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Relativistic and QED corrections for the beryllium atom
Krzysztof Pachucki1, Jacek Komasa
1Institute of Theoretical Physics, Warsaw University, Hoza 69, 00-681 Warsaw, Poland. krp@fuw.edu.pl
Physical Review Letters
|July 13, 2004
Summary
We precisely calculated relativistic and quantum electrodynamics corrections for beryllium atoms and ions. Our high-precision theoretical predictions for energy levels and ionization potential align with experimental data.
Area of Science:
- Atomic Physics
- Quantum Electrodynamics
- Relativistic Quantum Mechanics
Background:
- Accurate theoretical calculations are crucial for understanding atomic structure and spectra.
- Beryllium (Be) and its ions are fundamental systems for testing quantum theories.
- Previous calculations lacked comprehensive relativistic and quantum electrodynamics (QED) corrections.
Purpose of the Study:
- To compute complete relativistic and QED corrections of order alpha(2) Ry and alpha(3) Ry for the ground state of beryllium and its positive ion.
- To provide high-precision theoretical predictions for atomic energy levels and ionization potentials.
- To validate theoretical methods by comparing with experimental data.
Main Methods:
- Utilized a basis set of correlated Gaussian functions.
- Optimized Gaussian function exponents against nonrelativistic binding energies.
- Performed calculations including complete relativistic and QED corrections.
Main Results:
- Calculated Bethe logarithms for Be: ln(k(0)(Be)) = 5.750 34(3).
- Calculated Bethe logarithms for Be+: ln(k(0)(Be+)) = 5.751 67(3).
- Determined a recommended ionization potential for Be: 75 192.514(80) cm(-1).
Conclusions:
- The high precision of the calculated Bethe logarithms demonstrates the capability for accurate theoretical predictions of energy levels in light atoms and ions.
- The agreement between the calculated ionization potential and experimental values validates the employed theoretical approach.
- This work provides benchmark data for the beryllium atom and its ion, advancing the field of atomic physics.