2011
DOI: 10.1016/j.optcom.2011.08.009
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Tunable terahertz generation from one CO2 laser in a GaSe crystal

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Cited by 15 publications
(11 citation statements)
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“…The relation of the optimized cavity length in a GaAs crystal sheet Λ at room temperature and the THz wavelength are shown in Fig.1 from Eqs. (3) and (4). It can be seen that Λ is increased from 0.16 to 1.96 mm when THz wavelength is increased from 100 to 1000µm in the CPM scheme.…”
Section: Theory Of Scheme and Discussionmentioning
confidence: 89%
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“…The relation of the optimized cavity length in a GaAs crystal sheet Λ at room temperature and the THz wavelength are shown in Fig.1 from Eqs. (3) and (4). It can be seen that Λ is increased from 0.16 to 1.96 mm when THz wavelength is increased from 100 to 1000µm in the CPM scheme.…”
Section: Theory Of Scheme and Discussionmentioning
confidence: 89%
“…Among the variety of nonlinear crystals, GaAs meet the requirements for high transparency in both 10 µm band and relatively high transparency in the THz region. A lot of work has been carried out enhancing THz power [ [4][5][6][7]. We demonstrate a tunable THz source based on the collinear DFG in GaSe crystal with a dual-wavelength CO 2 laser [7].…”
Section: Introductionmentioning
confidence: 99%
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“…The strong covalent bonding within the multi-layer and weak van der Waals bonding between the multi-layers make ε-GaSe a quasi-two-dimensional, highly anisotropic material with a birefringence of about 0.35 in the infrared range. [1] Combining its other excellent performances, such as large nonlinear coefficient (54 pm/V at 10.6 µm), wide transparency range (0.62 µm-18 µm) and high damage threshold, ε-GaSe have been successfully used to generate coherent laser radiation in an extremely wide spectral range from mid-to far-infrared [2][3][4][5] and further to terahertz regions [6][7][8] by nonlinear frequency conversion. On the other hand, the layer structure of ε-GaSe results in its pronounced cleavability and almost zero hardness; its bad mechanical properties lead to uncontrolled layer stacking defects (an admixture of γ, δ or β polytypes) in the growth process and hamper the cutting and polishing along arbitrary directions, which holds back its outof-lab applications in nonlinear optics.…”
Section: Introductionmentioning
confidence: 99%
“…However, all of the reported DFG terahertz sources pumped by CO 2 lasers were established with two lasers [4,10], made the system huge and complex. Previously we have reported an tunable THZ sources based on DFG in GaAs wih one CO2 laser, the THz pulse of a peak power 35 W was obtained using non-collinear phase matching in a 20mm length GaAs crystal, and acquired the THz pulse of a peak power 182 mW using collinear phase matching in a 8mm length GaSe crystal [8][9] .…”
Section: Introductionmentioning
confidence: 99%