Physical stress, mass, and energy for non-relativistic matter
- Univ. of California, Davis, CA (United States). Center for Quantum Mathematics and Physics (QMAP)
- Cornell Univ., Ithaca, NY (United States). Cornell Lab. for Accelerator-based Sciences and Education (CLASSE)
- Univ. of Chicago, Chicago, IL (United States). Kadanoff Center for Theoretical Physics
For theories of relativistic matter fields there exist two possible definitions of the stress-energy tensor, one defined by a variation of the action with the coframes at fixed connection, and the other at fixed torsion. These two stress-energy tensors do not necessarily coincide and it is the latter that corresponds to the Cauchy stress measured in the lab. In this note we discuss the corresponding issue for non-relativistic matter theories. We point out that while the physical non-relativistic stress, momentum, and mass currents are defined by a variation of the action at fixed torsion, the energy current does not admit such a description and is naturally defined at fixed connection. Any attempt to define an energy current at fixed torsion results in an ambiguity which cannot be resolved from the background spacetime data or conservation laws. In conclusion, we also provide computations of these quantities for some simple non-relativistic actions.
- Research Organization:
- Univ. of Chicago, IL (United States)
- Sponsoring Organization:
- USDOE
- Grant/Contract Number:
- FG02-13ER41958; SC0009924
- OSTI ID:
- 1465514
- Journal Information:
- Journal of High Energy Physics (Online), Vol. 2017, Issue 6; ISSN 1029-8479
- Publisher:
- Springer BerlinCopyright Statement
- Country of Publication:
- United States
- Language:
- English
Web of Science
Covariant Poisson’s equation in torsional Newton-Cartan gravity
|
journal | April 2019 |
Newton-Cartan gravity and torsion
|
journal | October 2017 |
Covariant Poisson's equation in torsional Newton-Cartan gravity | text | January 2019 |
Similar Records
Hadamard renormalization of the stress-energy tensor for a quantized scalar field in a general spacetime of arbitrary dimension
Gauge Fixing in the Maxwell Like Gravitational Theory in Minkowski Spacetime and in the Equivalent Lorentzian Spacetime