2009
DOI: 10.1103/physrevlett.102.043906
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Statistical Properties of One-Dimensional Random Lasers

Abstract: Statistical properties of a laser based on a one-dimensional disordered superlattice open at one side are studied numerically. The passive normal modes of the system are determined using the Feshbach projection technique. It is found that the mode competition due to the spacial hole burning leads to a saturation of the number of lasing modes with increasing pump rate. It is also responsible for nonmonotonic dependence of intensities of lasing modes as functions of pumping. Computed distributions of spectral sp… Show more

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Cited by 20 publications
(25 citation statements)
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(34 reference statements)
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“…Both these methods reduce noticeably the lasing threshold as compared to 3D random lasing systems. Because the frequencies of the modes and the locations of the effective cavities vary from sample to sample randomly, in the most cases they are described statistically [20][21][22][23][24] . However, usually we deal with a specific random sample, and it is important to know how many modes and at which frequencies can be excited in a given frequency range; where these modes are localized inside this sample, etc 11 .…”
Section: B Random Lasersmentioning
confidence: 99%
“…Both these methods reduce noticeably the lasing threshold as compared to 3D random lasing systems. Because the frequencies of the modes and the locations of the effective cavities vary from sample to sample randomly, in the most cases they are described statistically [20][21][22][23][24] . However, usually we deal with a specific random sample, and it is important to know how many modes and at which frequencies can be excited in a given frequency range; where these modes are localized inside this sample, etc 11 .…”
Section: B Random Lasersmentioning
confidence: 99%
“…We also analyze separate contributions from three different types of interactions, namely from quadruplets (all four modes are different), triplets (only three of four modes are different) and pairs (only two different modes participate in the interaction). For quadruplets all indices in (21) should be different, i.e. µ 1 = ν, µ 2 = ν, µ 3 = ν, µ 1 = µ 2 , µ 1 = ν, µ 1 = µ 3 , µ 2 = µ 3 .…”
Section: Resonancesmentioning
confidence: 99%
“…This mechanism is of pure statistical origin and does not require localization or interference [17]. It was also proposed that such systems can exhibit Lévy-type statistics in the distribution of intensities [18][19][20], and crossovers among different statistics have been predicted [21].…”
mentioning
confidence: 98%