2006
DOI: 10.1016/j.jlumin.2006.01.025
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Laser excitation and excited state dynamics in vanadium dioxide thin film

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Cited by 8 publications
(5 citation statements)
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“…The responses observed in all cases here are due purely to thermal effects caused by the voltage or light pulses. Since ultrafast changes in optical properties of VO 2 have been demonstrated before, [14][15][16] it may be expected that sufficiently intense ultrashort light pulses can be similarly used to access different "states" of the material. However, the time evolution of the material's response will be more complex in this case, as is known from previous work with VO 2 , 17 and relaxation to a thermally determined condition should determine the final stable state.…”
Section: Discussionmentioning
confidence: 99%
“…The responses observed in all cases here are due purely to thermal effects caused by the voltage or light pulses. Since ultrafast changes in optical properties of VO 2 have been demonstrated before, [14][15][16] it may be expected that sufficiently intense ultrashort light pulses can be similarly used to access different "states" of the material. However, the time evolution of the material's response will be more complex in this case, as is known from previous work with VO 2 , 17 and relaxation to a thermally determined condition should determine the final stable state.…”
Section: Discussionmentioning
confidence: 99%
“…A light-induced PT in sufficiently thin uniform VO 2 film occurs simultaneously in entire film volume at critical excitation level, while during thermally induced PT the PT temperature range is broadened through several degrees near PT point T c = 340 K. Apparently, the driven force for light-induced and thermally induced PT is different. [16][17][18][19][20] At present, the problem related to PT dynamics of VO 2 materials, including the modification of optical nonlinear constants, transient heterogeneity, and degradation, remains open.…”
Section: Introductionmentioning
confidence: 99%
“…Similarly, the conductivity of Ge was varied from 1 to 4 × 10 3 S/m to simulate the influence of optical pump irradiation [ 49 , 54 ]. It is essential to mention that a 400 nm optical pump (3.1 eV) is typically used to activate the photoinduced carriers in Ge (0.66 eV), and the pump frequency enables the Ge conductivity change to 4 × 10 3 S/m that only leads to a slight alteration in undoped VO 2 conductivity, thus ensuring independence between the two modulation approaches [ 52 , 55 , 56 , 57 ]. The normalized transmission spectra were calculated via the formula: |T(ω)| = |E s (ω)/E r (ω)| with E s (ω) and E r (ω) representing the amplitude of THz waves transmitted through the device and the thickness of bare sapphire, respectively [ 58 ].…”
Section: Methodsmentioning
confidence: 99%