Opto-Electronic Advances, Volume. 4, Issue 10, 200029-1(2021)

Optical properties and applications of SnS2 SAs with different thickness

Mengli Liu, Hongbo Wu, Ximei Liu, Yaorong Wang, Ming Lei, Wenjun Liu*, Wei Guo*, and Zhiyi Wei*
References(51)

[1] Observation and optimization of 2 μm mode-locked pulses in all-fiber net anomalous dispersion laser cavity. Opto-Electron Adv, 3, 200001(2020).

[2] Passively Q-switched Tm/Ho composite laser. Opto-Electron Adv, 3, 190031(2020).

[3] CVD-grown MoSe2 with high modulation depth for ultrafast mode-locked erbium-doped fiber laser. Nanotechnology, 29, 394002(2018).

[4] Mid-infrared all-fiber gain-switched pulsed laser at 3 μm. Opto-Electron Adv, 3, 190032(2020).

[5] Nonlinear optical properties of MoS2-WS2 heterostructure in fiber lasers. Opt Express, 27, 6689-6699(2019).

[6] WS2 as a saturable absorber for ultrafast photonic applications of mode-locked and Q-switched lasers. Opt Express, 23, 11453-11461(2015).

[7] Q-switched fiber laser operating at 1.5 μm based on WTe2. Chin Opt Lett, 17, 020006(2019).

[8] Nonlinear optical properties of WSe2 and MoSe2 films and their applications in passively Q-switched erbium doped fiber lasers. Photonics Res, 6, C15-C21(2018).

[9] Revealing the plasmon coupling in gold nanochains directly from the near field. Opto-Electron Adv, 2, 180030(2019).

[10] 8 ns fiber laser Q switched by the resonant saturable absorber mirror. Opt Lett, 32, 2677-2679(2007).

[11] Large energy mode locking of an erbium-doped fiber laser with atomic layer graphene. Opt Express, 17, 17630-17635(2009).

[12] Atomic-layer graphene as a saturable absorber for ultrafast pulsed lasers. Adv Funct Mater, 19, 3077-3083(2009).

[13] Optical modulators with 2D layered materials. Nat. Photonics, 10, 227-238(2016).

[14] MoTe2 saturable absorber with high modulation depth for erbium-doped fiber laser. J Lightwave Technol, 37, 3100-3105(2019).

[15] Sub-200 fs soliton mode-locked fiber laser based on bismuthene saturable absorber. Opt Express, 26, 22750-22760(2018).

[16] Broadband nonlinear optical response in multi-layer black phosphorus: an emerging infrared and mid-infrared optical material. Opt Express, 23, 11183-11194(2015).

[17] Synthesis of high quality silver nanowires and their applications in ultrafast photonics. Opt Express, 27, 16440-16448(2019).

[18] Large-area tungsten disulfide for ultrafast photonics. Nanoscale, 9, 1871-1877(2017).

[19] MoS2 saturable absorber prepared by chemical vapor deposition method for nonlinear control in Q-switching fiber laser. Chin Phys B, 27, 084211(2018).

[20] Two-dimensional SnS2 nanoplates with extraordinary high discharge capacity for lithium ion batteries. Adv Mater, 20, 4269-4273(2008).

[21] SnS2 nanosheets for Er-doped fiber lasers. ACS Appl Nano Mater, 3, 674-681(2020).

[22] Passively mode-locked Er-doped fiber laser based on SnS2 nanosheets as a saturable absorber. Photonics Res, 6, 72-76(2018).

[23] Tin disulfide-an emerging layered metal dichalcogenide semiconductor: materials properties and device characteristics. ACS Nano, 8, 10743-10755(2014).

[24] High-performance top-gated monolayer SnS2 field-effect transistors and their integrated logic circuits. Nanoscale, 5, 9666-9670(2013).

[25] Vertically aligned graphene-like SnS2 ultrathin nanosheet arrays: excellent energy storage, catalysis, photoconduction, and field-emitting performances. J Phys Chem C, 116, 9319-9326(2012).

[26] Dissipative soliton generation in Er-doped fibre laser using SnS2 as a saturable absorber. Appl Phys Express, 12, 102008(2019).

[27] Dual-wavelength mode-locked erbium-doped fiber laser based on tin disulfide thin film as saturable absorber. J Appl Phys, 125, 243104(2019).

[28] Noise-like mode-locked Yb-doped fiber laser in a linear cavity based on SnS2 nanosheets as a saturable absorber. Appl Optics, 58, 6007-6011(2019).

[29] Thickness-dependent ultrafast photonics of SnS2 nanolayers for optimizing fiber lasers. ACS Appl Nano Mater, 2, 2697-2705(2019).

[30] Passively Q-switched erbium-doped fiber laser based on SnS2 saturable absorber. Opt Mater Express, 7, 3934-3943(2017).

[31] Thickness-dependent structure and properties of SnS2 thin films prepared by atomic layer deposition. Jpn J Appl Phys, 56, 031201(2017).

[32] [32] 322 single crystals and vertical nanostructures: role of edges. In Proceedings of the 43rd International Conference on Infrared, Millimeter, and Terahertz Waves (IRMMW-THz, 2018) (IEEE, 2018);http://doi.org/10.1109/IRMMW-THz.2018.8509909.

[33] Q-switching stability limits of continuous-wave passive mode locking. J Opt Soc Am B, 16, 46-56(1999).

[34] Evanescent-light deposition of graphene onto tapered fibers for passive Q-switch and mode-locker. IEEE Photonics J, 4, 1295-1305(2012).

[35] Mechanically exfoliated black phosphorus as a new saturable absorber for both Q-switching and Mode-locking laser operation. Opt Express, 23, 12823-12833(2015).

[36] Q-switched fiber laser based on transition metal dichalcogenides MoS2, MoSe2, WS2, and WSe2. Opt Express, 23, 26723-26737(2015).

[37] Widely-tunable, passively Q-switched erbium-doped fiber laser with few-layer MoS2 saturable absorber. Opt Express, 22, 25258-25266(2014).

[38] Efficiency of ab-initio total energy calculations for metals and semiconductors using a plane-wave basis set. Comput Mater Sci, 6, 15-50(1996).

[39] Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set. Phys Rev B, 54, 11169-11186(1996).

[40] Projector augmented-wave method. Phys Rev B, 50, 17953-17979(1994).

[41] From ultrasoft pseudopotentials to the projector augmented-wave method. Phys Rev B, 59, 1758-1775(1999).

[42] Generalized gradient approximation made simple. Phys Rev Lett, 77, 3865-3868(1996).

[43] A consistent and accurate ab initio parametrization of density functional dispersion correction (DFT-D) for the 94 elements H-Pu. J Chem Phys, 132, 154104(2010).

[44] Special points for Brillouin-zone integrations. Phys Rev B, 13, 5188-5192(1976).

[45] Hybrid functionals based on a screened Coulomb potential. J Chem Phys, 118, 8207-8215(2003).

[46] [46] 46J Chem Phys 124, 219906 (2006).

[47] Deformation potentials and mobilities in non-polar crystals. Phys Rev, 80, 72-80(1950).

[48] Ab-initio simulations of deformation potentials and electron mobility in chemically modified graphene and two-dimensional hexagonal boron-nitride. Appl Phys Lett, 99, 222108(2011).

[49] High-mobility transport anisotropy and linear dichroism in few-layer black phosphorus. Nat Commun, 5, 4475(2014).

[50] Calculated carrier mobility of h-BN/γ-InSe/h-BN van der Waals heterostructures. 2D Mater, 4, 045014(2017).

[51] First-principles calculation of intrinsic carrier mobility of silicene. J Appl Phys, 114, 093712(2013).

Tools

Get Citation

Copy Citation Text

Mengli Liu, Hongbo Wu, Ximei Liu, Yaorong Wang, Ming Lei, Wenjun Liu, Wei Guo, Zhiyi Wei. Optical properties and applications of SnS2 SAs with different thickness[J]. Opto-Electronic Advances, 2021, 4(10): 200029-1

Download Citation

EndNote(RIS)BibTexPlain Text
Save article for my favorites
Paper Information

Category: Original Article

Received: Jul. 10, 2020

Accepted: Sep. 29, 2020

Published Online: Dec. 28, 2021

The Author Email: Wenjun Liu (jungliu@bupt.edu.cn), Wei Guo (weiguo7@bit.edu.cn), Zhiyi Wei (zywei@iphy.ac.cn)

DOI:10.29026/oea.2021.200029

Topics