Solutions to Yang-Mills Equations on Four-Dimensional de Sitter Space

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Original languageEnglish
Article number061601
JournalPhysical review letters
Volume119
Issue number6
Publication statusPublished - 11 Aug 2017

Abstract

We consider pure SU(2) Yang-Mills theory on four-dimensional de Sitter space dS4 and construct a smooth and spatially homogeneous magnetic solution to the Yang-Mills equations. Slicing dS4 as R×S3, via an SU(2)-equivariant ansatz, we reduce the Yang-Mills equations to ordinary matrix differential equations and further to Newtonian dynamics in a double-well potential. Its local maximum yields a Yang-Mills solution whose color-magnetic field at time τR is given by Ba=-12Ia/(R2cosh2τ), where Ia for a=1, 2, 3 are the SU(2) generators and R is the de Sitter radius. At any moment, this spatially homogeneous configuration has finite energy, but its action is also finite and of the value -12j(j+1)(2j+1)π3 in a spin-j representation. Similarly, the double-well bounce produces a family of homogeneous finite-action electric-magnetic solutions with the same energy. There is a continuum of other solutions whose energy and action extend down to zero.

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Solutions to Yang-Mills Equations on Four-Dimensional de Sitter Space. / Ivanova, Tatiana A.; Lechtenfeld, Olaf; Popov, Alexander D.
In: Physical review letters, Vol. 119, No. 6, 061601, 11.08.2017.

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Ivanova TA, Lechtenfeld O, Popov AD. Solutions to Yang-Mills Equations on Four-Dimensional de Sitter Space. Physical review letters. 2017 Aug 11;119(6):061601. doi: 10.1103/PhysRevLett.119.061601
Ivanova, Tatiana A. ; Lechtenfeld, Olaf ; Popov, Alexander D. / Solutions to Yang-Mills Equations on Four-Dimensional de Sitter Space. In: Physical review letters. 2017 ; Vol. 119, No. 6.
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abstract = "We consider pure SU(2) Yang-Mills theory on four-dimensional de Sitter space dS4 and construct a smooth and spatially homogeneous magnetic solution to the Yang-Mills equations. Slicing dS4 as R×S3, via an SU(2)-equivariant ansatz, we reduce the Yang-Mills equations to ordinary matrix differential equations and further to Newtonian dynamics in a double-well potential. Its local maximum yields a Yang-Mills solution whose color-magnetic field at time τR is given by Ba=-12Ia/(R2cosh2τ), where Ia for a=1, 2, 3 are the SU(2) generators and R is the de Sitter radius. At any moment, this spatially homogeneous configuration has finite energy, but its action is also finite and of the value -12j(j+1)(2j+1)π3 in a spin-j representation. Similarly, the double-well bounce produces a family of homogeneous finite-action electric-magnetic solutions with the same energy. There is a continuum of other solutions whose energy and action extend down to zero.",
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AU - Ivanova, Tatiana A.

AU - Lechtenfeld, Olaf

AU - Popov, Alexander D.

N1 - Publisher Copyright: © 2017 American Physical Society. Copyright: Copyright 2017 Elsevier B.V., All rights reserved.

PY - 2017/8/11

Y1 - 2017/8/11

N2 - We consider pure SU(2) Yang-Mills theory on four-dimensional de Sitter space dS4 and construct a smooth and spatially homogeneous magnetic solution to the Yang-Mills equations. Slicing dS4 as R×S3, via an SU(2)-equivariant ansatz, we reduce the Yang-Mills equations to ordinary matrix differential equations and further to Newtonian dynamics in a double-well potential. Its local maximum yields a Yang-Mills solution whose color-magnetic field at time τR is given by Ba=-12Ia/(R2cosh2τ), where Ia for a=1, 2, 3 are the SU(2) generators and R is the de Sitter radius. At any moment, this spatially homogeneous configuration has finite energy, but its action is also finite and of the value -12j(j+1)(2j+1)π3 in a spin-j representation. Similarly, the double-well bounce produces a family of homogeneous finite-action electric-magnetic solutions with the same energy. There is a continuum of other solutions whose energy and action extend down to zero.

AB - We consider pure SU(2) Yang-Mills theory on four-dimensional de Sitter space dS4 and construct a smooth and spatially homogeneous magnetic solution to the Yang-Mills equations. Slicing dS4 as R×S3, via an SU(2)-equivariant ansatz, we reduce the Yang-Mills equations to ordinary matrix differential equations and further to Newtonian dynamics in a double-well potential. Its local maximum yields a Yang-Mills solution whose color-magnetic field at time τR is given by Ba=-12Ia/(R2cosh2τ), where Ia for a=1, 2, 3 are the SU(2) generators and R is the de Sitter radius. At any moment, this spatially homogeneous configuration has finite energy, but its action is also finite and of the value -12j(j+1)(2j+1)π3 in a spin-j representation. Similarly, the double-well bounce produces a family of homogeneous finite-action electric-magnetic solutions with the same energy. There is a continuum of other solutions whose energy and action extend down to zero.

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