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首页> 外文期刊>Journal of Molecular Spectroscopy >The X-2 Sigma(+)(g) and B-2 Sigma(+)(u) states of N-2(+): hyperfine and nuclear quadrupole coupling constants, electric quadrupole moments, and electron-spin g-factors. A theoretical study
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The X-2 Sigma(+)(g) and B-2 Sigma(+)(u) states of N-2(+): hyperfine and nuclear quadrupole coupling constants, electric quadrupole moments, and electron-spin g-factors. A theoretical study

机译:N-2(+)的X-2 Sigma(+)(g)和B-2 Sigma(+)(u)状态:超精细和核四极耦合常数,电四极矩和电子自旋g因子。理论研究

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The variation with bond distance of hyperfine coupling constants (lifec) [A(iso), A(dip)], nuclear quadrupole coupling constants (nqcc) [chi], molecular electric quadrupole moments [Theta], and electron-spin g-factors is reported for X(2)Sigma(g)(+)(sigma(2)pi(u)(4)2sigma(g)) and B(2)Sigma(u)(+)(1sigma(u)gpiu(4)(2)sigma(g)(3)) of N-2(+). The hfcc's, nqcc's, and Theta's are studied with ab initio and density functional theory methods. Calculated A(iso)/A(dip) of 91.3/29.7 MHz for the X state have to be compared with experimental values of 102.4/23.3 MHz. For the B state, theoretical values A(iso)/A(dip) = 793/6.8 MHz support an experimental A(iso) = 708 MHz (1sigma(u) is largely s) but disagree with A(dip) = 26 MHz (large p). The nqcc chi(B) is one order of magnitude larger than chi(X), 4.80 versus -0.58 MHz, in line with literature results. Omission of nqcc contributions in the analysis of optical spectra is most probably responsible for the anomalously high "experimental" Adip(B). The quadrupole moment 0 is positive for both X and B states of N-2(+), whereas it is negative for neutral N-2(X). The vibrational absorption 2 intensity for the v = I <-- 0 quadrupole transition of N-2(+)(A) is about six times stronger than for N-2(X). The g(perpendicular to)-shift (Deltag(perpendicular to) = g(perpendicular to) - g(e)) is evaluated with multireference configuration interaction wavefunctions, via second-order sum-over-states expansions. The Deltag()'s are small (approximate to100 ppm), while Deltag(perpendicular to) (v = 0) is -2710 ppm for X(2)Sigma(g)(+) and -6165 ppm for B(2)Sigma(n)(+). Interaction parameters lpha(e), 31.12cm(-1) and beta(el) = 1.01 a.u. calculated for the A(2)Pi(u) similar to B(2)Sigma(u)(+) perturbation are in I me with 31.30 cm(-1) and 1.07 a.u. averaged over five experimental studies. Our Deltagperpendicular to(u)'s are compared with Curl's shifts obtained from experimental spin-rotation (gamma) and rotational constants. Good agreement is found for X but not for the B state, for which it is suggested that experimental - (B, U)'s recently reported-where gamma decreases sharply with vibrational level v-should be revised. (C) 2004 Elsevier Inc. All rights reserved.
机译:超精细偶合常数(lifec)[A(iso),A(dip)],核四极偶合常数(nqcc)[chi],分子电四极矩θ和电子自旋g因子随键距的变化报告X(2)Sigma(g)(+)( sigma(2) pi(u)(4)2sigma(g))和B(2)Sigma(u)(+)(1sigma(u) N-2(+)的g piu(4)(2)sigma(g)(3))。使用从头算和密度泛函理论方法研究hfcc,nqcc和Theta。必须将X态的91.3 / 29.7 MHz的A(iso)/ A(dip)计算值与102.4 / 23.3 MHz的实验值进行比较。对于B状态,理论值A(iso)/ A(dip)= 793 / 6.8 MHz支持实验性A(iso)= 708 MHz(1sigma(u)在很大程度上是s),但与A(dip)= 26 MHz不一致(大p)。与文献结果一致,nqcc chi(B)比chi(X)大一个数量级,为4.80对-0.58 MHz。在光谱分析中忽略nqcc贡献很可能是异常高的“实验” Adip(B)的原因。对于N-2(+)的X和B状态,四极矩0为正,而对于中性N-2(X)则为负。 N-2(+)(A)的v = I <-0四极跃迁的振动吸收2强度大约是N-2(X)的六倍。通过二阶求和状态展开式,利用多参考配置相互作用波函数来评估g(垂直于)位移(Deltag(垂直于)= g(垂直于)-g(e))。 Deltag()很小(大约100 ppm),而Deltag(垂直于(v = 0))对于X(2)Sigma(g)(+)为-2710 ppm,对于B(-6 2)Sigma(n)(+)。互动参数 alpha(e ),31.12cm(-1)和beta(el)= 1.01 a.u.对于A(2)Pi(u)计算的类似于B(2)Sigma(u)(+)摄动的计算值在我中为31.30 cm(-1)和1.07a.u。平均进行了五项实验研究。将我们的垂直于(u)的Deltag与从实验自旋旋转(γ)和旋转常数获得的Curl位移进行比较。对于X态,但对于B态,则发现有很好的一致性,因此建议修改实验-(B,U)最近报道的-伽马随振动水平v急剧下降的现象。 (C)2004 Elsevier Inc.保留所有权利。

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