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One-Loop Transition Amplitudes in the D1D5 CFT
High Energy Physics - Theory · Submitted 20 Jun 2016
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim In this paper we consider the deformation to second order in the twist, where we do find effects that can cause thermalization of an initial perturbation.
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The abstract, sentence by sentence
We consider the issue of thermalization in the D1D5 CFT. Thermalization is expected to correspond to the formation of a black hole in the dual gravity theory. We start from the orbifold point, where the theory is essentially free, and does not thermalize. In earlier work it was noted that there was no clear thermalization effect when the theory was deformed off the orbifold point to first order in the relevant twist perturbation. In this paper we consider the deformation to second order in the twist, where we do find effects that can cause thermalization of an initial perturbation. We consider a 1-loop process where two untwisted copies of the CFT are twisted to one copy and then again untwisted to two copies. We start with a single oscillator excitation on the initial CFT, and compute the effect of the two twists on this state. We find simple approximate expressions for the Bogoliubov coefficients and the behavior of the single oscillator excitation in the continuum limit, where the mode numbers involved are taken to be much larger than unity. We also prove a number of useful relationships valid for processes with an arbitrary number of twist insertions.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We consider the issue of thermalization in the D1D5 CFT. | background 0.84 | 0.54 | 0.02 | unclear 0.83 |
| s1 | Thermalization is expected to correspond to the formation of a black hole in the dual gravity theory. | background 0.94 | 0.05 | 0.03 | hedged possibility 0.91 |
| s2 | We start from the orbifold point, where the theory is essentially free, and does not thermalize. | background 0.93 | 0.12 | 0.02 | asserted 0.99 |
| s3 | In earlier work it was noted that there was no clear thermalization effect when the theory was deformed off the orbifold point to first order in the relevant twist perturbation. | background 0.64 | 0.04 | 0.03 | asserted 0.96 |
| s4 | In this paper we consider the deformation to second order in the twist, where we do find effects that can cause thermalization of an initial perturbation. | contribution 0.80 | 0.95 | 0.74 | asserted 0.98 |
| s5 | We consider a 1-loop process where two untwisted copies of the CFT are twisted to one copy and then again untwisted to two copies. | method 0.92 | 0.74 | 0.04 | asserted 0.92 |
| s6 | We start with a single oscillator excitation on the initial CFT, and compute the effect of the two twists on this state. | method 0.89 | 0.91 | 0.03 | asserted 0.94 |
| s7 | We find simple approximate expressions for the Bogoliubov coefficients and the behavior of the single oscillator excitation in the continuum limit, where the mode numbers involved are taken to be much larger than unity. | result 0.99 | 0.97 | 0.18 | asserted 1.00 |
| s8 | We also prove a number of useful relationships valid for processes with an arbitrary number of twist insertions. | result 0.69 | 0.96 | 0.06 | asserted 1.00 |
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The paper
Original abstract
We consider the issue of thermalization in the D1D5 CFT. Thermalization is expected to correspond to the formation of a black hole in the dual gravity theory. We start from the orbifold point, where the theory is essentially free, and does not thermalize. In earlier work it was noted that there was no clear thermalization effect when the theory was deformed off the orbifold point to first order in the relevant twist perturbation. In this paper we consider the deformation to second order in the twist, where we do find effects that can cause thermalization of an initial perturbation. We consider a 1-loop process where two untwisted copies of the CFT are twisted to one copy and then again untwisted to two copies. We start with a single oscillator excitation on the initial CFT, and compute the effect of the two twists on this state. We find simple approximate expressions for the Bogoliubov coefficients and the behavior of the single oscillator excitation in the continuum limit, where the mode numbers involved are taken to be much larger than unity. We also prove a number of useful relationships valid for processes with an arbitrary number of twist insertions.
Human review
How the literature uses it
14 arXiv papers cite this in 29 sentences
Papers citing it · 12 sentences without a confident label
Builds on it 1 paper
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In [ref] we extended our analysis to include initial excitations in the 1-loop process.
Full action of two deformation operators in the D1D5 CFT · Introduction · 0.84
Compares with it 2 papers
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Once again, the anticipated falloff from [ref] is a good approximation for the continuum limit.
Component twist method for higher twists in D1D5 CFT · The squeezed state matrix · 0.89
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These features distinguish it from the pair creation process with one or two twist operators [ref] , where there is no mixing between left and right movers: the left-moving pair creation is a holomorphic function, and the right-moving pair creation is an anti-holomorphic function.
Four-twist effects and monodromy in symmetric orbifold CFTs · Bogoliubov ansatz for four twist effects · 1.00
Cites it as background 12 papers
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For a discussion about redshift and thermalization in the context of fuzzballs, see section 8 of [ref] .
A freely falling graviton in the D1D5 CFT · Discussion · 0.96
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For additional works involving deformations away from the orbifold point see [ref] .
Bootstrapping the effect of the twist operator in the D1D5 CFT · Introduction · 0.99
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The effect of twist 2 operators in the D1D5 CFT has been studied before in the context of deformations towards a black hole spacetime description [ref] .
Component twist method for higher twists in D1D5 CFT · Introduction · 0.97
What it cites · 30 sentences without a confident label
Uses the method or tool of 5 papers
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In calculating each of our transition amplitdes $f$, we use the same mathematical techniques presented in [ref] .
Excitations in the deformed D1D5 CFT · The 1-Loop Case in Question · 1.00
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As detailed in [ref] , the supercharge contours can be removed from the twist by stretching them away until they act on the initial and final states of the process.
Deforming the D1D5 CFT away from the orbifold point · Introduction · 0.87
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More precisely, if we look at the emission from this latter state (following the methods of [ref] ), then we should get an emission of many low energy quanta rather than the few high energy quanta that we started with.
D-brane Approach to Black Hole Quantum Mechanics · Quantum quenches · 0.95
Compares with 1 paper
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We note that the result ([ref]) is schematically similar to the first-order deformation studied in [ref] .
Excitations in the deformed D1D5 CFT · Introduction · 1.00
Cites as background 11 papers
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While the exact dual CFT is strongly coupled, an examination of its 'free' or 'orbifold' point has garnered many fruitful results [ref] .
U(1) Charges and Moduli in the D1-D5 System · Introduction · 0.93
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While the exact dual CFT is strongly coupled, an examination of its 'free' or 'orbifold' point has garnered many fruitful results [ref] .
Three-point functions for M^N/S^N orbifolds with N=4 supersymmetry · Introduction · 0.93
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While the exact dual CFT is strongly coupled, an examination of its 'free' or 'orbifold' point has garnered many fruitful results [ref] .
Virasoro amplitude from the $S^N\R^{24}$ orbifold sigma model · Introduction · 0.93
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