Measurement of the Hydrogen Spin-Exchange Cross Section with the Hydrogen Maser

1968 ◽  
Vol 166 (1) ◽  
pp. 4-6 ◽  
Author(s):  
H. Hellwig
1973 ◽  
Vol 51 (18) ◽  
pp. 1901-1909 ◽  
Author(s):  
J. Vanier ◽  
R. Brousseau ◽  
R. Larouche

Experiments are described in which the phenomenon of stimulated emission with a delayed maximum of power is observed in a hydrogen maser and is studied in some detail. The results are coupled to measurements of relaxation rates made through a pulse technique in which the hydrogen beam is modulated. A solution of the rate equations describing the phenomenon for a two-level model is obtained on an analog computer and is compared with the experimental data. From the comparison, we conclude that the phenomenon is explained by the assumed theoretical model. It is found also that the published values of the spin-exchange cross section of hydrogen are consistent with our experimental data.


1968 ◽  
Vol 4 (5) ◽  
pp. 327-327
Author(s):  
C. Audoin ◽  
M. Desaintfuscien ◽  
J. Schermann

2000 ◽  
Vol 8 (3) ◽  
pp. 305-308 ◽  
Author(s):  
Y. Arimoto ◽  
N. Shimakura ◽  
K. Yonehara ◽  
T. Yamagata ◽  
M. Tanaka

1975 ◽  
Vol 8 (16) ◽  
pp. 2615-2619 ◽  
Author(s):  
A F Oluwole ◽  
H B Olaniyi ◽  
S G Schmelling ◽  
J B Aladekomo

2001 ◽  
Vol 64 (6) ◽  
Author(s):  
Y. Arimoto ◽  
N. Shimakura ◽  
T. Yamagata ◽  
K. Yonehara ◽  
M. Tanaka

1979 ◽  
Vol 57 (6) ◽  
pp. 904-916 ◽  
Author(s):  
J.-Y. Savard ◽  
G. Busca ◽  
S. Rovea ◽  
M. Desaintfuscien ◽  
P. Petit

The effects of transitions excited within the F = 1 multiplet of the ground state hydrogen atoms while radiating on the ΔmF = 0 transition are analyzed theoretically. The results are valid for low transition rates and unrestricted maser power. The predictions are: (a) an important modification of the well-known spin-exchange frequency shift of a hydrogen maser, due to the imaginary part of the spin-exchange cross section, (b) a frequency shift proportional to the asymmetry parameter between the 2-Zeeman frequencies in the upper multiplet F = 1, and (c) a frequency shift proportional to the polarization of the atoms in the storage bulb.Also shown is a displacement of the zero crossing of the maser detuning vs. the low frequency coherent transition frequency with respect to the dip of the maser absorption. This effect is visible for a maser tuned by spin-exchange and operated at a relatively high magnetic field and nonuniform Zeeman populations.An experimental verification of the theory is presented. A new method for tuning the hydrogen maser is suggested, and a proposal is made to measure the collisional frequency shift proportional to the average duration of hydrogen atom spin-exchange collisions.


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