Based on the results of accurate variational calculations we demonstrate stability of the five-body negatively charged ions a+b+μ−e−e−. Each of these five-body ions contains two electrons e−, one negatively charged muon μ− and two nuclei of the hydrogen isotopes a,b = (p,d,t). The bound state properties of these five-body ions, including their hyperfine structure, are briefly discussed. We also investigate the hyperfine structure of the ground states of the four-body muonic quasi-atoms a+b+μ−e−. In particular, we determine the hyperfine structure splittings for the ground state of the four-body muonic quasi-atoms: p+...
The energies of the high-lying multi-excited states 1s22s2pnl and 1s22p2nl 4Pe,o (n ≥ 2) for B-like ...
Abstract: The present knowledge of Lamb shift, fine-, and hyperfine structure of the 2S and 2P state...
The universal variational expansion for the non-relativistic three-body systems is explicitly constr...
The ground state hyperfine splitting of light muon-electron ions of lithium, beryllium, boron and he...
The results of highly accurate calculations are presented for all twenty-two known bound ...
Precision calculations of the fine and hyperfine structure of muonic atoms are performed in a relati...
Precision calculations of the fine and hyperfine structure of muonic atoms are performed in a relati...
A muonic hydrogen-like atom is formed when replacing the electron in it by a negative muon $$\mu ^-$...
We examine the muonium (μ−e+)-antimuonium (μ−e+) system in the models which accommodate thedilepton ...
We discuss the binding of three unit charges qi=±1,∓1,∓1, with various constituent masses mi. It is ...
We discuss the binding of three unit charges qi=±1,∓1,∓1, with various constituent masses mi. It is ...
Vacuum polarization, nuclear structure and recoil, radiative corrections to the hyperfine structure ...
We calculate hyperfine structure intervals for P–states in muonic ions of lithium, beryllium and bor...
We calculate hyperfine structure intervals for P–states in muonic ions of lithium, beryllium and bor...
We calculate hyperfine structure intervals for P–states in muonic ions of lithium, beryllium and bor...
The energies of the high-lying multi-excited states 1s22s2pnl and 1s22p2nl 4Pe,o (n ≥ 2) for B-like ...
Abstract: The present knowledge of Lamb shift, fine-, and hyperfine structure of the 2S and 2P state...
The universal variational expansion for the non-relativistic three-body systems is explicitly constr...
The ground state hyperfine splitting of light muon-electron ions of lithium, beryllium, boron and he...
The results of highly accurate calculations are presented for all twenty-two known bound ...
Precision calculations of the fine and hyperfine structure of muonic atoms are performed in a relati...
Precision calculations of the fine and hyperfine structure of muonic atoms are performed in a relati...
A muonic hydrogen-like atom is formed when replacing the electron in it by a negative muon $$\mu ^-$...
We examine the muonium (μ−e+)-antimuonium (μ−e+) system in the models which accommodate thedilepton ...
We discuss the binding of three unit charges qi=±1,∓1,∓1, with various constituent masses mi. It is ...
We discuss the binding of three unit charges qi=±1,∓1,∓1, with various constituent masses mi. It is ...
Vacuum polarization, nuclear structure and recoil, radiative corrections to the hyperfine structure ...
We calculate hyperfine structure intervals for P–states in muonic ions of lithium, beryllium and bor...
We calculate hyperfine structure intervals for P–states in muonic ions of lithium, beryllium and bor...
We calculate hyperfine structure intervals for P–states in muonic ions of lithium, beryllium and bor...
The energies of the high-lying multi-excited states 1s22s2pnl and 1s22p2nl 4Pe,o (n ≥ 2) for B-like ...
Abstract: The present knowledge of Lamb shift, fine-, and hyperfine structure of the 2S and 2P state...
The universal variational expansion for the non-relativistic three-body systems is explicitly constr...