2018
DOI: 10.1080/15421406.2018.1542071
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Narrowing the oscillation spectra of a cholesteric liquid crystal laser

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Cited by 4 publications
(2 citation statements)
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“…In this configuration a separate layer is formed for the gain medium that is sandwiched between two CLC layers ( Figure ). This structure creates a defect in the macroscopic helical structure and therefore a leaky mode within the band‐gap 13–17. Furthermore, as the gain medium is de‐coupled from the CLC the device architecture allows for a wide variety of emissive compounds to be used that would not otherwise be soluble in the CLC host 18,19…”
Section: Figurementioning
confidence: 99%
“…In this configuration a separate layer is formed for the gain medium that is sandwiched between two CLC layers ( Figure ). This structure creates a defect in the macroscopic helical structure and therefore a leaky mode within the band‐gap 13–17. Furthermore, as the gain medium is de‐coupled from the CLC the device architecture allows for a wide variety of emissive compounds to be used that would not otherwise be soluble in the CLC host 18,19…”
Section: Figurementioning
confidence: 99%
“…As the neat CLC exhibits a PBG, i.e., forbidden band for visible light, when the defect structure is formed, this discontinuity in the CLC helix creates one or more localized leaky modes within the gap from where light can escape. These leaky mode(s) are created by adding a defect in the helix and are therefore known as defect-modes [26][27][28] . When the defect layer is doped with an emissive material that exhibits photoluminescence (PL) emission so that the spectrum overlaps with the leaky mode(s), laser emission can be observed.…”
Section: Defect-mode Structurementioning
confidence: 99%