Cosmological solutions of a chiral self-gravitating model of F(R, (R)2,R) gravity
Section: ΠΡΠ°Π²ΠΈΡΠ°ΡΠΈΡ, ΠΊΠΎΡΠΌΠΎΠ»ΠΎΠ³ΠΈΡ ΠΈ ΡΡΠ½Π΄Π°ΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΡΠ΅ ΠΏΠΎΠ»Ρ
Article in issue: 2 (47), 2024.
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We study modified π(π , (βπ )2,β‘π ) gravity and show in detail how it can be reduced to Einstein gravity with a few scalar fields and then represented in the form of chiral self-gravitating model of the special type. In further investigation of the model we focus on cosmology and looking for solutions of the dynamic equations of chiral fields and the Einstein-Friedman equations in the Friedman-Robertson-Walker space-time. Exact solutions of the considered model for zero and constant potential are found. Between them power law solution corresponded to equation of state for stiff matter, de Sitter solution, trigonometric and hyperbolic expansion solution. Various type of chiral fields evolution support listed above solutions.
Short address: https://sciup.org/142243253
IDS: 142243253 | UDC: 53.1 | DOI: 10.17238/issn2226-8812.2024.2.4-17
ΠΠΎΡΠΌΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΠ΅ΡΠ΅Π½ΠΈΡ ΠΊΠΈΡΠ°Π»ΡΠ½ΠΎΠΉ ΡΠ°ΠΌΠΎΠ³ΡΠ°Π²ΠΈΡΠΈΡΡΡΡΠ΅ΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ F(R, (R)2,R) Π³ΡΠ°Π²ΠΈΡΠ°ΡΠΈΠΈ
ΠΡ ΠΈΠ·ΡΡΠ°Π΅ΠΌ ΠΌΠΎΠ΄ΠΈΡΠΈΡΠΈΡΠΎΠ²Π°Π½Π½ΡΡ Π³ΡΠ°Π²ΠΈΡΠ°ΡΠΈΡ π(π , (βπ )2,β‘π ) ΠΈ ΠΏΠΎΠ΄ΡΠΎΠ±Π½ΠΎ ΠΏΠΎΠΊΠ°Π·ΡΠ²Π°Π΅ΠΌ, ΠΊΠ°ΠΊ Π΅Π΅ ΠΌΠΎΠΆΠ½ΠΎ ΡΠ²Π΅ΡΡΠΈ ΠΊ ΡΠΉΠ½ΡΡΠ΅ΠΉΠ½ΠΎΠ²ΡΠΊΠΎΠΉ Π³ΡΠ°Π²ΠΈΡΠ°ΡΠΈΠΈ Ρ ΠΏΠΎΠΌΠΎΡΡΡ Π½Π΅ΡΠΊΠΎΠ»ΡΠΊΠΈΡ ΡΠΊΠ°Π»ΡΡΠ½ΡΡ ΠΏΠΎΠ»Π΅ΠΉ, Π° Π·Π°ΡΠ΅ΠΌ ΠΏΡΠ΅Π΄ΡΡΠ°Π²ΠΈΡΡ Π² Π²ΠΈΠ΄Π΅ ΠΊΠΈΡΠ°Π»ΡΠ½ΠΎΠΉ ΡΠ°ΠΌΠΎΠ³ΡΠ°Π²ΠΈΡΠΈΡΡΡΡΠ΅ΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΡΠΏΠ΅ΡΠΈΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΡΠΈΠΏΠ°. Π Π΄Π°Π»ΡΠ½Π΅ΠΉΡΠ΅ΠΌ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΈ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΌΡ ΡΠΎΡΡΠ΅Π΄ΠΎΡΠΎΡΠΈΠΌΡΡ Π½Π° ΠΊΠΎΡΠΌΠΎΠ»ΠΎΠ³ΠΈΠΈ ΠΈ ΠΏΠΎΠΈΡΠΊΠ΅ ΡΠ΅ΡΠ΅Π½ΠΈΠΉ Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ ΠΊΠΈΡΠ°Π»ΡΠ½ΡΡ ΠΏΠΎΠ»Π΅ΠΉ ΠΈ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ ΠΠΉΠ½ΡΡΠ΅ΠΉΠ½Π°-Π€ΡΠΈΠ΄ΠΌΠ°Π½Π° Π² ΠΏΡΠΎΡΡΡΠ°Π½ΡΡΠ²Π΅-Π²ΡΠ΅ΠΌΠ΅Π½ΠΈ Π€ΡΠΈΠ΄ΠΌΠ°Π½Π°-Π ΠΎΠ±Π΅ΡΡΡΠΎΠ½Π°-Π£ΠΎΠΊΠ΅ΡΠ°. ΠΠ°ΠΉΠ΄Π΅Π½Ρ ΡΠΎΡΠ½ΡΠ΅ ΡΠ΅ΡΠ΅Π½ΠΈΡ ΡΠ°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°Π΅ΠΌΠΎΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ Π΄Π»Ρ Π½ΡΠ»Π΅Π²ΠΎΠ³ΠΎ ΠΈ ΠΏΠΎΡΡΠΎΡΠ½Π½ΠΎΠ³ΠΎ ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»Π°. ΠΠ΅ΠΆΠ΄Ρ Π½ΠΈΠΌΠΈ ΡΡΠ΅ΠΏΠ΅Π½Π½ΠΎΠ΅ ΡΠ΅ΡΠ΅Π½ΠΈΠ΅, ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΡΡΡΠ΅Π΅ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ ΡΠΎΡΡΠΎΡΠ½ΠΈΡ ΠΡΠ΅Π»Π΅Π½Π½ΠΎΠΉ Ρ ΠΏΡΠ΅ΠΎΠ±Π»Π°Π΄Π°Π½ΠΈΠ΅ΠΌ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ, ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ Π΄Π΅ Π‘ΠΈΡΡΠ΅ΡΠ°, ΡΡΠΈΠ³ΠΎΠ½ΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΠΈ Π³ΠΈΠΏΠ΅ΡΠ±ΠΎΠ»ΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ Ρ ΡΠ°ΡΡΠΈΡΠ΅Π½ΠΈΠ΅ΠΌ. Π Π°Π·Π»ΠΈΡΠ½ΡΠ΅ ΡΠΈΠΏΡ ΡΠ²ΠΎΠ»ΡΡΠΈΠΈ ΠΊΠΈΡΠ°Π»ΡΠ½ΡΡ ΠΏΠΎΠ»Π΅ΠΉ ΠΏΠΎΠ΄Π΄Π΅ΡΠΆΠΈΠ²Π°ΡΡ ΠΏΠ΅ΡΠ΅ΡΠΈΡΠ»Π΅Π½Π½ΡΠ΅ Π²ΡΡΠ΅ ΡΠ΅ΡΠ΅Π½ΠΈΡ.
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