Mixed-order transition in the antiferromagnetic quantum Ising chain in a field
The antiferromagnetic quantum Ising chain has a quantum critical point which belongs to the universality class of the transverse Ising model (TIM). When a longitudinal field (h) is switched on, the phase transition is preserved, which turns to first order for h/Γ → ∞, Γ being the strength of the tra...
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description | The antiferromagnetic quantum Ising chain has a quantum critical point which belongs to the universality class of the transverse Ising model (TIM). When a longitudinal field (h) is switched on, the phase transition is preserved, which turns to first order for h/Γ → ∞, Γ being the strength of the transverse field. Here we will re-examine the critical properties along the phase transition line. During a quantum block renormalization group calculation, the TIM fixed point for h/Γ > 0 is found to be unstable. Using DMRG techniques, we calculated the entanglement entropy and the spin-spin correlation function, both of which signaled a divergent correlation length at the transition point with the TIM exponents. At the same time, the bulk correlation function has a jump and the end-to-end correlation function has a discontinuous derivative at the transition point. Consequently for finite h/Γ the transition is of mixed order. |
doi_str_mv | 10.1103/PhysRevB.103.174404 |
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When a longitudinal field (h) is switched on, the phase transition is preserved, which turns to first order for h/Γ → ∞, Γ being the strength of the transverse field. Here we will re-examine the critical properties along the phase transition line. During a quantum block renormalization group calculation, the TIM fixed point for h/Γ > 0 is found to be unstable. Using DMRG techniques, we calculated the entanglement entropy and the spin-spin correlation function, both of which signaled a divergent correlation length at the transition point with the TIM exponents. At the same time, the bulk correlation function has a jump and the end-to-end correlation function has a discontinuous derivative at the transition point. Consequently for finite h/Γ the transition is of mixed order.</description><identifier>ISSN: 2469-9950</identifier><identifier>EISSN: 2469-9969</identifier><identifier>DOI: 10.1103/PhysRevB.103.174404</identifier><language>eng</language><publisher>College Park: American Physical Society</publisher><subject>Antiferromagnetism ; Chains ; Correlation ; Critical point ; Entanglement ; Ising model ; Phase transitions ; Transition points</subject><ispartof>Physical review. 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Consequently for finite h/Γ the transition is of mixed order.</description><subject>Antiferromagnetism</subject><subject>Chains</subject><subject>Correlation</subject><subject>Critical point</subject><subject>Entanglement</subject><subject>Ising model</subject><subject>Phase transitions</subject><subject>Transition points</subject><issn>2469-9950</issn><issn>2469-9969</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><recordid>eNo9kN1LwzAUxYMoOOb-Al8CPncmTZo2jzr8GMwPRJ9DkiZrxppuSSruv7ez6sPl3nM43AM_AC4xmmOMyPVrc4hv5vN2Pog5LilF9ARMcsp4xjnjp_93gc7BLMYNQggzxEvEJ-D5yX2ZOutCbQJMQfrokus8dB6mxkDpk7MmhK6Va2-S03DfD17fwmV0fg11I91PWELrzLa-AGdWbqOZ_e4p-Li_e188ZquXh-XiZpVpUlUpsxXPNbNU8lJxWfCaaW5zZpFSFTE5lohJaimuS2oMIYoW2A4GL3NJlVKaTMHV-HcXun1vYhKbrg9-qBR5QVhB2TBDiowpHboYg7FiF1wrw0FgJI7sxB87cRQjO_INnmlkfw</recordid><startdate>20210504</startdate><enddate>20210504</enddate><creator>Lajkó, Péter</creator><creator>Iglói, Ferenc</creator><general>American Physical Society</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>H8D</scope><scope>JG9</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0003-2521-9298</orcidid></search><sort><creationdate>20210504</creationdate><title>Mixed-order transition in the antiferromagnetic quantum Ising chain in a field</title><author>Lajkó, Péter ; Iglói, Ferenc</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c388t-f892c6f4a97b9a59d6c9f26f0bb83e21a06a4f41d74ee33b451fa4f972a4bbbc3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Antiferromagnetism</topic><topic>Chains</topic><topic>Correlation</topic><topic>Critical point</topic><topic>Entanglement</topic><topic>Ising model</topic><topic>Phase transitions</topic><topic>Transition points</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Lajkó, Péter</creatorcontrib><creatorcontrib>Iglói, Ferenc</creatorcontrib><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physical review. 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During a quantum block renormalization group calculation, the TIM fixed point for h/Γ > 0 is found to be unstable. Using DMRG techniques, we calculated the entanglement entropy and the spin-spin correlation function, both of which signaled a divergent correlation length at the transition point with the TIM exponents. At the same time, the bulk correlation function has a jump and the end-to-end correlation function has a discontinuous derivative at the transition point. Consequently for finite h/Γ the transition is of mixed order.</abstract><cop>College Park</cop><pub>American Physical Society</pub><doi>10.1103/PhysRevB.103.174404</doi><orcidid>https://orcid.org/0000-0003-2521-9298</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Antiferromagnetism Chains Correlation Critical point Entanglement Ising model Phase transitions Transition points |
title | Mixed-order transition in the antiferromagnetic quantum Ising chain in a field |
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