2015
DOI: 10.1109/jphot.2014.2381662
|View full text |Cite
|
Sign up to set email alerts
|

Highly Efficient Tunable Dispersive Wave in a Tellurite Microstructured Optical Fiber

Abstract: We demonstrate a highly efficient, stable, and tunable dispersive wave (DW) emitted by the soliton in a tellurite microstructured optical fiber. The dependence of the generated DW properties on the average pump power is experimentally investigated.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
6
0

Year Published

2015
2015
2024
2024

Publication Types

Select...
8

Relationship

0
8

Authors

Journals

citations
Cited by 21 publications
(6 citation statements)
references
References 27 publications
0
6
0
Order By: Relevance
“…The center wavelength of the emitted FOCR is shifting from 1685 nm to 1626 nm as the pump power is increasing from 250 mW to 440 mW, and the conversion efficiency grows monotonously with the input pump power, reaching impressive 67.4% at ~495 mW. There are two potential reasons to explain such a very high efficiency of FOCR generation demonstrated in this work [39]. One is the high nonlinear refractive index of the tellurite glass as compared to silica glass.…”
Section: Current Progress In Fiber-optic Cherenkov Radiationmentioning
confidence: 87%
See 1 more Smart Citation
“…The center wavelength of the emitted FOCR is shifting from 1685 nm to 1626 nm as the pump power is increasing from 250 mW to 440 mW, and the conversion efficiency grows monotonously with the input pump power, reaching impressive 67.4% at ~495 mW. There are two potential reasons to explain such a very high efficiency of FOCR generation demonstrated in this work [39]. One is the high nonlinear refractive index of the tellurite glass as compared to silica glass.…”
Section: Current Progress In Fiber-optic Cherenkov Radiationmentioning
confidence: 87%
“…Most recently, Cheng et al reported extremely high conversion efficiency of FOCR over 65% with a four-hole tellurite microstructured optical fiber (TMOF) [39]. The calculated fundamental mode refractive index and dispersion curve of the TMOF with ~4.7 μm core diameter are shown in Figs.…”
Section: Current Progress In Fiber-optic Cherenkov Radiationmentioning
confidence: 99%
“…Currently, high-power fiber-optical amplifier with a Watt-level output was developed by double-claddingpumping technology so that the output power of 1.55 m femtosecond fiber-laser could be scaled up and commercially available [4]. And with higher pulse energy, the parameters for evaluating the nonlinear interactions between energetic femtosecond pump pulses and nonlinear wavelength conversion fiber, including the dispersion length and nonlinear length, at specific condition should be carefully calculated or simulated to determine the optimum length of the nonlinear fiber [20].Third, the only free-space part, showing in the point B in Fig. 1, in this demonstrated source can be replaced by proper fiber slicing technology as shown in [18].…”
Section: Application Of the Fiber-based Femtosecond Source On Nonline...mentioning
confidence: 99%
“…Liu et al has reported a 0.58-0.63 m DW [18] with a 4.8 mW maximum DW power while Nishizawa's group has demonstrated a 0.6-0.68 m DW with a $1 mW DW power [19]. In 2015, a highly efficient tunable 1.63 $ 1.68 m DW have been reported where an optical parametric oscillator (OPO) working at 1.76 m was used as excitation and a Tellurite microstructured fiber was utilized as a wavelength up convertor [20]. Compared with other's work, the reported optical power was high-enough to perform NLM.…”
Section: Introductionmentioning
confidence: 99%
“…The blueshifted DWs holds much attention of the scientific communities. The ample number authors have generated a blue-shifted DWs like, A range of DW was observed from 580 to 630 nm by employing 300-mW ytterbium laser [23], from 300 to 800 nm by using an erbium laser with 7% energy transfer efficiency [24], nearby 430 nm with 800-nm pumping with 15% of the total energy [25], nearby 640 nm with a fifth order soliton [26] and from 1626 to 1685 nm with the average pump power changing from 250 to 440 mW at the pump wavelength of 1760 nm [27]. The red-shifted DW depended mainly on ultra-short pulses with a verylow anomalous dispersion at the pumping wavelength.…”
Section: Introductionmentioning
confidence: 97%