[PDF][PDF] Direct measurement of the fine-structure interval and g_J factors of singly ionized atomic carbon by laser magnetic resonance

AL Cooksy, GA Blake…�- Astrophysical Journal�…, 1986 - authors.library.caltech.edu
Astrophysical Journal Letters, 1986authors.library.caltech.edu
We present the results of laser magnetic resonance measurements performed on the
ground^ 2P state of singly ionized atomic carbon (C_II). The 2^ P_ (3/2)←^ 2P_ (1/2) fine-
structure intervals of both^(12) C^+ and^(13) C^+ have been determined with a precision of
approximately 1 ppm, and the g_J factors to approximately one part in 10^ 4. Specifically, we
find that g_ (J=(1/2))= 0.66576 (11) and g_ (J=(3/2))= 1.33412 (11), while for^(12) C^+ ΔE_0
(^ 2P_ (3/2)←^ 2P_ (1/2))= 1900536.9 (1.3) MHz, with ΔE_0 (^ 2P_ (3/2)←^ 2P_ (1/2))�…
We present the results of laser magnetic resonance measurements performed on the ground ^2P state of singly ionized atomic carbon (C_II). The 2^P_(3/2) ← ^2P_(1/2) fine-structure intervals of both ^(12)C^+ and ^(13)C^+ have been determined with a precision of approximately 1 ppm, and the g_J factors to approximately one part in 10^4. Specifically, we find that g_(J=(1/2)) = 0.66576(11) and g_(J=(3/2)) = 1.33412(11), while for ^(12)C^+ ΔE_0(^2P_(3/2) ← ^2P_(1/2))= 1900536.9(1.3) MHz, with ΔE_0(^2P_(3/2) ← ^2P_(1/2)) = 1900545.8(2.1) and ΔE(^2P(3/2) ← ^2P_(1/2), F = 2 ← 1) = 1900466.1(2.3) MHz in ^(13)C^+. The highly precise values of the ^(12)C_II and ^(13)C_II fine-structure intervals verify the already secure far-infrared astronomical identification of C^+ and should allow the interstellar (^(12)C / ^(13)C) ratio to be unambiguously determined in a number of environments.
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