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Related papers: Precise measurement of positronium hyperfine split…

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Recent progress in the spectroscopy of antiprotonic helium has allowed for measuring the separation between components of the hyperfine structure (HFS) of the (37,35) metastable states with an accuracy of 300 MHz, equivalent to a relative…

Atomic Physics · Physics 2008-11-26 Dimitar Bakalov , Eberhard Widmann

Despite its very short lifetime positronium provides us with a number of accurate tests of the bound state QED. In this note a brief overview of QED theory and precision experiments on the spectrum and annihilation decay of the positronium…

High Energy Physics - Phenomenology · Physics 2009-11-07 Savely G. Karshenboim

While measurements of the hyperfine structure of hydrogen-like atoms are traditionally regarded as test of bound-state QED, we assume that theoretical QED predictions are accurate and discuss the information about the electromagnetic…

Quantum Physics · Physics 2009-11-10 Arnaud Dupays , Alberto Beswick , Bruno Lepetit , Carlo Rizzo , Dimitar Bakalov

In this letter, we recall the main facts concerning the g-factor of positronium and we show how the value of the g-factor of the positronium is important. Taking it better into consideration may provide a solution to the reported…

High Energy Physics - Phenomenology · Physics 2023-11-14 J. Agil , D. Bakalov , R. Battesti , C. Rizzo

For decades, improved theory and experiment of the $n=2$ $^3$P fine structure of helium have allowed for increasingly-precise tests of quantum electrodynamics, determinations of the fine-structure constant $\alpha$, and limitations on…

Atomic Physics · Physics 2018-10-10 K. Kato , T. D. G. Skinner , E. A. Hessels

The loop induced coupling of an intermediate mass Higgs boson to two photons is a sensitive and unique measure for precision tests of physics beyond the Standard Model. In this work we summarize recent results on the expected precision of…

High Energy Physics - Phenomenology · Physics 2009-10-31 Michael Melles

The differential and total cross sections for electron capture by positrons from helium atoms are calculated using a first-order distorted wave theory satisfying the Coulomb boundary conditions. In this formalism a parametric potential is…

Atomic Physics · Physics 2015-06-04 Ebrahim Ghanbari-Adivi

Increasing accuracy of the theory and experiment of the $n$$=$$2$ $^3$P fine structure of helium has allowed for increasingly-precise tests of quantum electrodynamics (QED), determinations of the fine-structure constant $\alpha$, and…

Atomic Physics · Physics 2023-10-27 F. Heydarizadmotlagh , T. D. G. Skinner , K. Kato , M. C. George , E. A. Hessels

By relating fine and hyperfine spittings for l=1 states in bottomium we can factor out the less tractable part of the perturbative and nonperturbative effects. Reliable predictions for one of the fine splittings and the hyperfine splitting…

High Energy Physics - Phenomenology · Physics 2016-09-01 S. Titard , F. J Yndurain

We report measurements of the branching fraction, hyperfine constant, and second-order Zeeman coefficient of the D$_{5/2}$ level in $^{171}$Yb$^+$ with up to two orders-of-magnitude improvement in precision compared to previously reported…

Atomic Physics · Physics 2021-08-04 T. R. Tan , C. L. Edmunds , A. R. Milne , M. J. Biercuk , C. Hempel

The measurement of the charge asymmetry $A_{FB}(e^-e^+\to \mu^-\mu^+)$ will play an important role at the high-luminosity circular electron-positron collider FCCee considered for construction at CERN. In particular, near the Z resonance,…

High Energy Physics - Phenomenology · Physics 2019-07-24 Stanislaw Jadach , Scott Yost

We perform precision microwave spectroscopy--aided by Stark deceleration--to reveal the low magnetic field behavior of OH in its ^2\Pi_{3/2} ro-vibronic ground state, identifying two field-insensitive hyperfine transitions suitable as…

Atomic Physics · Physics 2009-11-13 Benjamin L. Lev , Edmund R. Meyer , Eric R. Hudson , Brian C. Sawyer , John L. Bohn , Jun Ye

The latest experimental measurements of the hyperfine splitting $E_{\rm{hfs}}=M_{\Upsilon(1 S)}-M_{\eta_b(1 S)}$ done by the Belle collaboration and the perturbative and lattice QCD predictions show a tension with the current extraction…

High Energy Physics - Phenomenology · Physics 2015-11-17 Nikolai Zerf

Corrections of orders alpha^5 and alpha^6 are calculated in the hyperfine splittings of 1S and 2S - energy levels in the ion of muonic helium. The electron vacuum polarization effects, the nuclear structure corrections and recoil…

High Energy Physics - Phenomenology · Physics 2014-11-18 A. P. Martynenko

Hyperfine splitting of positronium is an important parameter for particle physics. This paper gives experimental techniques and results of R&D studies of our experiment to observe direct hyperfine transition of ortho-positronium to…

High Energy Physics - Experiment · Physics 2010-07-07 T. Suehara , A. Miyazaki , T. Yamazaki , G. Akimoto , A. Ishida , T. Namba , S. Asai , T. Kobayashi , H. Saito , M. Yoshida , T. Idehara , I. Ogawa , Y. Urushizaki , S. Sabchevski

The "recoil" correction of order $m \alpha^6$ to the hyperfine splitting of positronium ground state was found. The formalism employed is based on the noncovariant perturbation theory in QED. Equation for two-particle component of full…

High Energy Physics - Phenomenology · Physics 2009-10-31 A. P. Burichenko

We discuss the consequences of recent experimental results from CDF, SLC, LEP and elsewhere for the Standard Model and for new physics. A global fit to all indirect precision data yields $m_t = 175 \pm 11^{+17}_{-19}$~GeV,…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jens Erler , Paul Langacker

Muonic helium atom hyperfine structure (HFS) measurements are a sensitive tool to test the three-body atomic system and bound-state quantum electrodynamics theory, and determine fundamental constants of the negative muon magnetic moment and…

The hyperfine splitting for the 2S charmonium state is calculated and the predicted number is $\Delta_{\rm HF}(2S) = 57 \pm 8$ MeV, being by derivation the lower bound of this splitting. It results in $M(\eta_c(2S))= 3630 \pm 8$ MeV, which…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. M. Badalian , B. L. G. Bakker

We extend the formalism based on perturbative QCD that was developed in our previous work, and compute the hyperfine splittings of the bottomonium spectrum as well as the fine and hyperfine splittings of the charmonium spectrum. All the…

High Energy Physics - Phenomenology · Physics 2010-04-05 S. Recksiegel , Y. Sumino