نتایج جستجو برای: gauge function

تعداد نتایج: 1259516  

2006
Umut Gürsoy

Recently, a one-parameter deformation of the Maldacena-Núñez background was constructed in hep-th/0505100. According to the Lunin-Maldacena conjecture, the background is dual to pure N = 1 SYM in the IR coupled to a KK sector whose dynamics is altered by a dipole deformation that is proportional to the deformation parameter γ. Thus, the deformation serves to identify the aspects of the gravity ...

2003
Miguel Lorente

The idea of a discrete space-time has been introduced by physicists in the past in several different ways. Heisenberg advocated a fundamental length, Snyder has proposed a position operator with discrete spectrum, Ahmavaara has carried out a physical model on a cubic lattice, which is embedded in a finite linear space over a Galois field. Recently the use of discrete space-time variables in Lat...

1998
R. Johnson M. Teper

1. THE PROBLEM On a square lattice (we consider here a D=2+1 lattice for simplicity) the exact rotational symmetry is confined to rotations that are integer multiples of π/2. If we attempt to build operators of spin J from basic components that are identical – that is, related by a lattice symmetry – then there is an ambiguity: exp(iJθ) ≡ exp(iJ ′ θ) ∀θ = nπ 2 (1) if J ′ = J + 4N ∀N (2) Thus, f...

فارغ بال, رضا, کریمی, پدرام,

In this paper, we use the holographic renormalization method to calculate the two-point correlation functions of the CFT stress tensor. In the gravity side, we write the asymptotically AdS spacetimes in the BMS gauge and apply the standard holographic renormalization method for these space-times. The significance of using multi-point functions in this gauge is that its flat-space limit is well-...

2005
Robert T. Jantzen

The role of the Taub time gauge in cosmology is linked to the use of the densitized lapse function instead of the lapse function in the variational principle approach to the Einstein equations. The spatial metric variational equations then become the Ricci evolution equations, which are then supplemented by the Einstein constraints which result from the variation with respect to the densitized ...

2008
Toyoki Matsuyama Satoko Uchida

Dynamical mass generation of a two-component fermion in QED3 with a ChernSimons term is investigated by solving the Schwinger-Dyson equation formulated in the lowest ladder approximation. Dependence of the dynamical fermion mass on a gauge-fixing parameter, a gauge coupling constant, and a topological mass is examined by approximated analytical and also numerical methods. The inclusion of the C...

1998
N. J. Watson

It is shown how the pinch technique algorithm may be consistently extended beyond the one-loop level to obtain the gauge-independent two-loop fermion self-energy −iΣ̂(p) in QCD in the pinch technique approach. The starting point for the construction is the general diagrammatic representation of the two-loop quark self-energy in terms of renormalized one-loop twoand three-point function and tree ...

آقابابایی, سارا, حقیقت, منصور,

Non-commutative field theory as a theory including the Lorentz violation can be constructed in two different ways. In the first method, the non-commutative fields are the same as the ordinary ones while the gauge group is restricted to U(n). For example, the symmetry group of standard model in non-commutative space is U(3)×(2)×U(1) which can be reduced to SU(3)×SU(2)×U(1) by two appropriate spo...

Hossein Jalalifar Jaber TaheriShakib Mansour Fatehirad

The main task of drilling the formation by the bit is done via scraping, crushing and grinding. Discharging the fluid from the bit nozzles is done with high pressure which assists to break the rocks. Different parameters affect the bit selection and design for each drilling formation, but the most important one is drillability that depends on hardness of the formation. In this paper, the design...

Journal: :journal of nanostructures 2013
m. monemzadeh m. taie b. khoshnevisan

the bft approach is used to formulate the electronic states in graphene through a non-commutative space in the presence of a constant magnetic field b for the first time. in this regard, we introduce a second class of constrained system, which is not gauge symmetric but by applying bft method and extending phase space, the second class constraints  converts  to the first class constraints so th...

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