1998
DOI: 10.1103/physrevlett.81.3116
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Quantum Mechanical Study of Optical Emission Spectra of Rydberg-ExcitedH3and Its Isotopomers

Abstract: Optical emission spectra of Rydberg-excited H 3 , D 3 , H 2 D, and D 2 H, in the range 200 -400 nm, are investigated theoretically and compared with the experimental findings of Bruckmeier et al. [Phys. Rev. Lett. 72, 2550(1994]. The time-dependent wave packet method combined with the vibronic coupling theory for (E 3 e) Jahn-Teller systems is utilized in order to calculate the corresponding Franck-Condon emission profiles from the upper n 3 electronic state to the degenerate ͑2p͒1E 0 ground electronic manifol… Show more

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Cited by 44 publications
(32 citation statements)
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“…The JT effect in the C 2 E electronic manifold is also quite weak when compared to the similar other examples treated in the literature. [29][30][31] To this end we note that besides the model study presented here, which, in fact, reproduces the experimental results reasonably well, a more rigorous electronic structure calculations to establish the anionic and neutral potential energy surfaces and the nonadiabatic coupling elements are presently being carried out with an aim to perform wave packet dynamical simulations to study the decay of the excited electronic states of B 3 cluster.…”
Section: Discussionmentioning
confidence: 61%
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“…The JT effect in the C 2 E electronic manifold is also quite weak when compared to the similar other examples treated in the literature. [29][30][31] To this end we note that besides the model study presented here, which, in fact, reproduces the experimental results reasonably well, a more rigorous electronic structure calculations to establish the anionic and neutral potential energy surfaces and the nonadiabatic coupling elements are presently being carried out with an aim to perform wave packet dynamical simulations to study the decay of the excited electronic states of B 3 cluster.…”
Section: Discussionmentioning
confidence: 61%
“…The JT coupling within the C 2 E electronic manifold is also weak compared to similar strong (E ⊗ e)-JT coupling cases treated in the literature. [29][30][31] To this end we mention that photodetachment experiments for the smallest boron clusters are reported to be quite delicate because of weak cluster intensities and low photodetachment cross sections. 15 The resolution of the apparatus was ∼30 meV for 1 eV electrons.…”
mentioning
confidence: 98%
“…According to the symmetry rule the b 1 and b 2 modes cannot be active in first-order in the e X state, however, they are so in the e A state and can split the electronic degeneracy. The situation here is different from the extensively studied (E e)-JT effect (in which electronic degeneracy is split by degenerate e vibrational mode) in the literature [5,6,14,[18][19][20][21]. In the present case the splitting of the degeneracy of the E state is caused by the JT active nondegenerate b 1 and b 2 vibrational modes, known as the (E b)-JT effect [6,14].…”
Section: Introductionmentioning
confidence: 65%
“…The latter simulation is necessary to infer and assign the dominant progressions observed in the experiment. In the full e X-e A coupled state dynamical simulation performed here, we retained four a 1 (m 1 -m 4 ), two b 1 (m 6 -m 7 ), three b 2 (m 10 , m 11 and m 13 ) and four e (m 16 -m 19 ) vibrational modes. The number of SPF basis functions allocated to a given mode is estimated depending on its coupling strength and the convergence of the spectral envelope.…”
Section: Vibronic Spectrummentioning
confidence: 99%
“…7,11,[25][26][27][28][29][30] The e modes cease to be JT active in tetragonal systems. In this case, the JT perturbation of an E state is caused by the nondegenerate vibrational modes of b symmetry, known as (EXb)-JT effect.…”
Section: The Jahn-teller and Pseudojahn-teller Interactionsmentioning
confidence: 99%