Remarks on the quantum mechanical interpretation of the stark effect in the hydrogen atom

1962 ◽  
Vol 1 (6) ◽  
pp. 191-192 ◽  
Author(s):  
L.B. Rédei
1976 ◽  
Vol 31 (6) ◽  
pp. 517-523 ◽  
Author(s):  
H. G. Becker ◽  
K. Bleuler

Using the advantages of the O (4)-symmetry the second order Stark-effect of the hydrogen atom is calculated by the Dalgarno-Lewis perturbation method in a purely algebraic manner. The Starkeffect provides the first quantum mechanical example in which the Dalgarno-Lewis equation relevant for second and third order perturbation theory of the whole spectrum can be exactly solved


1981 ◽  
Vol 14 (24) ◽  
pp. 4737-4742 ◽  
Author(s):  
M Friedman ◽  
A Rabinovitch ◽  
R Thieberger
Keyword(s):  

Leonardo ◽  
1991 ◽  
Vol 24 (5) ◽  
pp. 581
Author(s):  
Leo Narodny

1981 ◽  
Vol 35 (1) ◽  
pp. 754-757
Author(s):  
V. V. Goncharuk ◽  
A. G. Grebenyuk ◽  
L. I. Savranskii ◽  
V. F. Gorchev ◽  
A. N. Chernega

Author(s):  
Engel Roza

It is shown that the Lambda component in the cosmological Lambda-CDM model can be conceived as vacuum energy, consisting of gravitational particles subject to Heisenberg’s energy-time uncertainty. These particles can be modelled as elementary polarisable Dirac-type dipoles (“darks”) in a fluidal space at thermodynamic equilibrium, with spins that are subject to the Bekenstein-Hawking entropy. Around the baryonic kernels, uniformly distributed in the universe, the spins are polarized, thereby invoking an increase of the effective gravitational strength of the kernels. It explains the dark matter effect to the extent that the numerical value of Milgrom’s acceleration constant can be assessed by theory. Non-polarized vacuum particles beyond the baryonic kernels compose the dark energy. The result is a quantum mechanical interpretation of gravity in terms of quantitatively established shares in baryonic matter, dark matter and dark energy, which correspond with the values of the Lambda-CDM model..


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