Han-Ying Guo
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The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
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Han-Ying Guo has a total of 39 co-authors. Here are the top co-authors by number of shared publications:
- Ke Wu
Institute of Theoretical Physics Academia Sinica P.O.Box 2735 100080 Beijing China
8 shared publications - Chao-Guang Huang
Institute of High Energy Physics Chinese Academy of Sciences P.O. Box 918-4 100049 Beijing China
7 shared publications - Bin Zhou
Beijing Normal University
4 shared publications Hong-Tu Wu
Department of Mathematics Capital Normal University 100048 Beijing China, and
4 shared publicationsBin Zhou
Beijing Normal University
3 shared publications- Bin Zhou
Department of Physics Beijing Normal University Beijing 100875 P. R. China
3 shared publications
Latest Publications
- Open Access
Poincaré-De Sitter Flow and Cosmological Meaning
We introduce the Poincar\'e-de Sitter flow with real numbers $\{r,s\}$ to parameterize the relativistic quadruple ${\frak Q}_{PoR}=[{\cal P}, {\cal P}_2, {\cal D}_+,{\cal D}_-]_{M/M_\pm/D_\pm}$ for the triple of Poincar\'e/\dS/\AdS\ group ${\cal P}/{\cal D}_+/{\cal D}_-$ invariant special relativity. The dual Poincar\'e group ${\cal P}_2$-invariant degenerated Einstein manifold $M_\pm$ of $\Lambda_\pm=\pm3l^{-2}$ is for the space/time-like domain $\dot R_\pm$ of the compact lightcone $\bar C_O$ associated to the common space/time-like region $R_\pm$ of the lightcone $C_O$ at common origin on Minkowski/\dS/\AdS\ spacetime $M/D_+/D_-$. Based on the principle of relativity with two universal constants $(c, l)$, there are the law of inertia, coordinate time simultaneity and so on for the flow on a Poincar\'e-\dS\ symmetric Einstein manifold of $\Lambda_{s}=3{s}l^{-2}$. Further, there is Robertson-Walker-like cosmos of the flow for the propertime simultaneity. The \dS\ special relativity with double $[{\cal D}_+,{\cal P}_2]_{D_+/M_+}$ can provide a consistent kinematics for the cosmic scale physics with an upper entropy bound $S_R=k_B\pi g^{-2}, g^2:=(\ell_P/R)^2 \simeq 10^{-122}$, for $R\simeq (3/\Lambda)^{1/2}\sim 13.7 Gly$.Open AccessPoincaré-De Sitter Flow and Cosmological Meaning
We introduce the Poincar\'e-de Sitter flow with real numbers $\{r,s\}$ to parameterize the relativistic quadruple ${\frak Q}_{PoR}=[{\cal P}, {\cal P}_2, {\cal D}_+,{\cal D}_-]_{M/M_\pm/D_\pm}$ for the triple of Poincar\'e/\dS/\AdS\ group ${\cal P}/{\cal D}_+/{\cal D}_-$ invariant special relativity. The dual Poincar\'e group ${\cal P}_2$-invariant degenerated Einstein manifold $M_\pm$ of $\Lambda_\pm=\pm3l^{-2}$ is for the space/time-like domain $\dot R_\pm$ of the compact lightcone $\bar C_O$ associated to the common space/time-like region $R_\pm$ of the lightcone $C_O$ at common origin on Minkowski/\dS/\AdS\ spacetime $M/D_+/D_-$. Based on the principle of relativity with two universal constants $(c, l)$, there are the law of inertia, coordinate time simultaneity and so on for the flow on a Poincar\'e-\dS\ symmetric Einstein manifold of $\Lambda_{s}=3{s}l^{-2}$. Further, there is Robertson-Walker-like cosmos of the flow for the propertime simultaneity. The \dS\ special relativity with double $[{\cal D}_+,{\cal P}_2]_{D_+/M_+}$ can provide a consistent kinematics for the cosmic scale physics with an upper entropy bound $S_R=k_B\pi g^{-2}, g^2:=(\ell_P/R)^2 \simeq 10^{-122}$, for $R\simeq (3/\Lambda)^{1/2}\sim 13.7 Gly$. - 27 March 2010
- Published by Springer Nature in Science China Physics, Mechanics & Astronomy
- Vol. 53 (4) , 591-597
The principle of relativity, kinematics and algebraic relations
- 27 March 2010
- Published by Springer Nature in Science China Physics, Mechanics & Astronomy
- Vol. 53 (4) , 591-597
The principle of relativity, kinematics and algebraic relations
- Open Access
The Principle of Relativity and Special Relativity Triple
Based on the principle of relativity and the postulate on universal invariant constants ($c,l$) as well as Einstein's isotropy conditions, three kinds of special relativity form a triple with a common Lorentz group as isotropy group under full Umov-Weyl-Fock-Lorentz transformations among inertial motions.
Open AccessThe Principle of Relativity and Special Relativity Triple
Based on the principle of relativity and the postulate on universal invariant constants ($c,l$) as well as Einstein's isotropy conditions, three kinds of special relativity form a triple with a common Lorentz group as isotropy group under full Umov-Weyl-Fock-Lorentz transformations among inertial motions.
- Open Access
The Principle of Relativity, Kinematics and Algebraic Relations
Based on the principle of relativity and the postulate on universal invariant constants (c,l), all possible kinematics can be set up with sub-symmetries of the Umov-Weyl-Fock transformations for the inertial motions. Further, in the combinatory approach, all these symmetries are intrinsically related to each other, e.g. to the very important dS kinematics for the cosmic scale physics.
Open AccessThe Principle of Relativity, Kinematics and Algebraic Relations
Based on the principle of relativity and the postulate on universal invariant constants (c,l), all possible kinematics can be set up with sub-symmetries of the Umov-Weyl-Fock transformations for the inertial motions. Further, in the combinatory approach, all these symmetries are intrinsically related to each other, e.g. to the very important dS kinematics for the cosmic scale physics.
- Open Access
Yang's Model as Triply Special Relativity and the Snyder's Model--de Sitter Special Relativity Duality
We show that if Yang's model as the earliest TSR is completed, it should contain both Snyder's quantized space-time model as the earliest DSR, the de Sitter SR and their duality.
Open AccessYang's Model as Triply Special Relativity and the Snyder's Model--de Sitter Special Relativity Duality
We show that if Yang's model as the earliest TSR is completed, it should contain both Snyder's quantized space-time model as the earliest DSR, the de Sitter SR and their duality.
- 8 April 2008
- Published by Springer Nature in Science China Mathematics
- Vol. 51 (4) , 568-603
Special relativity and theory of gravity via maximum symmetry and localization
- 8 April 2008
- Published by Springer Nature in Science China Mathematics
- Vol. 51 (4) , 568-603
Special relativity and theory of gravity via maximum symmetry and localization
- Open Access
On Principle of Inertia in Closed Universe
If our universe is asymptotic to a de Sitter space, it should be closed with curvature in $O(\Lambda)$ in view of dS special relativity. Conversely, its evolution can fix on Beltrami systems of inertia in the dS-space without Einstein's `argument in a circle'. Gravity should be local dS-invariant based on localization of the principle of inertia.Open AccessOn Principle of Inertia in Closed Universe
If our universe is asymptotic to a de Sitter space, it should be closed with curvature in $O(\Lambda)$ in view of dS special relativity. Conversely, its evolution can fix on Beltrami systems of inertia in the dS-space without Einstein's `argument in a circle'. Gravity should be local dS-invariant based on localization of the principle of inertia. - 1 September 2007
- Published by Elsevier in Physics Letters B
- Vol. 653 (1) , 88-94
On principle of inertia in closed universe
- 1 September 2007
- Published by Elsevier in Physics Letters B
- Vol. 653 (1) , 88-94
On principle of inertia in closed universe
- Open Access
Snyder's Model -- de Sitter Special Relativity Duality and de Sitter Gravity
Between Snyder's quantized space-time model in de Sitter space of momenta and the \dS special relativity on \dS-spacetime of radius $R$ with Beltrami coordinates, there is a one-to-one dual correspondence supported by a minimum uncertainty-like argument. Together with Planck length $\ell_P$, $R\simeq (3/\Lambda)^{1/2}$ should be a fundamental constant. They lead to a dimensionless constant $g{\sim\ell_PR^{-1}}=(G\hbar c^{-3}\Lambda/3)^{1/2}\sim 10^{-61}$. These indicate that physics at these two scales should be dual to each other and there is in-between gravity of local \dS-invariance characterized by $g$. A simple model of \dS-gravity with a gauge-like action on umbilical manifolds may show these characters. It can pass the observation tests and support the duality.Open AccessSnyder's Model -- de Sitter Special Relativity Duality and de Sitter Gravity
Between Snyder's quantized space-time model in de Sitter space of momenta and the \dS special relativity on \dS-spacetime of radius $R$ with Beltrami coordinates, there is a one-to-one dual correspondence supported by a minimum uncertainty-like argument. Together with Planck length $\ell_P$, $R\simeq (3/\Lambda)^{1/2}$ should be a fundamental constant. They lead to a dimensionless constant $g{\sim\ell_PR^{-1}}=(G\hbar c^{-3}\Lambda/3)^{1/2}\sim 10^{-61}$. These indicate that physics at these two scales should be dual to each other and there is in-between gravity of local \dS-invariance characterized by $g$. A simple model of \dS-gravity with a gauge-like action on umbilical manifolds may show these characters. It can pass the observation tests and support the duality. - 31 July 2007
- Published by IOP Publishing in Classical and Quantum Gravity
- Vol. 24 (16) , 4009-4035
Snyder's model—de Sitter special relativity duality and de Sitter gravity
Between Snyder's quantized space-time model in de Sitter space of momenta and the dS special relativity on dS-spacetime of radius $R$ with Beltrami coordinates, there is a one-to-one dual correspondence supported by a minimum uncertainty-like argument. Together with Planck length $ell_P$, $Rsimeq (3/Lambda)^{1/2}$ should be a fundamental constant. They lead to a dimensionless constant $g{simell_PR^{-1}}=(Ghbar c^{-3}Lambda/3)^{1/2}sim 10^{-61}$. These indicate that physics at these two scales should be dual to each other and there is in-between gravity of local dS-invariance characterized by $g$. A simple model of dS-gravity with a gauge-like action on umbilical manifolds may show these characters. It can pass the observation tests and support the duality.- 31 July 2007
- Published by IOP Publishing in Classical and Quantum Gravity
- Vol. 24 (16) , 4009-4035
Snyder's model—de Sitter special relativity duality and de Sitter gravity
Between Snyder's quantized space-time model in de Sitter space of momenta and the dS special relativity on dS-spacetime of radius $R$ with Beltrami coordinates, there is a one-to-one dual correspondence supported by a minimum uncertainty-like argument. Together with Planck length $ell_P$, $Rsimeq (3/Lambda)^{1/2}$ should be a fundamental constant. They lead to a dimensionless constant $g{simell_PR^{-1}}=(Ghbar c^{-3}Lambda/3)^{1/2}sim 10^{-61}$. These indicate that physics at these two scales should be dual to each other and there is in-between gravity of local dS-invariance characterized by $g$. A simple model of dS-gravity with a gauge-like action on umbilical manifolds may show these characters. It can pass the observation tests and support the duality.