Cosmological solutions of a chiral self-gravitating model of F(R, (R)2,R) gravity

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We study modified 𝑓(𝑅, (βˆ‡π‘…)2,░𝑅) 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.

chiral cosmological model \ scalar-tensor and 𝑓(𝑅) gravity theory

Short address: https://sciup.org/142243253

IDS: 142243253   |   UDC: 53.1   |   DOI: 10.17238/issn2226-8812.2024.2.4-17

ΠšΠΎΡΠΌΠΎΠ»ΠΎΠ³ΠΈΡ‡Π΅ΡΠΊΠΈΠ΅ Ρ€Π΅ΡˆΠ΅Π½ΠΈΡ ΠΊΠΈΡ€Π°Π»ΡŒΠ½ΠΎΠΉ ΡΠ°ΠΌΠΎΠ³Ρ€Π°Π²ΠΈΡ‚ΠΈΡ€ΡƒΡŽΡ‰Π΅ΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ F(R, (R)2,R) Π³Ρ€Π°Π²ΠΈΡ‚Π°Ρ†ΠΈΠΈ

ΠœΡ‹ ΠΈΠ·ΡƒΡ‡Π°Π΅ΠΌ ΠΌΠΎΠ΄ΠΈΡ„ΠΈΡ†ΠΈΡ€ΠΎΠ²Π°Π½Π½ΡƒΡŽ Π³Ρ€Π°Π²ΠΈΡ‚Π°Ρ†ΠΈΡŽ 𝑓(𝑅, (βˆ‡π‘…)2,░𝑅) ΠΈ ΠΏΠΎΠ΄Ρ€ΠΎΠ±Π½ΠΎ ΠΏΠΎΠΊΠ°Π·Ρ‹Π²Π°Π΅ΠΌ, ΠΊΠ°ΠΊ Π΅Π΅ ΠΌΠΎΠΆΠ½ΠΎ свСсти ΠΊ ΡΠΉΠ½ΡˆΡ‚Π΅ΠΉΠ½ΠΎΠ²ΡΠΊΠΎΠΉ Π³Ρ€Π°Π²ΠΈΡ‚Π°Ρ†ΠΈΠΈ с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ Π½Π΅ΡΠΊΠΎΠ»ΡŒΠΊΠΈΡ… скалярных ΠΏΠΎΠ»Π΅ΠΉ, Π° Π·Π°Ρ‚Π΅ΠΌ ΠΏΡ€Π΅Π΄ΡΡ‚Π°Π²ΠΈΡ‚ΡŒ Π² Π²ΠΈΠ΄Π΅ ΠΊΠΈΡ€Π°Π»ΡŒΠ½ΠΎΠΉ ΡΠ°ΠΌΠΎΠ³Ρ€Π°Π²ΠΈΡ‚ΠΈΡ€ΡƒΡŽΡ‰Π΅ΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΡΠΏΠ΅Ρ†ΠΈΠ°Π»ΡŒΠ½ΠΎΠ³ΠΎ Ρ‚ΠΈΠΏΠ°. Π’ дальнСйшСм исслСдовании ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΌΡ‹ сосрСдоточимся Π½Π° космологии ΠΈ поискС Ρ€Π΅ΡˆΠ΅Π½ΠΈΠΉ динамичСских ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠΉ ΠΊΠΈΡ€Π°Π»ΡŒΠ½Ρ‹Ρ… ΠΏΠΎΠ»Π΅ΠΉ ΠΈ ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠΉ Π­ΠΉΠ½ΡˆΡ‚Π΅ΠΉΠ½Π°-Π€Ρ€ΠΈΠ΄ΠΌΠ°Π½Π° Π² пространствС-Π²Ρ€Π΅ΠΌΠ΅Π½ΠΈ Π€Ρ€ΠΈΠ΄ΠΌΠ°Π½Π°-РобСртсона-Π£ΠΎΠΊΠ΅Ρ€Π°. НайдСны Ρ‚ΠΎΡ‡Π½Ρ‹Π΅ Ρ€Π΅ΡˆΠ΅Π½ΠΈΡ рассматриваСмой ΠΌΠΎΠ΄Π΅Π»ΠΈ для Π½ΡƒΠ»Π΅Π²ΠΎΠ³ΠΎ ΠΈ постоянного ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»Π°. ΠœΠ΅ΠΆΠ΄Ρƒ Π½ΠΈΠΌΠΈ стСпСнноС Ρ€Π΅ΡˆΠ΅Π½ΠΈΠ΅, ΡΠΎΠΎΡ‚Π²Π΅Ρ‚ΡΡ‚Π²ΡƒΡŽΡ‰Π΅Π΅ ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΡŽ состояния ВсСлСнной с ΠΏΡ€Π΅ΠΎΠ±Π»Π°Π΄Π°Π½ΠΈΠ΅ΠΌ излучСния, Ρ€Π΅ΡˆΠ΅Π½ΠΈΠ΅ Π΄Π΅ Π‘ΠΈΡ‚Ρ‚Π΅Ρ€Π°, тригономСтричСскоС ΠΈ гипСрболичСскоС Ρ€Π΅ΡˆΠ΅Π½ΠΈΠ΅ с Ρ€Π°ΡΡˆΠΈΡ€Π΅Π½ΠΈΠ΅ΠΌ. Π Π°Π·Π»ΠΈΡ‡Π½Ρ‹Π΅ Ρ‚ΠΈΠΏΡ‹ ΡΠ²ΠΎΠ»ΡŽΡ†ΠΈΠΈ ΠΊΠΈΡ€Π°Π»ΡŒΠ½Ρ‹Ρ… ΠΏΠΎΠ»Π΅ΠΉ ΠΏΠΎΠ΄Π΄Π΅Ρ€ΠΆΠΈΠ²Π°ΡŽΡ‚ пСрСчислСнныС Π²Ρ‹ΡˆΠ΅ Ρ€Π΅ΡˆΠ΅Π½ΠΈΡ.

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