Shin'ichi Nojiri

Prof. Shin'ichi Nojiri

Department of Physics, Nagoya University, Nagoya, 464-8602, Japan and Kobayashi-Maskawa Institute for the Origin of Particles and the Universe, Nagoya University, Nagoya 464-8602, Japan
orcid

Research Focus & Metrics

Academic Career Length

43Years (1984-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

View All Publications
1 August 2011 in Physics Reports
Verified
Journal Article
Closed access
Shin'ichi NojiriShin'ichi Nojiri
Shin'ichi Nojiri
SOSergei D. Odintsov
Sergei D. Odintsov

1 February 2007 in International Journal of Geometric Methods in Modern Physics
Verified
Journal Article
Closed access
PDF file
Shin'ichi NojiriShin'ichi Nojiri
Shin'ichi Nojiri
SOSergei D. Odintsov
Sergei D. Odintsov

13 July 2011 in Physical Review D
Verified
Journal Article
Open access
THTiberiu Harko
Tiberiu Harko
Francisco S. N. LoboFrancisco S. N. Lobo
Francisco S. N. Lobo
Shin'ichi NojiriShin'ichi Nojiri
Shin'ichi Nojiri
SOSergei D. Odintsov
Sergei D. Odintsov
We consider f(R,T) modified theories of gravity, where the gravitational Lagrangian is given by an arbitrary function of the Ricci scalar R and of the trace of the stress-energy tensor T. We obtain the gravitational field equations in the metric formalism, as well as the equations of motion for test particles, which follow from the covariant divergence of the stress-energy tensor. Generally, the gravitational field equations depend on the nature of the matter source. The field equations of several particular models, corresponding to some explicit forms of the function f(R,T), are also presented. An important case, which is analyzed in detail, is represented by scalar field models. We write down the action and briefly consider the cosmological implications of the f(R,T$\phi${}) models, where T$\phi${} is the trace of the stress-energy tensor of a self-interacting scalar field. The equations of motion of the test particles are also obtained from a variational principle. The motion of massive test particles is nongeodesic, and takes place in the presence of an extra-force orthogonal to the four velocity. The Newtonian limit of the equation of motion is further analyzed. Finally, we provide a constraint on the magnitude of the extra acceleration by analyzing the perihelion precession of the planet Mercury in the framework of the present model.

15 December 2003 in Physical Review D
Verified
Journal Article
Closed access
PDF file
Shin'ichi NojiriShin'ichi Nojiri
Shin'ichi Nojiri
SOSergei D. Odintsov
Sergei D. Odintsov
A modified gravity, which eliminates the need for dark energy and which seems to be stable, is considered. The terms with positive powers of curvature support the inflationary epoch while the terms with negative powers of curvature serve as effective dark energy, supporting current cosmic acceleration. The equivalent scalar-tensor gravity may be compatible with the simplest solar system experiments.

1 December 2005 in Physics Letters B
Verified
Journal Article
Closed access
Shin'ichi NojiriShin'ichi Nojiri
Shin'ichi Nojiri
SOSergei D. Odintsov
Sergei D. Odintsov

31 March 2005 in Physical Review D
Verified
Journal Article
Closed access
PDF file
Shin'ichi NojiriShin'ichi Nojiri
Shin'ichi Nojiri
SOSergei D. Odintsov
Sergei D. Odintsov
STShinji Tsujikawa
Shinji Tsujikawa
The properties of future singularities are investigated in the universe dominated by dark energy including the phantom-type fluid. We classify the finite-time singularities into four classes and explicitly present the models which give rise to these singularities by assuming the form of the equation of state of dark energy. We show the existence of a stable fixed point with an equation of state w<−1 and numerically confirm that this is actually a late-time attractor in the phantom-dominated universe. We also construct a phantom dark energy scenario coupled to dark matter that reproduces singular behaviors of the Big Rip type for the energy density and the curvature of the universe. The effect of quantum corrections coming from conformal anomaly can be important when the curvature grows large, which typically moderates the finite-time singularities.