Logarithmic corrections in the two-body qed problem. / Khriplovich, I. B.; Milstein, A. I.; Yelkhovsky, A. S.
In: Physica Scripta, Vol. 1993, No. T46, 01.01.1993, p. 252-260.Research output: Contribution to journal › Article › peer-review
}
TY - JOUR
T1 - Logarithmic corrections in the two-body qed problem
AU - Khriplovich, I. B.
AU - Milstein, A. I.
AU - Yelkhovsky, A. S.
PY - 1993/1/1
Y1 - 1993/1/1
N2 - The logarithmic part of the Lamb shift, the contribution of the relative order a3log (1/a) to the atomic state energy, is related to the usual infrared divergence. This fact allows one to calculate easily such corrections in positronium, and derive the recoil and electron-electron terms in the Lamb- shift Hamiltonian in many-electron atoms. Logarithmic energy corrections of the next order, a4 log (1/a), are of a different, relativistic nature. Their calculation is reduced to the ordinary perturbation theory for the nonrelativistic Schrodinger equation. The perturbation operators have the Breittype structure and are found by the calculation of on-mass-shell diagrams. For positronium, the calculated log-arithmic correction survives only in n3Sj states and constitutes ¿ma6 log (l/a)/n3. Logarithmic corrections of the relative order a2 log (1/a) to the positronium decay rate are also of the relativistic origin and can be easily computed within the same approach. Arguments are presented in favour of a large numerical factor in the (a/rc)2 correction to the positronium decay rate.
AB - The logarithmic part of the Lamb shift, the contribution of the relative order a3log (1/a) to the atomic state energy, is related to the usual infrared divergence. This fact allows one to calculate easily such corrections in positronium, and derive the recoil and electron-electron terms in the Lamb- shift Hamiltonian in many-electron atoms. Logarithmic energy corrections of the next order, a4 log (1/a), are of a different, relativistic nature. Their calculation is reduced to the ordinary perturbation theory for the nonrelativistic Schrodinger equation. The perturbation operators have the Breittype structure and are found by the calculation of on-mass-shell diagrams. For positronium, the calculated log-arithmic correction survives only in n3Sj states and constitutes ¿ma6 log (l/a)/n3. Logarithmic corrections of the relative order a2 log (1/a) to the positronium decay rate are also of the relativistic origin and can be easily computed within the same approach. Arguments are presented in favour of a large numerical factor in the (a/rc)2 correction to the positronium decay rate.
UR - http://www.scopus.com/inward/record.url?scp=84956125282&partnerID=8YFLogxK
U2 - 10.1088/0031-8949/1993/T46/040
DO - 10.1088/0031-8949/1993/T46/040
M3 - Article
AN - SCOPUS:84956125282
VL - 1993
SP - 252
EP - 260
JO - Physica Scripta Topical Issues
JF - Physica Scripta Topical Issues
SN - 0031-8949
IS - T46
ER -
ID: 36648643