Abstract
The Marchenko method is used to construct a Schrödinger operator which generates a given set of nucleon-nucleon experimental phase shifts. Three examples concerning np scattering are considered ( 1S 0, 3P 1, 1D 2). In each case the Marchenko method is employed with some modification, the most important being the choice of a non-zero reference potential. The phase shifts which are obtained agree quite well with the input ones. A striking result is brought to light: If one considers a case where only real phase shifts are used as the input and a case where the full complex phase shifts are used, the two resulting Schrödinger operators are intrinsically different in nature.
Sign-in/Register to access full text options 
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a callDisclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.
