PIRSA:16080052

Universal features of Lifshitz Green’s functions--- from holography and field theory

APA

Sun, K. (2016). Universal features of Lifshitz Green’s functions--- from holography and field theory. Perimeter Institute for Theoretical Physics. https://pirsa.org/16080052

MLA

Sun, Kai. Universal features of Lifshitz Green’s functions--- from holography and field theory. Perimeter Institute for Theoretical Physics, Aug. 26, 2016, https://pirsa.org/16080052

BibTex

          @misc{ scivideos_PIRSA:16080052,
            doi = {10.48660/16080052},
            url = {https://pirsa.org/16080052},
            author = {Sun, Kai},
            keywords = {Quantum Matter, Quantum Fields and Strings},
            language = {en},
            title = {Universal features of Lifshitz Green{\textquoteright}s functions--- from holography and field theory},
            publisher = {Perimeter Institute for Theoretical Physics},
            year = {2016},
            month = {aug},
            note = {PIRSA:16080052 see, \url{https://scivideos.org/index.php/pirsa/16080052}}
          }
          

Kai Sun University of Michigan–Ann Arbor

Talk numberPIRSA:16080052

Abstract

In this talk, we examine the behavior of the retarded Green’s function in theories with Lifshitz scaling symmetry, both through dual gravitational models and a direct field theory approach. In contrast with the case of a relativistic CFT, where the Green’s function is fixed (up to normalization) by symmetry, the generic Lifshitz Green’s function can a priori depend on an arbitrary function Nevertheless, we demonstrate that the imaginary part of the retarded Green’s function (i.e. the spectral function) of scalar operators is exponentially suppressed in a window of frequencies near zero. This behavior is universal in all Lifshitz theories without additional constraining symmetries. On the gravity side, this result is robust against higher derivative corrections, while on the field theory side we present two z>1 examples where the exponential suppression arises from summing the perturbative expansion to infinite order, as a consequence of the energy-momentum conservation.