Single Vibronic Level Emission Research Articles

Single vibronic level emission spectroscopy and fluorescence lifetime of the [formula omitted] system of CuOH and CuOD

We report new studies of the B ∼ 1 A ″ ↔ X ∼ 1 A ′ system of CuOH/CuOD, generated in a pulsed discharge source under jet-cooled conditions. Single vibronic level (SVL) emission spectra obtained from the 0 0 0 and 2 0 1 levels of the B ∼ 1 A ″ state reveal new information on the bending and Cu–O stretching frequencies in the ground state. The derived vibrational parameters are in good agreement with recent high level ab initio calculations. Rotationally resolved laser induced fluorescence excitation spectra of the 2 0 1 band were obtained, and a rotational analysis performed for the 63CuOD isotopomer. Additionally, B ∼ 1 A ″ state fluorescence lifetimes are reported.

Electronic Spectroscopy of an Isolated Halocarbocation: The Iodomethyl Cation CH2I+ and Its Deuterated Isotopomers

Building upon our recent observation of the gas-phase electronic spectrum of the iodomethyl cation (CH2I+), we report an extensive study of the electronic spectroscopy of CH2I+ and its deuterated isotopomers CHDI+ and CD2I+ using a combination of fluorescence excitation and single vibronic level (SVL) emission spectroscopies. The spectra were measured in the gas phase under jet-cooled conditions using a pulsed discharge source. Fluorescence excitation spectra reveal a dominant progression in nu3 (C-I stretch), the frequency of which is markedly smaller in the upper state. Rotational analysis shows that, while the A constant is similar in the two states, the excited state has significantly smaller B and C constants. These results indicate a lengthening of the C-I bond upon electronic excitation, consistent with calculations which show that this transition is analogous to the well-known pi-pi* transition in the isoelectronic substituted formaldehydes. SVL emission spectra show progressions involving four of the six vibrational modes; only the C-H(D) stretching modes remain unobserved. The vibrational parameters determined from a Dunham expansion fit of the ground state vibrational term energies are in excellent agreement with the predictions of density functional theory (DFT) calculations. A normal-mode analysis was completed to derive a harmonic force field for the ground state, where resonance delocalization of the positive charge leads to partial double bond character, H2C+-I <--> H2C=I+, giving rise to a C-I stretching frequency significantly larger than that of the iodomethyl radical.

Single vibronic level emission spectroscopy of the [formula omitted] system of bromochlorocarbene

In a search for transitions to the low-lying a ˜ 3 A ″ state, we have recorded single vibronic level (SVL) emission spectra of bromochlorocarbene, CBrCl, which probe the vibrational structure of the X ∼ 1 A ′ state up to ∼5500 cm −1 above the vibrationless level. These spectra reveal many previously unassigned levels, and a complete set of vibrational parameters was determined for the X ∼ 1 A ′ state. The derived parameters are compared with recent ab initio predictions.

Laser spectroscopy and dynamics of the jet-cooled AsH2 free radical

The A (2)A(1)-X (2)B(1) electronic transition of the jet-cooled AsH(2) free radical has been studied by laser-induced fluorescence (LIF), wavelength-resolved emission, and fluorescence lifetime measurements. The radical was produced by a pulsed electric discharge through a mixture of arsine (AsH(3)) and high pressure argon at the exit of a pulsed valve. Nine vibronic bands were identified by LIF spectroscopy in the 505-400 nm region, including a long progression in the bending mode and two bands (1(0) (1) and 1(0) (1)2(0) (1)) involving the excited state As-H symmetric stretch. Single vibronic level emission spectra showed similar activity in the bending and symmetric stretching frequencies of the ground state. High-resolution spectra of the 0(0) (0) band exhibited large spin splittings and small, resolved arsenic hyperfine splittings, due to a substantial Fermi contact interaction in the excited state. The rotational constants obtained in the analysis gave effective molecular structures of r"(0)=1.5183(1) A, theta"(0)=90.75(1) degrees and r'(0)=1.4830(1) A, theta'(0)=123.10(2) degrees . The excited state fluorescence lifetimes vary dramatically with rovibronic state, from a single value of 1.4 micros to many with lifetimes less than 10 ns, behavior which the authors interpret as signaling the onset of a predissociative process near the zero-point level of the ground state.

Electronic spectroscopy of the [formula omitted] system of CDCl

We report fluorescence excitation and single vibronic level emission spectra of the A ˜ 1 A ″ ↔ X ˜ 1 A ′ system of CDCl in the 500–740 nm region, measured under jet-cooled conditions using a pulsed discharge source. A total of 29 cold bands involving the pure bending levels 2 0 n ( n = 2–11), C–D stretching fundamental ( 1 0 1 ), and combination bands 2 0 n 3 0 1 ( n = 2–10), 2 0 n 3 0 2 ( n = 9), 1 0 1 2 0 n ( n = 2–8), and 1 0 1 2 0 n 3 0 1 ( n = 7) were observed; most of these are reported here for the first time. Rotational analysis typically yielded band origins and rotational constants for both isotopomers (CD 35Cl, CD 37Cl). The derived A ˜ 1 A ″ vibrational intervals are combined with previous studies at lower energy to determine excited state barriers to linearity for the 2 n , 2 n 3 1, and 1 12 n progressions. The A ˜ 1 A ″ state C–D stretching frequency (2229.6 cm −1) is determined here for the first time, in excellent agreement with ab initio theory. Following our observation of new bands in this system, we obtained single vibronic level (SVL) emission spectra which probe the vibrational structure of the X ˜ 1 A ′ state up to ∼8000 cm −1 above the vibrationless level. The total number of X ˜ 1 A ′ and a ˜ 3 A ″ levels observed is more than twice that previously reported, and a complete set of Dunham parameters was determined for the X ˜ 1 A ′ state of CD 35Cl and CD 37Cl. Comparisons with previous experimental and recent high level ab initio studies are reported. Our results shed new light on the vibrational structure of the X ˜ 1 A ′ , A ˜ 1 A ″ , and a ˜ 3 A ″ states of CDCl, and, more generally, spin–orbit coupling in the monohalocarbenes.

Single vibronic level emission spectroscopy of the [formula omitted] system of dibromocarbene

Following the development of an improved discharge recipe for production of dibromocarbene (CBr 2), and an extensive spectroscopic survey of the A ˜ 1 B 1 ← X ˜ 1 A 1 system that has led to a revision in the position of the origin, we have recorded single vibronic level (SVL) emission spectra of C 79Br 81Br and C 81Br 2 which probe the vibrational structure of the X ˜ 1 A 1 state up to ∼7000 cm −1 above the vibrationless level. These spectra reveal many previously unassigned levels. In the region between ∼3600 and 5900 cm −1, or between the singlet-triplet gap proposed by Hsu et al. [H.-J. Hsu, W.-Z. Chang, B.-C. Chang, Phys. Chem. Chem. Phys. 2005, 7, 2468–2473] to that predicted by theory, we find that ∼90% of the lines can be assigned to X ˜ 1 A 1 levels within three standard deviations of our Dunham expansion fit, suggesting that the vast majority of emission lines terminate on levels of the singlet state. A nearly complete set of vibrational parameters was determined for the X ˜ 1 A 1 state; the derived parameters are in good agreement with recent ab initio predictions.

Single vibronic level emission spectroscopic studies of the ground state energy levels and molecular structures of jet-cooled HGeBr, DGeBr, HGeI, and DGeI

Single vibronic level dispersed fluorescence spectra of jet-cooled HGeBr, DGeBr, HGeI, and DGeI have been obtained by laser excitation of selected bands of the A (1)A(")-X (1)A(') electronic transition. The measured ground state vibrational intervals were assigned and fitted to anharmonicity expressions, which allowed the harmonic frequencies to be determined for both isotopomers. In some cases, lack of a suitable range of emission data necessitated that some of the anharmonicity constants and vibrational frequencies be estimated from those of HGeClDGeCl and the corresponding silylenes (HSiX). Harmonic force fields were obtained for both molecules, although only four of the six force constants could be determined. The ground state effective rotational constants and force field data were combined to calculate average (r(z)) and approximate equilibrium (r(e) (z)) structures. For HGeBr r(e) (z)(GeH)=1.593(9) A, r(e) (z)(GeBr)=2.325(21) A, and the bond angle was fixed at our CCSD(T)/aug-cc-pVTZ ab initio value of 93.6 degrees . For HGeI we obtained r(e) (z)(GeH)=1.589(1) A, r(e) (z)(GeI)=2.525(5) A, and bond angle=93.2 degrees . Franck-Condon simulations of the emission spectra using ab initio Cartesian displacement coordinates reproduce the observed intensity distributions satisfactorily. The trends in structural parameters in the halogermylenes and halosilylenes can be readily understood based on the electronegativity of the halogen substituent.

Electronic spectroscopy of the ÃA″1↔X̃A′1 system of CDBr

We report fluorescence excitation and single vibronic level emission spectra of jet-cooled CDBr in the 450–750nm region. A total of 32 cold bands involving the pure bending levels 20n with n=3–10 and combination bands 20n301 (n=2–10), 20n302 (n=2–9), 10120n (n=7–10), and 10120n301 (n=6,8–9) in the ÃA″1←X̃A′1 system of this carbene were observed; most of these are reported and/or rotationally analyzed here for the first time. Rotational analysis yielded band origins and effective (B¯) rotational constants for both bromine isotopomers (CD79Br and CD81Br). The derived ÃA″1 vibrational intervals are combined with results of Yu et al. [J. Chem. Phys. 115, 5433 (2001)] to derive barriers to linearity for the 2n, 2n31, and 2n32 progressions. The ÃA″1 state C–D stretching frequency (2350cm−1) is determined for the first time, in excellent agreement with theory, as are the Br79–Br81 isotope splittings in the excited state. Our emission spectra probe the vibrational structure of the X̃A′1 and ãA″3 states up to ∼9000cm−1 above the vibrationless level of the X̃A′1 state; the total number of levels observed is around twice that previously reported. Unlike CHBr, where even the lowest bending levels are perturbed by spin-orbit interaction with the triplet origin, the term energy of every level save one below 3000cm−1 in CDBr is reproduced by a Dunham expansion to within a standard deviation of 1cm−1, and a spin-orbit coupling matrix element of ∼330cm−1 is derived from a deperturbation analysis of the triplet origin. The multireference configuration interaction (MRCI) calculations of Yu et al. [J. Chem. Phys. 115, 5433 (2001)] well reproduce triplet perturbations in the pure bending manifold, and globally, the vibrational frequencies of X̃A′1, ãA″3, and ÃA″1 are in excellent agreement with theoretical predictions.

The electronic spectrum of jet-cooled copper hydrosulfide (CuSH)

The electronic spectrum of copper hydrosulfide (CuSH) has been observed for the first time. CuSH and CuSD were produced in a pulsed discharge jet by the reaction of sputtered copper atoms with H(2)S or D(2)S. Strong laser-induced fluorescence bands observed in the 515-470 nm region were assigned as the ~A (1)A"-X (1)A' band system based on detailed rotational analysis and the correspondence with the predictions of our CCSD(T)6-311++G(3df,3pd) ab initio calculations. The laser-induced fluorescence and single vibronic level emission spectra consist primarily of a short progression in nu(3), the Cu-S stretching mode, indicative of only modest structural changes on electronic excitation. The rotational constants of four isotopomers of CuSH were used to determine effective zero-point structures in the combining states as r"(CuS)=2.0916(3) A, r"(SH)=1.364(3) A, theta"=93.5(3) degrees , r'(CuS)=2.172(3) A, r'(SH)=1.408(23) A, and theta'=93.5(24) degrees . A comparison of the ground state structures of the known metal hydrosulfides shows that they can be considered to be metal-substituted hydrogen sulfides. The electronic spectra and molecular structures of CuOH and CuSH are compared and contrasted.

Laser Spectroscopy of a Halocarbocation in the Gas Phase: CH2I+

We report the first gas-phase observation of the electronic spectrum of a simple halocarbocation, CH2I+. The ion was generated rotationally cold (Trot approximately 20 K) using pulsed discharge methods and was detected via laser spectroscopy. The identity of the spectral carrier was confirmed by modeling the rotational contour observed in the excitation spectra and by comparison of ground state vibrational frequencies determined by single vibronic level emission spectroscopy with Density Functional Theory (DFT) predictions. The transition was assigned as 3A1 <-- X1A1. This initial detection of the electronic spectrum of a halocarbocation in the gas phase should open new avenues for study of the structure and reactivity of these important ions.

Fluorescence excitation and single vibronic level emission spectroscopy of the ÃA″1←X̃A′1 system of CHCl

We report new fluorescence excitation and single vibronic level emission spectra of the A (1)A(")<-->X (1)A(') system of CHCl. A total of 21 cold bands involving the pure bending levels 2(0) (n) with n=1-7 and combination bands 2(0) (n)3(0) (1)(n=4-7), 2(0) (n)3(0) (2)(n=4-6), 1(0) (1)2(0) (n)(n=5-7), 1(0) (1)2(0) (n)3(0) (1)(n=4-6), and 1(0) (1)2(0) (n)3(0) (2)(n=4) were observed in the 450-750 nm region; around half of these are reported and/or rotationally analyzed here for the first time. Spectra were measured under jet-cooled conditions using a pulsed discharge source, and rotational analysis typically yielded band origins and rotational constants for both isotopomers (CH(35)Cl,CH(37)Cl). The derived A (1)A(") vibrational intervals are combined with results of Chang and Sears to determine the excited state barrier to linearity [V(b)=1920(50) cm(-1)]. The A (1)A(") state C-H stretching frequency is determined here for the first time, in excellent agreement with ab initio predictions. Following our observation of new bands in this system, we obtained the single vibronic level (SVL) emission spectra which probe the vibrational structure of the X (1)A(') state up to approximately 9000 cm(-1) above the vibrationless level. The total number of X (1)A(') levels observed is around three times than that previously reported, and we observe five new a (3)A(") state levels, including all three fundamentals. The results of a Dunham expansion fit of the ground state vibrational term energies, and comparisons with the previous experimental and recent high level ab initio studies, are reported. Our data confirm the previous assignment of the a (3)A(") origin, and our value for T(00)(a-X)=2172(2) cm(-1) is in excellent agreement with theory. By exploiting SVL spectra from excited state levels with K(a) (')=1, we determine the effective rotational constant (A-B) of the triplet origin, also in good agreement with theory. Our results shed new light on the vibrational structure of the X (1)A('), A (1)A("), and a (3)A(") states of CHCl, and, more generally, spin-orbit coupling in the monohalocarbenes.

Experimental and theoretical investigation of the dispersed fluorescence spectroscopy of HC4S

A high-resolution single vibronic level emission study from the A (2)Pi(32) state of the HC(4)S radical is reported. Ground state density functional theory frequencies have been used to assign ground state vibronic levels involving three stretching modes nu(2), nu(3), and nu(5) in the region of 0-3250 cm(-1), while the frequency of nu(4) remains speculative. Tentative assignments are given for the complicated structures arising from Renner-Teller and spin-orbit interactions within the bending energy levels. From analysis of the dispersed emission spectra, Fermi resonances involving pairs of bands have been identified in the A (2)Pi(32)<--X (2)Pi(32) laser induced fluorescence spectrum.

In search of the germanium halomethylidyne (GeC–X; X=F,Cl,Br) free radicals: Ab initio studies of their spectroscopic signatures

A variety of ab initio methods have been used to calculate the X (2)Pi and A (2)Sigma(+) state spectroscopic parameters of the GeCX (X=F,Cl,Br) free radicals. The theoretical methods and basis sets were tested on GeCH, for which extensive experimental data are available, and found to give predictions sufficiently reliable to guide experimental searches for spectra. In all cases, the linear Ge=C-X species was found to be the global minimum on the potential energy surface, with the bent X-Ge=C ((2)A(')) isomer as a local minimum much higher (62-36 kcal/mol) in energy. In both the ground and excited states, the GeC moiety is very similar to that of GeCH, with a double bond in the lower state and a triple bond in the excited state, indicating that halogenation does not radically perturb the energetics or structure of germanium methylidyne. Ground state GeCX radicals have suitable rotational constants for microwave studies, although they suffer from only modest dipole moments. Matrix infrared experiments are most likely to detect the nu(1) fundamentals in the 1450-1100 cm(-1) region or the nu(3) fundamentals at the transition between the mid- and far-infrared regions. We have used the ab initio values for the Renner-Teller parameter, the average bending frequency, and the spin-orbit coupling constant to calculate the ground state energy levels, which will be helpful in the interpretation of A-X single vibronic level emission spectra, if they can be observed. The electronic absorption spectra of the (2)Pi(32) spin component of the 0(0) (0) bands of all three radicals have been calculated assuming typical jet-expansion conditions and should be useful in future laser-induced fluorescence, resonance enhanced multiphoton ionization, or cavity ringdown searches for the electronic band systems.

The ground state energy levels and molecular structure of jet-cooled HGeCl and DGeCl from single vibronic level emission spectroscopy

Single vibronic level dispersed fluorescence spectra of jet-cooled HGeCl and DGeCl have been recorded by laser excitation of selected bands of the A 1A"-X 1A' electronic transition. Twenty-six ground state vibrational levels of HGeCl and 42 of DGeCl were measured, assigned, and fitted to standard anharmonicity expressions, which allowed all the harmonic frequencies to be determined for both isotopomers. A normal coordinate least squares analysis obtained by fitting the harmonic frequencies yielded reliable values for five of the six force constants. The ground state effective rotational constants and force field data were combined to calculate average (rz) and approximate equilibrium (re z) structures, with re z(GeH)=1.586(1) A, re z(GeCl)=2.171(2) A, and the bond angle fixed at our CCSD(T)/aug-cc-pVTZ ab initio value of 93.9 degrees . Comparisons show that the derived bond lengths are consistent with those of the appropriate diatomic molecules in their ground electronic states and the bond angle is similar to that of germylene (GeH2). A Franck-Condon simulation of the vibrational intensities in the 0(0) (0) band emission spectrum of HGeCl using ab initio force field data shows good agreement with experiment, lending credence to the vibrational analysis of the observed spectra.

Electronic and infrared spectroscopy of chiral (±)- cis-1-amino-indan-2-ol in a supersonic jet

The structure of isolated (±)- cis-1-amino-indan-2-ol in a supersonic jet has been investigated by laser-induced fluorescence (LIF) excitation, single vibronic level (SVL) emission and double resonance IR–UV spectra. Two conformers, whose S 0–S 1 transition origins are separated only by 3 cm −1, have been characterised by their dispersed emission and their IR absorption in the region of the CH, NH and OH stretch. The two observed species have been assigned with the aid of Density Functional Theory (DFT) calculation at the B3LYP/6-31 G** level of theory to the two lowest energy structures involving an intramolecular hydrogen bond between the OH and NH 2 groups. The ground state vibrational modes obtained from SVL emission for low frequency and IR spectra for high frequency modes have been compared with the calculated harmonic frequencies.

Laser-induced fluorescence and single vibronic level emission spectroscopy of chiral (R)-1-aminoindan and some of its clusters in a supersonic jet

Two low energy conformers of the chiral (R)-1-aminoindan molecule are identified in supersonic jet and their ground and excited states vibrational spectroscopy has been investigated by laser-induced fluorescence (LIF) excitation and single vibronic level (SVL) emission spectroscopy. Ab initio calculations confirm the existence of two lowest-energy structures, where the amino group is in equatorial position with its lone pair directed opposite to the aromatic electron cloud. Harmonic frequencies have been calculated for these two conformers at the DFT level with B3LYP functional. A low-frequency progression of 118 cm(-1) and 114 cm(-1), respectively, appears in the fluorescence excitation spectrum of the two conformers, with its ground state counterpart at approximately 147 cm(-1). It has been assigned to the puckering motion coupled with the ring flapping mode. The other calculated low-frequency mode corresponds to the puckering motion coupled with the ring twisting mode and its ground state frequency has been observed at 119 cm(-1) and 111 cm(-1) from SVL spectra. Both conformers form similar 1 : 1 water clusters, whose 0-0 transitions are shifted to the blue by 41 cm(-1) and 44 cm(-1), respectively, and whose SVL spectra are similar. Interestingly, one of the conformers seems to preferentially make complexes with (S)-methyllactate, while the other one shows selective complexation to (R)-methyllactate.

Probing spin–orbit mixing and the singlet–triplet gap in dichloromethylene via Ka-sorted emission spectra

The magnitude of the singlet-triplet gap in dichloromethylene (CCl(2)) has been a point of controversy in the recent literature. In this study, we report single vibronic level emission spectra of the A(1)B(1)-->X[combining tilde](1)A(1) system of the carbene C(35)Cl(2), which probes the vibrational structure of the X[combining tilde](1)A(1) state up to approximately 10,000 cm(-1) above the vibrationless level. By the careful selection of bands where complete isotope and K(a)' selectivity in excitation was possible, we measured K(a)'-sorted emission spectra in order to test the previously established hypothesis [M.-L. Liu, C.-L. Lee, A. Bezant, G. Tarczay, R. J. Clark, T. A. Miller and B.-C. Chang, Phys. Chem. Chem. Phys., 2003, 5, 1352] that unassigned lines lying above approximately 5,000 cm(-1) belong to levels of the ã(3)B(1) state. The K(a)'-sorting method discriminates between singlet and triplet levels via the (A''-B[combining macron]'') rotational constant, which is significantly larger for pure triplet levels due to the larger equilibrium bond angle. In the region between 3,500 and 9,000 cm(-1) above the vibrationless level of the X[combining tilde](1)A(1) state, we find only a very modest increase in (A''-B[combining macron]''), and approximately 86% of the lines observed between 5,000 and 9,000 cm(-1) can be assigned to X[combining tilde](1)A(1) levels within 3 standard deviations of our Dunham expansion fit, which included more than 140 levels in total. A nearly complete set of Dunham parameters was determined for the C(35)Cl(2) isotopomer, and the X[combining tilde](1)A(1) state term energies up to 4,000 cm(-1) are in excellent agreement with recent variational calculations of Tarczay, et al. [G. Tarczay, T. A. Miller, G, Czakó and A. G. Császár, Phys. Chem. Chem. Phys., 2005, 7, 2881]. Finally, the implication of our results for the singlet-triplet gap in dichloromethylene is discussed.

Observation of a new phosphorus-containing reactive intermediate: Electronic spectroscopy and excited-state dynamics of the HPBr free radical

The A (2)A(')-X (2)A(") electronic spectra of jet-cooled HPBr and DPBr have been obtained for the first time using the pulsed electric discharge technique with a precursor mixture of PBr(3) and H(2)/D(2). Laser-induced fluorescence and single vibronic level emission spectra gave the bending and P-Br stretching frequencies in the ground and excited states of both isotopomers. Rotational analyses of the HPBr and DPBr 0(0) (0) bands showed small spin splittings characteristic of a doublet-doublet transition of an asymmetric-top molecule. From the ground- and excited-state rotational constants, effective (r(0)) structures were derived with r(")(PH)=1.4307(86) A, r(")(PBr)=2.2021(9) A, and theta(")=95.2(8) degrees, and r(')(PH)=1.434(31) A, r(')(PBr)=2.1669(26) A, and theta(')=115.5(16) degrees . In a few favorable cases, further hyperfine splitting of the spin-rotation energy levels has been observed, due to the excited-state Fermi contact interaction of the unpaired electron with the spin magnetic moment of the (31)P nucleus, with a(F) (')=0.064(9) cm(-1) for HPBr. Fluorescence depletion spectroscopy and lifetime measurements indicate that higher vibrational levels of the A (2)A(') state are predissociated by a X (2)A(") dissociative continuum. CCSD(T)/aug-cc-pVTZ calculations predict that the most likely dissociation process is HPBr (X (2)A("))-->PH((3)Sigma(-))+Br((2)P(u)).

A Combined Ab Initio/Franck–Condon Study of the ÖX̃ Single‐Vibronic‐Level Emission Spectrum of CCl2 and the Photodetachment Spectrum of CCl2−

State-of-the-art ab initio calculations have been carried out on the X1A1, ã3B1 and A1B1 states of CCl2 and the X2B1 state of CCl2-. Franck-Condon factors including anharmonicity have been calculated, between the CCl2 states, and between the CCl2- X2B1 state and the CCl2 states. They are used to simulate the A-X single-vibronic-level (SVL) emission spectra of CCl2 determined by M.-L. Lui et al. [PCCP 2003, 5, 352] and the 364 nm laser photodetachment spectrum of CCl2- obtained by R. L. Schwartz et al. [J. Phys. Chem. A 1999, 103, 8213]. Comparison between simulated and observed spectra confirms the vibrational assignments of the X2B1 SVL emission spectra and the T0 position of the A1B1 state of CCl2. For the photodetachment spectrum of CCl2-, spectral simulation shows that the higher binding energy ã3B1(CCl2) <-- X2B1(CCl2-) band is well separated from the X1A1(CCl2) <-- X2B1(CCl2-) band. It is concluded that the observed second band, which overlaps heavily with the X1A1(CCl2) <-- X2B1(CCl2-) band in the photodetachment spectrum of CCl2- cannot be assigned to the CCl2(ã3B1) + e --> CCl2-(X2B1) detachment process. Further ab initio calculations carried out in the present investigation support the suggestion that the second band in the 364 nm photodetachment spectrum of CCl2- is due to detachment from an excited state of CCl2-, a linear quartet state, to a triplet state of CCl2. These calculations identify the anionic state to be the lowest 4Sigmag- (4Sigma-) state, which photodetaches vertically to the 3Sigmag- (3Sigma-; adiabatically ã3B1) and/or 3Pi(u) (3Pi) states of CCl2 to give the second band observed in the 364 nm photodetachment spectrum of CCl2-.

Renner–Teller vibronic analysis for a tetra-atomic molecule. II. The ground state of the HCCS free radical

We have studied the tetra-atomic Renner-Teller effect in the ground state of the jet-cooled HCCS and DCCS free radicals. The reactive intermediates were produced in a pulsed discharge jet using thiophene or deuterated thiophene precursors and the ground-state vibronic energies were measured using the single vibronic level emission spectroscopy technique. In HCCS, emission and fluorescence depletion experiments proved that some previously unassigned laser-induced fluorescence (LIF) features were anomalous 2Delta32-2Pi32 transitions, which gave information on several ground-state 2Delta32 levels. In DCCS, rotational mixing of the excited state v'=0(2Pi32) level with the 4(1)(1 2Sigma12) level allowed several ground-state 2Sigma levels to be observed in emission. In addition, we have shown that some previously unassigned weak LIF bands of DCCS are anomalous 2Pi12-2Pi32 transitions which have allowed us to accurately measure the ground-state spin-orbit splitting (259.0 cm(-1)) for the first time. All of the expected ground-state 2Pi32 levels and the majority of the 2Pi12 levels up to 1700 cm(-1) have been observed for both isotopomers. The data have been fitted by an effective Hamiltonian matrix treatment that included Renner-Teller, spin-orbit coupling, anharmonicity, and Fermi resonance effects for the two bending vibrations and the CS stretching mode. This has allowed an unusually complete description of the orbital angular momentum coupling effects, including the determination of the epsilon4, epsilon5, and epsilon45 terms for the first time. Subtle effects in both the LIF and emission spectra signal the presence of Sears resonances in both the ground and excited states of these radicals.