FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2023665797> ?p ?o ?g. }

• W2023665797 endingPage "B1293" @default.
• W2023665797 startingPage "B1272" @default.
• W2023665797 abstract "States of spin ${frac{7}{2}}^{ensuremath{-}}$ in ${mathrm{Ti}}^{47}$, ${mathrm{Ti}}^{49}$, ${mathrm{Cr}}^{51}$, ${mathrm{Fe}}^{53}$, ${mathrm{Fe}}^{55}$, ${mathrm{Fe}}^{57}$, ${mathrm{Ni}}^{57}$, ${mathrm{Ni}}^{59}$, and ${mathrm{Ni}}^{61}$ were observed by means of the ($p,d$) reaction with 28-MeV incident protons. In each case the highest ${frac{7}{2}}^{ensuremath{-}}$ state seen was found to be the isobaric analog of the lowest ${frac{7}{2}}^{ensuremath{-}}$ state of the isobar with one more neutron. Coulomb displacement energies were obtained which are in excellent agreement with known values in this mass region. The lower ${frac{7}{2}}^{ensuremath{-}}$ states were interpreted as configuration states, that is, states associated with the same configuration as the analog, but with isospin lower by unity. The angular distributions in all cases were in good agreement with distorted-wave calculations. Comparison of the spectroscopic factors for the analog and configuration states with the predictions of $jensuremath{-}j$-coupling sum rules revealed that the normal procedures used in distorted-wave calculations predict too large a $Q$ dependence. However, by using radial wave functions for the picked-up neutron that are identical for all $1{f}_{frac{7}{2}}$ states in a given nucleus, reasonable agreement with the sum rules was obtained. Reasonable agreement was also found with the strengths for various states computed from $1{f}_{frac{7}{2}}$ shell-model calculations. The energy splitting between the analog state and the strength-weighted mean of the configuration states was also found to be in agreement with theoretical estimates." @default.
• W2023665797 created "2016-06-24" @default.
• W2023665797 creator A5001013210 @default.
• W2023665797 creator A5014547270 @default.
• W2023665797 creator A5026716324 @default.
• W2023665797 creator A5031490624 @default.
• W2023665797 creator A5074017745 @default.
• W2023665797 date "1965-09-06" @default.
• W2023665797 modified "2023-10-17" @default.
• W2023665797 title "Excitation of Isobaric Analog States in Medium-Weight Nuclei by the (<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mi>d</mml:mi><mml:mo>,</mml:mo><mml:mi>p</mml:mi></mml:math>) Reaction at 28 MeV" @default.
• W2023665797 cites W1511146010 @default.
• W2023665797 cites W1540747732 @default.
• W2023665797 cites W1967913932 @default.
• W2023665797 cites W1972885222 @default.
• W2023665797 cites W1975323414 @default.
• W2023665797 cites W1983672735 @default.
• W2023665797 cites W1983839702 @default.
• W2023665797 cites W1990052327 @default.
• W2023665797 cites W1994368259 @default.
• W2023665797 cites W1998049748 @default.
• W2023665797 cites W2013006085 @default.
• W2023665797 cites W2014025320 @default.
• W2023665797 cites W2016181203 @default.
• W2023665797 cites W2028113640 @default.
• W2023665797 cites W2038487071 @default.
• W2023665797 cites W2039272951 @default.
• W2023665797 cites W2039983627 @default.
• W2023665797 cites W2040376121 @default.
• W2023665797 cites W2046099041 @default.
• W2023665797 cites W2047854057 @default.
• W2023665797 cites W2049500441 @default.
• W2023665797 cites W2050960357 @default.
• W2023665797 cites W2053905136 @default.
• W2023665797 cites W2056990735 @default.
• W2023665797 cites W2056999100 @default.
• W2023665797 cites W2057467627 @default.
• W2023665797 cites W2057932210 @default.
• W2023665797 cites W2062135504 @default.
• W2023665797 cites W2065010689 @default.
• W2023665797 cites W2067071930 @default.
• W2023665797 cites W2068573870 @default.
• W2023665797 cites W2070077805 @default.
• W2023665797 cites W2070627719 @default.
• W2023665797 cites W2074059850 @default.
• W2023665797 cites W2074936866 @default.
• W2023665797 cites W2076423369 @default.
• W2023665797 cites W2081445905 @default.
• W2023665797 cites W2087737250 @default.
• W2023665797 cites W2090164060 @default.
• W2023665797 cites W2092109274 @default.
• W2023665797 cites W2094646020 @default.
• W2023665797 cites W2094689531 @default.
• W2023665797 cites W2286861519 @default.
• W2023665797 cites W2997491364 @default.
• W2023665797 cites W3093715971 @default.
• W2023665797 cites W4241682136 @default.
• W2023665797 cites W4242818716 @default.
• W2023665797 doi "https://doi.org/10.1103/physrev.139.b1272" @default.
• W2023665797 hasPublicationYear "1965" @default.
• W2023665797 type Work @default.
• W2023665797 sameAs 2023665797 @default.
• W2023665797 citedByCount "208" @default.
• W2023665797 countsByYear W20236657972012 @default.
• W2023665797 countsByYear W20236657972014 @default.
• W2023665797 countsByYear W20236657972015 @default.
• W2023665797 countsByYear W20236657972016 @default.
• W2023665797 countsByYear W20236657972018 @default.
• W2023665797 crossrefType "journal-article" @default.
• W2023665797 hasAuthorship W2023665797A5001013210 @default.
• W2023665797 hasAuthorship W2023665797A5014547270 @default.
• W2023665797 hasAuthorship W2023665797A5026716324 @default.
• W2023665797 hasAuthorship W2023665797A5031490624 @default.
• W2023665797 hasAuthorship W2023665797A5074017745 @default.
• W2023665797 hasConcept C11413529 @default.
• W2023665797 hasConcept C121332964 @default.
• W2023665797 hasConcept C131584629 @default.
• W2023665797 hasConcept C146211579 @default.
• W2023665797 hasConcept C147120987 @default.
• W2023665797 hasConcept C172695262 @default.
• W2023665797 hasConcept C184779094 @default.
• W2023665797 hasConcept C185592680 @default.
• W2023665797 hasConcept C186370098 @default.
• W2023665797 hasConcept C190284468 @default.
• W2023665797 hasConcept C191897082 @default.
• W2023665797 hasConcept C192562407 @default.
• W2023665797 hasConcept C41008148 @default.
• W2023665797 hasConcept C48103436 @default.
• W2023665797 hasConcept C62520636 @default.
• W2023665797 hasConcept C8010536 @default.
• W2023665797 hasConcept C83581075 @default.
• W2023665797 hasConcept C93368182 @default.
• W2023665797 hasConcept C9342510 @default.
• W2023665797 hasConcept C97355855 @default.
• W2023665797 hasConceptScore W2023665797C11413529 @default.
• W2023665797 hasConceptScore W2023665797C121332964 @default.
• W2023665797 hasConceptScore W2023665797C131584629 @default.
• W2023665797 hasConceptScore W2023665797C146211579 @default.
• W2023665797 hasConceptScore W2023665797C147120987 @default.

• next