Quantum Self-Frictional Relativistic Nucleoseed Spinor-Type Tensor Field Theory of Nature

For study of quantum self-frictional (SF) relativistic nucleoseed spinor-type tensor (NSST) field theory of nature (SF-NSST atomic-molecular-nuclear and cosmic-universe systems) we use the complete orthogonal basis sets of 22s+1-component column-matrices type SF Ψnljmjδ⁎s-relativistic NSST orbitals...

Full description

Bibliographic Details
Main Author: I. I. Guseinov
Format: Article
Language:English
Published: Hindawi Limited 2017-01-01
Series:Advances in High Energy Physics
Online Access:http://dx.doi.org/10.1155/2017/6049079
id doaj-bd875e74a82c409296cb0e2dc985c84a
record_format Article
spelling doaj-bd875e74a82c409296cb0e2dc985c84a2020-11-24T23:14:13ZengHindawi LimitedAdvances in High Energy Physics1687-73571687-73652017-01-01201710.1155/2017/60490796049079Quantum Self-Frictional Relativistic Nucleoseed Spinor-Type Tensor Field Theory of NatureI. I. Guseinov0Department of Physics, Faculty of Arts and Sciences, Onsekiz Mart University, Çanakkale, TurkeyFor study of quantum self-frictional (SF) relativistic nucleoseed spinor-type tensor (NSST) field theory of nature (SF-NSST atomic-molecular-nuclear and cosmic-universe systems) we use the complete orthogonal basis sets of 22s+1-component column-matrices type SF Ψnljmjδ⁎s-relativistic NSST orbitals (Ψδ⁎s-RNSSTO) and SF Xnljmjs-relativistic Slater NSST orbitals (Xs-RSNSSTO) through the ψnlmlδ⁎-nonrelativistic scalar orbitals (ψδ⁎-NSO) and χnlml-nonrelativistic Slater type orbitals (χ-NSTO), respectively. Here δ⁎=pl⁎ or δ⁎=α⁎ and pl⁎=2l+2-α⁎,  α⁎ are the integer (α⁎=α, -∞<α≤2) or noninteger (α⁎≠α, -∞<α⁎<3) SF quantum numbers, where s=0,1/2,1,3/2,2,…. We notice that the nonrelativistic ψδ⁎-NSO and χ-NSTO orbitals themselves are obtained from the relativistic Ψδ⁎s-RNSSTO and Xs-RSNSSTO functions for s=0, respectively. The column-matrices-type SF Y1jmjls-RNSST harmonics (Y1ls-RNSSTH) and Y2jmjls-modified NSSTH (Y2ls-MNSSTH) functions for arbitrary spin s introduced by the author in the previous papers are also used. The one- and two-center one-range addition theorems for ψδ⁎-NSO and noninteger n  χ-NSTO orbitals are presented. The quantum SF relativistic nonperturbative theory for Vnljmjδ⁎-RNSST potentials (Vδ⁎-RNSSTP) and their derivatives is also suggested. To study the transportations of mass and momentum in nature the quantum SF relativistic NSST gravitational photon (gph) with s=1 is introduced.http://dx.doi.org/10.1155/2017/6049079
collection DOAJ
language English
format Article
sources DOAJ
author I. I. Guseinov
spellingShingle I. I. Guseinov
Quantum Self-Frictional Relativistic Nucleoseed Spinor-Type Tensor Field Theory of Nature
Advances in High Energy Physics
author_facet I. I. Guseinov
author_sort I. I. Guseinov
title Quantum Self-Frictional Relativistic Nucleoseed Spinor-Type Tensor Field Theory of Nature
title_short Quantum Self-Frictional Relativistic Nucleoseed Spinor-Type Tensor Field Theory of Nature
title_full Quantum Self-Frictional Relativistic Nucleoseed Spinor-Type Tensor Field Theory of Nature
title_fullStr Quantum Self-Frictional Relativistic Nucleoseed Spinor-Type Tensor Field Theory of Nature
title_full_unstemmed Quantum Self-Frictional Relativistic Nucleoseed Spinor-Type Tensor Field Theory of Nature
title_sort quantum self-frictional relativistic nucleoseed spinor-type tensor field theory of nature
publisher Hindawi Limited
series Advances in High Energy Physics
issn 1687-7357
1687-7365
publishDate 2017-01-01
description For study of quantum self-frictional (SF) relativistic nucleoseed spinor-type tensor (NSST) field theory of nature (SF-NSST atomic-molecular-nuclear and cosmic-universe systems) we use the complete orthogonal basis sets of 22s+1-component column-matrices type SF Ψnljmjδ⁎s-relativistic NSST orbitals (Ψδ⁎s-RNSSTO) and SF Xnljmjs-relativistic Slater NSST orbitals (Xs-RSNSSTO) through the ψnlmlδ⁎-nonrelativistic scalar orbitals (ψδ⁎-NSO) and χnlml-nonrelativistic Slater type orbitals (χ-NSTO), respectively. Here δ⁎=pl⁎ or δ⁎=α⁎ and pl⁎=2l+2-α⁎,  α⁎ are the integer (α⁎=α, -∞<α≤2) or noninteger (α⁎≠α, -∞<α⁎<3) SF quantum numbers, where s=0,1/2,1,3/2,2,…. We notice that the nonrelativistic ψδ⁎-NSO and χ-NSTO orbitals themselves are obtained from the relativistic Ψδ⁎s-RNSSTO and Xs-RSNSSTO functions for s=0, respectively. The column-matrices-type SF Y1jmjls-RNSST harmonics (Y1ls-RNSSTH) and Y2jmjls-modified NSSTH (Y2ls-MNSSTH) functions for arbitrary spin s introduced by the author in the previous papers are also used. The one- and two-center one-range addition theorems for ψδ⁎-NSO and noninteger n  χ-NSTO orbitals are presented. The quantum SF relativistic nonperturbative theory for Vnljmjδ⁎-RNSST potentials (Vδ⁎-RNSSTP) and their derivatives is also suggested. To study the transportations of mass and momentum in nature the quantum SF relativistic NSST gravitational photon (gph) with s=1 is introduced.
url http://dx.doi.org/10.1155/2017/6049079
work_keys_str_mv AT iiguseinov quantumselffrictionalrelativisticnucleoseedspinortypetensorfieldtheoryofnature
_version_ 1725595514633715712