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  1. J. H. Sanders, Phys. Rev. Letters 3, 86 (1959).
    [Crossref]
  2. A. Javan, Phys. Rev. Letters 3, 87 (1959).
    [Crossref]
  3. All transition probabilities used here are based on oscillator strengths from Trefftz, Schluter, Dettmar, and Jorgens, Z. Astrophys. 44, 1 (1957).

1959 (2)

J. H. Sanders, Phys. Rev. Letters 3, 86 (1959).
[Crossref]

A. Javan, Phys. Rev. Letters 3, 87 (1959).
[Crossref]

1957 (1)

All transition probabilities used here are based on oscillator strengths from Trefftz, Schluter, Dettmar, and Jorgens, Z. Astrophys. 44, 1 (1957).

Dettmar,

All transition probabilities used here are based on oscillator strengths from Trefftz, Schluter, Dettmar, and Jorgens, Z. Astrophys. 44, 1 (1957).

Javan, A.

A. Javan, Phys. Rev. Letters 3, 87 (1959).
[Crossref]

Jorgens,

All transition probabilities used here are based on oscillator strengths from Trefftz, Schluter, Dettmar, and Jorgens, Z. Astrophys. 44, 1 (1957).

Sanders, J. H.

J. H. Sanders, Phys. Rev. Letters 3, 86 (1959).
[Crossref]

Schluter,

All transition probabilities used here are based on oscillator strengths from Trefftz, Schluter, Dettmar, and Jorgens, Z. Astrophys. 44, 1 (1957).

Trefftz,

All transition probabilities used here are based on oscillator strengths from Trefftz, Schluter, Dettmar, and Jorgens, Z. Astrophys. 44, 1 (1957).

Phys. Rev. Letters (2)

J. H. Sanders, Phys. Rev. Letters 3, 86 (1959).
[Crossref]

A. Javan, Phys. Rev. Letters 3, 87 (1959).
[Crossref]

Z. Astrophys. (1)

All transition probabilities used here are based on oscillator strengths from Trefftz, Schluter, Dettmar, and Jorgens, Z. Astrophys. 44, 1 (1957).

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Tables (1)

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Table I Calculated ratio of populations of 3′D2 and 2′P1 states in helium at various currents and pressures.