Partition function of free conformal fields in 3-plet representation

被引:18
|
作者
Beccaria, Matteo [1 ,2 ]
Tseytlin, Arkady A. [3 ,4 ]
机构
[1] Univ Salento, Dipartimento Matemat & Fis Ennio De Giorgi, Via Arnesano, I-73100 Lecce, Italy
[2] Ist Nazl Fis Nucl, Via Arnesano, I-73100 Lecce, Italy
[3] Imperial Coll, Blackett Lab, London SW7 2AZ, England
[4] Lebedev Inst, Moscow, Russia
来源
JOURNAL OF HIGH ENERGY PHYSICS | 2017年 / 05期
基金
俄罗斯科学基金会;
关键词
AdS-CFT Correspondence; Conformal Field Theory; STRING THEORY; SUPERGRAVITY; TRANSITION;
D O I
10.1007/JHEP05(2017)053
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
Simplest examples of AdS/CFT duality correspond to free CFTs in d dimensions with fields in vector or adjoint representation of an internal symmetry group dual in the large N limit to a theory of massless or massless plus massive higher spins in AdS(d+1). One may also study generalizations when conformal fields belong to higher dimensional representations, i.e. carry more than two internal symmetry indices. Here we consider the case of the 3-fundamental ("3-plet") representation. One motivation is a conjectured connection to multiple M5-brane theory: heuristic arguments suggest that it may be related to an (interacting) CFT of 6d (2,0) tensor multiplets in 3-plet representation of large N symmetry group that has an AdS 7 dual. We compute the singlet partition function Z on S-1 x Sd-1 for a free field in 3-plet representation of U(N) and analyse its novel large N behaviour. The large N limit of the low temperature expansion of Z which is convergent in the vector and adjoint cases here is only asymptotic, reflecting the much faster growth of the number of singlet operators with dimension, indicating a phase transition at very low temperature. Indeed, while the critical temperatures in the vector (T-c similar to N-gamma; gamma > 0) and adjoint (T-c similar to 1) cases are finite, we find that in the 3-plet case T-c similar to (log N)(-1), i.e. it approaches zero at large N. We discuss some details of large N solution for the eigenvalue distribution. Similar conclusions apply to higher p-plet representations of U( N) or O ( N) and also to the free p- tensor theories invariant under [U(N)](p) or [O (N)] p with p >= 3.
引用
收藏
页数:43
相关论文
共 50 条
  • [1] Partition function of free conformal fields in 3-plet representation
    Matteo Beccaria
    Arkady A. Tseytlin
    Journal of High Energy Physics, 2017
  • [2] Partition function of free conformal higher spin theory
    Beccaria, Matteo
    Bekaert, Xavier
    Tseytlin, Arkady A.
    JOURNAL OF HIGH ENERGY PHYSICS, 2014, (08):
  • [3] Partition function of free conformal higher spin theory
    Matteo Beccaria
    Xavier Bekaert
    Arkady A. Tseytlin
    Journal of High Energy Physics, 2014
  • [4] On partition function and Weyl anomaly of conformal higher-spin fields
    Tseytlin, A. A.
    NUCLEAR PHYSICS B, 2013, 877 (02) : 598 - 631
  • [5] CT for conformal higher spin fields from partition function on conically deformed sphere
    Matteo Beccaria
    Arkady A. Tseytlin
    Journal of High Energy Physics, 2017
  • [6] CT for conformal higher spin fields from partition function on conically deformed sphere
    Beccaria, Matteo
    Tseytlin, Arkady A.
    JOURNAL OF HIGH ENERGY PHYSICS, 2017, (09):
  • [7] Conformal transformations and the SLE partition function martingale
    Bauer, M
    Bernard, D
    ANNALES HENRI POINCARE, 2004, 5 (02): : 289 - 326
  • [8] Conformal Transformations and the SLE Partition Function Martingale
    Michel Bauer
    Denis Bernard
    Annales Henri Poincaré, 2004, 5 : 289 - 326
  • [9] A finite spectral representation of the partition function
    Michael Weba
    The Ramanujan Journal, 2017, 42 : 29 - 42
  • [10] A finite spectral representation of the partition function
    Weba, Michael
    RAMANUJAN JOURNAL, 2017, 42 (01): : 29 - 42