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Related papers: Spectral function in QED3

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To remove the linear infrared divergences in quenched approximation we include the massive fermion loop to the photon spectral function.Spectral function of fermion has no one particle singularity if we fix the anomalous dimension to be…

High Energy Physics - Theory · Physics 2017-08-23 Yuichi Hoshino

To study the infrared behaviour of the propagator, exponentiation of the lowest order spectral function has been known.We show this method is helpful in super renormalizable theory with dimension-full coupling constant.In the 1/N…

High Energy Physics - Theory · Physics 2009-01-28 Yuichi Hoshino

Minkowski structure of the Fermion propagator in QED$_{2+1}$ is evaluated using dispersion like method Including massive fermion loop to the photon spectral function there is no infrared divergences in the gauge d=-1.Screening effects…

High Energy Physics - Theory · Physics 2009-06-10 Yuichi Hoshino

We discuss the infrared and ultraviolet behavior of the fermion propagator in (2+1)-dimensional QED based on spectral representation.If we choose soft-photon exponentiation to include all orders of soft-photon emission by electron,its…

High Energy Physics - Theory · Physics 2014-03-17 Yuichi Hoshino

Using spectral function of photon we find the reliable results for the effects of vacuum polarization for the dressed fermion propagator in three-dimensional QED.

High Energy Physics - Theory · Physics 2007-05-23 Yuichi Hoshino

We investigate the influence of the full vacuum polarization and vertex function on the fermion propagator, using the coupled Dyson--Schwinger equations for the photon and fermion propagator. We show that, within a range of vertex…

High Energy Physics - Phenomenology · Physics 2009-10-28 P. Maris

Analytical properties of the photon propagator in QED3 in the N^1-approximation are considered. It is noticed that in given approximation if the dynamical fermions mass is nonzero this propagator has a single pole at the point k^2=0 and a…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Sh. Pevzner

The infrared behaviour of the gauge-invariant dressed fermion propagator in massless QED_3 is discussed for three choices of dressing. It is found that only the propagator with the isotropic (in three Euclidean dimensions) choice of…

High Energy Physics - Theory · Physics 2008-11-26 Indrajit Mitra , Raghunath Ratabole , H. S. Sharatchandra

We discuss the properties of the position space fermion propagator in three dimensional QED which has been found previouly based on Ward-Takahashi-identity for soft-photon emission vertex and spectral representation.There is a new type of…

High Energy Physics - Theory · Physics 2008-11-26 Yuichi Hoshino

Infrared behaviour of the fermion propagator is examined by spectral representation.Assuming asymptotic states and using LSZ reduction formula we evaluate the the lowest order spectral function by definition.After exponentiation of it we…

High Energy Physics - Theory · Physics 2009-01-19 Yuichi Hoshino

In this work we consider a coupled system of Schwinger-Dyson equations for self-energy and vertex functions in QED_3. Using the concept of a semi-amputated vertex function, we manage to decouple the vertex equation and transform it in the…

High Energy Physics - Theory · Physics 2009-10-31 N. E. Mavromatos , J. Papavassiliou

We establish that QED3 can possess a critical number of flavours, N_f^c, associated with dynamical chiral symmetry breaking if, and only if, the fermion wave function renormalisation and photon vacuum polarisation are homogeneous functions…

High Energy Physics - Phenomenology · Physics 2008-12-18 A. Bashir , A. Raya , I. C. Cloet , C. D. Roberts

The infrared properties of QED are investigated within the framework of the Dyson-Schwinger equations. Our study finds that, independently of the value of the coupling constant, requiring the photon self-energy to be finite for any momenta,…

High Energy Physics - Phenomenology · Physics 2025-11-05 Orlando Oliveira

The three-dimensional non-compact QED is known to exhibit weak confinement when fermions acquire a finite mass via the mechanism of dynamical chiral symmetry breaking. In this paper, we study the effect of fermion damping caused by elastic…

High Energy Physics - Theory · Physics 2015-11-23 Jing Wang , Jing-Rong Wang , Wei Li , Guo-Zhu Liu

For massless quenched QED in three dimensions, we evaluate a non-perturbative expression for the fermion propagator which agrees with its two loop perturbative expansion in the weak coupling regime. This calculation is carried out by making…

High Energy Physics - Theory · Physics 2009-10-31 A. Bashir

We study chiral symmetry breaking in $\rm QED_3$ with $N_f$ flavors of four-component fermions. A closed system of Schwinger-Dyson equations for fermion and photon propagators and the full fermion-photon vertex is proposed, which is…

High Energy Physics - Phenomenology · Physics 2009-10-28 V. P. Gusynin , A. H. Hams , M. Reenders

We have systematically constructed the general structure of the fermion self-energy and the effective quark propagator in presence of a nontrivial background like hot magnetised medium. This is applicable to both QED and QCD. The hard…

High Energy Physics - Phenomenology · Physics 2018-02-28 Aritra Das , Aritra Bandyopadhyay , Pradip K. Roy , Munshi G. Mustafa

Non-compact QED3 is simulated both in the quenched and unquenched cases. In particular, we investigate the restoration of chiral symmetry at finite temperature. We also compute the zero temperature spectrum of the theory, including (in the…

High Energy Physics - Lattice · Physics 2009-10-22 J. B. Kogut , J. -F. Lagae

Using the Zumino identities it is shown that in a class of non-local gauges, massless QED_3 has an infrared behaviour of a conformal field theory with a continuously varying anomalous dimension of the fermion. In the usual Lorentz gauge,…

High Energy Physics - Theory · Physics 2008-11-26 Indrajit Mitra , Raghunath Ratabole , H. S. Sharatchandra

Dong, Munczek and Roberts have shown how the full 3-point vertex that appears in the Schwinger-Dyson equation for the fermion propagator can be expressed in terms of a constrained function $W_1$ in massless quenched QED. However, this…

High Energy Physics - Phenomenology · Physics 2009-10-30 A. Bashir , A. Kizilersu , M. R. Pennington
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