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dc.contributor.authorVahala, Georgeen_US
dc.contributor.authorSoe, Minen_US
dc.contributor.authorKououtsis, Efstratiosen_US
dc.contributor.authorHizanidis, Kyriakosen_US
dc.contributor.authorVahala, Lindaen_US
dc.contributor.authorRam, Abhay K.en_US
dc.date.accessioned2025-03-21T20:22:23Z
dc.date.available2025-03-21T20:22:23Z
dc.date.issued2023-07
dc.identifier23ja024
dc.identifier.urihttps://hdl.handle.net/1721.1/158723
dc.descriptionSubmitted for publication in IntechOpen
dc.description.abstractIt is well known that Maxwell equations can be expressed in a unitary Schrodinger-Dirac representation for homogeneous media. However, difficulties arise when considering inhomogeneous media. A Dyson map points to a unitary field qubit basis, but the standard qubit lattice algorithm of interleaved unitary collision-stream operators must be augmented by some sparse non-unitary potential operators that recover the derivatives on the refractive indices. The effect of the steepness of these derivatives on two-dimensional scattering is examined with simulations showing quite complex wavefronts emitted due to transmissions/reflections within the dielectric objects. Maxwell equations are extended to handle dissipation using Kraus operators. Then, our theoretical algorithms are extended to these open quantum systems. A quantum circuit diagram is presented as well as estimates on the required number of quantum gates for implementation on a quantum computer.
dc.publisherIntechOpenen_US
dc.relation.isversionofdoi.org/10.5772/intechopen.112692
dc.sourcePlasma Science and Fusion Centeren_US
dc.titleQubit Lattice Algorithms Based on the Schrodinger-Dirac Representation of Maxwell Equations and Their Extensionsen_US
dc.typeArticleen_US
dc.contributor.departmentMassachusetts Institute of Technology. Plasma Science and Fusion Center
dc.relation.journalIntechOpen


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