Single-Valued Hamiltonian via Legendre-Fenchel Transformation and Time Translation Symmetry
arXiv:1310.3769 · doi:10.1016/j.nuclphysb.2014.05.017
Abstract
Under conventional Legendre transformation, systems with a non-convex Lagrangian will result in a multi-valued Hamiltonian as a function of conjugate momentum. This causes problems such as non-unitary time evolution of quantum state and non-determined motion of classical particles, and is physically unacceptable. In this work, we propose a new construction of single-valued Hamiltonian by applying Legendre-Fenchel transformation, which is a mathematically rigorous generalization of conventional Legendre transformation, valid for non-convex Lagrangian systems, but not yet widely known to the physics community. With the new single-valued Hamiltonian, we study spontaneous breaking of time translation symmetry and derive its vacuum state. Applications to theories of cosmology and gravitation are discussed.
Journal Version, 16pp. All results + conclusions un-changed, only minor refinements to clarify the importance of our new LFT method and its physics applications; references added
References in corpus (4)
Cited by in corpus (14)
- Colloquium: Quantum and Classical Discrete Time Crystals
- Generalized phase transitions in Lovelock gravity
- Oscillatory Attractors: A New Cosmological Phase
- Resolving the issue of branched Hamiltonian in modified Lanczos-Lovelock gravity
- Canonical structure of higher derivative theories
- History of cosmic evolution with modified Gauss-Bonnet-dilatonic coupled term
- Order by disorder: saving collective motion from topological defects in a conservative model
- The issue of Branched Hamiltonian in F(T) Teleparallel Gravity
- General Null Lagrangians and Their Novel Role in Classical Dynamics
- Inflation and cosmological evolution with gravity theory
- Branched Hamiltonians for a class of Velocity Dependent Potentials
- Perusing Buchbinder--Lyakhovich canonical formalism for Higher-Order Theories of Gravity
- Conflict between some higher-order curvature invariant terms
- The Inertial Spin Model of flocking with position-dependent forces