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Electronic spectra


The laboratory astrophysics group at the CfA has continued to provide quantitative, high spectral resolution measurements of molecules of atmospheric and astrophysical interest in the ultraviolet. Theoretical studies of the predissociation of the Schumann-Runge (S-R) bands of O2 have been carried out for both rotational10 and isotopic dependency.11 Absorption bands of the S-R system have been observed at 670 K at high resolution, and precise wavelength measurements have led to the molecular constants of the ground state of O2.12 Two highly excited states of O2 have been identified in collaboration with colleagues at the Photon Factory, Japan, and NRC, Canada.13 Absorption measurements at Doppler limited resolution have been carried out by Yoshino and colleagues with a VUV Fourier transform spectrometer (FTS) in combination with a White cell at Imperial College (IC), London, U.K. The O2 Herzberg I band system () has been measured at a resolution of 0.06 cm-1;14 band oscillator strengths and rotational line strengths have been obtained.15 These are the first absorption intensity measurements of the Herzberg bands free of problems arising from inadequate spectral resolution. In addition, the NO and bands have been measured at a resolution 0.06 cm-1 with the VUV FTS at IC.16 To extend the high resolution measurements to shorter wavelengths, the CfA/IC group moved this apparatus to the Photon Factory, Japan, where VUV radiation from a synchrotron source with a narrow band predisperser is available.17 Analysis of the measurements of the NO bands and the S-R bands of O2 obtained with this facility are in progress. The absorption cross sections for the VUV diffuse bands of CO218 and H2O19 have been measured.


The VUV spectrum of CO continues to be intensively studied by several groups. The CfA group has obtained photoabsorption cross sections of CO in the wavelength region 92.5 nm to 97.4 nm at ~20 K, thus greatly simplifying their application to astrophysical models.20 The band oscillator strengths of the A(v')-X(0) fourth positive bands of CO for v'=11 - 14 have been obtained with high resolution21 and have confirmed the values of Chan et al.22 The Meudon group has also studied the AX transition for 12C18O and 13C18O.23,24 Using the A state term values a new set of term levels for the B, C and E states has been established.25


A new triplet state of CO (k) has been analyzed through its interactions with the E and B states and by direct absorption measurements.26,27,28 The B (v=3) level situated above the BD' crossing has been observed and calculated with the semi-empirical potentials established earlier.29 A pulsed jet has been used in conjunction with the 10m vacuum spectrograph and the BRV pulsed continuum to obtain cooled spectra of the CO Rydberg states.30


Predissociative and radiative lifetimes of the excited states of CO have been determined from line broadening measurements on singly resolved rotational states using a coherent and tunable VUV source by Ubachs and co-workers.31,32,33 For several states, the predissociation rates were found to depend on rotational state, parity and isotope. The E v=0 and 1 levels were carefully studied for 12CO and 13CO and were found to be strongly predissociated by the k bound state. The lifetime of the (4p)L v=0 state (f parity) was determined at 1.0 ns, typical of a radiative rather than a predissociative lifetime.


Basic spectroscopic work on the most important astrophysical molecule, H2, continues by the Meudon group. The photographic atlas of the Lyman and Werner bands has been published.34 More than 12000 lines are tabulated, 96% of which have at least one assignment. New calculations concerning the B' and D states have been published.35 Together with previous work concerning the B and C, states these allow precise calculations of the Werner and Lyman bands. Comprehensive tables of line positions and intensities are now available.36,37


A new set of molecular constants for the ground state of N2 has been established using all the data available in the different spectral ranges.38 A comprehensive model of the first seven singlet Rydberg and valence states has been established. This will allow precise modeling of the VUV emission of N2 in the atmosphere of Titan and the Earth around 100 nm.39 The nf Rydberg levels of 14N2 converging on the state of N have been studied.40


Studies of the N molecular ion have been made by the Berkeley group with a Pointolite arc which produces highly excited levels of the ion, and with a cooled hollow cathode lamp. The analysis was extended to much higher rotational energies as compared to the hollow cathode or furnace spectra.41 Bernath and co-workers used the Fourier Transform technique to study the electronic spectra of a number of astrophysically relevant molecules including CoH45, CH46 and the Swan system of C2.47


Extensive electronic structure calculations continue to provide valuable information on potential energy surfaces, transition moments, spectroscopic constants and line intensities. A theoretical study of the NO , the 11000 Å, and the b bands has been made by the NASA-Ames group,42,43,44 who also computed the electronic states of MgC.49 The ground and excited states of SiH+152 and CP153 have been calculated by the Wuppertal group. Potential surfaces and line intensities of Si2C,48 N3+,50 NH2+,51 and CO252 have been investigated theoretically by the French group. The flat shape of the N3+ X ground state along the asymmetric displacement coordinate leads to strong anharmonic resonances. For NH2+, the quasilinear ground state and the bent quasi-linear a1A1 - b1B1 Renner-Teller system have been studied up to high energies. An exhaustive study of the excited electronic states of CO2 suggests that the observed peculiar splittings of the first dipole-allowed electronic transition X are due to complex avoided crossings and vibronic coupling effects between the Rydberg and valence states.


The Leiden group has performed comprehensive theoretical calculations of the absorption spectra of the lowest 10 electronic states of CH2 and its isotopes.53-57 Similar work on NH2 is in progress.58 The HCO+ ion appears to be remarkably transparent to ultraviolet radiation, since all its dipole-allowed transitions lie at very high energies.59,60


The transition rates for ZrO have been measured from a laboratory absorption spectrum by the Berkeley group, for the purpose of resolving differences between an earlier analysis of an emission spectrum, and experimental results and theoretical treatments.61 The spectrum of LaS from a carbon tube furnace has been produced and analyzed.62 A major theoretical effort by Langhoff on the g f values for all absorption lines of low-lying electronic states of TiO that would contribute to the opacity of cool evolved stars has just been finished.63,64


The SCAN data base by Jørgenson9 contains information about the identification, frequency, excitation energy and strength of ~70 million lines from the molecules CN, CH65, TiO, H2O, HCN, C2H2 and C3. The Harvard-Smithsonian data base on TiO, C2, SiO, CN, CO, H2, CH, NH, OH, MgH and SiH was recently reviewed by Kurucz.66


There has been major progress in experimental and theoretical studies of larger molecules. The photofragmentation of model PAH monocations such as deuterated naphtalene67 and benzene68 has been studied using synchrotron radiation in the range 15-35 eV. The effect of molecular size has been evaluated.69 The single and double ionization potentials of PAH's have been modeled by an empirical expression.70 The formation, relaxation and destruction of negative PAH ions has been studied by an electron diffusion technique.71 The formation of PAH's in stellar envelopes has been modeled on the basis of the laboratory data. Small PAH's appear to be formed near the star and destroyed further out. Larger ones are formed at larger distances by condensation of the small PAH's produced initially.72,73 Ab initio studies of the electronic absorption spectra of some PAH cations have been made in the Bonn group.57


The possibility that linear carbon chains are responsible for some of the diffuse interstellar bands has received renewed attention.74,75 Detailed absorption spectra of these chains and their cations in neon matrices have been obtained by Maier and co-workers.76-82 A possible assignment of two diffuse interstellar bands observed at near-infrared wavelengths with C60+ was made by Foing & Ehrenfreund,83 based on spectra by Fulara et al.84 The electronic spectroscopy of C60 has been studied in the Meudon laboratory between 200 and 750 nm by electron energy loss spectroscopy.85,70 Rotational band contours of C60 and linear carbon chains have been calculated and compared to the diffuse interstellar bands.86 It is concluded that most DIB's would be due to molecules containing more than 10 atoms provided the excited states are coupled with isoenergetic vibronic levels of lower electronic states.



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