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首页> 外文期刊>Chemical Physics: A Journal Devoted to Experimental and Theoretical Research Involving Problems of Both a Chemical and Physical Nature >A He(I) photoelectron spectroscopic study of the (X-tilde)~2A'_2 state of NH_3~+ and ND_3~+. A reanalysis and evidence for the coriolis coupling between the bending v_2 and v_4 modes
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A He(I) photoelectron spectroscopic study of the (X-tilde)~2A'_2 state of NH_3~+ and ND_3~+. A reanalysis and evidence for the coriolis coupling between the bending v_2 and v_4 modes

机译:NH_3〜+和ND_3〜+的(X-tilde)〜2A“ _2状态的He(I)光电子能谱研究。弯曲v_2和v_4模式的科氏耦合的重新分析和证据

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In the high-resolution He(I) photoelectron spectrum of NH_3 and its isotopomer ND_3, the complete vibrational structure of the (X-tilde)~2A"_2 state of NH_3~+ and ND_3~+ is examined in detail. Three vibrational progressions are identified. The well-known strongest progression, already unambiguously assigned to the v_2 out-of-plane bending mode, is observed from v = 0-17 in NH_3~+ and from v = 0-20 in ND_3~+. For NH_3~+ this vibration could be characterized not only by its energy hcω_2 = 0.109 250L?0.001 eV (or ω_2 = 878 ± 7 cm~(-1)), but also by its first anharmonicity constant hcω_(22)x_(22) = -(16.2 ± 1.2) * 10~(-4) eV (or ω_(22)x_(22) = -13.0 ± 1.0 cm~(-1)). The best fit of the experimental data required the introduction of a second anharmonicity constant, i.e. hcω_(22)y_(22) = -(30.7 ± 4.2) * 10~(-6) eV (or ω_(22)y_(22) = -0.248 ± 0.034 cm~(-1)). the earlier reported weak progression, assigned to the vibrational combination v_1 + nv_2 transitions has been reexamined. Suitable handling of the data leads to two possible energies for the v_1 degenerate NH stretching vibrational normal mode, i.e. hcω_1 = 0.306 ± 0.006 or 0.422 ± 0.005 eV. Several arguments are brought to favour the value of hcω_1 = 0.422 eV (or ω_1 = 3404 cm~(-1). Finally a third weak progression, reported for the first time, is assigned to v_4 + nv_2 transitions where the v_4 in-plane bending mode is optically forbidden. This vibrational normal mode is characterized by an energy hcω_4 = 0.186 ± 0.010 eV (ω_4 = 1500 ± 80 cm~(-1)). In agreement with theoretical predictions, this transition becomes allowed through a strong Coriolis vibro-rotational coupling between the v_4 and the v_2 vibrational normal modes. The same measurements and the isotope effect on the molecular constants are investigated in ND_3~+ too.
机译:在NH_3及其同位异构体ND_3的高分辨率He(I)光电子能谱中,详细研究了NH_3〜+和ND_3〜+的(X-tilde)〜2A“ _2状态的完整振动结构。三个振动过程从NH_3〜+的v = 0-17和ND_3〜+的v = 0-20可以观察到已经明确分配给v_2平面外弯曲模式的最著名的最强曲线。 〜+这种振动不仅可以通过其能量hcω_2= 0.109250L?0.001 eV(或ω_2= 878±7 cm〜(-1))来表征,还可以通过其第一非谐常数hcω_(22)x_(22)来表征。 =-(16.2±1.2)* 10〜(-4)eV(或ω_(22)x_(22)= -13.0±1.0 cm〜(-1))。实验数据的最佳拟合要求引入第二个非谐常数,即hcω_(22)y_(22)=-(30.7±4.2)* 10〜(-6)eV(或ω_(22)y_(22)= -0.248±0.034 cm〜(-1)) 。已经重新检查了早期报告的弱级数,已将其指定为振动组合v_1 + nv_2的过渡。数据的处理导致v_1退化的NH拉伸振动法线模式的两个可能能量,即hcω_1= 0.306±0.006或0.422±0.005 eV。提出了几个论据来支持hcω_1= 0.422 eV(或ω_1= 3404 cm〜(-1)。最后,首次报道的第三个弱级数被分配给v_4 + nv_2跃迁,其中v_4面内光学上禁止弯曲模式,这种振动法向模式的特征是能量hcω_4= 0.186±0.010 eV(ω_4= 1500±80 cm〜(-1))。与理论预测相一致,这种转变通过强的科氏力得以实现v_4和v_2振动正态之间的旋转耦合,在ND_3〜+中也研究了相同的测量和同位素对分子常数的影响。

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