Solutions of a two-particle interacting quantum walk
We study the solutions of the interacting Fermionic cellular automaton introduced in Ref. [Phys Rev A 97, 032132 (2018)]. The automaton is the analogue of the Thirring model with both space and time discrete. We present a derivation of the two-particles solutions of the automaton, which exploits the...
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description | We study the solutions of the interacting Fermionic cellular automaton introduced in Ref. [Phys Rev A 97, 032132 (2018)]. The automaton is the analogue of the Thirring model with both space and time discrete. We present a derivation of the two-particles solutions of the automaton, which exploits the symmetries of the evolution operator. In the two-particles sector, the evolution operator is given by the sequence of two steps, the first one corresponding to a unitary interaction activated by two-particle excitation at the same site, and the second one to two independent one-dimensional Dirac quantum walks. The interaction step can be regarded as the discrete-time version of the interacting term of some Hamiltonian integrable system, such as the Hubbard or the Thirring model. The present automaton exhibits scattering solutions with nontrivial momentum transfer, jumping between different regions of the Brillouin zone that can be interpreted as Fermion-doubled particles, in stark contrast with the customary momentum-exchange of the one dimensional Hamiltonian systems. A further difference compared to the Hamiltonian model is that there exist bound states for every value of the total momentum, and even for vanishing coupling constant. As a complement to the analytical derivations we show numerical simulations of the interacting evolution. |
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[Phys Rev A 97, 032132 (2018)]. The automaton is the analogue of the Thirring model with both space and time discrete. We present a derivation of the two-particles solutions of the automaton, which exploits the symmetries of the evolution operator. In the two-particles sector, the evolution operator is given by the sequence of two steps, the first one corresponding to a unitary interaction activated by two-particle excitation at the same site, and the second one to two independent one-dimensional Dirac quantum walks. The interaction step can be regarded as the discrete-time version of the interacting term of some Hamiltonian integrable system, such as the Hubbard or the Thirring model. The present automaton exhibits scattering solutions with nontrivial momentum transfer, jumping between different regions of the Brillouin zone that can be interpreted as Fermion-doubled particles, in stark contrast with the customary momentum-exchange of the one dimensional Hamiltonian systems. A further difference compared to the Hamiltonian model is that there exist bound states for every value of the total momentum, and even for vanishing coupling constant. As a complement to the analytical derivations we show numerical simulations of the interacting evolution.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.1804.08508</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Brillouin zones ; Cellular automata ; Computer simulation ; Evolution ; Fermions ; Hamiltonian functions ; Mathematical models ; Mathematics - Mathematical Physics ; Momentum transfer ; Physics - High Energy Physics - Lattice ; Physics - Mathematical Physics ; Physics - Quantum Physics ; Physics - Strongly Correlated Electrons</subject><ispartof>arXiv.org, 2018-04</ispartof><rights>2018. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). 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[Phys Rev A 97, 032132 (2018)]. The automaton is the analogue of the Thirring model with both space and time discrete. We present a derivation of the two-particles solutions of the automaton, which exploits the symmetries of the evolution operator. In the two-particles sector, the evolution operator is given by the sequence of two steps, the first one corresponding to a unitary interaction activated by two-particle excitation at the same site, and the second one to two independent one-dimensional Dirac quantum walks. The interaction step can be regarded as the discrete-time version of the interacting term of some Hamiltonian integrable system, such as the Hubbard or the Thirring model. The present automaton exhibits scattering solutions with nontrivial momentum transfer, jumping between different regions of the Brillouin zone that can be interpreted as Fermion-doubled particles, in stark contrast with the customary momentum-exchange of the one dimensional Hamiltonian systems. A further difference compared to the Hamiltonian model is that there exist bound states for every value of the total momentum, and even for vanishing coupling constant. As a complement to the analytical derivations we show numerical simulations of the interacting evolution.</description><subject>Brillouin zones</subject><subject>Cellular automata</subject><subject>Computer simulation</subject><subject>Evolution</subject><subject>Fermions</subject><subject>Hamiltonian functions</subject><subject>Mathematical models</subject><subject>Mathematics - Mathematical Physics</subject><subject>Momentum transfer</subject><subject>Physics - High Energy Physics - Lattice</subject><subject>Physics - Mathematical Physics</subject><subject>Physics - Quantum Physics</subject><subject>Physics - Strongly Correlated Electrons</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><sourceid>BENPR</sourceid><sourceid>GOX</sourceid><recordid>eNotj8tOwzAURC0kJKrSD2BFJNYJ14_rOEtU8ZIqsaD7yIlt5JLGqeNQ-HtCy2oWczSaQ8gNhUIoRLjX8dt_FVSBKEAhqAuyYJzTXAnGrshqHHcAwGTJEPmCiPfQTcmHfsyCy3SWjiEfdEy-7Wzm-2SjbpPvP7LDpPs07bOj7j6vyaXT3WhX_7kk26fH7fol37w9v64fNrlGVuUMJbjSKGtoY5AykFwoS0UjhbAGuEOKyunGKWilQSOsaDly2WhN587wJbk9z56U6iH6vY4_9Z9afVKbibszMcRwmOyY6l2YYj9_qhmUXFacYcV_AZQ8UL0</recordid><startdate>20180423</startdate><enddate>20180423</enddate><creator>Bisio, Alessandro</creator><creator>Giacomo Mauro D'Ariano</creator><creator>Mosco, Nicola</creator><creator>Perinotti, Paolo</creator><creator>Tosini, Alessandro</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>AKZ</scope><scope>GOX</scope></search><sort><creationdate>20180423</creationdate><title>Solutions of a two-particle interacting quantum walk</title><author>Bisio, Alessandro ; Giacomo Mauro D'Ariano ; Mosco, Nicola ; Perinotti, Paolo ; Tosini, Alessandro</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a529-2560f7d8ed1bd51206348e14b644ed03f5158fabf80c6d5d4e4c3536baa1f51d3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Brillouin zones</topic><topic>Cellular automata</topic><topic>Computer simulation</topic><topic>Evolution</topic><topic>Fermions</topic><topic>Hamiltonian functions</topic><topic>Mathematical models</topic><topic>Mathematics - Mathematical Physics</topic><topic>Momentum transfer</topic><topic>Physics - High Energy Physics - Lattice</topic><topic>Physics - Mathematical Physics</topic><topic>Physics - Quantum Physics</topic><topic>Physics - Strongly Correlated Electrons</topic><toplevel>online_resources</toplevel><creatorcontrib>Bisio, Alessandro</creatorcontrib><creatorcontrib>Giacomo Mauro D'Ariano</creatorcontrib><creatorcontrib>Mosco, Nicola</creatorcontrib><creatorcontrib>Perinotti, Paolo</creatorcontrib><creatorcontrib>Tosini, Alessandro</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection (ProQuest)</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>Engineering Collection</collection><collection>arXiv Mathematics</collection><collection>arXiv.org</collection><jtitle>arXiv.org</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Bisio, Alessandro</au><au>Giacomo Mauro D'Ariano</au><au>Mosco, Nicola</au><au>Perinotti, Paolo</au><au>Tosini, Alessandro</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Solutions of a two-particle interacting quantum walk</atitle><jtitle>arXiv.org</jtitle><date>2018-04-23</date><risdate>2018</risdate><eissn>2331-8422</eissn><abstract>We study the solutions of the interacting Fermionic cellular automaton introduced in Ref. [Phys Rev A 97, 032132 (2018)]. The automaton is the analogue of the Thirring model with both space and time discrete. We present a derivation of the two-particles solutions of the automaton, which exploits the symmetries of the evolution operator. In the two-particles sector, the evolution operator is given by the sequence of two steps, the first one corresponding to a unitary interaction activated by two-particle excitation at the same site, and the second one to two independent one-dimensional Dirac quantum walks. The interaction step can be regarded as the discrete-time version of the interacting term of some Hamiltonian integrable system, such as the Hubbard or the Thirring model. The present automaton exhibits scattering solutions with nontrivial momentum transfer, jumping between different regions of the Brillouin zone that can be interpreted as Fermion-doubled particles, in stark contrast with the customary momentum-exchange of the one dimensional Hamiltonian systems. A further difference compared to the Hamiltonian model is that there exist bound states for every value of the total momentum, and even for vanishing coupling constant. As a complement to the analytical derivations we show numerical simulations of the interacting evolution.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.1804.08508</doi><oa>free_for_read</oa></addata></record> |
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subjects | Brillouin zones Cellular automata Computer simulation Evolution Fermions Hamiltonian functions Mathematical models Mathematics - Mathematical Physics Momentum transfer Physics - High Energy Physics - Lattice Physics - Mathematical Physics Physics - Quantum Physics Physics - Strongly Correlated Electrons |
title | Solutions of a two-particle interacting quantum walk |
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