scholarly journals N $$ \mathcal{N} $$ = 4 super-Yang-Mills in LHC superspace part I: classical and quantum theory

2017 ◽  
Vol 2017 (2) ◽  
Author(s):  
Dmitry Chicherin ◽  
Emery Sokatchev
Keyword(s):  
2010 ◽  
Vol 19 (14) ◽  
pp. 2379-2384 ◽  
Author(s):  
SUDARSHAN ANANTH

Three of the four forces of Nature are described by quantum Yang–Mills theories with remarkable precision. The fourth force, gravity, is described classically by the Einstein–Hilbert theory. There appears to be an inherent incompatibility between quantum mechanics and the Einstein–Hilbert theory which prevents us from developing a consistent quantum theory of gravity. The Einstein–Hilbert theory is therefore believed to differ greatly from Yang–Mills theory (which does have a sensible quantum mechanical description). It is therefore very surprising that these two theories actually share close perturbative ties. This essay focuses on these ties between Yang–Mills theory and the Einstein–Hilbert theory. We discuss the origin of these ties and their implications for a quantum theory of gravity.


1982 ◽  
Vol 67 (4) ◽  
pp. 1206-1215 ◽  
Author(s):  
T. Fukuda ◽  
M. Monda ◽  
M. Takeda ◽  
K.-i. Yokoyama

1981 ◽  
Vol 66 (5) ◽  
pp. 1827-1842 ◽  
Author(s):  
T. Fukuda ◽  
M. Monda ◽  
M. Takeda ◽  
K.-i. Yokoyama

2020 ◽  
pp. 2150019
Author(s):  
Abhinash Kumar Roy ◽  
Anmol Sahu ◽  
Tejinder P. Singh

We have recently proposed a Lagrangian in trace dynamics to describe a possible unification of gravity, Yang–Mills fields, and fermions, at the Planck scale. This Lagrangian for the unified entity — called the aikyon — is invariant under global unitary transformations, and as a result possesses a novel conserved charge, known as the Adler–Millard charge. In this paper, we derive an eigenvalue equation, analogous to the time-independent Schrödinger equation, for the Hamiltonian of the theory. We show that in the emergent quantum theory, the energy eigenvalues of the aikyon are characterized in terms of a fundamental frequency times Planck’s constant. The eigenvalues of this equation can, in principle, determine the values of the parameters of the standard model. We also report a ground state, in this theory of spontaneous quantum gravity, which could characterize a non-singular initial epoch in quantum cosmology.


Author(s):  
Roman G. Shulyakovsky ◽  
Alexander S. Gribowsky ◽  
Alexander S. Garkun ◽  
Maxim N. Nevmerzhitsky ◽  
Alexei O. Shaplov ◽  
...  

Instantons are non-trivial solutions of classical Euclidean equations of motion with a finite action. They provide stationary phase points in the path integral for tunnel amplitude between two topologically distinct vacua. It make them useful in many applications of quantum theory, especially for describing the wave function of systems with a degenerate vacua in the framework of the path integrals formalism. Our goal is to introduce the current situation about research on instantons and prepare for experiments. In this paper we give a review of instanton effects in quantum theory. We find in stanton solutions in some quantum mechanical problems, namely, in the problems of the one-dimensional motion of a particle in two-well and periodic potentials. We describe known instantons in quantum field theory that arise, in particular, in the two-dimensional Abelian Higgs model and in SU(2) Yang – Mills gauge fields. We find instanton solutions of two-dimensional scalar field models with sine-Gordon and double-well potentials in a limited spatial volume. We show that accounting of instantons significantly changes the form of the Yukawa potential for the sine-Gordon model in two dimensions.


1976 ◽  
Vol 37 (3) ◽  
pp. 172-175 ◽  
Author(s):  
R. Jackiw ◽  
C. Rebbi
Keyword(s):  

1999 ◽  
Vol 14 (14) ◽  
pp. 2139-2172 ◽  
Author(s):  
HONG-MO CHAN ◽  
SHEUNG TSUN TSOU

A loop space formulation of Yang–Mills theory highlighting the significance of monopoles for the existence of gauge potentials is used to derive a generalization of electric–magnetic duality to the non-Abelian theory. The result implies that the gauge symmetry is doubled from SU (N) to [Formula: see text], while the physical degrees of freedom remain the same, so that the theory can be described in terms of either the usual Yang–Mills potential Aμ(x) or its dual Ãμ(x). Non-Abelian "electric" charges appear as sources of Aμ but as monopoles of Ãμ, while their "magnetic" counterparts appear as monopoles of Aμ but sources of Ãμ. Although these results have been derived only for classical fields, it is shown for the quantum theory that the Dirac phase factors (or Wilson loops) constructed out of Aμ and Ãμ satisfy the 't Hooft commutation relations, so that his results on confinement apply. Hence one concludes, in particular, that since colour SU (3) is confined, dual colour [Formula: see text] is broken. Such predictions can lead to many very interesting physical consequences, which are explored in a companion paper.


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