We study point particles to illustrate the various symmetries such as the Poincaré group and its non-relativistic version. In order to find the Noether charges and the Noether currents, which are conserved under physical symmetries, we study Noether’s theorem. We describe the Pauli-Lubanski spin vector, which is invariant under the Poincaré group and describes the spin of a particle in field theory. By promoting the Pauli-Lubanski spin vector to an operator in the quantized theory we will see that it describes the spin of a particle. Moreover, we find an action for a smooth spinning bosonic particle by compactifying one string dimension together with one embedding dimension. As with the Pauli-Lubanski spin vector, we need to quantize this a...
We construct a relativistic spinning-particle Lagrangian where spin is considered as a composite qua...
We present a new treatment for the spin of a massive relativistic particle in the context of quantum...
To describe a massive particle with fixed, but arbitrary, spin on d=4 anti-de Sitter space M"4,...
All particles inside the Standard Model fall inside some of these representations, which are labelle...
The connection between spin and symmetry was established by Wigner in his 1939 paper on the Poincar\...
Abstract Due to proton spin crisis it is necessary to understand the gauge invariant definition of t...
The concept of elementary particle rests on the idea that it is a physical system with no excited st...
It has been shown that the massless irreducible representations of the Poincaré group with continuou...
This thesis deals with the construction of models for spinning relativistic particles and their cova...
The spin-statistics conection is obtained for classical point particles. The connection holds within...
It is proven that the Poincare symmetry determines equations of motion, which are for massless parti...
We discuss the role of spin in Poincaré invariant formulations of quantum mechanics
Till now, for a 3-dimensional spinning particle only non-Noetherian conservation laws are known([3])...
AbstractIn the framework of vector model of spin, we discuss the problem of a covariant formalism [3...
An examination is made of the consequences for the quantum mechanics of spinning particles of equati...
We construct a relativistic spinning-particle Lagrangian where spin is considered as a composite qua...
We present a new treatment for the spin of a massive relativistic particle in the context of quantum...
To describe a massive particle with fixed, but arbitrary, spin on d=4 anti-de Sitter space M"4,...
All particles inside the Standard Model fall inside some of these representations, which are labelle...
The connection between spin and symmetry was established by Wigner in his 1939 paper on the Poincar\...
Abstract Due to proton spin crisis it is necessary to understand the gauge invariant definition of t...
The concept of elementary particle rests on the idea that it is a physical system with no excited st...
It has been shown that the massless irreducible representations of the Poincaré group with continuou...
This thesis deals with the construction of models for spinning relativistic particles and their cova...
The spin-statistics conection is obtained for classical point particles. The connection holds within...
It is proven that the Poincare symmetry determines equations of motion, which are for massless parti...
We discuss the role of spin in Poincaré invariant formulations of quantum mechanics
Till now, for a 3-dimensional spinning particle only non-Noetherian conservation laws are known([3])...
AbstractIn the framework of vector model of spin, we discuss the problem of a covariant formalism [3...
An examination is made of the consequences for the quantum mechanics of spinning particles of equati...
We construct a relativistic spinning-particle Lagrangian where spin is considered as a composite qua...
We present a new treatment for the spin of a massive relativistic particle in the context of quantum...
To describe a massive particle with fixed, but arbitrary, spin on d=4 anti-de Sitter space M"4,...