2003
DOI: 10.1103/physrevd.67.086009
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Thermal correlators in little string theory

Abstract: We calculate, using holographic duality, the thermal two-point function in finite temperature little string theory. The analysis of those correlators reveals possible instabilities of the thermal ensemble, as in previous discussions of the thermodynamics of little string theory. We comment on the dependence of the instability on the spatial volume of the system.

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Cited by 16 publications
(23 citation statements)
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“…45 In this subsection (see also [155,58]) we will consider the thermodynamics of the near-extremal NS5-brane in type IIA string theory using as a starting point the S-dual description as a near-extremal M5-brane on a transverse circle and the input of the phases obtained from six-dimensional neutral Kaluza-Klein black holes in Section 3. Other interesting work on the thermodynamics of LST can be found in [171,164,172,173,174,175,176,177,178,179,180].…”
Section: Little String Theorymentioning
confidence: 99%
“…45 In this subsection (see also [155,58]) we will consider the thermodynamics of the near-extremal NS5-brane in type IIA string theory using as a starting point the S-dual description as a near-extremal M5-brane on a transverse circle and the input of the phases obtained from six-dimensional neutral Kaluza-Klein black holes in Section 3. Other interesting work on the thermodynamics of LST can be found in [171,164,172,173,174,175,176,177,178,179,180].…”
Section: Little String Theorymentioning
confidence: 99%
“…Schenker et al 2012;Dijkstra et al 2014) are quite weak and highly model-dependent. Various efforts have been made to explore the 21 cm signatures from the neutral hydrogen present in the IGM during the EoR, and people pin hope on the low frequency radio experiments such as the Precision Array for Probing the Epoch of Re-ionization (PAPER; Parsons et al 2010;Ali et al 2015), the Murchison Widefield Array (MWA; Tingay et al 2013;Ewall-Wice et al 2016), the LOw Frequency ARray (LOFAR; van Haarlem et al 2013), the Long Wavelength Array (LWA; Ellingson et al 2009), as well as the future Hydrogen Epoch of Reionization Array 1 (HERA; DeBoer et al 2016) and the Square Kilometre Array 2 (SKA; Huynh & Lazio 2013). These 21 cm experiments will greatly push forward the frontiers of our understanding on reionization.…”
Section: Introductionmentioning
confidence: 99%
“…Even this leakage, however, has been shown in recent years to have a predictable "wedge" signature on the k ⊥ -k plane, limiting the contaminated region to a triangular-shaped region at high k ⊥ and low k (Datta et al 2010;Vedantham et al 2012;Morales et al 2012;Parsons et al 2012b;Trott et al 2012;Thyagarajan et al 2013;Pober et al 2013a;Dillon et al 2014;Hazelton et al 2013;Thyagarajan et al 2015b,a;Liu et al 2014a,b;Chapman et al 2016;Pober et al 2016;Seo & Hirata 2016;Jensen et al 2016;Kohn et al 2016). In fact, the foreground wedge is considered sufficiently robust that some instruments have been designed around it (Pober et al 2014;DeBoer et al 2016;Dillon & Parsons 2016;Neben et al 2016b;Ewall-Wice et al 2016b;Thyagarajan et al 2016), implicitly pursuing a strategy of foreground avoidance where the power spectrum can be measured in relatively uncontaminated Fourier modes outside the wedge. This mitigates the need for extremely detailed models of the foregrounds, providing a conservative path towards early detections of the power spectrum.…”
Section: Introductionmentioning
confidence: 99%