Photon Pairing and the Strong-Coupling Phase of Massive Quantum Electrodynamics

1989 ◽  
Vol 63 (13) ◽  
pp. 1442-1442
Author(s):  
R. Fukuda
1990 ◽  
Vol 05 (09) ◽  
pp. 1789-1800 ◽  
Author(s):  
M. UKITA ◽  
M. KOMACHIYA ◽  
R. FUKUDA

The strong coupling phase of massless Quantum Electrodynamics is studied in a gauge invariant way. The formalism is given in which the order parameter of the chiral symmetry breaking is calculated through the vacuum polarization diagrams. Applying this method, the critical coupling constant is shown to exist that is independent of the gauge parameter but is now dependent on the ratio of the two kinds of cutoff. Implication of this new parameter on the renormalization scheme in the strong coupling phase is discussed.


1990 ◽  
Vol 05 (05) ◽  
pp. 309-314 ◽  
Author(s):  
M. INOUE ◽  
T. MUTA ◽  
J. SAITO ◽  
H.-L. YU

We discuss observable effects of the assumption that the strong coupling phase of quantum electrodynamics is realized in the surface region of heavy nuclei with large atomic number Z under a suitable external disturbance. We present some comments on anomalous peaks in electron-positron systems observed in heavy ion reactions and on effects expected in electron and positron scatterings off large-Z nuclei. We propose some experiments to test our assumption: (1) coincidence measurement of e+e− and γγ signals from the decays of large-Z nuclei, and (2) spectroscopy of large-Z muonic atoms.


1990 ◽  
Vol 05 (06) ◽  
pp. 381-390 ◽  
Author(s):  
T. INAGAKI ◽  
M. KOMACHIYA ◽  
R. FUKUDA

Through the Cooper equation of the photon pairing, the instability of the normal vacuum of the Quantum Electrodynamics with the massive electron is studied. Using the low energy effective Lagrangian, the normal vacuum is shown to be unstable against the condensation of the photon pairs above the critical value of the fine structure constant. These agree with the previous results obtained by the Bethe-Salpeter equation. The presence of the weak electric external field enhances the instability thus lowering the critical value. This can be a basis for the explanation of the anomalous GSI e+e− events.


2001 ◽  
Vol 16 (12) ◽  
pp. 2253-2266
Author(s):  
KOU SU-PENG

In this paper, we use Parisi and Sourlas dimensional reduction to show that QED has two phases, the strong coupling phase and weak coupling phase. Because chiral symmetry is spontaneously broken, particles with fractional charges are confined in the strong coupling phase by the condensation of topological configurations, and particles with integer charges are screened by fermion pairs.


2017 ◽  
Vol 114 (12) ◽  
pp. 3026-3034 ◽  
Author(s):  
Johannes Flick ◽  
Michael Ruggenthaler ◽  
Heiko Appel ◽  
Angel Rubio

1979 ◽  
Vol 161 (2-3) ◽  
pp. 397-416 ◽  
Author(s):  
J.-M. Drouffe ◽  
G. Parisi ◽  
N. Sourlas

2018 ◽  
Vol 175 ◽  
pp. 03004 ◽  
Author(s):  
David Schaich ◽  
Simon Catterall

We present ongoing investigations of a four-dimensional lattice field theory with four massless reduced staggered fermions coupled through an SU(4)-invariant fourfermion interaction. As in previous studies of four-fermion and Higgs–Yukawa models with different lattice fermion discretizations, we observe a strong-coupling phase in which the system develops a mass gap without breaking any lattice symmetry. This symmetric strong-coupling phase is separated from the symmetric weak-coupling phase by a narrow region of four-fermi coupling in which the system exhibits long-range correlations.


1981 ◽  
Vol 24 (10) ◽  
pp. 2706-2723 ◽  
Author(s):  
Fred Cooper ◽  
Richard Kenway

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