Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Springer eBooks

The “Galilean” components of a position operator for the photon

M. J. Perrin

Published Apr 6, 2008• 0 citations
Publisher
DOI
10.1007/3-540-07789-8_62

Related papers

Canonical Photon Position Operator with Commuting Components

Michał Dobrski, Maciej Przanowski, Jaromir Tosiek +1 more

Trends in mathematics•Jan 1, 2023•0 citations

An extended Galilean group and its application to time operators

Helmut Bez

The representation theory of the Galilean group extended by a one-dimensional group of dilations (which leave invariant the free Schrodinger equation) is studied. The existence of position and time operators is investigated from the standpoint of the imprimitivity theorem, for quantum particles whose states carry a projective representation of the extended group. Position and time operators are shown to exist for some two-component direct sums with non-trivial multipliers and for vector representations with zero helicity.

Journal of Physics A Mathematical and General•Jul 1, 1976•2 citations

A new position operator for the photon

J. Bertrand

Nuovo cimento della Società italiana di fisica. A, Nuclei, particles and fields•May 1, 1973•7 citations

Fundamental dynamical equations for spinor wavefunctions: I. Lévy-Leblond and Schrödinger equations

R. Huegele, Z. E. Musielak, John L. Fry

A search for fundamental (Galilean invariant) dynamical equations for two- and four-component spinor wavefunctions is conducted in Galilean spacetime. A dynamical equation is considered as fundamental if it is invariant under the symmetry operators of the group of the Galilei metric and if its state functions transform like the irreducible representations of the group of the metric. It is shown that there are no Galilean invariant equations for two-component spinor wavefunctions. A method to derive the Levy-Leblond equation for a four-component spinor wavefunction is presented. It is formally proved that the Levy-Leblond and Schrodinger equations are the only Galilean invariant four-component spinor equations that can be obtained with the Schrodinger phase factor. Physical implications of the obtained results and their relationships to the Pauli–Schrodinger equation are discussed.

Journal of Physics A Mathematical and Theoretical•Mar 22, 2012•3 citations

On the photon position observable

M. Comi

Nuovo cimento della Società italiana di fisica. A, Nuclei, particles and fields•Apr 1, 1980•1 citation

Photon momentum operator

Steven B. Berger

Lettere al nuovo cimento della societa italiana di fisica/Lettere al nuovo cimento•Jun 1, 1976•0 citations
The representation theory of the Galilean group extended by a one-dimensional group of dilations (which leave invariant the free Schrodinger equation) is studied. The existence of position and time operators is investigated from the standpoint of the imprimitivity theorem, for quantum particles whose states carry a projective representation of the extended group. Position and time operators are shown to exist for some two-component direct sums with non-trivial multipliers and for vector representations with zero helicity.
A search for fundamental (Galilean invariant) dynamical equations for two- and four-component spinor wavefunctions is conducted in Galilean spacetime. A dynamical equation is considered as fundamental if it is invariant under the symmetry operators of the group of the Galilei metric and if its state functions transform like the irreducible representations of the group of the metric. It is shown that there are no Galilean invariant equations for two-component spinor wavefunctions. A method to derive the Levy-Leblond equation for a four-component spinor wavefunction is presented. It is formally proved that the Levy-Leblond and Schrodinger equations are the only Galilean invariant four-component spinor equations that can be obtained with the Schrodinger phase factor. Physical implications of the obtained results and their relationships to the Pauli–Schrodinger equation are discussed.