Xueming Liu’s research while affiliated with Nanjing University of Information Science and Technology and other places

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Publications (170)


Dual-state vector soliton in mode-locked fiber laser
  • Article

January 2023

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100 Reads

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12 Citations

Optics & Laser Technology

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Lin Huang

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Xueming Liu

Vector soliton originates from the soliton trapping dynamics via cross-phase modulation (XPM) which has been used to achieve supercontinuum, optical switching and optical analog of gravity-like potentials. Dual-state vector soliton (DSVS) is reported in mode-locked fiber laser under appropriate birefringence. Two vector soliton states emitted alternatively display double-peak and Lorentz-shaped spectral profile, respectively. The two orthogonally polarized components of the double-peak spectrum exhibit obvious redshift and blueshift, respectively, while the frequency shift for the other state is limited even with the reversed shift direction, which illustrates a unique vector soliton evolution dynamic. DSVS originates from the pulse trapping induced by XPM, as well as the periodical evolution and frequency shift induced by self-phase modulation under dispersion-managed condition. The vector period-doubling phenomenon will further enrich the understanding about soliton, and also guide the design of mode-locked laser.


Figure 1. (a) Conceptual illustration of SMC. Pulses with red and blue colors correspond to the two frequencies that are trapped via XPM. When the light-red pulse is absent, the illustration describes the 2+1 SMC, and all the four pulses can model 2+2 SMC. Panel-Ⅰ: spectrum of 2+1 SMC; Panel-Ⅱ: temporal profile of 2+1 SMC; Panel-Ⅲ: spectrum of 2+2 SMC; Panel-Ⅳ:
Figure 2. Characterizations of the 2+1 SMC. (a) Real-time spectral evolution measured using DFT. The energy evolution of pulses at 1550 nm and 1570 nm are the grey and white lines, respectively. (b) Single-shot spectrum corresponding to the last frame of (a). (c) Autocorrelation traces calculated via the Fourier transform of single-shot spectrum in (b). (d) Pulse train measured directly by OSC. Insert: Fundamental RF spectrum with the range of 10 kHz. (e) Optical spectra of 2+1 SMC for three other cases measured by OSA.
Fig. 4. Simulation results of 2+1 SMC. (a) Optical spectrum and (b) tempotal profile of stable 2+1SMC. (c) Spectral evolution of vibrating 2+1 SMC with respect to roundtrips. (d) Evolution of pulse with respect to roundtrips. (e) Evolution of the temporal separation and relative phase of TSM at 1550 nm. (f) Evolution of wavelength separation.
Fig. 5. Simulation results of 2+2 SMC. (a) Spectral evolution of vibrating 2+2 SMC. Evolution of the temporal separation and relative phase of TSMs at (b) 1550 nm and (c) 1570 nm. (d) Evolution of wavelength separation (Δλ) between two wavelengths.
Dichromatic soliton-molecular compounds in synchronized mode-locked fiber lasers
  • Preprint
  • File available

November 2022

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375 Reads

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Yusheng Zhang

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Soliton molecules have been a striking research area, which is significant for the exploration of physical mechanism in various nonlinear systems, the analog to the molecule of matter, and the potential applications in multilevel encoding of optical communications. Here, we demonstrate a novel dichromatic soliton-molecular compound (SMC) that is a hybrid bound states of multiple pulses with two different frequencies connected by two different binding mechanisms. It exhibits unique temporal and spectral profiles that can be described as the bounded temporal and dichromatic soliton molecules. The vibrating SMCs are generated experimentally and numerically to demonstrate the intrinsic solution in the dissipative nonlinear system, which is characterized with the vibration both in time and frequency dimensions and dual-peak evolution trajectory induced by the time-frequency coupling. These results enrich the concept of soliton molecules and further promote the analogy to matter molecules.

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Solitons: XPM‐Induced Vector Asymmetrical Soliton with Spectral Period Doubling in Mode‐Locked Fiber Laser (Laser Photonics Rev. 15(3)/2021)

March 2021

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81 Reads

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1 Citation

In article number 2000216, Xueming Liu and co‐workers demonstrate novel optical nonlinear dynamics in a mode‐locked laser induced by the coupling interaction of two orthogonally polarized pulses via cross‐phase modulation (XPM). The XPM‐induced vector asymmetrical soliton displays period‐doubling spectral evolution with alternate redshift and blueshift, which is helpful to laser design and brings useful insights into the optical nonlinearity and chaos for solitons.


XPM‐Induced Vector Asymmetrical Soliton with Spectral Period Doubling in Mode‐Locked Fiber Laser

February 2021

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671 Reads

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53 Citations

Cross phase modulation (XPM) can induce soliton trapping in nonlinear medium, which has been employed to achieve vector soliton, optical switching, and optical analog of gravity‐like potentials. Here, the first observation of a novel soliton operation is reported whose wavelength exhibits redshift and blueshift periodically in a mode‐locked fiber laser under appropriate birefringence and dispersion map. XPM dominates the dynamics by inducing and sustaining the vector asymmetrical soliton (VAS) with spectral period doubling, and exhibits a unique trajectory of pulse trapping. The XPM‐induced VAS is an idiosyncratic steady state featured with asymmetry in the model based on the coupled Ginzburg–Landau equation, which depicts the distinct pulse features in comparison with vector soliton, soliton molecule, and traditional period‐doubling evolutions. The two orthogonal polarized directions of mode‐locked fiber laser can be regarded as the XPM‐coupled dissipative resonators guiding the further study of the optical nonlinear dynamics and chaos for soliton, which is helpful to laser design and brings useful insights into nonlinear science and applications.


Experiment setup for the mode-locking fiber laser and the measuring system. LD, laser diode. ${D_s}$ , ${D_p}$ , and ${D_i}$ are the dispersion values of the dispersion-compensating fiber, through which the signal, pump, and idler pulses pass, respectively. The time lens system performed through FWM in a 100 m highly nonlinear optical fiber.
Real-time spectral and temporal evolution dynamics for stable dissipative solitons. (a) Temporal evolution recorded by the time lens. The extracted pulse duration ( $\Delta \tau$ ) and single-shot temporal profile are shown in the right subfigure and top subfigure, respectively. (b) Spectral evolution recorded by the DFT technique. The extracted spectral bandwidth ( $\Delta \lambda$ ) and single-shot spectral profile are shown in the right subfigure and top subfigure, respectively. (c) Averaged spectrum recorded by an OSA. (d) RF spectrum.
Real-time spectral and temporal evolution dynamics for creeping solitons. (a) Temporal evolution recorded by the time-lens technique. Right subfigures: evolution of (i) pulse peak position ( ${t_p}$ ) and (ii) temporal width ( $\Delta \tau$ ). (b) Extracted single-shot temporal profiles at RT-200 and RT-700. (c) Pulse train recorded by oscilloscope directly; (d) real-time spectral evolution with extracted spectral bandwidth shown in the right subfigure. (e) Extracted single-shot spectral profiles at RT-200 and RT-700.
Real-time spectral and temporal dynamics for creeping soliton with different motion distances. Single-shot temporal intensity recorded by the time lens with the extracted pulse duration shown in the top subfigure for (a) small distance and (c) large distance. Real-time spectra recorded by the DFT technique with extracted spectral bandwidth shown in the top subfigure for (b) small distance and (d) large distance.
Full-field real-time characterization of creeping solitons dynamics in a mode-locked fiber laser

November 2020

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106 Reads

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57 Citations

Creeping solitons, which belong to the class of pulsating solitons, can be meaningful for fundamental physics owing to their fruitful nonlinear dynamics. Their characteristics in mode-locked lasers have been studied theoretically, but it is difficult to experimentally observe evolution dynamics in real time. Here, we have experimentally observed the temporal and spectral evolution dynamics of creeping solitons in a passively mode-locked fiber laser by employing time-lens and dispersive Fourier transform technique. With the aid of Raman amplification, the measured recording length of the time lens in the asynchronous mode could be substantially improved. Temporal soliton snaking motion and spectral breathing dynamics are experimentally obtained, confirming intrinsic feature of pulsation dynamics. These results display how single-shot measurements can offer new insights into ultrafast transient dynamics in nonlinear optics.


(a) TEM image, (b) HRTEM Image, (c) SAED image of LPE α-In2Se3 nanosheets. (d) AFM Image of GIHS. Above: height variation near the edge of graphene (red line); Below: height variation of α-In2Se3 nanosheets on graphene substrate (blue line). (e) Raman spectrum of GIHS. (f) Optical transmission spectrum of graphene, α-In2Se3, GIHS and quartz substrate.
Open-aperture Z-scan measurement of (a) graphene, (b) α-In2Se3 and (c) GIHS.
(a) Transient absorption dynamics of Graphene, α-In2Se3 and GIHS with pump and probe wavelengths of 800 nm and 750 nm, respectively. (b) Long scale of transient absorption dynamics of α-In2Se3 and GIHS.
(a) Optical image of GIHS on fiber facet. (b) Nonlinear saturable absorption curve of in-line GIHS SA and graphene. (c) Schematics of the typical erbium-doped fiber laser for passive mode-locking operation with GIHS SA. (d) Output spectrum with 0.02 nm spectral resolution. (e) Oscilloscope trace of output pulse trains; inset: RF spectrum; (f) Interferometric autocorrelation trace of output pulses after amplification and compression.
Graphene/α-In2Se3 heterostructure for ultrafast nonlinear optical applications

October 2020

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85 Reads

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7 Citations

Two-dimensional (2D) heterostructure materials have attracted increasing attention in ultrafast nonlinear optical applications due to their intriguing properties. Here, we fabricate a graphene/α-In2Se3 heterostructure by dropping α-In2Se3 dispersion onto the surface of few-layered graphene film and investigate its nonlinear optical responses. We show that the graphene/α-In2Se3 heterostructure has combined advantages of ultrafast relaxation (τ1 ∼ 78 fs, τ2 ∼ 14 ps) and a large effective nonlinear absorption coefficient (βeff ∼ −1.2 × 10⁴ cm/GW) with relatively large modulation depth. We have further integrated the heterostructure into an erbium-doped fiber laser for mode-locked pulse generation. These results indicate that graphene/α-In2Se3 heterostructures are a promising 2D material for ultrafast nonlinear optical applications.


Schematic representation of the AFTM system. The repetition period difference between the signal and pump is $|{T_1} - {T_2}|$ .
(a) Experimental setup of asynchronous, single-shot measurement system. (b) Three different snapshots of the optical spectrum after the HNLF from an optical spectrum analyzer.
(a), (c), and (e) Different single-shot measured temporal evolution dynamics over 1000 RTs for soliton pairs with narrower separation. (b), (d), and (f) Corresponding measured waveforms at three different evolution RTs.
Real-time temporal characterization of soliton pairs with wider separation. Experimental measured temporal evolution dynamics over 1000 RTs for soliton separation of (a) 18.9 ps and (c) 79 ps. Measured waveforms at three different evolution RTs for soliton separation of (b) 18.9 ps and (d) 79 ps.
Unveiling external motion dynamics of solitons in passively mode-locked fiber lasers

August 2020

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236 Reads

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11 Citations

Real-time measurement of ultrafast pulses together with high temporal resolution and long recording length is an urgent requirement of all optical communication systems and nonlinear science. Here, external motion dynamics of soliton pairs in mode-locking ultrafast fiber lasers can be single-shot characterized with long recording length, by using an asynchronous four-wave-mixing (FWM)-based temporal magnifier (AFTM) system. Recording length of more than one thousand roundtrips can be achieved through the AFTM system. Temporal propagation dynamics of soliton pairs with tunable separations are observed, revealing that soliton pairs with narrower separation display vibration-like dynamics, while the two solitons with wider separation remain relatively unchanged. We believe our results will provide a promising solution for real-time measurement of ultrafast pulse and can offer novel insights for ultrafast transient dynamics in nonlinear optics.


Citations (84)


... Compared to conventional spectrometers, the DFT technique offers the additional benefit of the dispersive medium also functioning as an optical amplifier, optimizing the balance between the sensitivity, speed, and resolution through the distributed amplification of optical pulses in the dispersive fibres [106], [148], [149]. Subsequently, the DFT technique has been extensively employed by researchers to observe and analyse complex soliton dynamics, paving the way for real-time observations of interactions in complex nonlinear systems [150]- [152]. ...

Reference:

Temporal and spatiotemporal soliton molecules in ultrafast fibre lasers
Dual-state vector soliton in mode-locked fiber laser
  • Citing Article
  • January 2023

Optics & Laser Technology

... The emergence of group-velocity-locked vector solitons results from the soliton trapping effect related to the birefringence of the fiber cavity. 41,42 When the net birefringence of the cavity is weak, it can be compensated by the nonlinearity. To travel at the same group velocity, both orthogonal pulses of the vector soliton hold the same central wavelengths, as shown in Fig. 4(a). ...

XPM‐Induced Vector Asymmetrical Soliton with Spectral Period Doubling in Mode‐Locked Fiber Laser

... Thus, complicated nonlinear soliton dynamics could be expected, regardless of whether it is the single soliton [2][3][4] or multiple soliton states [5][6][7] . Over the several years, various ultrafast processes, including noise-like pulse 8,9 , optical rogue waves [10][11][12][13] , soliton explosion 14,15 , soliton molecule evolution [16][17][18][19][20] , pulsating solitons [21][22][23][24][25] , and buildup dynamics of solitons in mode-locked lasers [26][27][28][29][30] , have been explored in real-time thanks to the time-stretched Dispersive Fourier transform (TS-DFT) 31 and time-lens techniques 29,32,33 . Real-time spectral dynamics of many ultrafast or transient (non-repeatable) nonlinear phenomena have been unveiled utilizing the simple but powerful TS-DFT technique, which largely provides insights into the complicated nonlinear soliton dynamics in ultrafast lasers, which are typical dissipative systems. ...

Full-field real-time characterization of creeping solitons dynamics in a mode-locked fiber laser

... Benefiting from a strong or rapid near-field interaction between light and nanomaterials, the nonlinearity of MNFs decorated with nanomaterials could be enhanced (Zhang H et al., 2012;Duan et al., 2015;He et al., 2016). Therefore, this composite structure can be exploited as a saturated absorber to generate ultrashort pulses (Luo ZC et al., 2018;Li YH et al., 2019;Liu M et al., 2020;Wang LZ et al., 2020) and provide advantages over nanomaterials alone, such as a high optical damage threshold (Liu M et al., 2020). The commonly used nanomaterials include graphene (He et al., 2016;Liu XM et al., 2016;Yang G et al., 2016;Cai et al., 2017;Wu et al., 2022), MXenes (Ahmad et al., 2021), topological insulators (Ahmad et al., 2022), and quantum dots (Du et al., 2017). ...

Graphene/α-In2Se3 heterostructure for ultrafast nonlinear optical applications

... Moreover, by analysing real-time DFT-based spectra, the vibrational roundtrip-to-roundtrip evolution of SM parameters, such as separations and phases, has been indirectly probed 11,12 . On the other hand, time lens (TL) technology, a subset of TM, enables direct observation of the dynamics of soliton pairs with tunable separations 13,14 and creeping solitons 15 with sub-picosecond resolutions. These measurement methods share the common objective of understanding ultrafast pulse dynamics by successively capturing single-shot pulses. ...

Unveiling external motion dynamics of solitons in passively mode-locked fiber lasers

... Second, the optoacoustic effect gives rise to both attraction and repulsion [128]- [130], induced in the fibre through electrostriction by high-intensity optical pulses, can create a weak frequency shift between successive pulses. This interaction leads to the pulse-to-pulse attraction, affecting the pulse bunching and stability over the course of multiple round-trips [131], [132]. In fibre lasers employing NPR, a CW component can coexist with solitons and induce their central-frequency shift [133]. ...

Microfiber-assisted gigahertz harmonic mode-locking in ultrafast fiber laser

... This has led to advanced UO-TDT techniques such as temporal imaging 27,28 , time-stretch imaging 29 , serial time-encoded amplified microscopy (STEAM) 30 , free-space angular chirp-enhanced delay (FACED) 31 and dispersive temporal interferometry (DTI) 32 . Temporal resolutions of hundreds of femtoseconds, with frame rates up to hundreds of megahertz, can be achieved, leading to applications including velocimetry 33 , spectroscopy 34 , imaging 29 and quantum science 35 . ...

Dynamics of carbon nanotube-based mode-locking fiber lasers

... Other approach based on evanescent filed can be a candidate and SWNTs can be coated on a D-shaped fiber [171,172], microfiber [173,174], or injected into microslot [175,176], photonic crystal fiber [177] and hollow core fiber [178]. Recently, the development of SWNT SAs pays more attention on power handing, environmental stability and more outstanding SA characteristics including sol-gel method and glass doping [179,180]. ...

Glass-Hosted Carbon Nanotubes as a Saturable Absorber for Ultrafast Laser
  • Citing Conference Paper
  • June 2019

... most promising materials for photonic devices, which benefit from its advantages in absorption rate, mobility and saturation drift velocity. [21][22][23][24][25][26] Consequently, its operational performance has been experimentally investigated for pulsed laser generation in both solid-state and fiber lasers. [27][28][29][30][31] However, for ultrafast lasers, one of the most critical specifications is the pulse width. ...

Harmonic Mode‐Locking: Revealing the Buildup Dynamics of Harmonic Mode‐Locking States in Ultrafast Lasers (Laser Photonics Rev. 13(9)/2019)
  • Citing Article
  • September 2019

... Two widely adopted real-time measurement techniques-dispersive Fourier transform (DFT) 4 and time microscopy (TM) 5 -have enabled the spectral and temporal observation of pulse transient dynamics with fine resolutions, surpassing that of current commercial measurement instruments. DFT-based real-time spectroscopy has provided insights into the transient spectral buildup processes of diverse pulse patterns, including solitons 6 , SMs 7 , harmonic mode-locking states 8 , soliton explosions 9 , and rogue waves 10 . Moreover, by analysing real-time DFT-based spectra, the vibrational roundtrip-to-roundtrip evolution of SM parameters, such as separations and phases, has been indirectly probed 11,12 . ...

Revealing the Buildup Dynamics of Harmonic Mode‐Locking States in Ultrafast Lasers