Control random laser modes by local pumping

Author(s):  
Jonathan Andreasen ◽  
Christian Vanneste ◽  
Li Ge ◽  
Hui Cao
Keyword(s):  
2007 ◽  
Vol 24 (10) ◽  
pp. A26 ◽  
Author(s):  
Xiaohua Wu ◽  
Jonathan Andreasen ◽  
Hui Cao ◽  
Alexey Yamilov

2009 ◽  
Vol 3 (5) ◽  
pp. 279-282 ◽  
Author(s):  
Johannes Fallert ◽  
Roman J. B. Dietz ◽  
Janos Sartor ◽  
Daniel Schneider ◽  
Claus Klingshirn ◽  
...  
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Nonlinearity ◽  
2012 ◽  
Vol 25 (3) ◽  
pp. 851-868 ◽  
Author(s):  
Jonathan Andreasen ◽  
Hui Cao

2007 ◽  
Vol 98 (14) ◽  
Author(s):  
Karen L. van der Molen ◽  
R. Willem Tjerkstra ◽  
Allard P. Mosk ◽  
Ad Lagendijk

2015 ◽  
Vol 23 (2) ◽  
pp. 1456 ◽  
Author(s):  
Sara García-Revilla ◽  
Joaquín Fernández ◽  
Macarena Barredo-Zuriarrain ◽  
Luís D. Carlos ◽  
Edison Pecoraro ◽  
...  
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Author(s):  
X. Wu ◽  
J. Andreasen ◽  
H. Cao ◽  
A. Yamilov
Keyword(s):  

Author(s):  
Andreas Lubatsch ◽  
Regine Frank

The spatial formation of coherent random laser modes in strongly scattering disordered random media is a central feature in the understanding of the physics of random lasers. We derive a quantum field theoretical method for random lasing in disordered samples of complex amplifying Mie resonators which is able to provide self-consistently and free of any fit parameter the full set of transport characteristics at and above the laser phase transition. The coherence length and the correlation volume respectively is derived as an experimentally measurable scale of the phase transition at the laser threshold. We find that the process of stimulated emission in extended disordered arrangements of active Mie resonators is ultimately connected to time-reversal symmetric multiple scattering in the sense of photonic transport while the diffusion coefficient is finite. A power law is found for the random laser mode diameters in stationary state with increasing pump intensity.


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