52 research outputs found
Characterisation of a new VUV beamline at the Daresbury SRS using a dispersed fluorescence apparatus incorporating CCD detection
The design and performance of a new normal incidence monochromator at the Daresbury Synchrotron Radiation Source, optimised for experiments requiring high flux of vacuum-UV radiation, are described. The re-developed beamline 3.1, based on the Wadsworth design of monochromator, is the source of tunable vacuum-UV photons in the range 4 – 31 eV, providing over two orders of magnitude more flux than the vacuum-UV, Seya monochromator in its previous manifestation. The undispersed and dispersed fluorescence spectra resulting from photoexcitation of N, CO, CF and CF are presented. Emitting species observed were N B - X, CO Aď€ - Xď€ and Bď€ - Xď€, CF Cď€T - Xď€T and Cď€T - Aď€T, CF* A - A, and CF Bď€A - Xď€E. A CCD multi-channel detector has significantly reduced the time period needed to record dispersed fluorescence spectra with a comparable signal-to-noise ratio
Studies of Diffuse Interstellar Bands. V. Pairwise Correlations of Eight Strong DIBs and Neutral Hydrogen, Molecular Hydrogen, and Color Excess
We establish correlations between equivalent widths of eight diffuse
interstellar bands (DIBs), and examine their correlations with atomic hydrogen,
molecular hydrogen, and EB-V . The DIBs are centered at \lambda\lambda 5780.5,
6204.5, 6283.8, 6196.0, 6613.6, 5705.1, 5797.1, and 5487.7, in decreasing order
of Pearson\^as correlation coefficient with N(H) (here defined as the column
density of neutral hydrogen), ranging from 0.96 to 0.82. We find the equivalent
width of \lambda 5780.5 is better correlated with column densities of H than
with E(B-V) or H2, confirming earlier results based on smaller datasets. We
show the same is true for six of the seven other DIBs presented here. Despite
this similarity, the eight strong DIBs chosen are not well enough correlated
with each other to suggest they come from the same carrier. We further conclude
that these eight DIBs are more likely to be associated with H than with H2, and
hence are not preferentially located in the densest, most UV shielded parts of
interstellar clouds. We suggest they arise from different molecules found in
diffuse H regions with very little H (molecular fraction f<0.01). Of the 133
stars with available data in our study, there are three with significantly
weaker \lambda 5780.5 than our mean H-5780.5 relationship, all of which are in
regions of high radiation fields, as previously noted by Herbig. The
correlations will be useful in deriving interstellar parameters when direct
methods are not available. For instance, with care, the value of N(H) can be
derived from W{\lambda}(5780.5).Comment: Accepted for publication in The Astrophysical Journal; 37 pages, 11
figures, 6 table
The Rotational Excitation Temperature of the 6614 Diffuse Interstellar Band Carrier
Analysis of high spectral resolution observations of the 6614
diffuse interstellar band (DIB) line profile show systematic variations in the
positions of the peaks in the substructure of the profile. These variations --
shown here for the first time -- can be understood most naturally in the
framework of rotational contours of large molecules, where the variations are
caused by changes in the rotational excitation temperature. We show that the
rotational excitation temperature for the DIB carrier is likely significantly
lower than the gas kinetic temperature -- indicating that for this particular
DIB carrier angular momentum buildup is not very efficient.Comment: Accepted by ApJ Letters; 16 pages, 2 figure
A coincidence between a hydrocarbon plasma absorption spectrum and the lambda 5450 DIB
The aim of this work is to link the broad lambda 5450 diffuse interstellar
band (DIB) to a laboratory spectrum recorded through an expanding acetylene
plasma. Cavity ring-down direct absorption spectra and astronomical
observations of HD 183143 with the HERMES spectrograph on the Mercator
Telescope in La Palma and the McKellar spectrograph on the DAO 1.2 m Telescope
are compared. In the 543-547 nm region a broad band is measured with a band
maximum at 545 nm and FWHM of 1.03(0.1) nm coinciding with a well-known diffuse
interstellar band at lambda 5450 with FWHM of 0.953 nm. A coincidence is found
between the laboratory and the two independent observational studies obtained
at higher spectral resolution. This result is important, as a match between a
laboratory spectrum and a - potentially lifetime broadened - DIB is found. A
series of additional experiments has been performed in order to unambiguously
identify the laboratory carrier of this band. This has not been possible. The
laboratory results, however, restrict the carrier to a molecular transient,
consisting of carbon and hydrogen.Comment: 6 pages, 3 figures, accepted for publication in A&
VUV-absorption cross section of carbon dioxide from 150 to 800 K and applications to warm exoplanetary atmospheres
The Diffuse Interstellar Bands: A Major Problem in Astronomical Spectroscopy
A critical review of the very long-standing problem of the diffuse
interstellar bands is presented with emphasis on spectroscopic aspects of
observational, modelling and laboratory-based research. Some research themes
and ideas that could be explored theoretically and experimentally are
discussed. The article is based on the Journal of Molecular Spectroscopy Review
Lecture presented at the 60th Ohio State University International Symposium on
Molecular Spectroscopy, June 2005
ChemInform Abstract: HIGH-RESOLUTION GAS PHASE EMISSION AND LASER-INDUCED FLUORESCENCE EXCITATION SPECTRA OF 1,3,5-TRIFLUOROBENZENE(1+) ION (1,3,5-C6F3H3+) AND 1,3,5-TRIFLUOROTRIDEUTEROBENZENE(1+) ION (1,3,5-C6F3D3+): CRITICAL BANDS IN THE JAHN-TELLER EFF
ChemInform Abstract: Rotational Contour Analysis of Selected Absorption Bands of Benzyl Produced by Flash Photolysis
Rotational contour analysis of selected absorption bands of benzyl produced by flash photolysis
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