1973Journal of the Physical Society of JapanRequires access

Stark Effect of F1(2) Line of Methane at 3.39 µm Observed by the Method of Inverted Lamb Dip

Kiyoji Uehara

Open publisher page 13 citations

Abstract

The small Stark effect of the F 1 (2) line of methane at 3.39 µm is studied. The observed Stark pattern does not reveal resolved Stark components at the maximum applied field intensity of 40 kV/cm. But it shows a broadening of particular asymmetry and it is in satisfactory agreement with the theoretical pattern of the second-order Stark shift as given by Δ ν=5.31×10 -2 M 2 E 2 kHz where M is the quantum number for the component of angular momentum along the Stark field and E is the magnitude of Stark field in kV/cm. Thus the Stark shift of this line in a weak field is extremely small so that a high accuracy as a frequency standard can be guaranteed.

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What this paper is about

The small Stark effect of the F 1 (2) line of methane at 3.39 µm is studied. The observed Stark pattern does not reveal resolved Stark components at the maximum applied field intensity of 40 kV/cm. But it shows a broadening of particular asymmetry and it is in satisfactory agreement with the theoretical pattern of the second-order Stark shift as given by Δ ν=5.31×10 -2 M 2 E 2 kHz where M is the quantum number for the component of angular momentum along the Stark field and E is the magnitude of Stark field in kV/cm. Thus the Stark shift of this line in a weak field is extremely small so that a high accuracy as a frequency standard can be guaranteed.

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Available abstract

The small Stark effect of the F 1 (2) line of methane at 3.39 µm is studied. The observed Stark pattern does not reveal resolved Stark components at the maximum applied field intensity of 40 kV/cm. But it shows a broadening of particular asymmetry and it is in satisfactory agreement with the theoretical pattern of the second-order Stark shift as given by Δ ν=5.31×10 -2 M 2 E 2 kHz where M is the quantum number for the component of angular momentum along the Stark field and E is the magnitude of Stark field in kV/cm. Thus the Stark shift of this line in a weak field is extremely small so that a high accuracy as a frequency standard can be guaranteed.

Key concepts: Stark effect, Physics, Atomic physics, Asymmetry, Quantum-confined Stark effect, Line (geometry), Field (mathematics), Electric field

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