Comments on the classical approach to non-Rutherford cross section calculations
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Cited by (6)
Non-Rutherford cross-sections for alpha elastic scattering off Z = 28–38 elements in the energy range up to 10 MeV
2018, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsCitation Excerpt :At an elevated energy the cross-section becomes non-Rutherford also for medium heavy nuclei. The approaches to predict the energy at which heavy matrix scattering is no longer purely Rutherford were discussed in several papers [3–5] and a rough guidance for IBA practitioners as to when they need to worry about the scattering process being non-Rutherford was given in [6]. In practice this “non-Rutherford threshold” sets a limit on the increase of the projectile energy.
Energy levels of light nuclei A = 12
2017, Nuclear Physics ACitation Excerpt :Nucleon excitation studies are discussed in [1993RO13,1995NI01,1995ZO01,1997GI02,1997GI12,1998GA25,1999BA31,2004BO47,2008BO24,2011VA11]. Effects such as transparency of the nuclear medium have been studied by [1990FR11,1992BE23,1992FR17,1992GA02,1992JE03,1992PA03,1993LO01,1993NI11,1994FR12,1994FR16,1994GR05,1994IR02,1994KO21,1994MA23,1994NI05,1995FR04,1996KE14,1996NI13,1997AL20,1997IW03,1999RY06,2000DU12,2000LA23,2001FR06,2002DE11,2002GA43,2002ME11,2002ME17,2003DU23,2003RY02,2004BA99,2004BO47,2004HA63,2004LA13,2005RO38,2006RO37,2007CL04,2009KA02,2010QI02,2013RO06]. Discussion on other final state effects is given in [1991CA09,1994IR02,1994JE04,1994RY04,1995BI07,1995BI19,1995NI02,1996BI01,1996BI21,1996JE04,1999KE04,2002DE07,2004BA99,2004BB15,2005BA07,2005BA23,2005PR02,2007AL14,2007PI05], and discussion on the reaction mechanism is found in [1990LO09,1991VA05,1992DR02,1993CI05,1993OF01,1994IR01,1994RY03,1994TA11,1994WE06,1999MO02,2002ME17,2004FR27,2004MU29,2004RO35,2004TA18,2011RY03].
Increase in coercivity of Fe-Pt thin film permanent magnets by N <inf>2</inf><sup>+</sup> ion implantation and heat treatment in hydrogen gas
2012, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsOn the concept of an actual Coulomb barrier
2004, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsProton elastic scattering cross section for carbon: confrontation of theory and experiment
1999, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms