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The '''J1-J2 model''' is a [[quantum spin model]] like the [[Heisenberg model (quantum)|Heisenberg model]] but also includes a term for the interaction between next-nearest neighbor spins.
The '''J1–J2 model''' is a [[quantum spin model]] like the [[Heisenberg model (quantum)|Heisenberg model]] but also includes a term for the interaction between next-nearest neighbor spins.


==Hamiltonian==
==Hamiltonian==
In this model, the term <math>J_1</math> represents the usual nearest-neighbor interaction as seen in the Heisenberg model, and <math>J_2</math> represents the exchange interaction to the ''next'' nearest-neighbor.


<math>\hat H = J_1 \sum_{<ij>}\vec S_i \cdot \vec S_j + J_2 \sum_{<<ij>>} \vec S_i \cdot \vec S_j</math>
: <math>\hat H = J_1 \sum_{\langle ij \rangle}\vec S_i \cdot \vec S_j + J_2 \sum_{\langle\langle ij \rangle\rangle} \vec S_i \cdot \vec S_j </math>


==See also==
[[File:J1_J2_model.png]]

==See Also==
*[[Spin model]]
*[[Spin model]]
*[[Heisenberg model (quantum)]]
*[[Heisenberg model (quantum)]]
*[[Hubbard model]]
*[[Hubbard model]]
*[[t-J model]]
*[[t-J model]]
*[[Majumdar–Ghosh model]]


==References==
==References==
*{{cite journal|last1=Sirker|first1=J.|last2=Weihong|first2=Zheng|last3=Sushkov|first3=O. P.|last4=Oitmaa|first4=J.|title=J1−J2model: First-order [[phase transition]] versus deconfinement of spinons|journal=Physical Review B|volume=73|issue=18|year=2006|page=184420 |issn=1098-0121|doi=10.1103/PhysRevB.73.184420|arxiv=cond-mat/0601183|s2cid=54172992 }}
*{{cite journal|last1=Ceccatto|first1=H. A.|last2=Gazza|first2=C. J.|last3=Trumper|first3=A. E.|title=J1-J2model: Energy, correlations, and order-parameter fluctuations on finite lattices|journal=Physical Review B|volume=45|issue=14|year=1992|pages=7832–7836|issn=0163-1829|doi=10.1103/PhysRevB.45.7832}}
*{{cite journal|last1=Dagotto|first1=Elbio|last2=Moreo|first2=Adriana|author2-link= Adriana Moreo |title=Phase diagram of the frustrated spin-1/2 Heisenberg antiferromagnet in 2 dimensions|journal=Physical Review Letters|volume=63|issue=19|year=1989|pages=2148–2151|issn=0031-9007|doi=10.1103/PhysRevLett.63.2148|url=http://sces.phys.utk.edu/mostcited/mc15_1114.pdf}}
*{{cite journal|last1=Majumdar|first1=Chanchal K.|last2=Ghosh|first2=Dipan K.|title=On Next‐Nearest‐Neighbor Interaction in Linear Chain. I|journal=Journal of Mathematical Physics|volume=10|issue=8|year=1969|pages=1388–1398|issn=0022-2488|doi=10.1063/1.1664978}}
*{{cite journal|last1=Majumdar|first1=Chanchal K.|last2=Ghosh|first2=Dipan K.|title=On Next‐Nearest‐Neighbor Interaction in Linear Chain. II|journal=Journal of Mathematical Physics|volume=10|issue=8|year=1969|pages=1399–1402|issn=0022-2488|doi=10.1063/1.1664979}}


*J1-J2 model: First-order phase transition versus deconfinement of spinons Phys. Rev. B 73, 184420 (2006) [7 pages] [http://scitation.aip.org/getabs/servlet/GetabsServlet?prog=normal&id=PRBMDO000073000018184420000001&idtype=cvips&gifs=yes]

*J1-J2 model: Energy, correlations, and order-parameter fluctuations on finite lattices (1992) Phys. Rev. B 45, 7832 (1992) [http://prola.aps.org/showrefs/PRB/v45/i14/p7832_1]

*Phase diagram of the frustrated spin-1/2 Heisenberg antiferromagnet in 2 dimensions (1989) Phys. Rev. Lett. 63, 2148 - 2151 (1989) [http://prola.aps.org/abstract/PRL/v63/i19/p2148_1]

*On Next-Nearest-Neighbor Interaction in Linear Chain. II (1969) J. Math. Phys. 10, 1388 (1969); DOI:10.1063/1.1664978 [http://link.aip.org/link/?JMAPAQ/10/1388/1]

*On Next-Nearest-Neighbor Interaction in Linear Chain. I (1969) J. Math. Phys. 10, 1388 (1969); DOI:10.1063/1.1664978 [http://link.aip.org/link/?JMAPAQ/10/1388/1]

[[Category:Magnetism]]
[[Category:Spin models]]
[[Category:Spin models]]
[[Category:Statistical mechanics]]
[[Category:Quantum magnetism]]

Latest revision as of 18:21, 27 April 2024

The J1–J2 model is a quantum spin model like the Heisenberg model but also includes a term for the interaction between next-nearest neighbor spins.

Hamiltonian

[edit]

In this model, the term represents the usual nearest-neighbor interaction as seen in the Heisenberg model, and represents the exchange interaction to the next nearest-neighbor.

See also

[edit]

References

[edit]
  • Sirker, J.; Weihong, Zheng; Sushkov, O. P.; Oitmaa, J. (2006). "J1−J2model: First-order phase transition versus deconfinement of spinons". Physical Review B. 73 (18): 184420. arXiv:cond-mat/0601183. doi:10.1103/PhysRevB.73.184420. ISSN 1098-0121. S2CID 54172992.
  • Ceccatto, H. A.; Gazza, C. J.; Trumper, A. E. (1992). "J1-J2model: Energy, correlations, and order-parameter fluctuations on finite lattices". Physical Review B. 45 (14): 7832–7836. doi:10.1103/PhysRevB.45.7832. ISSN 0163-1829.
  • Dagotto, Elbio; Moreo, Adriana (1989). "Phase diagram of the frustrated spin-1/2 Heisenberg antiferromagnet in 2 dimensions" (PDF). Physical Review Letters. 63 (19): 2148–2151. doi:10.1103/PhysRevLett.63.2148. ISSN 0031-9007.
  • Majumdar, Chanchal K.; Ghosh, Dipan K. (1969). "On Next‐Nearest‐Neighbor Interaction in Linear Chain. I". Journal of Mathematical Physics. 10 (8): 1388–1398. doi:10.1063/1.1664978. ISSN 0022-2488.
  • Majumdar, Chanchal K.; Ghosh, Dipan K. (1969). "On Next‐Nearest‐Neighbor Interaction in Linear Chain. II". Journal of Mathematical Physics. 10 (8): 1399–1402. doi:10.1063/1.1664979. ISSN 0022-2488.