Improved Measurement of the Hydrogen<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mn>1</mml:mn><mml:mi>S</mml:mi><mml:mo>–</mml:mo><mml:mn>2</mml:mn><mml:mi>S</mml:mi></mml:math>Transition Frequency

Parthey, Christian G.; Matveev, A.; Alnis, Jānis; Bernhardt, Birgitta; Beyer, Axel; Holzwarth, Ronald; Maistrou, Aliaksei; Pohl, Randolf; Predehl, Katharina; Udem, Thomas; Wilken, Tobias; Kolachevsky, Nikolai N.; Abgrall, M.; Rovera, Daniele; Salomon, Christophe; Laurent, Philippe; Hänsch, Theodor W.

doi:10.1103/physrevlett.107.203001

Cited by 387 publications

(285 citation statements)

References 20 publications

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“…In addition, the difference with the most accurately determined D 1S-2S experimental value (extracted from Refs. [13,25]; f D MPI ) is reduced to 0.82 ppb in comparison to 4.2 ppb in the ISIS measurement.…”

Section: S-2s Contributionsmentioning

confidence: 88%

Refined determination of the muonium-deuterium 1S-2Sisotope shift through improved frequency calibration of iodine lines

Fan

Chang²,

Wang

et al. 2014

Phys. Rev. A

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Use policyThe full-text may be used and/or reproduced, and given to third parties in any format or medium, without prior permission or charge, for personal research or study, educational, or not-for-pro t purposes provided that:• a full bibliographic reference is made to the original source • a link is made to the metadata record in DRO • the full-text is not changed in any way The full-text must not be sold in any format or medium without the formal permission of the copyright holders.Please consult the full DRO policy for further details. We report a refined determination of muonium 1S-2S transition frequency and its isotope shift with deuterium by recalibrating the iodine reference lines using an optical frequency comb. The reference lines for the muonium and deuterium 1S-2S transitions are determined with a precision of 2.4 × 10 −10 and 1.7 × 10 −10 , respectively. An updated muonium-deuterium 1S-2S isotope-shift frequency is derived from these references to be 11 203 464.9(9.2)(4.0) MHz, in agreement with an updated bound-state quantum-electrodynamics prediction based on 2010 adjustments of Committee on Data for Science and Technology and 2.3 times better in the systematic uncertainty than V. Meyer et al.

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Section: S-2s Contributionsmentioning

confidence: 88%

Refined determination of the muonium-deuterium 1S-2Sisotope shift through improved frequency calibration of iodine lines

Fan

Chang²,

Wang

et al. 2014

Phys. Rev. A

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“…The most recent result was reported by the Hänsch group in 2011, in which they determined the transition to a fractional frequency uncertainty of 4.2 × 10 −15 [10]. By that time, the UV laser source had evolved to an all solid state system that produced 13 mW of 243 nm cw radiation.…”

Section: Introductionmentioning

confidence: 84%

Yb Fiber Amplifier at 972.5 nm with Frequency Quadrupling to 243.1 nm

Burkley¹,

Rasor²,

Cooper³

et al. 2018

Exploring the World With the Laser

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“…Very precise experiments correspond to the measurements of the spectroscopic properties of this atom. In particular, the frequency measurements of the two-photon transitions 2s-1s [1][2][3] and 3s-1s or 3d-1s [4,5] in hydrogen have established the highest order of accuracy for the spectroscopic experiments. On the other hand, the recent success in the production of antihydrogen atoms offers the possibility for a detailed comparison of spectroscopic properties of the H andH atoms.…”

Section: Introductionmentioning

confidence: 99%

Rydberg-state mixing in the presence of an external electric field: Comparison of the hydrogen and antihydrogen spectra

Solovyeva

2015

Phys. Rev. A

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We analyze the influence of an external electric field on the ns and np Rydberg states. The impact of an electric field leads to a significant modification of the decay rate. Namely, the additional (linear and quadratic in the field) terms arise in the differential transition probabilities. In contrast to the quadratic term, the linear summand leads to a difference of the hydrogen (H) and antihydrogen (H) spectra. However, this difference vanishes after the integration over photon-emission directions and does not contribute to the total emission probability. The quadratic term results in the significant change of the total decay rate and level width, respectively. The analysis of the linear and quadratic terms depending on the field strength is discussed.

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Improved Measurement of the Hydrogen1S–2STransition Frequency

Cited by 387 publications

References 20 publications

Refined determination of the muonium-deuterium 1S-2Sisotope shift through improved frequency calibration of iodine lines

Refined determination of the muonium-deuterium 1S-2Sisotope shift through improved frequency calibration of iodine lines

Yb Fiber Amplifier at 972.5 nm with Frequency Quadrupling to 243.1 nm

Rydberg-state mixing in the presence of an external electric field: Comparison of the hydrogen and antihydrogen spectra

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