scholarly journals Lifshitz field theories, Snyder noncommutative spacetime and momentum-dependent metric

2015 ◽  
Vol 30 (29) ◽  
pp. 1550155 ◽  
Author(s):  
Juan M. Romero ◽  
J. David Vergara

In this paper, we propose three different modified relativistic particles. In the first case, we propose a particle with metrics depending on the momenta and we show that the quantum version of these systems includes different field theories, as Lifshitz field theories. As a second case, we propose a particle that implies a modified symplectic structure and we show that the quantum version of this system gives different noncommutative spacetimes, for example the Snyder spacetime. In the third case, we combine both structures before mentioned, namely noncommutative spacetimes and momentum-dependent metrics. In this last case, we show that anisotropic field theories can be seen as a limit of noncommutative field theory.

2008 ◽  
Vol 23 (14n15) ◽  
pp. 2277-2278
Author(s):  
YUYA SASAI ◽  
NAOKI SASAKURA

Domain wall solitons are the simplest topological objects in field theories. The conventional translational symmetry in a field theory is the generator of a one-parameter family of domain wall solutions, and induces a massless moduli field which propagates along a domain wall. We study similar issues in braided noncommutative field theories possessing Hopf algebraic translational symmetries. As a concrete example, we discuss a domain wall soliton in the scalar braided noncommutative field theory in Lie-algebraic noncommutative spacetime, which has a Hopf algebraic translational symmetry. We construct explicitly a one-parameter family of solutions in perturbation of the noncommutativity parameter. We then find the massless moduli field which propagates on the domain wall soliton. This work is based on arXiv:0711.3059.


Author(s):  
MARIJA DIMITRIJEVIĆ ◽  
LARISA JONKE

Although the meaning of twisted symmetry is still not fully understood, the twist approach has its advantages in the construction of field theories on noncommutative spaces. We discuss these advantages on the example of κ-Minkowski space-time. We construct the noncommutative U(1) gauge field theory. Especially the action is written as an integral of a maximal form, thus solving the cyclicity problem of the integral in κ-Minkowski. Using the Seiberg-Witten map to relate noncommutative and commutative degrees of freedom the effective action with the first order corrections in the deformation parameter is obtained.


Author(s):  
Roman Baudrimont

The purpose of this paper is to find a quantum formulation of entropic gravity, incorporating the bijective theory. In a first part, we will describe the basis of the bijective theory. In a second part, we will incorporate the stress energy quantum tensor defined in the linear approximation of the Einstein’s equation in its quantum version to entropy. In the third part, we will integrate the bijective theory with the newly created relativistic quantum entropy. This will lead us four part where we will formalize quantum entropic gravity.


Author(s):  
Roman Baudrimont

The purpose of this paper is to find a quantum formulation of entropic gravity, incorporating the bijective theory. In a first part, we will describe the basis of the bijective theory. In a second part, we will incorporate the stress energy quantum tensor defined in the linear approximation of the Einstein’s equation in its quantum version to entropy. In the third part, we will integrate the bijective theory with the newly created relativistic quantum entropy. This will lead us four part where we will formalize quantum entropic gravity.


2009 ◽  
Author(s):  
Yuya Sasai ◽  
Naoki Sasakura ◽  
Jerzy Kowalski-Glikman ◽  
R. Durka ◽  
M. Szczachor

Author(s):  
Xun Liu ◽  
Tsukasa Tada

Abstract We reexamine two-dimensional Lorentzian conformal field theory using the formalism previously developed in a study of sine-square deformation of Euclidean conformal field theory. We construct three types of Virasoro algebra. One of them reproduces the result by Lüscher and Mack, while another type exhibits divergence in the central charge term. The third leads to a continuous spectrum and contains no closed time-like curve in the system.


1992 ◽  
Vol 07 (28) ◽  
pp. 7119-7134 ◽  
Author(s):  
J.W. VAN HOLTEN

A generalization of BRST field theory is presented, based on wave operators for the fields constructed out of, but different from the BRST operator. We discuss their quantization, gauge fixing and the derivation of propagators. We show, that the generalized theories are relevant to relativistic particle theories in the Brink-Di Vecchia-Howe-Polyakov (BDHP) formulation, and argue that the same phenomenon holds in string theories. In particular it is shown, that the naive BRST formulation of the BDHP theory leads to trivial quantum field theories with vanishing correlation functions.


2013 ◽  
Vol 28 (04) ◽  
pp. 1250239 ◽  
Author(s):  
JIA-HUI HUANG ◽  
WEIJIAN WANG

In this paper, the microcausality of quantum field theory on spin-induced noncommutative spacetime is discussed. It is found that for space-like separation the microcausality is not obeyed by the theory generally. It means that Lorentz covariance cannot guarantee microcausality in quantum field theory. We also give some comments about quantum field theories on such noncommutative spacetime and the relations between noncommutative spacetime and causality.


2004 ◽  
Vol 19 (12) ◽  
pp. 1837-1861 ◽  
Author(s):  
RICHARD J. SZABO

This paper is a rudimentary introduction, geared at nonspecialists, to how noncommutative field theories arise in physics and their applications to string theory, particle physics and condensed matter systems.


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