Jun Ye

Dr. Jun Ye

orcid

Research Focus & Metrics

Academic Career Length

11Years (2016-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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23 September 2019 in Optics Express
Verified
Journal Article
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YZYang Zhang
Yang Zhang
JSJiaxin Song
Jiaxin Song
JYJun Ye
Jun Ye
JXJiangming Xu
Jiangming Xu
TYTianfu Yao
Tianfu Yao
PZPu Zhou
Pu Zhou
We demonstrate a tunable, high order cascaded random Raman fiber laser (RRFL) with high purity at 1.7 µm band by using a high power amplified spontaneous emission source (ASE) with both wavelength and linewidth tunability as pump source. The influence of the spectral bandwidth of the ASE source on the spectral purity of the output at 1.7 µm band is investigated. By adjusting the spectral bandwidth of the ASE source to the optimized 20 nm, output power >14 W with spectral purity up to 98.29% at 1715 nm is achieved. As far as we know, this is the highest spectral purity ever reported for a RRFL at 1.7 µm region. Furthermore, by adjusting the central wavelength of ASE source, the output of the RRFL can be tuned from 1695 to 1725 nm with >10 W output power. What’s more, the spectral purity is above 92% over a tuning range from 1705 to 1725 nm.

6 December 2019 in Photonics Research
Verified
Journal Article
Closed access
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JXJiangming Xu
Jiangming Xu
JWJian Wu
Jian Wu
JYJun Ye
Jun Ye
JSJiaxin Song
Jiaxin Song
BYBaicheng Yao
Baicheng Yao
YRYunjiang Rao
Yunjiang Rao
The famous demonstration of optical rogue waves (RWs), a powerful tool to reveal the fundamental physics in different laser scenarios, opened a flourishing time for temporal statistics. Random fiber laser (RFL) has likewise attracted wide attention due to its great potential in multidisciplinary demonstrations and promising applications. However, owing to the distinctive cavity-free structure, it is a scientific challenge to achieve temporal localized RWs in RFLs, whose feedback arises from multiple scattering in disordered medium. Here, we report the exploration of RW in the highly skewed, transient intensity of an incoherently pumped RFL for the first time, to our knowledge, and unfold the involved kinetics successfully. The corresponding frequency domain measurements demonstrate that the RW event arises from a crucial sustained stimulated Brillouin scattering process with intrinsic stochastic nature. This investigation highlights a novel path to fully understanding the complex physics, such as photon propagation and localization, in disordered media.

23 January 2023 in Photonics Research
Verified
Journal Article
Closed access
SLSicheng Li
Sicheng Li
JXJiangming Xu
Jiangming Xu
JLJunrui Liang
Junrui Liang
JYJun Ye
Jun Ye
YZYang Zhang
Yang Zhang
PZPu Zhou
Pu Zhou
In past decades, multi-wavelength lasers have attracted much attention due to their wide applications in many fields. In this paper, we demonstrate a multi-wavelength random fiber laser with customizable spectra enabled by an acousto–optic tunable filter. The operating wavelength range can be tuned from 1114.5 to 1132.5 nm with a maximal output power of 5.55 W, and spectral channel tuning can also be realized with a maximal number of five. The effect of gain competition and the interaction between Raman gain and insertion loss are also analyzed. Furthermore, the output spectra can be ordered by radiating appropriate radio frequency signals to the acousto–optic tunable filter. This work may provide a reference for agile shape spectrum generation and promote multi-wavelength random fiber laser practicability in sensing, telecommunications, and precise spectroscopy.

5 February 2021 in Optics Express
Verified
Journal Article
Open access
PDF file
YZYang Zhang
Yang Zhang
JYJun Ye
Jun Ye
XMXiaoya Ma
Xiaoya Ma
JXJiangming Xu
Jiangming Xu
JSJiaxin Song
Jiaxin Song
PZPu Zhou
Pu Zhou
Multiwavelength fiber lasers, especially those operating at optical communication wavebands such as 1.3 μm and 1.5 μm wavebands, have huge demands in wavelength division multiplexing communications. In the past decade, multiwavelength fiber lasers operating at 1.5 μm waveband have been widely reported. Nevertheless, 1.3 μm waveband multiwavelength fiber laser is rarely studied due to the lack of proper gain mechanism. Random fiber laser (RFL), owing to its good temporal stability and flexible wavelength tunability, is a great candidate for multiwavelength generation. Here, we reported high power multiwavelength generation at 1.3 μm waveband in RFL for the first time. At first, we employed a section of 10 km G655C fiber to provide Raman gains, as a result of which, 1.07 W multiwavelength generation at 1.3 μm waveband with an optical to signal noise ratio of ∼33 dB is demonstrated. By tuning the pump wavelength from 1055 nm to 1070 nm, tunable multiwavelength output covering the range of 1300-1330 nm can be achieved. Furtherly, we realized 4.67 W multiwavelength generation at 1.3 μm waveband by shortening the fiber length to 4 km. To the best of our knowledge, this is the highest output power ever reported for multiwavelength fiber lasers.

7 August 2019 in Photonics Research
Verified
Journal Article
Closed access
JYJun Ye
Jun Ye
JXJiangming Xu
Jiangming Xu
JSJiaxin Song
Jiaxin Song
YZYang Zhang
Yang Zhang
HZHanwei Zhang
Hanwei Zhang
PZPu Zhou
Pu Zhou

19 March 2020 in Optics Letters
Verified
Journal Article
Closed access
JYJun Ye
Jun Ye
YZYang Zhang
Yang Zhang
JXJiangming Xu
Jiangming Xu
JSJiaxin Song
Jiaxin Song
TYTianfu Yao
Tianfu Yao
PZPu Zhou
Pu Zhou
A flat-amplitude multi-wavelength random Raman fiber laser with broad spectral coverage and a high optical signal-to-noise ratio (OSNR) is challenging and of great interest. In this Letter, we theoretically and experimentally proved that broadband pumping can help realize a broader, flat-amplitude multi-wavelength random Raman fiber laser. The influence of pump bandwidth, tunability of the spectral envelope, and channel spacing are investigated. As a result, with a 40 nm pump bandwidth, a spectral coverage of 1116–1125 nm with 19 laser lines and 31 dB OSNR is achieved, and the standard deviation in the peak intensities of the central nine lines is ∼ 1 . 1 d B m . This technique can also be applied to the multi-wavelength Raman (or random Raman) fiber lasers at other wavelengths and provide a reference for multi-wavelength applications in sensing, communication, and optical component testing.