Integrable Spin Chains with U(1)^3 symmetry and generalized Lunin-Maldacena backgrounds

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Integrable Spin Chains with U(1)^3 symmetry and generalized Lunin-Maldacena backgrounds. / Freyhult, L.; Kristjansen, C.; Mansson, T.

I: Journal of High Energy Physics, Bind 2005, Nr. 12, 26.10.2005.

Publikation: Bidrag til tidsskriftTidsskriftartikelfagfællebedømt

Harvard

Freyhult, L, Kristjansen, C & Mansson, T 2005, 'Integrable Spin Chains with U(1)^3 symmetry and generalized Lunin-Maldacena backgrounds', Journal of High Energy Physics, bind 2005, nr. 12. https://doi.org/10.1088/1126-6708/2005/12/008

APA

Freyhult, L., Kristjansen, C., & Mansson, T. (2005). Integrable Spin Chains with U(1)^3 symmetry and generalized Lunin-Maldacena backgrounds. Journal of High Energy Physics, 2005(12). https://doi.org/10.1088/1126-6708/2005/12/008

Vancouver

Freyhult L, Kristjansen C, Mansson T. Integrable Spin Chains with U(1)^3 symmetry and generalized Lunin-Maldacena backgrounds. Journal of High Energy Physics. 2005 okt. 26;2005(12). https://doi.org/10.1088/1126-6708/2005/12/008

Author

Freyhult, L. ; Kristjansen, C. ; Mansson, T. / Integrable Spin Chains with U(1)^3 symmetry and generalized Lunin-Maldacena backgrounds. I: Journal of High Energy Physics. 2005 ; Bind 2005, Nr. 12.

Bibtex

@article{dd64694f402c46fd8b065c7a93beaffb,
title = "Integrable Spin Chains with U(1)^3 symmetry and generalized Lunin-Maldacena backgrounds",
abstract = "We consider the most general three-state spin chain with U(1)^3 symmetry and nearest neighbour interaction. Our model contains as a special case the spin chain describing the holomorphic three scalar sector of the three parameter complex deformation of N=4 SYM, dual to type IIB string theory in the generalized Lunin-Maldacena backgrounds discovered by Frolov. We formulate the coordinate space Bethe ansatz, calculate the S-matrix and determine for which choices of parameters the S-matrix fulfills the Yang-Baxter equations. For these choices of parameters we furthermore write down the R-matrix. We find in total four classes of integrable models. In particular, each already known model of the above type is nothing but one in a family of such models.",
keywords = "hep-th",
author = "L. Freyhult and C. Kristjansen and T. Mansson",
note = "16 pages, 3 figures, references corrected",
year = "2005",
month = oct,
day = "26",
doi = "10.1088/1126-6708/2005/12/008",
language = "English",
volume = "2005",
journal = "Journal of High Energy Physics (Online)",
issn = "1126-6708",
publisher = "Springer",
number = "12",

}

RIS

TY - JOUR

T1 - Integrable Spin Chains with U(1)^3 symmetry and generalized Lunin-Maldacena backgrounds

AU - Freyhult, L.

AU - Kristjansen, C.

AU - Mansson, T.

N1 - 16 pages, 3 figures, references corrected

PY - 2005/10/26

Y1 - 2005/10/26

N2 - We consider the most general three-state spin chain with U(1)^3 symmetry and nearest neighbour interaction. Our model contains as a special case the spin chain describing the holomorphic three scalar sector of the three parameter complex deformation of N=4 SYM, dual to type IIB string theory in the generalized Lunin-Maldacena backgrounds discovered by Frolov. We formulate the coordinate space Bethe ansatz, calculate the S-matrix and determine for which choices of parameters the S-matrix fulfills the Yang-Baxter equations. For these choices of parameters we furthermore write down the R-matrix. We find in total four classes of integrable models. In particular, each already known model of the above type is nothing but one in a family of such models.

AB - We consider the most general three-state spin chain with U(1)^3 symmetry and nearest neighbour interaction. Our model contains as a special case the spin chain describing the holomorphic three scalar sector of the three parameter complex deformation of N=4 SYM, dual to type IIB string theory in the generalized Lunin-Maldacena backgrounds discovered by Frolov. We formulate the coordinate space Bethe ansatz, calculate the S-matrix and determine for which choices of parameters the S-matrix fulfills the Yang-Baxter equations. For these choices of parameters we furthermore write down the R-matrix. We find in total four classes of integrable models. In particular, each already known model of the above type is nothing but one in a family of such models.

KW - hep-th

U2 - 10.1088/1126-6708/2005/12/008

DO - 10.1088/1126-6708/2005/12/008

M3 - Journal article

VL - 2005

JO - Journal of High Energy Physics (Online)

JF - Journal of High Energy Physics (Online)

SN - 1126-6708

IS - 12

ER -

ID: 186915321