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Effect of screening on the phonon-polaron states in diluted magnetic semiconductor nanotubes
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10.1063/1.4811335
/content/aip/journal/ltp/39/6/10.1063/1.4811335
http://aip.metastore.ingenta.com/content/aip/journal/ltp/39/6/10.1063/1.4811335
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

The polaron binding energy (a) and the polaron correction to the electron mass (b) as functions of magnetic field: without exchange interactions or screening (1); including exchange interactions without screening (2); including screening without exchange interactions (3); including both screening and exchange interactions (4). Transitions from the ground state = 0 to the subbands are taken into account and .

Image of FIG. 2.
FIG. 2.

The polaron binding energy (a) and the polaron contribution to the electron mass (b) as functions of nanotube radius: without exchange interactions or screening (1); including screening without exchange interactions (2); including exchange interactions without screening (3); including both screening and exchange interactions (4). Transitions from the ground state = 0 to the subbands are taken into account and = 0.1 T.

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/content/aip/journal/ltp/39/6/10.1063/1.4811335
2013-06-27
2014-04-18
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Effect of screening on the phonon-polaron states in diluted magnetic semiconductor nanotubes
http://aip.metastore.ingenta.com/content/aip/journal/ltp/39/6/10.1063/1.4811335
10.1063/1.4811335
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