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Effect of strongly coupled plasma on the magnetic dipolar and quadrupolar transitions of two-electron ions
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10.1063/1.4801001
/content/aip/journal/pop/20/4/10.1063/1.4801001
http://aip.metastore.ingenta.com/content/aip/journal/pop/20/4/10.1063/1.4801001

Figures

Image of FIG. 1.
FIG. 1.

Variation of transition energies (a.u.) for M1 [A1:1s 2:1 S e →1s2s:3 S e; A2:1s 2:1 S e →1s3s:3 S e; A3:1s 2:1 S e →1s4s:3 S e] and M2 [B1:1s 2:1 S e →1s2p:3 P o; B2:1s 2:1 S e →1s3p:3 P o; B3:1s 2:1 S e →1s4p:3 P o] transitions of C 4+ with plasma density (/c.c.).

Image of FIG. 2.
FIG. 2.

Variation of transition energies (a.u.) for M1 [A1:1s 2:1 S e →1s2s:3 S e; A2:1s 2:1 S e →1s3s:3 S e; A3:1s 2:1 S e →1s4s:3 S e] and M2 [B1:1s 2:1 S e →1s2p:3 P o; B2:1s 2:1 S e →1s3p:3 P o; B3:1s 2:1 S e →1s4p:3 P o] transitions of Si 12+ with plasma density (/c.c.).

Image of FIG. 3.
FIG. 3.

Variation of transition energies (a.u.) for M1 [A1:1s 2:1 S e →1s2s:3 S e; A2:1s 2:1 S e →1s3s:3 S e; A3:1s 2:1 S e →1s4s:3 S e] and M2 [B1:1s 2:1 S e →1s2p:3 P o; B2:1s 2:1 S e →1s3p:3 P o; B3:1s 2:1 S e →1s4p:3 P o] transitions with Z for 1019/c.c. and 1.5 × 1023/c.c. plasma densities.

Image of FIG. 4.
FIG. 4.

Variation of transition probabilities (/sec) for M1 [A1:1s 2:1 S e →1s2s:3 S e; A2:1s 2:1 S e →1s3s:3 S e; A3:1s 2:1 S e →1s4s:3 S e] and M2 [B1:1s 2:1 S e →1s2p:3 P o; B2:1s 2:1 S e →1s3p:3 P o; B3:1s 2:1 S e →1s4p:3 P o] transitions of O 6+ with plasma density (/c.c.).

Image of FIG. 5.
FIG. 5.

Variation of transition probabilities (/sec) for M1 [A1:1s 2:1 S e →1s2s:3 S e; A2:1s 2:1 S e →1s3s:3 S e; A3:1s 2:1 S e →1s4s:3 S e] and M2 [B1:1s 2:1 S e →1s2p:3 P o; B2:1s 2:1 S e →1s3p:3 P o; B3:1s 2:1 S e →1s4p:3 P o] transitions of S 14+ with plasma density (/c.c.).

Image of FIG. 6.
FIG. 6.

Variation of transition probabilities (a.u.) for M1 [A1:1s 2:1 S e →1s2s:3 S e; A2:1s 2:1 S e →1s3s:3 S e; A3:1s 2:1 S e →1s4s:3 S e] and M2 [B1:1s 2:1 S e →1s2p:3 P o; B2:1s 2:1 S e →1s3p:3 P o; B3:1s 2:1 S e →1s4p:3 P o] transitions with Z for 1019/c.c. and 1.5   1023/c.c. plasma densities.

Image of FIG. 7.
FIG. 7.

Variation of thermodynamic pressure (P) (in atm) with plasma density (n/c.c.) for different two-electron ions.

Tables

Generic image for table
Table I.

Transition energies (a.u.) of M1 [A1:1s 2:1 S e →1s2s:3 S e; A2:1s 2:1 S e →1s3s:3 S e; A3:1s 2:1 S e →1s4s:3 S e] and M2 [B1:1s 2:1 S e →1s2p:3 P o; B2:1s 2:1 S e →1s3p:3 P o; B3:1s 2:1 S e →1s4p:3 P o] transitions of different ions for various plasma density (/c.c.).

Generic image for table
Table II.

Transition probabilities (/sec) of M1 [A1:1s 2:1 S e →1s2s:3 S e; A2:1s 2:1 S e →1s3s:3 S e; A3:1s 2:1 S e →1s4s:3 S e] and M2 [B1:1s 2:1 S e →1s2p:3 P o; B2:1s 2:1 S e →1s3p:3 P o; B3:1s 2:1 S e →1s4p:3 P o] transitions of different ions for various plasma density (/c.c.).

Generic image for table
Table III.

Fitting parameters A and b of the variation (P = Anb ) between thermodynamic pressure (P in atm.) and different plasma density (/c.c.) for all the ions.

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/content/aip/journal/pop/20/4/10.1063/1.4801001
2013-04-10
2014-04-21
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Effect of strongly coupled plasma on the magnetic dipolar and quadrupolar transitions of two-electron ions
http://aip.metastore.ingenta.com/content/aip/journal/pop/20/4/10.1063/1.4801001
10.1063/1.4801001
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