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Electronic Band Systems of SF_2 Radicals Observed by Resonance-Enhanced Multiphoton Ionization

机译:共振增强多光子电离观察到的SF_2自由基电子带系统

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摘要

A pulsed dc electric discharge in a pulsed supersonic beam has been used as an efficient source of producing radicals. The (2+1) REMPI spectra of the SF_2 radicals were investigated between 245 and 365 nm (54945-81630 cm~(-1)). Eight electronic band systems have been observed in this range. One series with quantum defect δ = 1.961(6) is comprised of the B-tilde ~1B_1(4s) and J-tilde ~1B_1(5s) Rydberg states which have origins at v_(0-0) = 54470 and 68951 cm~(-1), respectively. vibrational analyses of these Rydberg states showed that in the B-tilde ~1B_1(4s) state ω_1'(a_1 sym str) = 981(23) cm~(-1) J-tilde ~1B_1(5s) state ω_1'(a_1 sym str) = 942(3) cm~(-1). A second Rydberg series E-tilde (4p) with quantum defect δ = 1.61 is characterized with the spectroscopic values v_(0-0) = 62025 cm~(-1), ω_1'(a_1 sym str) = 941(27) cm~(-1), and ω_2'(a_1, bend) = 413(12) cm~(-1). Incompletely rotational analysis revealed that the F electronic state with v_(0-0) = 63812 cm~(-1), ω_1'(a_1 sym str) = 966(6) cm~(-1), and ω_2'(a_1, bend) = 417(23) cm~(-1) merges with the vibrational progression of the E-tilde (4p) state. The F-tilde state might be a 4p Rydberg state of another hybrid symmetry with the quantum defect δ = 1.50. A third Rydberg series is comprised of the G-tilde (3d) (v_(0-0) = 68378 cm~(-1), ω_1' = 939(12) cm~(-1), δ = 0.086), the H-tilde (3d) (v_(0-0) = 68571 cm~(-1), ω_1' = 936(4) cm~(-1), δ = 0.064), and the I-tilde (3d) (v_(0-0) = 68847 cm~(-1), ω_1' = 933(4) cm~(-1), δ = 0.032). In addition, two valence states labeled as the B-tilde' state (38623 cm~(-1)) and C-tilde state (56219-61278 cm~(-1)) were also observed. A fit of the Rydberg formula to the ns(~1B_1) (n = 4,5) origins found the adiabatic ionization potential of SF_2 radicals to be IP_a = 10.021(1) eV.
机译:脉冲超声波束中的脉冲直流放电已被用作产生自由基的有效来源。在245和365 nm(54945-81630 cm〜(-1))之间研究了SF_2自由基的(2 + 1)REMPI光谱。在此范围内已观察到八个电子波段系统。量子缺陷δ= 1.961(6)的一个序列由B波浪〜1B_1(4s)和J波浪〜1B_1(5s)的Rydberg态组成,起源于v_(0-0)= 54470和68951 cm〜 (-1)。这些Rydberg态的振动分析表明,在B波浪〜1B_1(4s)状态ω_1'(a_1 sym str)= 981(23)cm〜(-1)J波浪〜1B_1(5s)状态ω_1'(a_1 sym str)= 942(3)cm〜(-1)。具有光谱缺陷δ= 1.61的第二Rydberg级数E-tilde(4p)的特征在于光谱值v_(0-0)= 62025 cm〜(-1),ω_1'(a_1 sym str)= 941(27)cm 〜(-1)和ω_2'(a_1,弯曲)= 413(12)cm〜(-1)。不完全旋转分析显示v_(0-0)= 63812 cm〜(-1),ω_1'(a_1 sym str)= 966(6)cm〜(-1)和ω_2'(a_1,弯曲)= 417(23)cm〜(-1)与E波浪(4p)状态的振动进程合并。 F波浪态可能是另一种具有对称缺陷δ= 1.50的混合对称的4p Rydberg状态。第三个Rydberg级数由G-波浪线(3d)(v_(0-0)= 68378 cm〜(-1),ω_1'= 939(12)cm〜(-1),δ= 0.086), H波浪线(3d)(v_(0-0)= 68571 cm〜(-1),ω_1'= 936(4)cm〜(-1),δ= 0.064)和I波浪线(3d)( v_(0-0)= 68847 cm〜(-1),ω_1'= 933(4)cm〜(-1),δ= 0.032)。此外,还观察到两个价态,分别标记为B-波浪态(38623 cm〜(-1))和C-波浪态(56219-61278 cm〜(-1))。将Rydberg公式与ns(〜1B_1)(n = 4,5)的原点拟合,发现SF_2自由基的绝热电离电势为IP_a = 10.021(1)eV。

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