Bulletin of the American Physical Society
75th Annual Meeting of the Division of Fluid Dynamics
Volume 67, Number 19
Sunday–Tuesday, November 20–22, 2022; Indiana Convention Center, Indianapolis, Indiana.
Session G19: General Fluid Dynamics I
3:00 PM–4:05 PM,
Sunday, November 20, 2022
Room: 205
Chair: Haithem Taha, UC Irvine
Abstract: G19.00003 : The Generalized Newton's Laws (GNL) - A Complete Conformal Field Theory of Quantum Gravity
3:26 PM–3:39 PM
Presenter:
Zhi an Luan
(University of British Columbia)
Author:
Zhi an Luan
(University of British Columbia)
Collaboration:
Zhi-An Luan
(1). Theorem 1.
Let SL be the Liouville Action functional, in the case of the Riemann sphere, there exists a metric as: eγφ(z) |dz|2 and the law of φ is:
ν(dφ) = e-SL ν0(dφ). (1)
then we can prove that this law is an isomorphism manifold with the Heat Kernel in the Unitary Space-Time of the GNL such as:
Ker= e-x∗x/(2t)/√2πt. Hence these two CFT theories are an isomorphism map, in topological structures, specially.
(2). Theorem 2.
The LCFT has two parameters γ and μ, is characterized by its central charge:
cM = 25 - 6 Q2 (2)
Q = 2/γ + γ/2. (3)
hence if the central charge cM = 0 and therefore to
γ = √(8/3) then we induce to a global topology on Quantum Gravity in the GNL:
GM 4(1- M2) = GM 4(1+ M)(1-M) (4)
In normal cases, the Newton's gravity constant G = 2/3 = 0.666..., which leads to
8/3 M(1+ M)(1- M) = Id = 1. (5)
We clearly can use the parameters of the LCFT to lead to the main results on the relation between Mass and Velocity of the GNL:
V = 4(1- M2) = (2cos(φ))2= 4 cos2(φ) (6)
and
M = √(1 - V/4). (7)
(3). Theorem 3.
The GNL is a complele and exact Quantum Gravity theory, since it can give a global dynamics on Expansion and Retraction of the Universe and Fundamental Particle (Using Courant Algebroid):
2 ± √3 + 1/(2 ± √3) = 4. (8)
and
2 ± √5 - 1/(2 ±√5) = 4. (9)
Finally, there exists an ergodic topological form of the quasi-stable light speed v = 3x ... km/s and the limit photon speed vmax= 4:
2n ± √3 + 1/(2n ±√3) ↔ 2n ± √5 - 1/(2n ± √5) (10)
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