2023
DOI: 10.1063/5.0137542
|View full text |Cite
|
Sign up to set email alerts
|

Order controllable enhanced stimulated Brillouin scattering utilizing cascaded diamond Raman conversion

Abstract: We report on the design and operation of a laser, which outputs wavelengths in the 1.2 and 1.5  μm ranges by leveraging two non-linear processes of stimulated Raman scattering and stimulated Brillouin scattering in diamond. By precisely controlling characteristics of the laser resonator formed around the diamond crystal, we are able to selectively control the onset of each non-linear process so as to tailor laser output characteristics both in way of wavelength and output power. This work demonstrates the high… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

1
0
0

Year Published

2023
2023
2024
2024

Publication Types

Select...
8

Relationship

3
5

Authors

Journals

citations
Cited by 19 publications
(6 citation statements)
references
References 45 publications
1
0
0
Order By: Relevance
“…When the cavity length was precisely increased and decreased by only 14 μm, the spectrum was as illustrated in Figures 3(c) and 3(e), respectively. A satellite peak at a separation of about 70 GHz appeared on the longer wavelength side of the SRS, which matched the theoretical diamond Brillouin frequency shift reported previously [ 29 31 ] . At that time, the FPI trace was as shown in Figures 3(d) and 3(f), respectively, and the longitudinal structure was tuned to multiple-longitudinal modes.…”
Section: Resultssupporting
confidence: 90%
“…When the cavity length was precisely increased and decreased by only 14 μm, the spectrum was as illustrated in Figures 3(c) and 3(e), respectively. A satellite peak at a separation of about 70 GHz appeared on the longer wavelength side of the SRS, which matched the theoretical diamond Brillouin frequency shift reported previously [ 29 31 ] . At that time, the FPI trace was as shown in Figures 3(d) and 3(f), respectively, and the longitudinal structure was tuned to multiple-longitudinal modes.…”
Section: Resultssupporting
confidence: 90%
“…When the input voltage is set to 900 V, the pump energy is 428 mJ, the Stokes energy is 388 mJ, and the energy reflectivity is 90.7%. Moreover, the beam profile of the injected pump light was improved to some extent via the action of SBS-PCM, and the energy distribution of the laser spot output became more uniform [20,21].…”
Section: Resultsmentioning
confidence: 99%
“…When the input voltage is set to 900 V, the pump energy is 428 mJ, the Stokes energy is 388 mJ, and the energy reflectivity is 90.7%. Moreover, the beam profile of the injected pump light was improved to some extent via the action of SBS-PCM, and the energy distribution of the laser spot output became more uniform [20,21]. In the Stokes light amplification experiment, the generated Stokes beam is separately injected into two amplification cells for amplification, and the injected Stokes light is amplified by extracting the energy from the injected pump light; the energy change in the two is shown in Figure 6.…”
Section: Resultsmentioning
confidence: 99%
“…According to the principle of optical communication [18], it is possible to calculate the time delay of the small angle analysis method as follows:…”
Section: Frontiers In Physics Frontiersinorg Modelmentioning
confidence: 99%