Compact high stable passively Q-switched Nd:YVO4 laser with Cr4+:YAG

Song, Qi; Wang, Guoju; Zhang, Bingyuan; Li, Shuhong; Gao, Xuexi; Liu, Yunlong; Wang, Wenjun

doi:10.1016/j.ijleo.2015.06.001

Cited by 6 publications

(1 citation statement)

References 21 publications

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“…Note that these superalkalis have been experimentally synthesized, [ 42–44 ] and they can serve as basic building blocks for new complexes. [ 45–48 ] The evolution of their first hyperpolarizability with varying superalkali atom and pore size of GY has been analyzed in order to explore new high‐performance NLO molecules. The structures, stability, and static first hyperpolarizabilities of the investigated complexes are explored by employing density functional theory (DFT).…”

Section: Introductionmentioning

confidence: 99%

Effects of the atomic number of alkali atom and pore size of graphyne on the second‐order nonlinear optical response of superalkali salts of graphynesOM₃⁺@GYs⁻(M = Li, Na, and K)

Hou

Feng

et al. 2020

Int J of Quantum Chemistry

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Based on the combination of novel carbon material graphynes (GYs) and superalkalis (OM3), a class of GY superalkali complexes, OM3+@(GY/GDY/GTY)− (M = Li, Na, and K), has been designed and investigated using the density functional theory method. Computational results reveal that these complexes with high stability can be regarded as novel superalkali salts of GYs due to electron transfer from OM3 to GYs. For second‐order nonlinear optical response, these superalkali salts exhibit large first hyperpolarizabilities (β0). Two essential effects on β0 values are found, namely, the atomic number of alkali atom in superalkali and the pore size of GY. Integrating the two effects, the selected combination of OLi3 with large pore size graphtrigne (GTY) can lead to a considerable β0 value (6.5 × 105 au), which is a new record for superatom‐doped GYs. In the resulting complex, the OLi3 unit is located at the center of the pore of GTY, forming a planar structure with the highest stability among these salts. Besides large β0 values, these superalkali salts of GYs have a deep‐ultraviolet working region; hence, they can be considered a kind of high‐performance deep‐ultraviolet NLO molecule.

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Section: Introductionmentioning

confidence: 99%

Effects of the atomic number of alkali atom and pore size of graphyne on the second‐order nonlinear optical response of superalkali salts of graphynesOM₃⁺@GYs⁻(M = Li, Na, and K)

Hou

Feng

et al. 2020

Int J of Quantum Chemistry

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Passively Q-Switched Mode-Locking Nd:(Gd0.3Y0.7)2SiO5 Laser Based on Semiconductor Saturable Absorber Mirror†

et al. 2019

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Compact stable passively Q-switched Nd:YVO4 laser with tungsten disulfide saturable absorber

Zhang¹,

Zhang

Wang

et al. 2016

Optik

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Compact high stable passively Q-switched Nd:YVO4 laser with Cr4+:YAG

Cited by 6 publications

References 21 publications

Effects of the atomic number of alkali atom and pore size of graphyne on the second‐order nonlinear optical response of superalkali salts of graphynesOM₃⁺@GYs⁻(M = Li, Na, and K)

Effects of the atomic number of alkali atom and pore size of graphyne on the second‐order nonlinear optical response of superalkali salts of graphynesOM₃⁺@GYs⁻(M = Li, Na, and K)

Passively Q-Switched Mode-Locking Nd:(Gd0.3Y0.7)2SiO5 Laser Based on Semiconductor Saturable Absorber Mirror†

Compact stable passively Q-switched Nd:YVO4 laser with tungsten disulfide saturable absorber

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Compact high stable passively Q-switched Nd:YVO4 laser with Cr4+:YAG

Cited by 6 publications

References 21 publications

Effects of the atomic number of alkali atom and pore size of graphyne on the second‐order nonlinear optical response of superalkali salts of graphynesOM3+@GYs−(M = Li, Na, and K)

Effects of the atomic number of alkali atom and pore size of graphyne on the second‐order nonlinear optical response of superalkali salts of graphynesOM3+@GYs−(M = Li, Na, and K)

Passively Q-Switched Mode-Locking Nd:(Gd0.3Y0.7)2SiO5 Laser Based on Semiconductor Saturable Absorber Mirror†

Compact stable passively Q-switched Nd:YVO4 laser with tungsten disulfide saturable absorber

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Effects of the atomic number of alkali atom and pore size of graphyne on the second‐order nonlinear optical response of superalkali salts of graphynesOM₃⁺@GYs⁻(M = Li, Na, and K)

Effects of the atomic number of alkali atom and pore size of graphyne on the second‐order nonlinear optical response of superalkali salts of graphynesOM₃⁺@GYs⁻(M = Li, Na, and K)