Resolved hyperfine structure in the C–X electronic transition of VO. An internal hyperfine perturbation in the C4Σ− state

1981 ◽  
Vol 59 (2) ◽  
pp. 266-270 ◽  
Author(s):  
W. H. Hocking ◽  
A. J. Merer ◽  
D. J. Milton

New grating and laser excitation spectra of VO show resolved nuclear hyperfine structure in the lines of the F1 and F4 electron spin components in the C4Σ−–X4Σ−electronic transition. It is shown that the C4Σ− state has a sizeable hyperfine structure, with the Fermi contact parameter bF (the coefficient of I∙S in the magnetic hyperfine Hamiltonian) equal to −0.00773 cm−1. Another internal hyperfine perturbation, of the type described by Richards and Barrow for the ground state, occurs in the C4Σ−state near N = 5; the line doublings are consistent with the Fermi contact parameter derived from the F1 and F4 lines.

1980 ◽  
Vol 58 (5) ◽  
pp. 642-656 ◽  
Author(s):  
R. M. Gordon ◽  
A. J. Merer

The (0,0), (0,1), and (1,0) bands of the A6Σ+–X6Σ+ transition of MnO near 5500 Å have been photographed at high dispersion, and partial rotational analyses carried out. The spectrum is unusually complicated because of the high electron multiplicity, the manganese hyperfine structure, and extensive rotational perturbations. It is found that hyperfine perturbations frequently accompany the rotational perturbations. These are a new type of perturbation, resulting from a mixing of the F3 and F4 electron spin components in the upper state through hyperfine matrix elements of the type ΔN = 0, ΔJ ± 1, ΔF = 0 as a result of rotational perturbations. Extra lines, obeying the selection rules ΔJ = 0, ± 2, are induced: these give the energy separations of the F3 and F4 electron spin components of the ground state. As a result it has been possible to determine the electron spin fine structure parameters for the two states despite the parallel polarization of the electronic transition. The reason for the great complexity of the A6Σ+ ν = 0 level is the occurrence of a large avoided crossing near N = 26 with a level which is possibly a highly excited vibrational level of the ground state. The ground state Mn—O bond length is r0 = 1.6477 Å, and ΔG1/2(X6Σ+) = 832.41 cm−1.


1988 ◽  
Vol 116 ◽  
Author(s):  
S. Zemon ◽  
C. Jagannath ◽  
S. K. Shastry ◽  
W. J. Miniscalco ◽  
G. Lambert

AbstractWe describe new results observed during resonant excitation in the excitonic region of GaAs grown directly on Si by organometallic vapor phase epitaxy. Two resolved features were found in the light hole photoluminescence (PL) region, one identified with a free exciton process and the other with donor-related transitions. Features which track the laser excitation line were observed and identified with a process in which a donor is excited from the n=l ground state to an n=2 excited state. The PL excitation spectra associated with these features have spectral widths as narrow as 1.5 meV. PL spectral widths of ~3 meV have been attained for the heavy hole exciton band, representing the narrowest value obtained for OMVPE material and an improvement of about 30% over our best previous results.


1968 ◽  
Vol 165 (4) ◽  
pp. 1360-1362 ◽  
Author(s):  
Alan T. Ramsey ◽  
Sanford Stein

1975 ◽  
Vol 54 (4) ◽  
pp. 293-294 ◽  
Author(s):  
P. Boolchand ◽  
M. Tenhover ◽  
S. Jha ◽  
G. Langouche ◽  
B.B. Triplett ◽  
...  

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