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首页> 外文期刊>Journal of Raman Spectroscopy: An International Journal for Original Work in All Aspects of Raman Spectroscopy, Including Higher Order Processes, and Also Brillouin- and Rayleigh Scattering >Measurement of the third-order nonlinear optical susceptibility χ ~(3) for the 1002-cm ~(-1) mode of benzenethiol using coherent anti-Stokes Raman scattering with continuous-wave diode lasers
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Measurement of the third-order nonlinear optical susceptibility χ ~(3) for the 1002-cm ~(-1) mode of benzenethiol using coherent anti-Stokes Raman scattering with continuous-wave diode lasers

机译:使用相干反斯托克斯拉曼散射和连续波二极管激光器测量1002-cm〜(-1)模式的苯硫酚的三阶非线性光学磁化率χ〜(3)

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摘要

The components of the third-order nonlinear optical susceptibility χ ~(3) for the 1002-cm ~(-1) mode of neat benzenethiol have been measured using coherent anti-Stokes Raman scattering with continuous-wave diode pump and Stokes lasers at 785.0 and 852.0 nm, respectively. Values of 2.8 ± 0.3 × 10 ~(-12), 2.0 ± 0.2 × 10 ~(-12), and 0.8 ± 0.1 × 10 ~(-12) cm·g ~(-1)·s ~2 were measured for the xxxx, xxyy, and xyyx components of |3χ ~(3)|, respectively. We have calculated these quantities using a microscopic model, reproducing the same qualitative trend. The Raman cross-section σ _(RS) for the 1002-cm ~(-1) mode of neat benzenethiol has been determined to be 3.1 ± 0.6 × 10 ~(-29) cm ~2 per molecule. The polarization of the anti-Stokes Raman scattering was found to be parallel to that of the pump laser, which implies negligible depolarization. The Raman linewidth (full-width at half-maximum) Γ was determined to be 2.4 ± 0.3 cm ~(-1) using normal Stokes Raman scattering. The measured values of σ RS and Γ yield a value of 2.1 ± 0.4 × 10 ~(-12) cm·g ~(-1)·s ~2 for the resonant component of 3χ ~(3). A value of 1.9 ± 0.9 × 10 ~(-12) cm·g ~(-1)·s ~2 has been deduced for the nonresonant component of 3χ ~(3).
机译:使用相干反斯托克斯拉曼散射,连续波二极管泵浦和斯托克斯激光在785.0上测量了1002-cm〜(-1)净苯硫醇模式的三阶非线性光学磁化率χ〜(3)的分量。和852.0 nm。分别测量2.8±0.3×10〜(-12),2.0±0.2×10〜(-12)和0.8±0.1×10〜(-12)cm·g〜(-1)·s〜2的值|3χ〜(3)|的xxxx,xxyy和xyyx分量分别。我们已经使用微观模型计算了这些数量,从而再现了相同的定性趋势。净苯硫醇的1002-cm〜(-1)模的拉曼截面σ_(RS)已确定为每分子3.1±0.6×10〜(-29)cm〜2。发现反斯托克斯拉曼散射的偏振与泵浦激光器的偏振平行,这意味着可忽略的去偏振。使用正常的斯托克斯拉曼散射将拉曼线宽(半峰全宽)Γ确定为2.4±0.3 cm〜(-1)。对于3χ〜(3)的谐振分量,σRS和Γ的测量值得出的值为2.1±0.4×10〜(-12)cm·g〜(-1)·s〜2。对于3χ〜(3)的非谐振分量,得出了1.9±0.9×10〜(-12)cm·g〜(-1)·s〜2的值。

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