2020
DOI: 10.1039/c9nr07034f
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A ring-shaped random laser in momentum space

Abstract: A color-switchable random laser is designed through directly coupling random laser with a commercial optical fiber. By using a simple approach of selectively coating the random gain layer on the surface of fiber, the red and yellow random lasers are respectively achieved with low threshold and good emission direction due to the guiding role of optical fibers. Moreover, the unique coupling mechanism leads to the random lasing with ring-shape in momentum space, indicating an excellent illuminating source for hig… Show more

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Cited by 40 publications
(22 citation statements)
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References 39 publications
(38 reference statements)
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“…If the ratio δ = δν/Δν is less than one, the optical path is in a localized regime as shown in previous studies. , Indeed, our measured spectra (Figure a) do fulfill this criteria. To examine a more detailed characteristic of the random laser action, we have performed PFT analysis to calculate the effective cavity length of the random laser as shown in Figure S2. The obtained effective cavity length of around 11.01 μm is in the same order of magnitude as previous reports. , By comparing the cavity length and the thickness of the device, we find that most of the close-loop resonance paths should be horizontal to the top surface. In addition, since metal nanoparticles play an important role in the localization, the fact that the close-loop resonance paths are close to the top surface further confirms the illustration shown in Figure c.…”
Section: Resultssupporting
confidence: 54%
“…If the ratio δ = δν/Δν is less than one, the optical path is in a localized regime as shown in previous studies. , Indeed, our measured spectra (Figure a) do fulfill this criteria. To examine a more detailed characteristic of the random laser action, we have performed PFT analysis to calculate the effective cavity length of the random laser as shown in Figure S2. The obtained effective cavity length of around 11.01 μm is in the same order of magnitude as previous reports. , By comparing the cavity length and the thickness of the device, we find that most of the close-loop resonance paths should be horizontal to the top surface. In addition, since metal nanoparticles play an important role in the localization, the fact that the close-loop resonance paths are close to the top surface further confirms the illustration shown in Figure c.…”
Section: Resultssupporting
confidence: 54%
“…An estimate of the effective cavity length L c of the RL can be obtained by the power Fourier transform (PFT) method. [ 44,45 ] Specifically, emission spectra were recalculated with respect to inverted wavelength scale k = 2π/λ and used for calculating PFT as a function of path length in microns. [ 46 ] The positions of local maxima are related to the optical cavity lengths L c via the equation pm = mnLnormalcπ, where p m is the peak in PFT plot, m is the order of the Fourier harmonic and n is the refractive index of the gain medium.…”
Section: Resultsmentioning
confidence: 99%
“…The divergences in fluoride phase separation and the corresponding nanocrystallization lead to varieties in the lasing behavior. Under 980 nm ns‐pulsed laser excitation, random lasing occurs when the pumping power density exceeds the threshold value, 72 which is represented by the sudden increase in the slope of emission intensity against power density (insets in Figure and generated in Table 4). To become ideal random lasing with a lower threshold value, optical materials are required to have larger, uniformly dispersed and high refractive index phases to support the strong scattering in active random medium 73,74 .…”
Section: Resultsmentioning
confidence: 99%