High Precision Wavelength Measurements of QED-Sensitive Forbidden Transitions 
in Highly Charged Argon Ions

Draganic, I.; Crespo López-Urrutia, J.R.; DuBois, R.; Fritzsche, S.; Shabaev, V.M.; Soria Orts, R.; Tupitsyn, I.I.; Zou, Y.; Ullrich, J.

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High Precision Wavelength Measurements of QED-Sensitive Forbidden Transitions in Highly Charged Argon Ions

MPG-Autoren

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Draganic, I.
Division Prof. Dr. Joachim H. Ullrich, MPI for Nuclear Physics, Max Planck Society;

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Crespo López-Urrutia, J.R.
Division Prof. Dr. Joachim H. Ullrich, MPI for Nuclear Physics, Max Planck Society;

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DuBois, R.
Division Prof. Dr. Werner Hofmann, MPI for Nuclear Physics, Max Planck Society;

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Fritzsche, S.
Division Prof. Dr. Joachim H. Ullrich, MPI for Nuclear Physics, Max Planck Society;

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Soria Orts, R.
Division Prof. Dr. Joachim H. Ullrich, MPI for Nuclear Physics, Max Planck Society;

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Tupitsyn, I.I.
Division Prof. Dr. Joachim H. Ullrich, MPI for Nuclear Physics, Max Planck Society;

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Ullrich, J.
Division Prof. Dr. Joachim H. Ullrich, MPI for Nuclear Physics, Max Planck Society;

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Zitation

Draganic, I., Crespo López-Urrutia, J., DuBois, R., Fritzsche, S., Shabaev, V., Soria Orts, R., et al. (2003). High Precision Wavelength Measurements of QED-Sensitive Forbidden Transitions in Highly Charged Argon Ions. Physical Review Letters, 91(18): 183001, pp. 1-4.

Zitierlink: https://hdl.handle.net/11858/00-001M-0000-0011-8DDC-8

Zusammenfassung

We present the results of an experimental study of magnetic dipole (M1) transitions in highly charged argon ions (Ar X, Ar XI, Ar XIV, Ar XV) in the visible spectral range using an electron beam ion trap. Their wavelengths were determined with, for highly charged ions, unprecedented accuracy up to the sub-ppm level and compared with theoretical calculations. The QED contributions, calculated in this Letter, are found to be 4 orders of magnitude larger than the experimental error and are absolutely indispensable to bring theory and experiment to a good agreement. This method shows great potential for the study of QED effects in relativistic few-electron systems