2013
DOI: 10.3116/16091833/14/3/146/2013
|View full text |Cite
|
Sign up to set email alerts
|

Optically pumped mirrorless lasing. A review. Part I. Random lasing

Abstract: Abstract. Currently optically pumped mirrorless lasing is represented by three distinct branches, which concern lasing in different types of the gain media: optically random and photonic media, and microcavities. This article is a first part of our review on optically pumped mirrorless lasing, with the random lasing in scattering media being a main subject. The other mirrorless lasing mechanisms will be addressed in the second part. Considering light localization as a key function of the feedback, we discuss p… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
8
0

Year Published

2015
2015
2022
2022

Publication Types

Select...
7

Relationship

0
7

Authors

Journals

citations
Cited by 19 publications
(8 citation statements)
references
References 116 publications
0
8
0
Order By: Relevance
“…A more detailed explanation and comparison of SF, SL/ASE and SR refers to [ 40 ]. The RL is distinguished from the rest as the RL is mirror-less but not feedback-less [ 41 , 42 ]. The random medium induces the essential feedback for light amplification through the multiple scattering, whereas the features and disorders of the random medium can be represented by the RL emission properties [ 42 ].…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…A more detailed explanation and comparison of SF, SL/ASE and SR refers to [ 40 ]. The RL is distinguished from the rest as the RL is mirror-less but not feedback-less [ 41 , 42 ]. The random medium induces the essential feedback for light amplification through the multiple scattering, whereas the features and disorders of the random medium can be represented by the RL emission properties [ 42 ].…”
Section: Introductionmentioning
confidence: 99%
“…In the last two decades, several review articles have provided an extensive insight of the physics [ 41 , 42 , 63 , 64 , 65 , 66 , 67 , 68 ] and potential applications of RLs [ 68 , 69 , 70 , 71 , 72 , 73 ]. Along with a deeper physical understanding and rapid development of new materials and new findings [ 74 , 75 , 76 ], an updated review article seems in high demand.…”
Section: Introductionmentioning
confidence: 99%
“…Modern laser resonators are produced with high quality optical elements and require precision alignment, resulting in a bottleneck in production. Recently, significant effort has been focused on developing lasers utilizing mirrorless principles of optical feedback. , One of these mirrorless feedback mechanisms is selective light reflection in cholesteric liquid crystals (ChLC), which under special conditions act as 1D photonic crystals . Light emission from a fluorescent dye dissolved in cholesteric liquid crystals is inhibited within the spectral range of the photonic band gap (PhBG), which is the selective reflection band for a ChLC, but leaks as strongly amplified laser radiation , at the PhBG edges.…”
Section: Resultsmentioning
confidence: 99%
“…Achievement of gain in lasers is complicated as well as a difficult task. Regarding mirrorless lasing, gain media mainly falls into the following categories: random optical media, photonic media, and microcavities 38 . Laser dyes and QDs are the most popularly used gain materials.…”
Section: General Considerations and Examples For Active Platforms Of Rlmentioning
confidence: 99%
“…Regarding mirrorless lasing, gain media mainly falls into the following categories: random optical media, photonic media, and microcavities. 38 Laser dyes and QDs are the most popularly used gain materials. In RLs, some experiments utilise semiconductors (ZnO, [39][40][41] ZnS, [42][43][44] GaAs 45,46 etc.)…”
Section: General Considerations and Examples For Active Platforms Of Rlmentioning
confidence: 99%