Quantum electrodynamics of heavy ions and atoms: current status and prospects

2008 ◽  
Vol 178 (11) ◽  
pp. 1220 ◽  
Author(s):  
Vladimir M. Shabaev
JETP Letters ◽  
2017 ◽  
Vol 106 (12) ◽  
pp. 765-770 ◽  
Author(s):  
A. V. Malyshev ◽  
V. M. Shabaev ◽  
D. A. Glazov ◽  
I. I. Tupitsyn

2018 ◽  
Vol 179 ◽  
pp. 01014 ◽  
Author(s):  
P. Mastrolia ◽  
M. Passera ◽  
A. Primo ◽  
U. Schubert ◽  
W. J. Torres Bobadilla

We report on the current status of the analytic evaluation of the two-loop corrections to the μescattering in Quantum Electrodynamics, presenting state-of-the art techniques which have been developed to address this challenging task.


2006 ◽  
Author(s):  
V. M. Shabaev ◽  
A. N. Artemyev ◽  
D. A. Glazov ◽  
I. I. Tupitsyn ◽  
A. V. Volotka ◽  
...  

2003 ◽  
Vol 2 (5) ◽  
pp. 377-387 ◽  
Author(s):  
O. Jäkel ◽  
D. Schulz-Ertner ◽  
C.P. Karger ◽  
A. Nikoghosyan ◽  
J. Debus

Starting with the pioneering work at the University of California in Berkeley in 1977, heavy ion radiotherapy has been of increasing interest especially in Japan and Europe in the last decade. There are currently 3 facilities treating patients with carbon ions, two of them in Japan within a clinical setting. In Germany, a research therapy facility is in operation and the construction of a new hospital based facility at the Heidelberg university will be started soon. An outline of the current status of heavy ion radiotherapy is given with emphasis to the technical aspects of the respective facilities. This includes a description of passive and active beam shaping systems, as well as their implications for treatment planning and dosimetry. The clinical trials and routine treatments performed at the German heavy ion facility are summarized. An overview over the upcoming new facilities and their technical possibilities is given. It is discussed what the necessary improvements are to fully exploit the potential of these facilities. Especially the new Heidelberg facility with the possibility of active beam scanning in combination with the first isocentric gantry for ions and offering beams of protons, helium, oxygen and carbon ions has implications on treatment planning, dosimetry and quality assurance. The necessary and ongoing developments in these areas are summarized. The new facilities also offer the possibilities to perform more extensive clinical studies and to explore future indications for radiotherapy with heavy ions. An overview over the indications and treatment schemes is also given.


2019 ◽  
Vol 198 ◽  
pp. 00003 ◽  
Author(s):  
P. Strasser ◽  
M. Abe ◽  
M. Aoki ◽  
S. Choi ◽  
Y. Fukao ◽  
...  

High precision measurements of the ground state hyperfine structure (HFS) of muonium is a stringent tool for testing bound-state quantum electrodynamics (QED) theory, determining fundamental constants of the muon magnetic moment and mass, and searches for new physics. Muonium is the most suitable system to test QED because both theoretical and experimental values can be precisely determined. Previous measurements were performed decades ago at LAMPF with uncertainties mostly dominated by statistical errors. At the J-PARC Muon Science Facility (MUSE), the MuSEUM collaboration is planning complementary measurements of muonium HFS both at zero and high magnetic field. The new high-intensity muon beam that will soon be available at H-Line will provide an opportunity to improve the precision of these measurements by one order of magnitude. An overview of the different aspects of these new muonium HFS measurements, the current status of the preparation for high-field measurements, and the latest results at zero field are presented.


2014 ◽  
Vol 29 (02) ◽  
pp. 1430003 ◽  
Author(s):  
TOICHIRO KINOSHITA

This paper presents the current status of the theory of electron anomalous magnetic moment ae ≡(g-2)/2, including a complete evaluation of 12,672 Feynman diagrams in the tenth-order perturbation theory. To solve this problem, we developed a code-generator which converts Feynman diagrams automatically into fully renormalized Feynman-parametric integrals. They are evaluated numerically by an integration routine VEGAS. The preliminary result obtained thus far is 9.16 (58) (α/π)5, where (58) denotes the uncertainty in the last two digits. This leads to ae( theory ) = 1.159 652 181 78 (77) ×10-3, which is in agreement with the latest measurement ae ( exp :2008) = 1.159 652 180 73 (28) ×10-3. It shows that the Feynman–Dyson method of perturbative QED works up to the precision of 10-12.


2020 ◽  
Vol 128 (8) ◽  
pp. 1085
Author(s):  
Н.А. Зубова ◽  
М.Ю. Кайгородов ◽  
Ю.С. Кожедуб ◽  
А.В. Малышев ◽  
Р.В. Попов ◽  
...  

The precision calculations of the isotope shifts of the $n = 1$, $n = 2$ energy levels and the corresponding transition energies in helium-like highly charged ions are performed. The total isotope shift is mainly determined by a sum of the field and mass shifts. The field shift is calculated by the configuration-interaction Dirac-Fock-Sturm method. The quantum electrodynamics corrections to this contribution are taken into account approximately by using the corresponding one-electron formulas. The calculation of the mass shift is performed within the framework of the Breit approximation and includes the quantum electrodynamics contributions, which become very significant for heavy ions. For the thorium and uranium ions the nuclear polarization and deformation corrections are taken into account.


2011 ◽  
Author(s):  
V. M. Shabaev ◽  
O. V. Andreev ◽  
A. I. Bondarev ◽  
D. A. Glazov ◽  
Y. S. Kozhedub ◽  
...  

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