Perturbation Theory

2019 ◽  
pp. 259-322
Author(s):  
P.J.E. Peebles

This chapter examines applications drawn from perturbation theory. The main topic in perturbation theory is the energy and spontaneous decay rate of the 21-cm hyperfine line in atomic hydrogen. Before there were electronic computers, people had quite an accurate theoretical understanding of the energy levels in helium and more complicated systems. The trick was (and is) to find approximation schemes that treat unimportant parts of a physical system in quite crude approximations while reducing the interesting parts to a problem simple enough that it is feasible to compute but yet detailed enough to yield accurate results. The approximation methods in the chapter deal with the effects of small changes in the Hamiltonian, resulting for example from the application of a static or time variable electric or magnetic field. This may cause small changes in energy levels, and it may induce transitions among eigenstates of the original Hamiltonian.

1988 ◽  
Vol 102 ◽  
pp. 343-347
Author(s):  
M. Klapisch

AbstractA formal expansion of the CRM in powers of a small parameter is presented. The terms of the expansion are products of matrices. Inverses are interpreted as effects of cascades.It will be shown that this allows for the separation of the different contributions to the populations, thus providing a natural classification scheme for processes involving atoms in plasmas. Sum rules can be formulated, allowing the population of the levels, in some simple cases, to be related in a transparent way to the quantum numbers.


2013 ◽  
Vol 114 (3) ◽  
pp. 359-367 ◽  
Author(s):  
A. D. Bykov ◽  
K. V. Kalinin ◽  
A. N. Duchko

2016 ◽  
Vol 714 ◽  
pp. 012009
Author(s):  
R Kh Gainutdinov ◽  
M A Khamadeev ◽  
O V Steryakov ◽  
K A Ziyatdinova ◽  
M Kh Salakhov

2019 ◽  
Vol 100 (3) ◽  
Author(s):  
Jacek Komasa ◽  
Mariusz Puchalski ◽  
Paweł Czachorowski ◽  
Grzegorz Łach ◽  
Krzysztof Pachucki

1991 ◽  
Vol 02 (01) ◽  
pp. 387-390
Author(s):  
ERNA KARULE

Multiphoton ionization happens in an intense light beam when atoms absorb more than one photon. In strong fields an atom may absorb not only the minimum energetically necessary number of photons for ionization, but also excess photons. The last process is the so called “above threshold ionization” (ATI) which as well as “normal” multiphoton ionization (MPI) takes place in the strong laser fields. Both processes are between those responsible for the energy transfer from the laser to the plasma. The paper deals with the quantum mechanical calculation of MPI and ATI of atomic hydrogen. At the moderate intensities of light these processes may be treated by methods of perturbation theory.


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