Mattauch-Herzog Type Mass Spectrograph with Two-Stage Electrostatic Field

ISAO TAKESHITA

doi:10.5702/massspec1953.14.59

ISAO TAKESHITA

著者情報

ジャーナルフリー

1966 年 14 巻 2 号 p. 59-71

DOI https://doi.org/10.5702/massspec1953.14.59

詳細

Published: 1966/06/01 Received: 1966/04/15 Available on J-STAGE: 2010/06/28 Accepted: - Advance online publication: - Revised: -
訂正情報
訂正日: 2010/06/28 訂正理由: - 訂正箇所: 論文抄録訂正内容: Wrong : An earlier work on a Mattauch-Herzog type mass spectrograph with two-stage electrostatic field is extended to investigating the conditions of simultaneous elimination ofαβ aberration for all masses. The design parameters are numerically calculated. The other coefficients of the second-order aberrations are examined and the total image defects are calculated for typical examples. An instrument according to the present study has sufficiently small and approximately constant image defects and has a high potential for use in the chemical analysis of solid.
Right : An earlier work on a Mattauch-Herzog type mass spectrograph with two-stage electrostatic field is extended to investigating the conditions of simultaneous elimination of αβ aberration for all masses. The design parameters are numerically calculated. The other coefficients of the second-order aberrations are examined and the total image defects are calculated for typical examples. An instrument according to the present study has sufficiently small and approximately constant image defects and has a high potential for use in the chemical analysis of solid.

訂正日: 2010/06/28 訂正理由: - 訂正箇所: 引用文献情報訂正内容: Wrong : E
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Right : Takeshita, Z. Naturforschg. 20a,624(1965).
I. Takeshita, Z. Naturforschg. 21a,14(1966).
S. Penner, Rev. Sci. Instr. 32,150(1961).
I. Takeshita, National Tech. Rep.(Japan)9,99(1963).
I. Takeshita, Z. Naturforschg. 21a,9(1966).
K. L. Brown, Reu. Sci. Instr. 35,481(1964).
I. Takeshita, Mass Spectroscopy(Japan)11,25(1963).

訂正日: 2010/06/28 訂正理由: - 訂正箇所: PDFファイル訂正内容: -

抄録

An earlier work on a Mattauch-Herzog type mass spectrograph with two-stage electrostatic field is extended to investigating the conditions of simultaneous elimination of αβ aberration for all masses. The design parameters are numerically calculated. The other coefficients of the second-order aberrations are examined and the total image defects are calculated for typical examples. An instrument according to the present study has sufficiently small and approximately constant image defects and has a high potential for use in the chemical analysis of solid.

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