Quantum derivation of the use of classical electromagnetic potentials in relativistic Coulomb excitation
We prove that a relativistic Coulomb excitation calculation in which the classical electromagnetic field of the projectile is used to induce transitions between target states gives the same target transition amplitudes, to all orders of perturbation theory, as would a calculation in which the intera...
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Veröffentlicht in: | Physical review. C, Nuclear physics Nuclear physics, 2005-05, Vol.71 (5), Article 054906 |
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container_title | Physical review. C, Nuclear physics |
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creator | Bayman, B. F. Zardi, F. |
description | We prove that a relativistic Coulomb excitation calculation in which the classical electromagnetic field of the projectile is used to induce transitions between target states gives the same target transition amplitudes, to all orders of perturbation theory, as would a calculation in which the interaction between projectile and target is mediated by a quantized electromagnetic field. |
doi_str_mv | 10.1103/PhysRevC.71.054906 |
format | Article |
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C, Nuclear physics</title><description>We prove that a relativistic Coulomb excitation calculation in which the classical electromagnetic field of the projectile is used to induce transitions between target states gives the same target transition amplitudes, to all orders of perturbation theory, as would a calculation in which the interaction between projectile and target is mediated by a quantized electromagnetic field.</description><subject>BASIC INTERACTIONS</subject><subject>COULOMB EXCITATION</subject><subject>ELECTROMAGNETIC FIELDS</subject><subject>ENERGY LEVELS</subject><subject>HEAVY ION REACTIONS</subject><subject>NUCLEAR PHYSICS AND RADIATION PHYSICS</subject><subject>PERTURBATION THEORY</subject><subject>POTENTIALS</subject><subject>RELATIVISTIC RANGE</subject><subject>TRANSITION AMPLITUDES</subject><issn>0556-2813</issn><issn>1089-490X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2005</creationdate><recordtype>article</recordtype><recordid>eNo1UE1LxDAUDKLguvoHPAU8d02aNG2PUvyCBT9Q8BaS9NVG2mRp0sX992ZdfZc38ObNDIPQJSUrSgm7fu534RW2zaqkK1LwmogjtKCkqrOEP47RghSFyPKKslN0FsIXScOYWKD-ZVYuziNuYbJbFa132Hc49oDnAHtoBhWCNWrAMICJkx_Vp4NoDd74CC5aNQRsHZ5gSO9bG_anxs-DHzWGb2Pjr-o5OukSEy7-9hK9392-NQ_Z-un-sblZZybPRcxYXVBBi4pxozpNlOLQQleW1PCSs0KVjCtFWSsqXbRMG9ZqntNat7pqjRYdW6Krg65PQWRI9mB6451L2WVORF2JOk-s_MAykw9hgk5uJjuqaScpkftG5X-jsqTy0Cj7AUc7bnY</recordid><startdate>200505</startdate><enddate>200505</enddate><creator>Bayman, B. 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source | American Physical Society Journals |
subjects | BASIC INTERACTIONS COULOMB EXCITATION ELECTROMAGNETIC FIELDS ENERGY LEVELS HEAVY ION REACTIONS NUCLEAR PHYSICS AND RADIATION PHYSICS PERTURBATION THEORY POTENTIALS RELATIVISTIC RANGE TRANSITION AMPLITUDES |
title | Quantum derivation of the use of classical electromagnetic potentials in relativistic Coulomb excitation |
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