Metric-Affine Version of Myrzakulov <em>F</em>(<em>R</em>,<em>T</em>,<em>Q</em>,<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi mathvariant="script">T</mi></semantics></math></inline-formula>) Gravity and Cosmological Applications
We derive the full set of field equations for the metric-affine version of the Myrzakulov gravity model and also extend this family of theories to a broader one. More specifically, we consider theories whose gravitational Lagrangian is given by <inline-formula><math xmlns="http://www.w...
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doaj-eeaf25bf361640589ec11d9a0bb22dd22021-08-26T14:25:16ZengMDPI AGUniverse2218-19972021-07-01726226210.3390/universe7080262Metric-Affine Version of Myrzakulov <em>F</em>(<em>R</em>,<em>T</em>,<em>Q</em>,<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi mathvariant="script">T</mi></semantics></math></inline-formula>) Gravity and Cosmological ApplicationsDamianos Iosifidis0Nurgissa Myrzakulov1Ratbay Myrzakulov2Institute of Theoretical Physics, Department of Physics, Aristotle University of Thessaloniki, 54124 Thessaloniki, GreeceInstitute of Theoretical Physics, Department of Physics, Aristotle University of Thessaloniki, 54124 Thessaloniki, GreeceInstitute of Theoretical Physics, Department of Physics, Aristotle University of Thessaloniki, 54124 Thessaloniki, GreeceWe derive the full set of field equations for the metric-affine version of the Myrzakulov gravity model and also extend this family of theories to a broader one. More specifically, we consider theories whose gravitational Lagrangian is given by <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>F</mi><mo>(</mo><mi>R</mi><mo>,</mo><mi>T</mi><mo>,</mo><mi>Q</mi><mo>,</mo><mi mathvariant="script">T</mi><mo>,</mo><mi mathvariant="script">D</mi><mo>)</mo></mrow></semantics></math></inline-formula> where <i>T</i>, <i>Q</i> are the torsion and non-metricity scalars, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi mathvariant="script">T</mi></semantics></math></inline-formula> is the trace of the energy-momentum tensor and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi mathvariant="script">D</mi></semantics></math></inline-formula> the divergence of the dilation current. We then consider the linear case of the aforementioned theory and, assuming a cosmological setup, we obtain the modified Friedmann equations. In addition, focusing on the vanishing non-metricity sector and considering matter coupled to torsion, we obtain the complete set of equations describing the cosmological behavior of this model along with solutions.https://www.mdpi.com/2218-1997/7/8/262cosmologytorsion |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Damianos Iosifidis Nurgissa Myrzakulov Ratbay Myrzakulov |
spellingShingle |
Damianos Iosifidis Nurgissa Myrzakulov Ratbay Myrzakulov Metric-Affine Version of Myrzakulov <em>F</em>(<em>R</em>,<em>T</em>,<em>Q</em>,<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi mathvariant="script">T</mi></semantics></math></inline-formula>) Gravity and Cosmological Applications Universe cosmology torsion |
author_facet |
Damianos Iosifidis Nurgissa Myrzakulov Ratbay Myrzakulov |
author_sort |
Damianos Iosifidis |
title |
Metric-Affine Version of Myrzakulov <em>F</em>(<em>R</em>,<em>T</em>,<em>Q</em>,<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi mathvariant="script">T</mi></semantics></math></inline-formula>) Gravity and Cosmological Applications |
title_short |
Metric-Affine Version of Myrzakulov <em>F</em>(<em>R</em>,<em>T</em>,<em>Q</em>,<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi mathvariant="script">T</mi></semantics></math></inline-formula>) Gravity and Cosmological Applications |
title_full |
Metric-Affine Version of Myrzakulov <em>F</em>(<em>R</em>,<em>T</em>,<em>Q</em>,<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi mathvariant="script">T</mi></semantics></math></inline-formula>) Gravity and Cosmological Applications |
title_fullStr |
Metric-Affine Version of Myrzakulov <em>F</em>(<em>R</em>,<em>T</em>,<em>Q</em>,<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi mathvariant="script">T</mi></semantics></math></inline-formula>) Gravity and Cosmological Applications |
title_full_unstemmed |
Metric-Affine Version of Myrzakulov <em>F</em>(<em>R</em>,<em>T</em>,<em>Q</em>,<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi mathvariant="script">T</mi></semantics></math></inline-formula>) Gravity and Cosmological Applications |
title_sort |
metric-affine version of myrzakulov <em>f</em>(<em>r</em>,<em>t</em>,<em>q</em>,<inline-formula><math xmlns="http://www.w3.org/1998/math/mathml" display="inline"><semantics><mi mathvariant="script">t</mi></semantics></math></inline-formula>) gravity and cosmological applications |
publisher |
MDPI AG |
series |
Universe |
issn |
2218-1997 |
publishDate |
2021-07-01 |
description |
We derive the full set of field equations for the metric-affine version of the Myrzakulov gravity model and also extend this family of theories to a broader one. More specifically, we consider theories whose gravitational Lagrangian is given by <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>F</mi><mo>(</mo><mi>R</mi><mo>,</mo><mi>T</mi><mo>,</mo><mi>Q</mi><mo>,</mo><mi mathvariant="script">T</mi><mo>,</mo><mi mathvariant="script">D</mi><mo>)</mo></mrow></semantics></math></inline-formula> where <i>T</i>, <i>Q</i> are the torsion and non-metricity scalars, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi mathvariant="script">T</mi></semantics></math></inline-formula> is the trace of the energy-momentum tensor and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi mathvariant="script">D</mi></semantics></math></inline-formula> the divergence of the dilation current. We then consider the linear case of the aforementioned theory and, assuming a cosmological setup, we obtain the modified Friedmann equations. In addition, focusing on the vanishing non-metricity sector and considering matter coupled to torsion, we obtain the complete set of equations describing the cosmological behavior of this model along with solutions. |
topic |
cosmology torsion |
url |
https://www.mdpi.com/2218-1997/7/8/262 |
work_keys_str_mv |
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