摘要:

AbstractSome aspects of medium energy (∼ 150 MeV to 1 GeV) proton and pion scattering theory from complex nuclei are reviewed with emphasis on inelastic scattering as a tool to extract nuclear structure informatio

ISSN:0015-8208    

DOI:10.1002/prop.19760240102

出版商:WILEY‐VCH Verlag    

年代:1976

数据来源: WILEY

摘要:

AbstractDirac's perturbation solution of the time‐dependent Schrödinger equationih\documentclass{article}\pagestyle{empty}\begin{document}$ ih\frac{d}{{dt}}\left| {\Phi \left. {\left( t \right)} \right\rangle = H} \right|\Phi \left. {\left( t \right)} \right\rangle $\end{document},\documentclass{article}\pagestyle{empty}\begin{document}$ H = H_0 + \Psi $\end{document}is formulated by means of a well‐defined operatorPDwith the properties\documentclass{article}\pagestyle{empty}\begin{document}$$ \Phi ^n \left. {\left( t \right)} \right\rangle = \frac{1}{n}\gamma _D \left| {\Phi ^{n - 1} } \right\rangle ,\left| {\Phi \left( t \right)} \right\rangle = \sum\limits_n {\left| {\Phi ^n \left( t \right)} \right\rangle = \exp \left( {\gamma _D } \right)\left| {\Phi ^0 \left( t \right)} \right\rangle } ,H = \exp \left( {\gamma _D } \right)H_0 \exp \left( { - \gamma _D } \right) $$\end{document}where ϕn(t)〉 is then‐th order correction of ϕ(t)〉. This operatorPDcan be used to solve the equation of motion of the evolution operator, of the statistical operator, and of quantum mechanical conserved quantities in a corresponding way. A simple proof of the quantum mechanical adiabatic theorem shows this formulation of perturbation corrections

ISSN:0015-8208    

DOI:10.1002/prop.19760240103

出版商:WILEY‐VCH Verlag    

年代:1976

数据来源: WILEY

ISSN:0015-8208    

DOI:10.1002/prop.19760240101

出版商:WILEY‐VCH Verlag    

年代:1976

数据来源: WILEY