2018
DOI: 10.1515/nanoph-2018-0034
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The transition from incoherent to coherent random laser in defect waveguide based on organic/inorganic hybrid laser dye

Abstract: This paper systematically demonstrated a variety of experimental phenomena of random lasers (RLs) of N,N′-di-(3-(isobutyl polyhedral oligomeric silsesquioxanes)propyl) perylene diimide (DPP) organic/inorganic hybrid laser dye, which is composed of perylene diimide (PDI) as gain media and polyhedral oligomeric silsesquioxanes (POSS) as scattering media at a mole ratio of 1:2. In this work, we observe the transition from incoherent RL in the DPP-doped solutions and polymer membrane systems using dip-coating meth… Show more

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Cited by 24 publications
(14 citation statements)
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“…Thus, incoherent processes have been the mechanisms for the random lasers, which explain the broad lasing spectrum in the measurement results shown in Figure 4. The spectral bandwidth of roughly 5 nm or even larger than 7 nm at FWHM has been observed with the incoherent random lasers, as reported in the studies by Xia et al and Weng et al, [ 35,36 ] verifying the random lasing nature of the observed emission spectra.…”
Section: Random Lasing Performancesupporting
confidence: 75%
“…Thus, incoherent processes have been the mechanisms for the random lasers, which explain the broad lasing spectrum in the measurement results shown in Figure 4. The spectral bandwidth of roughly 5 nm or even larger than 7 nm at FWHM has been observed with the incoherent random lasers, as reported in the studies by Xia et al and Weng et al, [ 35,36 ] verifying the random lasing nature of the observed emission spectra.…”
Section: Random Lasing Performancesupporting
confidence: 75%
“…When the optical gain property was further characterized, we observed that the neat film exhibited a remarkably low threshold EthASE, 6.0 µJ cm −2 ) with an exceptional narrow FWHM (2.6 nm) under the vacuum condition (10 −4 Pa), which is similar to the previously reported organic lasers (Figure 1b). [ 12,57–65 ] This deep‐blue ASE emission exhibited a peak at 427 nm, belonging to the 0–1 transition, and the emission can be achieved repeatedly with films spin coated from the toluene solution of MC8‐Th (10 mg mL −1 ). Furthermore, after dispersing MC8‐Th (10 wt%) into inert PS matrix, we achieved a kind of deep‐blue random laser emission (under vacuum condition) with a lower EthASE of 4.1 µJ cm −2 (Figure 1c).…”
Section: Photophysical Properties Of Mc8‐th In Various Statesmentioning
confidence: 96%
“…Random lasers (RLs) have been the subject of intense research owing to their easy fabrication, low coherence, and small size [8][9][10][11][12][13][14][15][16][17]. The lasing feedback mechanism is synergistically achieved by multiple light scattering, which is different from traditional lasers [18][19][20][21][22][23][24][25][26][27].…”
Section: Introductionmentioning
confidence: 99%