In two spatial dimensions, spin characterizes how particle states re-phase under changes of frame that leave their momentum and energy invariant. Massless particles can in principle have non-trivial spin in this sense, but all existing field theories only describe the trivial case. This letter presents a field theory for a massless particle with non-trivial physical spin. These particles are the (2+1) -dimensional analogues of “continuous-spin” particles in 3+1 dimensions, but here they have only two real degrees of freedom, related by parity. They can be understood as massless generalizations of anyons, but are simpler in key respects
We present new geometric formulations for the fractional spin particle models on the minimal phase s...
AbstractLetting the mass depend on the spin-field coupling as M2=m2−(eg/2c2)FαβSαβ, we propose a new...
We present a new model of <math altimg="si1.gif" xmlns="http://www.w3.org/1998/Math/MathML"><mi>D</m...
In two spatial dimensions, spin characterizes how particle states re-phase under changes of frame th...
AbstractIn two spatial dimensions, spin characterizes how particle states re-phase under changes of ...
Construction of one-particle states as unitary representations of the Poincare algebra in 2 + 1 dime...
We show that two particles interacting via spin exchange exhibit topological features found in one-d...
It seems more and more legitimate to think that elementary particles acquire their mass by interacti...
We delve into the first principles of quantum field theory to prove that the so-called spin-1/2 "bos...
It seems more and more legitimate to think that elementary particles acquire their mass by interacti...
There are gauge-transformation operators applicable to massless spin-1/2 particles within the little...
The two-by-two representation of the SL(2,c) group is for spin-1/2 particles. Starting from this two...
We derive the stabiliser group of the four-vector, also known as Wigner's little group, in case of m...
The general model of an arbitrary spin massive particle in any dimensional space-time is derived on ...
We delve into the first principles of quantum field theory to prove that the so-called spin-1/2 “bos...
We present new geometric formulations for the fractional spin particle models on the minimal phase s...
AbstractLetting the mass depend on the spin-field coupling as M2=m2−(eg/2c2)FαβSαβ, we propose a new...
We present a new model of <math altimg="si1.gif" xmlns="http://www.w3.org/1998/Math/MathML"><mi>D</m...
In two spatial dimensions, spin characterizes how particle states re-phase under changes of frame th...
AbstractIn two spatial dimensions, spin characterizes how particle states re-phase under changes of ...
Construction of one-particle states as unitary representations of the Poincare algebra in 2 + 1 dime...
We show that two particles interacting via spin exchange exhibit topological features found in one-d...
It seems more and more legitimate to think that elementary particles acquire their mass by interacti...
We delve into the first principles of quantum field theory to prove that the so-called spin-1/2 "bos...
It seems more and more legitimate to think that elementary particles acquire their mass by interacti...
There are gauge-transformation operators applicable to massless spin-1/2 particles within the little...
The two-by-two representation of the SL(2,c) group is for spin-1/2 particles. Starting from this two...
We derive the stabiliser group of the four-vector, also known as Wigner's little group, in case of m...
The general model of an arbitrary spin massive particle in any dimensional space-time is derived on ...
We delve into the first principles of quantum field theory to prove that the so-called spin-1/2 “bos...
We present new geometric formulations for the fractional spin particle models on the minimal phase s...
AbstractLetting the mass depend on the spin-field coupling as M2=m2−(eg/2c2)FαβSαβ, we propose a new...
We present a new model of <math altimg="si1.gif" xmlns="http://www.w3.org/1998/Math/MathML"><mi>D</m...