2008
DOI: 10.1002/crat.200800423
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New nonlinear‐laser effects in GdVO4 – host‐crystal for Ln3+ lasants

Abstract: We discovered several new nonlinear-laser χ-properties in tetragonal GdVO 4 vanadate, which is hostcrystal for lanthanide lasant ions, and attractive gain media for Raman laser converters. We hope that observed many-phonon SRS, almost two-octave Stokes and anti-Stokes lasing comb, cascaded self-frequency "tripling" and self-sum-frequency generation in the blue and UV spectral range could significantly enriche funcional laser potential of this crystal. Dedicated to Prof. Ladislav Bohatý on the occasion of his 6… Show more

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Cited by 8 publications
(4 citation statements)
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“…Knowing energy gaps between SRS-active phonon modes in GdVO 4 crystal, which were recorded in the steady-state pumping condition (see, e.g. [1,12,18]), we chose the pumppulse duration to provide the desired spectral resolution for ISRS Stokes lasing components. One of the recorded ISRSlasing spectra of a tetragonal GdVO 4 single crystal is shown in figure 2(b).…”
Section: Impulsive Srs-lasingmentioning
confidence: 99%
See 1 more Smart Citation
“…Knowing energy gaps between SRS-active phonon modes in GdVO 4 crystal, which were recorded in the steady-state pumping condition (see, e.g. [1,12,18]), we chose the pumppulse duration to provide the desired spectral resolution for ISRS Stokes lasing components. One of the recorded ISRSlasing spectra of a tetragonal GdVO 4 single crystal is shown in figure 2(b).…”
Section: Impulsive Srs-lasingmentioning
confidence: 99%
“…One of the recorded ISRSlasing spectra of a tetragonal GdVO 4 single crystal is shown in figure 2(b). In this measurement to determine more clearly the spectral position of the four recorded Stokes components (ω SRS1 ≈ 882 cm −1 , ω SRS2 ≈ 807 cm −1 , ω SRS3 ≈ 823 cm −1 and ω SRS7 ≈ 378 cm −1 ), we used τ p ≈ 600 fs pump-pulses and at the same time to maintain the required conditions for impulsive χ (3) -nonlinear lasing τ p < T 2 = (πΔν R ) −1 = (1.2-3.5) ps [12,18] (here T 2 and Δν R are the dephasing time and linewidth of the Raman shifted lines in spontaneous Raman scattering spectra related to SRS-promoting vibration modes, respectively). It is important to note the direct cascaded four-phonon ISRS lasing ).…”
Section: Impulsive Srs-lasingmentioning
confidence: 99%
“…Rare earth doped materials are used in a wide variety of optical applications including and high power solid state and fiber lasers [1][2][3][4][5]. For one micron lasers, Yb-doped materials are being used with increasing frequency for high-power laser applications because of their sharp absorption at 976 nm and small quantum defect.…”
Section: Introductionmentioning
confidence: 99%
“…The thermal-optic coefficient dn/dT of a laser crystal is explicitly associated with the thermally induced lensing effect that significantly influences the cavity stability, the oscillation mode size, the maximum achievable average power and the quality of the output beam [6,7]. There are some reported values of dn/dT obtained by different methods for Nd:GdVO 4 , Nd:YVO 4 and Nd:LuVO 4 crystals near 1064 nm [8][9][10][11][12][13][14]. However, the reported data are found to differ considerably from each other.…”
Section: Introductionmentioning
confidence: 99%