Rapid customization of image processors using Halide

Author(s):  
Ville Korhonen ◽  
Pekka Jaaskelainen ◽  
Matias Koskela ◽  
Timo Viitanen ◽  
Jarmo Takala
Keyword(s):  
1998 ◽  
Vol 09 (01) ◽  
pp. 1-35 ◽  
Author(s):  
S. BANDYOPADHYAY ◽  
V. P. ROYCHOWDHURY ◽  
D. B. JANES

Recent advances in chemical self-assembly will soon make it possible to synthesize extremely powerful computing machinery from metallic clusters and organic molecules. These self-organized networks can function as Boolean logic circuits, associative memory, image processors, and combinatorial optimizers. Computational or signal processing activity is elicited from simple charge interactions between clusters which are resistively/capacitively linked by conjugated molecular wires or ribbons. The resulting circuits are massively parallel, fault-tolerant, ultrafast, ultradense and dissipate very little power.


2017 ◽  
Vol 27 (03) ◽  
pp. 1750041 ◽  
Author(s):  
Andrew Adamatzky

A thin-layer Belousov–Zhabotinsky (BZ) medium is a powerful computing device capable for implementing logical circuits, memory, image processors, robot controllers, and neuromorphic architectures. We design the reversible logical gates — Fredkin gate and Toffoli gate — in a BZ medium network of excitable channels with subexcitable junctions. Local control of the BZ medium excitability is an important feature of the gates’ design. An excitable thin-layer BZ medium responds to a localized perturbation with omnidirectional target or spiral excitation waves. A subexcitable BZ medium responds to an asymmetric perturbation by producing traveling localized excitation wave-fragments similar to dissipative solitons. We employ interactions between excitation wave-fragments to perform the computation. We interpret the wave-fragments as values of Boolean variables. The presence of a wave-fragment at a given site of a circuit represents the logical truth, absence of the wave-fragment — logically false. Fredkin gate consists of ten excitable channels intersecting at 11 junctions, eight of which are subexcitable. Toffoli gate consists of six excitable channels intersecting at six junctions, four of which are subexcitable. The designs of the gates are verified using numerical integration of two-variable Oregonator equations.


Author(s):  
Bill M. Halkias ◽  
Kostas Papandreou ◽  
Pantelis Kopelias ◽  
Vily Vegiri ◽  
Panos D. Prevedouros

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