“…In this limit the dynamics of the theory is believed to reduce to a string theory without gravity called Little String Theory (LST), or more precisely (2, 0) LST of type A N −1 [166,167,168,169,170]. 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].…”