dc.contributor.author |
Bhadury, Samapan |
|
dc.contributor.author |
Das, Arpan |
|
dc.contributor.author |
Florkowski, Wojciech |
|
dc.contributor.author |
Gowthama, K. K. |
|
dc.contributor.author |
Ryblewski, Radoslaw |
|
dc.coverage.spatial |
United States of America |
|
dc.date.accessioned |
2024-02-08T13:08:17Z |
|
dc.date.available |
2024-02-08T13:08:17Z |
|
dc.date.issued |
2024-02 |
|
dc.identifier.citation |
Bhadury, Samapan; Das, Arpan; Florkowski, Wojciech; Gowthama, K. K. and Ryblewski, Radoslaw, "Polarization of spin-1/2 particles with effective spacetime dependent masses", Physics Letters B, DOI: 10.1016/j.physletb.2024.138464, vol. 849, Feb. 2024. |
|
dc.identifier.issn |
0370-2693 |
|
dc.identifier.issn |
1873-2445 |
|
dc.identifier.uri |
https://doi.org/10.1016/j.physletb.2024.138464 |
|
dc.identifier.uri |
https://repository.iitgn.ac.in/handle/123456789/9732 |
|
dc.description.abstract |
Semiclassical expansion of the Wigner function for spin-
fermions having an effective spacetime-dependent mass is used to analyze spin-polarization effects. The existing framework is reformulated to obtain a differential equation directly connecting the particle spin tensor with the effective mass. It reflects the conservation of the total angular momentum in a system. In general, we find that the gradients of mass act as a source of the spin polarization. Although this effect is absent for simple boost-invariant dynamics, an extension to non-boost-invariant systems displays a non-trivial dependence of the spin density on the mass indicating that the spin polarization effects may be intertwined with the phenomenon of chiral restoration. |
|
dc.description.statementofresponsibility |
by Samapan Bhadury, Arpan Das, Wojciech Florkowski, K. K. Gowthama and Radoslaw Ryblewski |
|
dc.format.extent |
vol. 849 |
|
dc.language.iso |
en_US |
|
dc.publisher |
Elsevier |
|
dc.title |
Polarization of spin-1/2 particles with effective spacetime dependent masses |
|
dc.type |
Article |
|
dc.relation.journal |
Physics Letters B |
|