By using the multichannel quantum defect theory (MQDT), we have evaluated the energy levels and lifetimes of 2sns ()3S1,2snd()3D(n=3-25) of BeⅠ and 1sns()3S1,1snd ()3D(n=3-25) of BeⅢ. These energies an...By using the multichannel quantum defect theory (MQDT), we have evaluated the energy levels and lifetimes of 2sns ()3S1,2snd()3D(n=3-25) of BeⅠ and 1sns()3S1,1snd ()3D(n=3-25) of BeⅢ. These energies and lifetimes that we have calculated not only agree with the recent measurements and theoretical calculation of Ref.4 and Ref.3, but also predict the lifetimes of 66 other highly excited states.展开更多
We have develop an effective frozen core approximation to calculate energy levels and ionization enegies of the beryllium atom in magnetic field strengths up to 2.35 × 10^5T. Systematic improvement over the Hartr...We have develop an effective frozen core approximation to calculate energy levels and ionization enegies of the beryllium atom in magnetic field strengths up to 2.35 × 10^5T. Systematic improvement over the Hartree-Fock results for the beryllium low-lying states has been accomplished.展开更多
文摘By using the multichannel quantum defect theory (MQDT), we have evaluated the energy levels and lifetimes of 2sns ()3S1,2snd()3D(n=3-25) of BeⅠ and 1sns()3S1,1snd ()3D(n=3-25) of BeⅢ. These energies and lifetimes that we have calculated not only agree with the recent measurements and theoretical calculation of Ref.4 and Ref.3, but also predict the lifetimes of 66 other highly excited states.
文摘We have develop an effective frozen core approximation to calculate energy levels and ionization enegies of the beryllium atom in magnetic field strengths up to 2.35 × 10^5T. Systematic improvement over the Hartree-Fock results for the beryllium low-lying states has been accomplished.