Abstract
The presented program is designed to simulate the characteristics of resonant coherent excitation of hydrogen-like ions planar-channeled in a crystal. The program realizes the numerical algorithm to solve the Schrödinger equation for the ion-bound electron at a special resonance excitation condition. The calculated wave function of the bound electron defines probabilities for the ion to be in the either ground or first excited state, or to be ionized. Finally, in the outgoing beam the fractions of ions in the ground state, in the first excited state, and ionized by collisions with target electrons, are defined. The program code is written on C++ and is designed for multiprocessing systems (clusters). The output data are presented in the table.
| Original language | English |
|---|---|
| Pages (from-to) | 705-710 |
| Number of pages | 6 |
| Journal | Computer Physics Communications |
| Volume | 183 |
| Issue number | 3 |
| DOIs | |
| Publication status | Published - Mar 2012 |
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Keywords
- Channeling
- Fine structure
- Hydrogen-like ions
- Resonant coherent excitation
- Schrödinger equation
- Stark effect
ASJC Scopus subject areas
- Hardware and Architecture
- Physics and Astronomy(all)
Cite this
Resonant coherent excitation of hydrogen-like ions planar channeled in a crystal; Transition into the first excited state. / Babaev, Anton Anatolievich; Pivovarov, Yu L.
In: Computer Physics Communications, Vol. 183, No. 3, 03.2012, p. 705-710.Research output: Contribution to journal › Article
}
TY - JOUR
T1 - Resonant coherent excitation of hydrogen-like ions planar channeled in a crystal; Transition into the first excited state
AU - Babaev, Anton Anatolievich
AU - Pivovarov, Yu L.
PY - 2012/3
Y1 - 2012/3
N2 - The presented program is designed to simulate the characteristics of resonant coherent excitation of hydrogen-like ions planar-channeled in a crystal. The program realizes the numerical algorithm to solve the Schrödinger equation for the ion-bound electron at a special resonance excitation condition. The calculated wave function of the bound electron defines probabilities for the ion to be in the either ground or first excited state, or to be ionized. Finally, in the outgoing beam the fractions of ions in the ground state, in the first excited state, and ionized by collisions with target electrons, are defined. The program code is written on C++ and is designed for multiprocessing systems (clusters). The output data are presented in the table.
AB - The presented program is designed to simulate the characteristics of resonant coherent excitation of hydrogen-like ions planar-channeled in a crystal. The program realizes the numerical algorithm to solve the Schrödinger equation for the ion-bound electron at a special resonance excitation condition. The calculated wave function of the bound electron defines probabilities for the ion to be in the either ground or first excited state, or to be ionized. Finally, in the outgoing beam the fractions of ions in the ground state, in the first excited state, and ionized by collisions with target electrons, are defined. The program code is written on C++ and is designed for multiprocessing systems (clusters). The output data are presented in the table.
KW - Channeling
KW - Fine structure
KW - Hydrogen-like ions
KW - Resonant coherent excitation
KW - Schrödinger equation
KW - Stark effect
UR - http://www.scopus.com/inward/record.url?scp=84855449016&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=84855449016&partnerID=8YFLogxK
U2 - 10.1016/j.cpc.2011.11.009
DO - 10.1016/j.cpc.2011.11.009
M3 - Article
VL - 183
SP - 705
EP - 710
JO - Computer Physics Communications
JF - Computer Physics Communications
SN - 0010-4655
IS - 3
ER -