TL;DR: In this article, the position expectation value is defined by means of a simple many-body operator acting on the wave function of the extended system, and the relationships of the present findings to the Berry-phase theory of polarization are discussed.
Abstract: The position operator (defined within the Schr\"odinger representation in the standard way) becomes meaningless when periodic boundary conditions are adopted for the wave function, as usual in condensed matter physics. I show how to define the position expectation value by means of a simple many-body operator acting on the wave function of the extended system. The relationships of the present findings to the Berry-phase theory of polarization are discussed.
TL;DR: In this article, the Hamiltonian and Lagrangian formalism of free κ-relativistic particles with their four-moment constrained to the mass shell is considered.
TL;DR: A number of important properties of Teager's energy operators are shown that make it possible to determine the energy functions of quite complicated functions, provided these functions can be expressed as products of simpler functions.
Abstract: Teager's energy operators are defined in both the continuous and discrete domains and are very useful tools for analyzing single component signals from an energy point of view. A number of important properties of these operators are shown that make it possible to determine the energy functions of quite complicated functions, provided these functions can be expressed as products of simpler functions, this operation of function multiplication being typical of a modulation process. Some of the eigenfunction properties of the energy operator that illustrate the special role of the trigonometric, Gaussian, and single soliton functions are also given. >
TL;DR: In this article, it was shown that light-ray operators can be computed via the integral of a double-commutator against a conformal block, which can be used to derive a simple derivation of Caron-Huot's Lorentzian OPE inversion formula.
Abstract: We argue that every CFT contains light-ray operators labeled by a continuous spin J. When J is a positive integer, light-ray operators become integrals of local operators over a null line. However for non-integer J , light-ray operators are genuinely nonlocal and give the analytic continuation of CFT data in spin described by Caron-Huot. A key role in our construction is played by a novel set of intrinsically Lorentzian integral transforms that generalize the shadow transform. Matrix elements of light-ray operators can be computed via the integral of a double-commutator against a conformal block. This gives a simple derivation of Caron-Huot’s Lorentzian OPE inversion formula and lets us generalize it to arbitrary four-point functions. Furthermore, we show that light-ray operators enter the Regge limit of CFT correlators, and generalize conformal Regge theory to arbitrary four-point functions. The average null energy operator is an important example of a light-ray operator. Using our construction, we find a new proof of the average null energy condition (ANEC), and furthermore generalize the ANEC to continuous spin.
TL;DR: The conformal anomaly number for new two-dimensional critical points obtained by adding a slightly relevant perturbation φ (renormalization group eigenvalue y ⪡ 1) to a given critical theory is obtained to lowest order in y to be c ′ = c − y 3 / b 2 + …, where b is the operator product expansion coefficient in φφ ∼ (− b ) φ.