Add to ORKGThe hyperfine structure splitting of the ground state of hydrogen-like "2"0"9Bi is calculated for an extended nuclear charge distribution. The probability density of the odd proton in "2"0"9Bi is taken into account explicitly in order to compute the effect of an extended magnetization distribution on the energy splitting. The probability density of the odd proton is deduced from a mean-field model and the magnetization correction is evaluated within the Bohr-Weisskopf formalism. We obtained a transition wave length of #DELTA##lambda#=242.3 nm. An estimate for the QED corrections is provided. (orig.)Available from TIB Hannover: RO 801(93-44) / FIZ - Fachinformationszzentrum Karlsruhe / TIB - Technische Informati...
Corrections of order alpha^5, alpha^6 are calculated in the hyperfine splitting of muonic hydrogen g...
Systematic model calculations are performed for the magnetization distributions and the hyperfine st...
The hyperfine structure splitting in the 6p2 4S3/2 -> 6p27s 4P1/2 transition at 307 nm in atomic 208...
Studies of the hyperfine splitting in hydrogen are strongly motivated by the level of accuracy achie...
A calculation of the vacuum-polarization contribution to the hyperfine splitting for hydrogenlike at...
High-precision measurements and calculations of energy spectra of hydrogen-like atoms provide tests ...
The theory of QED corrections to hyperfine structure in light hydrogenic atoms and ions has recently...
In previous papers, corrections to the hyperfine structure (hfs) in hydrogen of relative order αm / ...
The finite nuclear size effect on the hyperfine splitting of low-Z hydrogen-like atoms is studied in...
The hyperfine structure splitting in the 6p2 4S3/2 -> 6p27s 4P1/2 transition at 307 nm in atomic 208...
AbstractQED theory of the hyperfine splitting of the 1s and 2s state in hydrogen isotopes and helium...
QED theory of the hyperfine splitting of the 1s and 2s state in hydrogen isotopes and helium-3 ion i...
This thesis is a calculation of the energy shift in the hyperfine structure of atomic H due to the f...
The hyperfine structure splitting in the 6p3S3/24→6p27sP1/24 transition at 307 nm in atomic 208Bi wa...
We revisit the mα6(m/M) order corrections to the hyperfine splitting in the H2+ ion and find a hithe...
Corrections of order alpha^5, alpha^6 are calculated in the hyperfine splitting of muonic hydrogen g...
Systematic model calculations are performed for the magnetization distributions and the hyperfine st...
The hyperfine structure splitting in the 6p2 4S3/2 -> 6p27s 4P1/2 transition at 307 nm in atomic 208...
Studies of the hyperfine splitting in hydrogen are strongly motivated by the level of accuracy achie...
A calculation of the vacuum-polarization contribution to the hyperfine splitting for hydrogenlike at...
High-precision measurements and calculations of energy spectra of hydrogen-like atoms provide tests ...
The theory of QED corrections to hyperfine structure in light hydrogenic atoms and ions has recently...
In previous papers, corrections to the hyperfine structure (hfs) in hydrogen of relative order αm / ...
The finite nuclear size effect on the hyperfine splitting of low-Z hydrogen-like atoms is studied in...
The hyperfine structure splitting in the 6p2 4S3/2 -> 6p27s 4P1/2 transition at 307 nm in atomic 208...
AbstractQED theory of the hyperfine splitting of the 1s and 2s state in hydrogen isotopes and helium...
QED theory of the hyperfine splitting of the 1s and 2s state in hydrogen isotopes and helium-3 ion i...
This thesis is a calculation of the energy shift in the hyperfine structure of atomic H due to the f...
The hyperfine structure splitting in the 6p3S3/24→6p27sP1/24 transition at 307 nm in atomic 208Bi wa...
We revisit the mα6(m/M) order corrections to the hyperfine splitting in the H2+ ion and find a hithe...
Corrections of order alpha^5, alpha^6 are calculated in the hyperfine splitting of muonic hydrogen g...
Systematic model calculations are performed for the magnetization distributions and the hyperfine st...
The hyperfine structure splitting in the 6p2 4S3/2 -> 6p27s 4P1/2 transition at 307 nm in atomic 208...