Rotationally invariant space time constellations

Author(s):  
Jun Shi ◽  
R.D. Wesel
1975 ◽  
Vol 28 (1) ◽  
pp. 93-104
Author(s):  
F. S. Klotz

2019 ◽  
Vol 99 (2) ◽  
Author(s):  
Murat Yessenov ◽  
Basanta Bhaduri ◽  
H. Esat Kondakci ◽  
Ayman F. Abouraddy

Author(s):  
Basanta Bhaduri ◽  
Murat Yessenov ◽  
H. Esat Kondakci ◽  
Ayman F. Abouraddy

2020 ◽  
Author(s):  
Amrit S. Sorli

In bijective modelling, the physical reality is represented by the set X, the model of physical reality by the set Y. Every element in the set X has exactly one correspondent element in the set Y. Set X and set X are related by the bijective function f:X→Y. Bijective modelling is confirming that time is the duration of given system entropy increasing in time-invariant space. Time-invariant space is the fundamental arena of the Nowless Universe.


Mind ◽  
1934 ◽  
Vol XLIII (170) ◽  
pp. 199-203
Author(s):  
A. USHENKO
Keyword(s):  

2017 ◽  
Vol 32 (33) ◽  
pp. 1750190
Author(s):  
Mario J. Neves ◽  
Everton M. C. Abreu

The noncommutative (NC) framework elaborated by Doplicher, Fredenhagen and Roberts (DFR) has a Lorentz invariant space–time structure in order to be considered as a candidate to understand the physics of the early Universe. In DFR formalism, the NC parameter [Formula: see text] is a coordinate operator in an extended Hilbert space and it has a conjugate momentum. Since [Formula: see text] and [Formula: see text] are independent coordinates, the Moyal–Weyl (MW) product can be used in this framework. With these elements, in this work, we have constructed the standard electroweak model. To accomplish this task, we have begun with the MW-product basis group of symmetry. After that we have introduced the spontaneous symmetry breaking and the hypercharge in DFR framework. The electroweak symmetry breaking was analyzed and the masses of the new bosons were computed. Finally, the gauge symmetry and gauge transformations were discussed.


Sign in / Sign up

Export Citation Format

Share Document