scholarly journals Modified Friedmann equation and survey of solutions in effective Bianchi-I loop quantum cosmology

2013 ◽  
Vol 31 (1) ◽  
pp. 015018 ◽  
Author(s):  
Linda Linsefors ◽  
Aurelien Barrau
2020 ◽  
Vol 35 (29) ◽  
pp. 2050185
Author(s):  
You Ding ◽  
Xiangdong Zhang

We study the anisotropic Bianchi I loop quantum cosmology in [Formula: see text] dimensions. The [Formula: see text] scheme is considered in the present paper and the following expected results are established: (i) the massless scalar field again play the role of emergent time variables and serves as an internal clock; (ii) by imposing the fundamental discreteness of length operator, the total Hamiltonian constraint is obtained and gives rise the evolution as a difference equation; and (iii) the exact solutions of Friedmann equation are constructed rigorously for both classical and effective level. The investigation extends the domain of validity of loop quantum cosmology to beyond the four dimensions.


2009 ◽  
Vol 2009 ◽  
pp. 1-9 ◽  
Author(s):  
Li-Fang Li ◽  
Jian-Yang Zhu

Loop quantum cosmology (LQC) is very powerful to deal with the behavior of early universe. Moreover, the effective loop quantum cosmology gives a successful description of the universe in the semiclassical region. We consider the apparent horizon of the Friedmann-Robertson-Walker universe as a thermodynamical system and investigate the thermodynamics of LQC in the semiclassical region. The effective density and effective pressure in the modified Friedmann equation from LQC not only determine the evolution of the universe in LQC scenario but also are actually found to be the thermodynamic quantities. This result comes from the energy definition in cosmology (the Misner-Sharp gravitational energy) and is consistent with thermodynamic laws. We prove that within the framework of loop quantum cosmology, the elementary equation of equilibrium thermodynamics is still valid.


2020 ◽  
Vol 101 (2) ◽  
Author(s):  
Alejandro García-Quismondo ◽  
Guillermo A. Mena Marugán

2012 ◽  
Vol 360 ◽  
pp. 012031 ◽  
Author(s):  
M Martín-Benito ◽  
L J Garay ◽  
G A Mena Marugán ◽  
E Wilson-Ewing

2009 ◽  
Vol 80 (8) ◽  
Author(s):  
Mercedes Martín-Benito ◽  
Guillermo A. Mena Marugán ◽  
Tomasz Pawlowski

2010 ◽  
Vol 25 (26) ◽  
pp. 4993-5007 ◽  
Author(s):  
KUI XIAO ◽  
JIAN-YANG ZHU

The dynamical behaviors of interacting dark energy in loop quantum cosmology are discussed in this paper. Based on three defined dimensionless variables, we simplify the equations of the fixed points. The fixed points for interacting dark energy can be determined by the Friedmann equation coupled with the dynamical equations in Einstein cosmology. But in loop quantum cosmology, besides the Friedmann equation, the conversation equation also gives a constrain on the fixed points. The difference of stability properties for the fixed points in loop quantum cosmology and the ones in Einstein cosmology are also discussed.


2011 ◽  
Vol 28 (8) ◽  
pp. 085020 ◽  
Author(s):  
Przemysław Małkiewicz ◽  
Włodzimierz Piechocki ◽  
Piotr Dzierżak

2021 ◽  
Vol 81 (11) ◽  
Author(s):  
Marcello Miranda ◽  
Daniele Vernieri ◽  
Salvatore Capozziello ◽  
Francisco S. N. Lobo

AbstractLoop quantum cosmology (LQC) is a theory which renders the Big Bang initial singularity into a quantum bounce, by means of short-range repulsive quantum effects at the Planck scale. In this work, we are interested in reproducing the effective Friedmann equation of LQC, by considering a generic f(R, P, Q) theory of gravity, where $$R=g^{\mu \nu }R_{\mu \nu }$$ R = g μ ν R μ ν is the Ricci scalar, $$P=R_{\mu \nu }R^{\mu \nu }$$ P = R μ ν R μ ν , and $$Q=R_{\alpha \beta \mu \nu }R^{\alpha \beta \mu \nu }$$ Q = R α β μ ν R α β μ ν is the Kretschmann scalar. An order reduction technique allows us to work in f(R, P, Q) theories which are perturbatively close to General Relativity, and to deduce a modified Friedmann equation in the reduced theory. Requiring that the modified Friedmann equation mimics the effective Friedmann equation of LQC, we are able to derive several functional forms of f(R, P, Q). We discuss the necessary conditions to obtain viable bouncing cosmologies for the proposed effective actions of f(R, P, Q) theory of gravity.


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