首页> 外文期刊>The Journal of Chemical Physics >COLLISIONAL DEACTIVATION OF VIBRATIONALLY HIGHLY EXCITED AZULENE IN COMPRESSED LIQUIDS AND SUPERCRITICAL FLUIDS
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COLLISIONAL DEACTIVATION OF VIBRATIONALLY HIGHLY EXCITED AZULENE IN COMPRESSED LIQUIDS AND SUPERCRITICAL FLUIDS

机译:压缩液体和超临界流体中振动性高激发氮原子的集体失活

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The collisional deactivation of vibrationally highly excited azulene was studied from the gas to the. compressed liquid phase. Employing supercritical fluids like He, Xe, CO2, and ethane at pressures of 6-4000 bar and temperatures greater than or equal to 380 K, measurements over the complete gas-liquid transition were performed. Azulene with an energy of 18 000 cm(-1) was generated by laser excitation into the S-1 and internal conversion to the S-0*-ground state. The subsequent loss of vibrational energy was monitored by transient absorption at the red edge of the S-3<--S-0 absorption band near 290 nm. Transient signals were converted into energy-time profiles using hot band absorption coefficients from shock wave experiments for calibration and accounting for solvent shifts of the spectra. Under all conditions, the decays were monoexponential. At densities below 1 mol/l, collisional deactivation rates increased linearly with fluid density. Average energies [Delta E] transferred per collision agreed with data from dilute gas phase experiments. For Xe, CO2, and C2H6, the linear relation between cooling rate and diffusion coefficient scaled collision frequencies Z(D) turned over to a much weaker dependence at Z(D)>0.3 ps(-1). Up to collision frequencies of Z(D)=15 ps(-1) this behavior can well be rationalized by a model employing an effective collision frequency related to the finite lifetime of collision complexes. (C) 1996 American Institute of Physics. [References: 64]
机译:从气体到气体,研究了振动高激发的z的碰撞失活。压缩液相。使用压力为6-4000 bar且温度大于或等于380 K的He,Xe,CO2和乙烷等超临界流体,对整个气液转变进行了测量。通过激光激发进入S-1并内部转换为S-0 *基态,生成了能量为18000 cm(-1)的氮杂。随后振动能量的损失通过在290 nm附近的S-3 <-S-0吸收带的红色边缘处的瞬态吸收来监测。使用来自冲击波实验的热带吸收系数将瞬态信号转换为能量-时间曲线,以进行校准并考虑光谱的溶剂漂移。在所有条件下,衰减都是单指数的。密度低于1 mol / l时,碰撞失活速率随流体密度线性增加。每次碰撞转移的平均能量[ΔE]与稀气相实验的数据一致。对于Xe,CO2和C2H6,在Z(D)> 0.3 ps(-1)时,冷却速率与扩散系数缩放的碰撞频率Z(D)之间的线性关系变得非常弱。高达Z(D)= 15 ps(-1)的碰撞频率,可以通过采用与碰撞复合体的有限寿命相关的有效碰撞频率的模型来合理化此行为。 (C)1996年美国物理研究所。 [参考:64]

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