The Galilei group involves mass as a central charge. We show that the associated superselection rule is incompatible with the observed phenomenology of superfluid helium 4: this is recovered only under the assumption that mass is spontaneou.519 broken. This remark is somewhat immaterial for the real world, where the correct space-time symmetries are encoded by the Poincare group, which has no central charge. Yet it provides an explicit example of how superselection rules can be experimentally tested. -We elaborate on what conditions must be met for our ideas to be generalizable to the relativistic case of the integer/half-integer angular momentum superselection rule
- Physics, as we know it, attempts to interpret the diverse natural phenomena as particular manifest...
We construct N = 1 supergravity models where the gauge symmetry and supersymmetry are both spontaneo...
Driven by the mass problem, we raise some issues of the fundamental interactions in terms of non tri...
We reinvestigate Bargmann's superselection rule for the overall mass of n particles in ordinary quan...
It is argued that superselection rules originate not from symmetry but from the initial state of the...
The Galilei group has been taken as the fundamental symmetry for 'nonrelativistic' physics, quantum ...
It is commonly believed that unbroken supersymmetry (SUSY) implies that all members of a supermultip...
Abstract The meaning of local observables is poorly understood in gauge theories, not to speak of qu...
The Galilean symmetry and the Poincare symmetry are usually taken as the fundamental (relativity) sy...
The overaraching goal of this paper is to elucidate the nature of superselection rules in a manner t...
The meaning of superselection rules in Bohm–Bell theories (i.e., quantum the-ories with particle tra...
We reexamine the dynamical generation of mass for fermions charged under various Lie groups with equ...
We demonstrate that, before spontaneous symmetry breaking (SSB), we could write the theory as though...
Strong evidence supports the idea that pure q~4 field theory is "trivial " or non-interact...
This work continues earlier investigations towards constructing a consistent new Quantum Field Theor...
- Physics, as we know it, attempts to interpret the diverse natural phenomena as particular manifest...
We construct N = 1 supergravity models where the gauge symmetry and supersymmetry are both spontaneo...
Driven by the mass problem, we raise some issues of the fundamental interactions in terms of non tri...
We reinvestigate Bargmann's superselection rule for the overall mass of n particles in ordinary quan...
It is argued that superselection rules originate not from symmetry but from the initial state of the...
The Galilei group has been taken as the fundamental symmetry for 'nonrelativistic' physics, quantum ...
It is commonly believed that unbroken supersymmetry (SUSY) implies that all members of a supermultip...
Abstract The meaning of local observables is poorly understood in gauge theories, not to speak of qu...
The Galilean symmetry and the Poincare symmetry are usually taken as the fundamental (relativity) sy...
The overaraching goal of this paper is to elucidate the nature of superselection rules in a manner t...
The meaning of superselection rules in Bohm–Bell theories (i.e., quantum the-ories with particle tra...
We reexamine the dynamical generation of mass for fermions charged under various Lie groups with equ...
We demonstrate that, before spontaneous symmetry breaking (SSB), we could write the theory as though...
Strong evidence supports the idea that pure q~4 field theory is "trivial " or non-interact...
This work continues earlier investigations towards constructing a consistent new Quantum Field Theor...
- Physics, as we know it, attempts to interpret the diverse natural phenomena as particular manifest...
We construct N = 1 supergravity models where the gauge symmetry and supersymmetry are both spontaneo...
Driven by the mass problem, we raise some issues of the fundamental interactions in terms of non tri...