Null-plane quantum electrodynamics in an external radiation field

1976 ◽  
Vol 54 (22) ◽  
pp. 2246-2271 ◽  
Author(s):  
R. A. Neville

The formalism developed in this paper is designed to treat the interaction of an electron with a laser pulse. Precisely, it is a formulation on null hyperplanes of quantum electrodynamics in an external radiation field.The result is a quantum electrodynamic formulation in which one works in the Furry picture. The electron field operator in this picture is a solution to the Dirac equation with external field, and is appropriately represented by an expansion in terms of wave packets of Volkov solutions, the latter being exact, explicitly known solutions to the above named equation. The null-plane formulation is required for the consistent construction and implementation of the Volkov wave packets.This formalism permits one to do calculations which take the external field (laser field) into account exactly while treating the quantized photon field (self-field) via the usual perturbation method as adapted to null planes.

1983 ◽  
Vol 61 (1) ◽  
pp. 85-92 ◽  
Author(s):  
A. R. Neghabian ◽  
W. Glöckle

The multiphoton exchange between two charged spin [Formula: see text] particles of light (m) and heavy (M) mass is considered and it is shown how, in the limit M → ∞, the Dirac equation with an external potential including radiative corrections emerges. This result can only be achieved if diagrams with photons attached to the heavy particle line cancel among themselves for M → ∞. We have shown this in the lowest order where the individual diagrams have nonvanishing limits.


Photonics ◽  
2021 ◽  
Vol 8 (6) ◽  
pp. 192
Author(s):  
Theocharis Lamprou ◽  
Rodrigo Lopez-Martens ◽  
Stefan Haessler ◽  
Ioannis Liontos ◽  
Subhendu Kahaly ◽  
...  

Quantum-optical spectrometry is a recently developed shot-to-shot photon correlation-based method, namely using a quantum spectrometer (QS), that has been used to reveal the quantum optical nature of intense laser–matter interactions and connect the research domains of quantum optics (QO) and strong laser-field physics (SLFP). The method provides the probability of absorbing photons from a driving laser field towards the generation of a strong laser–field interaction product, such as high-order harmonics. In this case, the harmonic spectrum is reflected in the photon number distribution of the infrared (IR) driving field after its interaction with the high harmonic generation medium. The method was implemented in non-relativistic interactions using high harmonics produced by the interaction of strong laser pulses with atoms and semiconductors. Very recently, it was used for the generation of non-classical light states in intense laser–atom interaction, building the basis for studies of quantum electrodynamics in strong laser-field physics and the development of a new class of non-classical light sources for applications in quantum technology. Here, after a brief introduction of the QS method, we will discuss how the QS can be applied in relativistic laser–plasma interactions and become the driving factor for initiating investigations on relativistic quantum electrodynamics.


1973 ◽  
Vol 46 (1) ◽  
pp. 102-104 ◽  
Author(s):  
F. Rohrlich ◽  
J.H. Ten Eyck

1978 ◽  
Vol 34 (2) ◽  
pp. 98-105
Author(s):  
M. A. Braun ◽  
A. N. Vasil'ev ◽  
A. L. Kitanin ◽  
Yu. M. Pis'mak

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