2014
DOI: 10.1016/j.jlumin.2014.01.003
|View full text |Cite
|
Sign up to set email alerts
|

Multimode laser emission from free-standing cylindrical microcavities

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2

Citation Types

0
8
0

Year Published

2015
2015
2023
2023

Publication Types

Select...
6
1

Relationship

2
5

Authors

Journals

citations
Cited by 19 publications
(8 citation statements)
references
References 21 publications
0
8
0
Order By: Relevance
“…In our lasing experiment, external feedback at the cuvette sides might have encouraged the lasing action. It was expected that both the stimulated emission along with the gain guiding and the external feedback at the cuvette sides would induce a high gain for the laser action [16]. The occurrence of mode structure from dye solution was also reported by Guang et al, where the laser emission was attributed to the Fresnel reflection feedback from the two parallel optical windows of the cuvette [17].…”
Section: Resultsmentioning
confidence: 69%
“…In our lasing experiment, external feedback at the cuvette sides might have encouraged the lasing action. It was expected that both the stimulated emission along with the gain guiding and the external feedback at the cuvette sides would induce a high gain for the laser action [16]. The occurrence of mode structure from dye solution was also reported by Guang et al, where the laser emission was attributed to the Fresnel reflection feedback from the two parallel optical windows of the cuvette [17].…”
Section: Resultsmentioning
confidence: 69%
“…It should be also noted that compared with lateral pumping scheme, the laser peak wavelengths exhibits some red shift for longitudinal pumping scheme, which could be attributed to self‐absorption effect caused by the overlap between the absorption and emission spectra of rhodamine B. Since WGM laser is propagating surrounding the cross sectional periphery of the capillary, for longitudinal pumping scheme fluorescence light would be absorbed by rhodamine B molecules adjacent to the microcavity layer and converted into longer wavelength light through re‐emission process .…”
Section: Resultsmentioning
confidence: 99%
“…The self-propelling droplet was still able to generate strong WGM lasing due to total internal reflection on its spherical surface, as shown in Figure c. However, the slow dissolution of nematic LC molecules triggered a small blue-shift tendency in the spectrum due to the Stokes shift and two-photon absorption. , Interestingly, the swimming motions and trajectories of the microlaser change with the droplet diameter, including random, zigzag, and straight motions (Figure d). This phenomenon is consistent with a phenomenological theory about self-propelled objects: linear motion becomes unstable under a large diameter or high velocity, and then helical motion spontaneously appears. Under a fixed droplet size, the velocity can also be manipulated by changing the surfactant concentrations (Figure e).…”
mentioning
confidence: 94%