Gauge theory of massless spin-(3/2) field in de Sitter space-time

  • On several levels of theoretical physics, especially particle physics and early universe cosmology, de Sitter space-time has become an attractive possibility. The principle of local gauge invariance governs all known fundamental interactions of elementary particles, from electromagnetism and weak interactions to strong interactions and gravity. This paper presents a procedure for defining the gauge-covariant derivative and gauge invariant Lagrangian density in de Sitter ambient space-time formalism. The gauge invariant field equation is then explicitly calculated in detail for a massless spin-(3/2) gauge field.
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S. Parsamehr and M. Mohsenzadeh. Gauge theory of massless spin-(3/2) field in de Sitter space-time[J]. Chinese Physics C, 2016, 40(11): 113102. doi: 10.1088/1674-1137/40/11/113102
S. Parsamehr and M. Mohsenzadeh. Gauge theory of massless spin-(3/2) field in de Sitter space-time[J]. Chinese Physics C, 2016, 40(11): 113102.  doi: 10.1088/1674-1137/40/11/113102 shu
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Received: 2016-05-26
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Gauge theory of massless spin-(3/2) field in de Sitter space-time

    Corresponding author: S. Parsamehr, sajad.parsamehr@srbiau.ac.ir
    Corresponding author: M. Mohsenzadeh, sajad.parsamehr@srbiau.ac.ir
  • 1.  Department of Physics, Science and Research Branch, Islamic Azad University, Tehran, Iran
  • 2.  Department of Physics, Qom Branch, Islamic Azad University, Qom, Iran

Abstract: On several levels of theoretical physics, especially particle physics and early universe cosmology, de Sitter space-time has become an attractive possibility. The principle of local gauge invariance governs all known fundamental interactions of elementary particles, from electromagnetism and weak interactions to strong interactions and gravity. This paper presents a procedure for defining the gauge-covariant derivative and gauge invariant Lagrangian density in de Sitter ambient space-time formalism. The gauge invariant field equation is then explicitly calculated in detail for a massless spin-(3/2) gauge field.

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