/ 92 10 15 8 v 1 3 0 O ct 1 99 2 Attractive Forces Between Electrons in QED 3
نویسندگان
چکیده
Vacuum polarization effects are non-perturbatively incorporated into the photon propagator to eliminate the severe infrared problems characteristic of QED 3. The theory is thus rephrased in terms of a massive vector boson whose mass is e 2 /(8π). Subsequently, it is shown that electron-electron bound states are possible in QED 3 .
منابع مشابه
06 5 v 2 1 1 O ct 1 99 8 Effective Actions for 0 + 1 Dimensional Scalar QED and its SUSY Generalization at T = / 0
We compute the effective actions for the 0+1 dimensional scalar field interacting with an Abelian gauge background, as well as for its supersymmetric generalization at finite temperature.
متن کاملar X iv : h ep - p h / 98 10 35 2 v 1 1 3 O ct 1 99 8 IUHET 396
This talk summarizes some theoretical features and experimental implications of a general Lorentz-violating extension of the minimal SU(3) × SU(2)× U(1) standard model that allows for both CPT-even and CPT-odd effects. The theory would arise as the low-energy limit of a fundamental theory that is Lorentz and CPT covariant but in which spontaneous Lorentz breaking occurs. The use of neutral-meso...
متن کامل/ 98 10 06 5 v 1 9 O ct 1 99 8 Effective Actions for 0 + 1 Dimensional Scalar QED and its SUSY Generalization at T = / 0
We compute the effective actions for the 0+1 dimensional scalar field interacting with an Abelian gauge background, as well as for its supersymmetric generalization at finite temperature.
متن کاملv 1 1 3 O ct 1 99 8 The Global Minimum of the Effective Potential of the Many - Electron System with Delta - Interaction
We prove that the global minimum of the real part of the full effective potential of the many electron system with attractive delta interaction is in fact given by the BCS mean field configuration. This is a consequence of a simple bound which is obtained by applying Hadamard’s inequality to the functional determinant. The second order Taylor expansion around the minimum is computed. ∗ e-mail: ...
متن کامل