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.
In this model, the term
J
1
{\displaystyle J_{1}}
represents the usual nearest-neighbor interaction as seen in the Heisenberg model, and
J
2
{\displaystyle J_{2}}
represents the exchange interaction to the next nearest-neighbor.
H
^
=
J
1
∑
⟨
i
j
⟩
S
→
i
⋅
S
→
j
+
J
2
∑
⟨
⟨
i
j
⟩
⟩
S
→
i
⋅
S
→
j
{\displaystyle {\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}}
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 .