Advanced Topological Insulators 2019
DOI: 10.1002/9781119407317.ch6
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Q‐Switching Pulses Generation Using Topology Insulators as Saturable Absorber

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Cited by 5 publications
(2 citation statements)
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“…becomes broader with raising the pump level due to laser pulses becoming shorter with high intensity. 51 To demonstrate the proposed EDFL performance, rate, width, and average output power of the generated pulses, as well as their optical energy versus LD power, were achieved. For the 3 dB optical coupler, the repetition rate and width of output laser pulses were determined for pump power range from 96.25 to 167 mW and plotted in Figure 6A.…”
Section: Resultsmentioning
confidence: 99%
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“…becomes broader with raising the pump level due to laser pulses becoming shorter with high intensity. 51 To demonstrate the proposed EDFL performance, rate, width, and average output power of the generated pulses, as well as their optical energy versus LD power, were achieved. For the 3 dB optical coupler, the repetition rate and width of output laser pulses were determined for pump power range from 96.25 to 167 mW and plotted in Figure 6A.…”
Section: Resultsmentioning
confidence: 99%
“…Therefore, the nonlinearities due to adding Cr 2 AlC SA within EDFL ring, such as self‐phase modulation and cross‐phase modulation, would push the center wavelength to the shorter wavelength. Also, the spectrum becomes broader with raising the pump level due to laser pulses becoming shorter with high intensity 51 …”
Section: Resultsmentioning
confidence: 99%