1982
DOI: 10.1016/0022-2852(82)90242-9
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The band system of acetylene

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Cited by 161 publications
(101 citation statements)
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“…Herzberg (1966) and Robin (1985) reviewed in detail the work reported before 1985. More recent aspects include measurements of the absolute cross section for photoabsorption in the Rydberg series of gaseous acetylene in the wavelength region 105-155 nm (Suto & Lee 1984;Cooper et al 1995) and the virtual valence band systemÃ←X at 214-248 nm (Watson et al 1982); the absorption spectrum in solid Ar at 10 K was measured in the wavelength region 107-220 nm (Wu et al 2010). The temperature-dependent measurements of absolute absorption cross sections of gaseous acetylene in the UV and VUV regions include the virtual valence statesÃ←X andB←X in 153-214 nm (Wu et al 1989;Chen et al 1991;Smith et al 1991) and extending to the Rydberg transitions near 120 nm (Wu et al 2001).…”
Section: Introductionmentioning
confidence: 99%
“…Herzberg (1966) and Robin (1985) reviewed in detail the work reported before 1985. More recent aspects include measurements of the absolute cross section for photoabsorption in the Rydberg series of gaseous acetylene in the wavelength region 105-155 nm (Suto & Lee 1984;Cooper et al 1995) and the virtual valence band systemÃ←X at 214-248 nm (Watson et al 1982); the absorption spectrum in solid Ar at 10 K was measured in the wavelength region 107-220 nm (Wu et al 2010). The temperature-dependent measurements of absolute absorption cross sections of gaseous acetylene in the UV and VUV regions include the virtual valence statesÃ←X andB←X in 153-214 nm (Wu et al 1989;Chen et al 1991;Smith et al 1991) and extending to the Rydberg transitions near 120 nm (Wu et al 2001).…”
Section: Introductionmentioning
confidence: 99%
“…12,14,[59][60][61][62][63][64][65][66] This state therefore provides optimal testing ground of the algebraic method. There are three fundamental bending vibrations of trans-S 1 with symmetry a u , b u , a g as shown in Fig.…”
Section: Description Of Trans-s 1 Bending Spectrummentioning
confidence: 99%
“…4 The transition is now known to be a π * ← π excitation from the linear ground state to a trans-bent excited state, S 1 (à 1 A u ). Further detailed analyses by Watson et al, [5][6][7] the Crim group, 8,9 Yamakita and Tsuchiya, [10][11][12] and Merer et al [13][14][15][16][17] have led to an essentially complete assignment of the vibrational and rotational structure up to 4500 cm −1 above the zero-point level of theà state. One of the most interesting results of these analyses has been the discovery 17,18 of bands that belong to the cis-bent isomer of theà state, the zero-point level of which lies about 2670 cm −1 higher in energy than that of the trans-bent isomer.…”
Section: Introductionmentioning
confidence: 99%