Magnetic susceptibility of the BH molecule as a function of its vibrational state

1983 ◽  
Vol 19 (2) ◽  
pp. 115-119
Author(s):  
P. A. Braun ◽  
T. K. Rebane ◽  
O. I. Semakova
Keyword(s):  
Magnetic Susceptibility ◽  
Vibrational State

gJ-Faktor der Molekeln SiO und PbTe und Anisotropie der Magnetisierbarkeit von SiO / Molecular gJ-Factor of SiO and PbTe and Magnetic Susceptibility Anisotropy of SiO

1974 ◽  
Vol 29 (11) ◽  
pp. 1695-1696 ◽  
Author(s):  
R. Honerjäger ◽  
R. Tischer
Keyword(s):  
Magnetic Susceptibility ◽  
Quadrupole Moment ◽  
Vibrational State ◽  
Rotational Constant ◽  
Magnetic Susceptibility Anisotropy ◽  
Ground Vibrational State ◽  
Electronic Part

The gJ-factor of the molecules 28Si16O and 208Pb130Te and the magnetic susceptibility anisotropy ξTof 28Si16O have been measured in the ground vibrational state:The molecular quadrupole moment and its electronic part are derived for the SiO molecule from gJ, ξT , and the rotational constant B0 .

Magnetische Konstanten der Molekeln CuF und GaF / Magnetic Constants of the CuF and GaF Molecule

1974 ◽  
Vol 29 (12) ◽  
pp. 1919-1921
Author(s):  
R. Honerjäger ◽  
R. Tischer
Keyword(s):  
Magnetic Susceptibility ◽  
Vibrational State ◽  
Zeeman Effect ◽  
Rotational Constant ◽  
Magnetic Shielding ◽  
Rotational Spectrum ◽  
Magnetic Susceptibility Anisotropy ◽  
Ground Vibrational State ◽  
Microwave Rotational Spectrum

The Zeeman effect in the microwave rotational spectrum of 63Cu19F and 69Ga19F has been measured in the ground vibrational state υ = 0 in order to determine the (gJ-factor and the molecular magnetic susceptibility anisotropy ξT : 63Cu19F: gJ = -0.0628(2) ; ξT/h = 540(60) Hz/(kG)2 ; 69Ga19F: gJ = -0,06012(12) ; ξT/h = 521 (17) Hz/(kG)2. The molecular quadrupole moment and its electronic part are derived from the values of gJ,ξT and the rotational constant B0 . - The hyperfine structure of the Zeeman lines enabled a more or less rough determination of the magnetic shielding anisotropy of the nuclei 63Cu and 69Ga respectively:σT(63Cu) = -1760(830) · 10-6 , σT (69Ga) = - 386(165)·10-6.

gJ-Faktor der Molekeln SnO und PbO und Anisotropie ihrer magnetischen Suszeptibilität / Molecular gJ-Factor and Magnetic Susceptibility Anisotropy of SnO and PbO

1973 ◽  
Vol 28 (8) ◽  
pp. 1372-1373
Author(s):  
R. Honerjäger ◽  
R. Tischer
Keyword(s):  
Magnetic Susceptibility ◽  
Charge Distribution ◽  
Quadrupole Moment ◽  
Vibrational State ◽  
Rotational Constant ◽  
Electronic Charge ◽  
Magnetic Susceptibility Anisotropy ◽  
Electronic Charge Distribution ◽  
The Asymmetry

The gJ-factor and the magnetic susceptibility anisotropy ξT have been measured for 120Sn18O and 208Pb16O in the vibrational state υ=0:120Sn16O gJ= -0,14631 (38), ξT/h = 1844(18) Hz/kG2,208Pb16O gJ= -0,16233 (39), ξT/h = 2598(18) Hz/kG2.The molecular quadrupole moment Θ and the asymmetry of the electronic charge distribution 〈Σ(zi2-xi2)〉 are derived from the values of gJ, ξt , and the rotational constant B0.

scholarly journals gJ-Faktor der Molekeln GeO und SiS und Anisotropie ihrer Magnetisierbarkeit / Molecular gJ-Factor and Magnetic Susceptibility Anisotropy of GeO and SiS

1973 ◽  
Vol 28 (8) ◽  
pp. 1374-1375 ◽  
Author(s):  
R. Honerjäger ◽  
R. Tischer
Keyword(s):  
Magnetic Susceptibility ◽  
Quadrupole Moment ◽  
Vibrational State ◽  
Vibrational States ◽  
Magnetic Susceptibility Anisotropy

The gJ-factor and the molecular magnetic susceptibility anisotropy ξT have been measured for 74Ge16O and 28Si32S in the vibrational states υ=0, 1, 2 and υ= 0, 1, 2, 3 respectively:Having measured gJ and ξT as functions of υ we were able to derive the molecular and electronic quadrupole moment equally as functions of the vibrational state according to the method of Newell and Ramsey.

MAGNETIC SUSCEPTIBILITY AND ANOMALOUS BEHAVIOUR OF KNIGHT SHIFT IN SmPt2 AND SmSn3

1971 ◽  
Vol 32 (C1) ◽  
pp. C1-1028-C1-1030 ◽  
Author(s):  
S. K. MALIK ◽  
R. VIJAYARAGHAVAN
Keyword(s):  
Magnetic Susceptibility ◽  
Knight Shift ◽  
Anomalous Behaviour

MAGNETIC SUSCEPTIBILITY AND ANISOTROPY OF THE ORGANIC SUPERCONDUCTOR (TMTSF)2ClO4

1983 ◽  
Vol 44 (C3) ◽  
pp. C3-893-C3-901 ◽  
Author(s):  
M. Miljak ◽  
J. R. Cooper ◽  
K. Bechgaard
Keyword(s):  
Magnetic Susceptibility ◽  
Organic Superconductor

Magnetic susceptibility of dilute alloys of rare earths in magnesium

1979 ◽  
Vol 40 (C5) ◽  
pp. C5-17-C5-18
Author(s):  
M. de Jong ◽  
P. Touborg ◽  
J. Bijvoet
Keyword(s):  
Magnetic Susceptibility ◽  
Rare Earths ◽  
Dilute Alloys
Sign in / Sign up

Export Citation Format

Share Document