Longitudinal–transverse mode interplay and conical emission in microchip lasers

1995 ◽  
Vol 12 (8) ◽  
pp. 1511 ◽  
Author(s):  
S. Longhi ◽  
P. Laporta
2005 ◽  
Vol 37 (12) ◽  
pp. 1109-1120 ◽  
Author(s):  
Wupeng Gong ◽  
Mali Gong ◽  
Qiang Liu ◽  
Fuyuan Lu

1999 ◽  
Author(s):  
John J. Zayhowski ◽  
Colby Dill ◽  
Cook III ◽  
Daneu Chris ◽  
John L.
Keyword(s):  

1993 ◽  
Vol 29 (7) ◽  
pp. 644
Author(s):  
A. Tajiri ◽  
K. Minakuchi ◽  
K. Komeda ◽  
Y. Bessho ◽  
Y. Inoue ◽  
...  
Keyword(s):  

2021 ◽  
Vol 2021 (6) ◽  
Author(s):  
Anson Hook ◽  
Gustavo Marques-Tavares ◽  
Clayton Ristow

Abstract We present the supernova constraints on an axion-photon-dark photon coupling, which can be the leading coupling to dark sector models and can also lead to dramatic changes to axion cosmology. We show that the supernova bound on this coupling has two unusual features. One occurs because the scattering that leads to the trapping regime converts axions and dark photons into each other. Thus, if one of the two new particles is sufficiently massive, both production and scattering become suppressed and the bounds from bulk emission and trapped (area) emission both weaken exponentially and do not intersection The other unusual feature occurs because for light dark photons, longitudinal modes couple more weakly than transverse modes do. Since the longitudinal mode is more weakly coupled, it can still cause excessive cooling even if the transverse mode is trapped. Thus, the supernova constraints for massive dark photons look like two independent supernova bounds super-imposed on top of each other.


Photonics ◽  
2021 ◽  
Vol 8 (2) ◽  
pp. 47
Author(s):  
Igor V. Smetanin ◽  
Alexey V. Shutov ◽  
Nikolay N. Ustinovskii ◽  
Vladimir D. Zvorykin ◽  
Anna V. Bogatskaya ◽  
...  

We develop theoretical background for the new nonlinear optical phenomenon of narrowly directed monochromatic IR conical emission which has been recently observed when 248-nm UV filaments propagate in xenon (V. D. Zvorykin, et al., Laser Phys. Lett. 13, 125404 (2016)). We treat it as coherent stimulated four-wave mixing process in which two pump KrF laser photons are converted into the coupled pair of resonance IR(828 nm) and VUV (147 nm) photons through 5p5(2P3/2)6p[1/2]0→5p5(2P3/2)6s[3/2]1o and 5p5(2P3/2)6s[3/2]1o→1S0 transitions. We explore the coherent interaction regime which proceeds at a time scale shorter than transverse relaxation time T2. The momentum and energy conservation laws determine the characteristic angle of conical emission. We find that the threshold of this coherent process is determined by the KrF laser pump pulse area.


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