Parity breaking transport in Lifshitz hydrodynamics
We derive the constitutive relations of first order charged hydrodynamics for theories with Lifshitz scaling and broken parity in 2 + 1 and 3 + 1 spacetime dimensions. In addition to the anomalous (in 3+1) or Hall (in 2+1) transport of relativistic hydrodynamics, there is an additional non-dissipati...
| Autores: | , , |
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| Tipo de recurso: | artículo |
| Fecha de publicación: | 2015 |
| País: | España |
| Institución: | Universidad de Oviedo (UNIOVI) |
| Repositorio: | RUO. Repositorio Institucional de la Universidad de Oviedo |
| Idioma: | inglés |
| OAI Identifier: | oai:digibuo.uniovi.es:10651/33964 |
| Acceso en línea: | http://hdl.handle.net/10651/33964 https://dx.doi.org/10.1007/JHEP09(2015)031 |
| Access Level: | acceso abierto |
| Palabra clave: | Space-Time Symmetries Anomalies in Field and String Theories Effective field theories |
| Sumario: | We derive the constitutive relations of first order charged hydrodynamics for theories with Lifshitz scaling and broken parity in 2 + 1 and 3 + 1 spacetime dimensions. In addition to the anomalous (in 3+1) or Hall (in 2+1) transport of relativistic hydrodynamics, there is an additional non-dissipative transport allowed by the absence of boost invariance. We analyze the non-relativistic limit and use a phenomenological model of a strange metal to argue that these effects can be measured in principle by using electromagnetic fields with non-zero gradients |
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