱
发表于 2025-3-29 02:40:58
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Jejune
发表于 2025-3-29 03:38:39
ly from the transistor-level netlist, placed globally, optimized locally, and then finally committed each to a specific shape-level form while concurrently optimizing for both density and routability. .The essential flaw in prior efforts is an over-reliance on geometric assumptions from large-scale
BILIO
发表于 2025-3-29 07:54:15
Helen Spencer-Oatey,Peter Franklinracted early from the transistor-level netlist, placed globally, optimized locally, and then finally committed each to a specific shape-level form while concurrently optimizing for both density and routability. .The essential flaw in prior efforts is an over-reliance on geometric assumptions from large-scale 978-1-4757-7951-6978-1-4020-8063-0
裹住
发表于 2025-3-29 11:59:51
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Osteoarthritis
发表于 2025-3-29 15:58:36
Helen Spencer-Oatey,Peter Franklinracted early from the transistor-level netlist, placed globally, optimized locally, and then finally committed each to a specific shape-level form while concurrently optimizing for both density and routability. .The essential flaw in prior efforts is an over-reliance on geometric assumptions from large-scale 978-1-4757-7951-6978-1-4020-8063-0
青石板
发表于 2025-3-29 20:05:39
Helen Spencer-Oatey,Peter Franklineristic polarization states. For the monostatic reciprocal case (S. = S.), treated here, it is shown that there exist in total five pairs of characteristic polarization states: The orthogonal cross-polarization null and co-polarization maximum state pairs, being identical and sharing one main circle