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EGAS41 - Swansea University

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41 st EGAS CP 208 Gdańsk 2009<br />

Reanalysis of the A 1 Π–X 1 Σ + bands system of the 13 CD + ion<br />

radical<br />

R. Hakalla ∗ ,, M. Zachwieja, W. Szajna ∗ , R. Kȩpa<br />

Atomic and Molecular Physics Laboratory, Institute of Physics <strong>University</strong> of Rzeszów,<br />

35-959 Rzeszów, Poland<br />

∗ Corresponding author: hakalla@univ.rzeszow.pl<br />

In the 13 CD + isotopic ion radical spectra of the A 1 Π–X 1 Σ + bands system have been<br />

obtained. Emission spectra of the bands were observed in the 22800–25100 cm −1 spectral<br />

region using a conventional spectroscopic technique. The 13 CD + molecules were produced<br />

by an electric discharge in an aluminum water-cooled hollow-cathode lamp, operated at<br />

400 V and 180÷200 mA DC. Nonflowing mixture of 3 Torr of He carried gas and 1 Torr of<br />

13 C 2 D 2 was found as optimal for production of strong A 1 Π–X 1 Σ + emission. The spectra<br />

were observed in the 6th order with the 2-m Ebert plane grating PGS-2 spectrograph<br />

equipped with 651-grooves/mm grating with a total number of grooves of 45 600, blazed<br />

at 1.0 µm. The reciprocal dispersion was in the range 0.066–0.075 nm/mm and theoretical<br />

resolving power was about 270 000. The spectrum of 13 CD + was recorded by translating<br />

on a linear stage an exit slit and photomultiplier tube (HAMAMATSU R943-02) along<br />

the focal curve of the spectrograph. The entrance and exit slit widths were 0.035 mm.<br />

The line intensities were measured by a single photon counting (HAMAMATSU C3866<br />

photon counting unit and M8784 photon counting board) with a counter gate time of 50-<br />

500 ms (no dead time between the gates) depending on spectrum intensity. Positions of<br />

the exit slit were measured using He-Ne laser interferometer synchronized with the photon<br />

counting board (during the counter gate time the position is measured 64 times and a<br />

mean value with the counts number are transmitted to PC as a measurement point). The<br />

total number of the measurement points was about 73 000 for one scan with the sample<br />

step of 3 µm (sample step it is the translation of the exit slit during the counter gate time).<br />

Simultaneously recorded some thorium atomic lines [1] obtained from several overlapped<br />

orders of the spectrum from a water-cooled hollow-cathode tube were used for absolute<br />

wavenumber calibration. For the wavenumber calculations seventh-order interpolation<br />

polynomials were used. The typical standard deviation of the least-squares fit for the<br />

70-80 calibration lines was about 0.0012–0.0016 cm −1 . The calibration procedure was<br />

tested (with two Th lamps simultaneously – one as an examination light source and the<br />

second one to provide the reference spectrum) to be ±0.0015 cm −1 . Comparison of the<br />

wavenumbers of the 0–0 band obtained in this study with those of [2] shows differences<br />

(about 0.015–0.020 cm −1 ) of both wavenumber values. Finally we improved molecular<br />

constants for both electronic states: A 1 Π as well as X 1 Σ + by means of the direct fit. Till<br />

nowadays only one experimental publication discussing 13 CD + ion molecule appeared [2].<br />

References<br />

[1] B.A. Palmer and R. Engleman Jr., Atlas of the Thorium Spectrum, (Los Alamos<br />

National Laboratory, Los Alamos NM 1983) - unpublished<br />

[2] Z. Bembenek, J. Mol. Spectrosc. 182, 439-443 (1997)<br />

268

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