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Comments on N=2 AdS Orbifolds
High Energy Physics - Theory · Submitted 21 Jun 1998
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Kaluza-Klein reduction on the fixed circle gives the correct conformal dimensions of operators in the superconformal theory and involves some aspects of monopole dynamics in the non-trivial background.
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We discuss twisted states of AdS orbifolds which couple to N=2 chiral primary operators not invariant under exchange of the gauge factors. Kaluza-Klein reduction on the fixed circle gives the correct conformal dimensions of operators in the superconformal theory and involves some aspects of monopole dynamics in the non-trivial background. As a byproduct we found evidence for decoupling of U(1) factors in the four-dimensional gauge theory.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We discuss twisted states of AdS orbifolds which couple to N=2 chiral primary operators not invariant under exchange of the gauge factors. | contribution 0.99 | 0.81 | 0.24 | asserted 0.94 |
| s1 | Kaluza-Klein reduction on the fixed circle gives the correct conformal dimensions of operators in the superconformal theory and involves some aspects of monopole dynamics in the non-trivial background. | result 0.52 | 0.78 | 0.23 | asserted 1.00 |
| s2 | As a byproduct we found evidence for decoupling of U(1) factors in the four-dimensional gauge theory. | result 1.00 | 0.94 | 0.20 | asserted 0.67 |
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Original abstract
We discuss twisted states of AdS orbifolds which couple to N=2 chiral primary operators not invariant under exchange of the gauge factors. Kaluza-Klein reduction on the fixed circle gives the correct conformal dimensions of operators in the superconformal theory and involves some aspects of monopole dynamics in the non-trivial background. As a byproduct we found evidence for decoupling of U(1) factors in the four-dimensional gauge theory.
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References
How the literature uses it
27 arXiv papers cite this in 63 sentences
Papers citing it · 49 sentences without a confident label
Uses its method or tool 3 papers
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Instead, we could follow the analysis of [ref] where blow-up of the orbifold was used to obtain the spectrum of the twisted sector states.
Superconformal Indices for Orbifold Chern-Simons Theories · $U$-type · 1.00
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Now, instead, following again [ref] we assume that the space where the scalars $b_α$ and $c_α$ propagate is of the form [equation] This represents the near-horizon geometry for the twisted fields.
Strong-coupling results for $\mathcal{N}=2$ superconformal quivers and holography · Near-horizon description · 0.80
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Alternatively, instead of starting with the 5+5 Ansatz 34 we may follow the idea of [ref] and attempt to construct an effective 6d action for twisted modes localised on $AdS_5S^1$.
On AdS/CFT duality in the twisted sector of string theory on $AdS_5 \times S^5/\mathbb{Z}_2$ orbifold background · Effective action for twisted sector modes · 0.85
Cites it as support 2 papers
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In section [ref] we analyse solutions for the $B_2$ and $C_2$ fields in this background and identify the 10d analogues of the twisted sector states localised on the $AdS_5 ×S^1$ subspace, thus supporting the logic behind the derivation of the action 18 in [ref] .
On AdS/CFT duality in the twisted sector of string theory on $AdS_5 \times S^5/\mathbb{Z}_2$ orbifold background · Structure of the paper · 0.97
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Moreover, the spectrum of the $AdS_5×S^1$ supergravity [ref] does indeed contain scalar fields of squared mass $n(n-4)$ in one-to-one correspondence with the twisted operators of dimension $n$ of the quiver gauge theory.
Strong-coupling results for $\mathcal{N}=2$ superconformal quivers and holography · Introduction · 0.96
Cites it as background 7 papers
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As mentioned above, the holographic dual description of the $ℤ_M$ quivers is given in terms of Type II B strings propagating in an orbifold geometry of the form AdS$_5×S^5/ℤ_M$ [ref] .
Localization vs holography in $4d$ $\mathcal{N}=2$ quiver theories · Summary of results · 0.83
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On the field theory side, the $ℤ_L$ quotient acts on 4d $𝒩=4$ SU$(LN)$ SYM theory, resulting in a 4d $𝒩=2$ circular quiver gauge theory with gauge group $SU(N)^L$ and matter content encoded in the diagram of Figure [ref] [ref] .
On quantum corrections to semiclassical strings on $\mathrm{AdS}_5\times S^5/\mathbb{Z}_{L}$ orbifold backgrounds · Background · 0.98
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One of the simplest generalisations of the duality between $=4$ SYM theory and type IIB superstring theory on background is based on taking its orbifold [ref] (see also, e.g., [ref] ).
On AdS/CFT duality in the twisted sector of string theory on $AdS_5 \times S^5/\mathbb{Z}_2$ orbifold background · Introduction · 0.88
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