Isotope shift measurements and electronic configuration assignments to the energy levels in 555- 833 nm wavelength region of Dy I spectrum with FTS

Author(s):  
B.K. Ankush ◽  
S.A. Ahmad ◽  
M.N. Deo
1985 ◽  
Vol 40 (8) ◽  
pp. 1059-1066 ◽  
Author(s):  
Pushpa M. Rao ◽  
A. Venugopalan ◽  
S.A. Ahmad ◽  
G.D. Saksena

2013 ◽  
Vol 27 (26) ◽  
pp. 1350152 ◽  
Author(s):  
AKSHU PAHUJA ◽  
SUNITA SRIVASTAVA

The structural and electronic properties of endohedral fullerenes formed by encapsulation of each of the group V elements inside the buckminsterfullerene cage have been investigated. The calculations reveal that all these species are thermodynamically stable, though the formation of Sb@C 60 and Bi@C 60 is slightly endothermic. The central atom preserves its electronic configuration and the quartet state. The energy gap and energy levels are perturbed by the inclusion of a foreign atom. The band gap of Sb@C 60 and Bi@C 60 is found to be significantly smaller than pristine C 60, suggesting the reactivity of these complexes.


2021 ◽  
Vol 54 (17) ◽  
pp. 175001
Author(s):  
S T Orson ◽  
C D McLaughlin ◽  
M D Lindsay ◽  
R J Knize

1997 ◽  
Vol 42 (2) ◽  
pp. 71-76 ◽  
Author(s):  
S.G. Nakhate ◽  
S.M. Afzal ◽  
S.A. Ahmad
Keyword(s):  

1976 ◽  
Vol 54 (20) ◽  
pp. 2028-2049 ◽  
Author(s):  
H. Lew

Many bands of the [Formula: see text] electronic emission spectrum of H2O+, occurring in the wavelength region 4000–7500 Å, have been analyzed. These include bands that have been observed in the tails of comets. The wavelengths and wave numbers of all assigned lines are tabulated. Accurate rotational constants for the first three bending vibrational levels of the ground state are given, as well as energy levels in the upper and lower electronic states. The O—H bond distance and the H—O—H angle in the [Formula: see text] (0, 0, 0) level are found to be 0.9988 Å and 110.46° respectively. Some predicted microwave and infrared lines that may be of astrophysical interest are included.


The photochemical decomposition of the ionic thallous azide to metallic thallium and nitrogen has been studied as a function of wavelength, temperature and light intensity. Two values have been obtained for the activation energies; 0⋅33 eV corresponding to the full output of a mercury lamp, and 0⋅14 eV for light in the wavelength region 3200 to 3800 Å. The quantum efficiency at 3650 Å is 2×10 -3 . Two exciton bands at 3415 and 3348 Å have been observed in thallous azide by the method of low-temperature spectroscopy developed by Nikitine and Gross. Two narrow bands have been resolved in silver azide which is also an ionic azide, in the region previously studied by McLaren & Rogers. These bands occur at 3608 and 3590 Å. The refractive index of thallous azide has been measured by the Brewster angle method, and the electron energy levels have been estimated. The results of the photochemical decomposition of thallous azide have been related to the electron energy levels, and to measurements of photoconductivity made by Evans & Yoffe.


MRS Bulletin ◽  
1999 ◽  
Vol 24 (9) ◽  
pp. 21-26 ◽  
Author(s):  
R. Moncorgé ◽  
L.D. Merkle ◽  
B. Zandi

An issue on novel applications of materials doped with rare-earth (RE) ions can scarcely fail to address lasers, but it need not address all RE-based lasers. Some Nd3+ -doped lasers, particularly Nd:YAG (Y3Al5O12, yttrium aluminum garnet), emitting light with a wavelength of 1064 nm, are very well-established commercial products—by no means novelties.1 Some other near-infrared (NIR) lasers, based on Er3+ or Tm3+, are also available commercially. That wavelength region is relatively easy for RE laser ions, involving energy spacings between initial and final energy levels small enough to give large stimulated emission cross sections for useful, long upper-state life-times, yet large enough to minimize thermal deexcitation mechanisms. On the other hand, RE-doped lasers for ultraviolet (UV) and visible wavelengths are quite novel, since efficient laser operation is more difficult to achieve in these spectral ranges. Intriguing progress on such devices has been made in recent years, driven by several important applications.In this article, we begin by noting some of the alternative ways to obtain laser light at these wavelengths, including their advantages and drawbacks. We then discuss basic properties of RE-doped laser materials and how these can be advantageous. We then review a few of the most important and recent RE-doped laser materials and techniques for obtaining UV and visible output.


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