000393458 001__ 393458
000393458 005__ 20211110144812.0
000393458 0247_ $$2ISSN$$a0375-9474
000393458 0247_ $$2ISSN$$a1873-1554
000393458 0247_ $$2datacite_doi$$a10.3204/PUBDB-2017-11485
000393458 037__ $$aPUBDB-2017-11485
000393458 041__ $$aEnglish
000393458 082__ $$a530
000393458 0881_ $$aDESY-74-020
000393458 088__ $$2DESY$$aDESY-74-020
000393458 1001_ $$0P:(DE-HGF)0$$aHeimlich, F. H.$$b0
000393458 245__ $$aHigh-energy electron scattering from $\mathrm{^6Li}$ and $\mathrm{^{12}C}$
000393458 260__ $$c1974
000393458 300__ $$a1-22
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000393458 3367_ $$0PUB:(DE-HGF)15$$2PUB:(DE-HGF)$$aInternal Report$$bintrep$$mintrep$$s1519051456_5483
000393458 520__ $$aWe have measured the spectra of electrons scattered from 6 Li and 12 C for invariant masses of the hadronic system W ≦ 1.5 GeV and four momentum transfers in the range 5 fm −2 ≦ q 2 ≦ 12 fm −2 . We compared the shape of the spectra with different nuclear models. The Fermigas model of the nucleus cannot reproduce the data. A shell model with short-range correlations fits the data with a correlation parameter q c ≈ 250 MeV/ c . From the absolute cross section the effective number of nucleons was derived for quasi-elastic scattering and found to be compatible with A , whereas the effective number of nucleons derived for the excitation of the Δ(1236) resonance was found to be 0.6 A .
000393458 536__ $$0G:(DE-HGF)POF3-899$$a899 - ohne Topic (POF3-899)$$cPOF3-899$$fPOF III$$x0
000393458 588__ $$aDataset connected to CrossRef, INSPIRE
000393458 650_7 $$2INSPIRE$$aelectron light nucleus: interaction
000393458 650_7 $$2INSPIRE$$ainteraction: electron light nucleus
000393458 650_7 $$2INSPIRE$$alithium
000393458 650_7 $$2INSPIRE$$acarbon
000393458 650_7 $$2INSPIRE$$aelectron: differential cross section
000393458 650_7 $$2INSPIRE$$adifferential cross section: electron
000393458 650_7 $$2INSPIRE$$aelectron light nucleus: elastic scattering
000393458 650_7 $$2INSPIRE$$aelastic scattering: electron light nucleus
000393458 650_7 $$2INSPIRE$$adelta(1236): electroproduction
000393458 650_7 $$2INSPIRE$$aelectroproduction: delta(1236)
000393458 650_7 $$2INSPIRE$$anucleon nucleon: correlation
000393458 650_7 $$2INSPIRE$$aradiative correction
000393458 650_7 $$2INSPIRE$$aelectron p: interaction
000393458 650_7 $$2INSPIRE$$ainteraction: electron p
000393458 650_7 $$2INSPIRE$$aelectron n: interaction
000393458 650_7 $$2INSPIRE$$ainteraction: electron n
000393458 650_7 $$2INSPIRE$$atotal cross section
000393458 650_7 $$2INSPIRE$$anucleon: form factor
000393458 650_7 $$2INSPIRE$$aform factor: nucleon
000393458 650_7 $$2INSPIRE$$anucleon: bound state
000393458 650_7 $$2INSPIRE$$anucleon: momentum
000393458 650_7 $$2INSPIRE$$amomentum: spectrum
000393458 650_7 $$2INSPIRE$$aspectrum: momentum
000393458 650_7 $$2INSPIRE$$ashell model
000393458 650_7 $$2INSPIRE$$amodel: fermi gas
000393458 650_7 $$2INSPIRE$$abaryon resonance: electroproduction
000393458 650_7 $$2INSPIRE$$aelectroproduction: baryon resonance
000393458 650_7 $$2INSPIRE$$abaryon resonance: nonstrange
000393458 650_7 $$2INSPIRE$$anonstrange: baryon resonance
000393458 650_7 $$2INSPIRE$$adesy es
000393458 650_7 $$2INSPIRE$$aFINAL STATE: ELECTRON
000393458 650_7 $$2INSPIRE$$aDEUTERON: FINAL STATE
000393458 650_7 $$2INSPIRE$$aFINAL STATE: DEUTERON
000393458 650_7 $$2INSPIRE$$aELECTRON LIGHT NUCLEUS --> LIGHT NUCLEUS P ELECTRON
000393458 650_7 $$2INSPIRE$$aELECTRON LIGHT NUCLEUS --> LIGHT NUCLEUS DEUTERON ELECTRO
000393458 650_7 $$2INSPIRE$$a2.0: 2.5: 2.7 gev: 5-12 q-squared (1/f)-squared
000393458 650_7 $$2INSPIRE$$a2.0-2.7 GEV
000393458 650_7 $$2INSPIRE$$aPOTENTIAL SCATTERING
000393458 650_7 $$2INSPIRE$$aCORRELATION: SHORT-RANGE
000393458 650_7 $$2INSPIRE$$aMODEL: CLUSTER
000393458 650_7 $$2INSPIRE$$aMODEL: OSCILLATOR
000393458 650_7 $$2INSPIRE$$aEMISSION: DEUTERON
000393458 650_7 $$2INSPIRE$$aEMISSION: MOMENTUM TRANSFER
000393458 650_7 $$2INSPIRE$$aELECTRON DEUTERON: ELASTIC SCATTERING
000393458 650_7 $$2INSPIRE$$aELASTIC SCATTERING: ELECTRON DEUTERON
000393458 650_7 $$2INSPIRE$$aCROSS SECTION: RATIO
000393458 650_7 $$2INSPIRE$$aDELTA(1236): ELECTROPRODUCTION
000393458 650_7 $$2INSPIRE$$aELECTROPRODUCTION: DELTA(1236)
000393458 650_7 $$2INSPIRE$$aMODEL: GUTBROD-SIMON
000393458 650_7 $$2INSPIRE$$aNUMERICAL CALCULATIONS: INTERPRETATION OF EXPERIMENTS
000393458 650_7 $$2INSPIRE$$aLIGHT NUCLEUS: FINAL STATE
000393458 650_7 $$2INSPIRE$$aFINAL STATE: LIGHT NUCLEUS
000393458 650_7 $$2INSPIRE$$aP: FINAL STATE
000393458 650_7 $$2INSPIRE$$aFINAL STATE: P
000393458 650_7 $$2INSPIRE$$aELECTRON: FINAL STATE
000393458 693__ $$0EXP:(DE-MLZ)NOSPEC-20140101$$5EXP:(DE-MLZ)NOSPEC-20140101$$eNo specific instrument$$x0
000393458 7001_ $$0P:(DE-HGF)0$$aKoebberling, M.$$b1
000393458 7001_ $$aMoritz, J.$$b2
000393458 7001_ $$aSchmidt, K. H.$$b3
000393458 7001_ $$aWegener, D.$$b4
000393458 7001_ $$0P:(DE-HGF)0$$aZeller, D.$$b5
000393458 7001_ $$aBienlein, J. K.$$b6
000393458 7001_ $$0P:(DE-HGF)0$$aBleckwenn, J.$$b7
000393458 7001_ $$0P:(DE-H253)PIP1021528$$aDinter, H.$$b8$$udesy
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