It is natural to believe that the free symmetric product orbifold CFT is dual to the tensionless limit of string theory on AdS 3 × S 3 × T 4 $$ {\mathbb{T}}^4 $$ . At this point in moduli space, string theory is expected to contain a Vasiliev higher spin theory as a subsector. We confirm this picture explicitly by showing that the large level limit of the N $$ \mathcal{N} $$ =4 cosets of arXiv:1305.4181, that are dual to a higher spin theory on AdS 3 , indeed describe a closed subsector of the symmetric product orbifold. Furthermore, we reorganise the full partition function of the symmetric product orbifold in terms of representations of the higher spin algebra (or rather its W ∞ $$ {\mathcal{W}}_{\infty } $$ extension). In particular, the...
We analyze the folded spinning string in AdS4 × Bbb P3 with spin S in AdS4 and angular momentum J in...
It has recently been argued that the symmetric orbifold theory of T4 is dual to string theory on AdS...
We observe that the partition function of the set of all free massless higher spins s = 0, 1, 2, 3,....
It is natural to believe that the free symmetric product orbifold CFT is dual to the tensionless lim...
We determine the asymptotic symmetry algebra (for fields of low spin) of the M × M matrix extended V...
It was recently shown that the CFT dual of string theory on AdS3 × S3 × T4, the symmetric orbifold o...
In this lecture I review recent work on higher spin holography. After a notational flash on the AdS/...
We study the holographic duality between the M × M matrix extension of Vasiliev higher spin theories...
The tensionless regime of string theory is exp ected to exhibit a large unbroken symmetry which is h...
In this lecture I review recent work done in collaboration with Beisert et al. [1-3] (For a concise ...
A Formal Higher Spin Gravity in five dimensions is constructed. It was shown recently that construct...
All correlation functions of conserved currents of the CFT that is dual to unbroken Vasiliev theory ...
We review the basic structure of the higher spin extension of D=4, N=8 AdS supergravity. The theory ...
We study the higher-spin gauge theory in six-dimensional anti-de Sitter space AdS(6) that is based o...
The strong version of Maldacena's AdS/CFT conjecture implies that the large Nexpansion of free N=4 s...
We analyze the folded spinning string in AdS4 × Bbb P3 with spin S in AdS4 and angular momentum J in...
It has recently been argued that the symmetric orbifold theory of T4 is dual to string theory on AdS...
We observe that the partition function of the set of all free massless higher spins s = 0, 1, 2, 3,....
It is natural to believe that the free symmetric product orbifold CFT is dual to the tensionless lim...
We determine the asymptotic symmetry algebra (for fields of low spin) of the M × M matrix extended V...
It was recently shown that the CFT dual of string theory on AdS3 × S3 × T4, the symmetric orbifold o...
In this lecture I review recent work on higher spin holography. After a notational flash on the AdS/...
We study the holographic duality between the M × M matrix extension of Vasiliev higher spin theories...
The tensionless regime of string theory is exp ected to exhibit a large unbroken symmetry which is h...
In this lecture I review recent work done in collaboration with Beisert et al. [1-3] (For a concise ...
A Formal Higher Spin Gravity in five dimensions is constructed. It was shown recently that construct...
All correlation functions of conserved currents of the CFT that is dual to unbroken Vasiliev theory ...
We review the basic structure of the higher spin extension of D=4, N=8 AdS supergravity. The theory ...
We study the higher-spin gauge theory in six-dimensional anti-de Sitter space AdS(6) that is based o...
The strong version of Maldacena's AdS/CFT conjecture implies that the large Nexpansion of free N=4 s...
We analyze the folded spinning string in AdS4 × Bbb P3 with spin S in AdS4 and angular momentum J in...
It has recently been argued that the symmetric orbifold theory of T4 is dual to string theory on AdS...
We observe that the partition function of the set of all free massless higher spins s = 0, 1, 2, 3,....