2000
DOI: 10.1007/s100520000464
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Measurement of spin observables in neutron-proton elastic scattering

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Cited by 13 publications
(6 citation statements)
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“…The trend of the new data in the resonance region deviates clearly from that exhibited by the data from previous experiments below and above this region [8][9][10][22][23][24][25][26][27]. The new partial-wave solutions (see below) connect all data within their uncertainties, whereas the SP07 solution obviously fails in the resonance region.…”
Section: Amentioning
confidence: 58%
“…The trend of the new data in the resonance region deviates clearly from that exhibited by the data from previous experiments below and above this region [8][9][10][22][23][24][25][26][27]. The new partial-wave solutions (see below) connect all data within their uncertainties, whereas the SP07 solution obviously fails in the resonance region.…”
Section: Amentioning
confidence: 58%
“…The solid symbols denote the results from this work, the open symbols those from previous work [7][8][9][19][20][21][22][23]. For the meaning of the curves see Fig.…”
Section: = 83mentioning
confidence: 93%
“…Starting from N 4 LO, we found that setting the maximum fitting energy E max lab ∼ 250 MeV leads to stable results for the LECs and phase shifts for all employed cutoff values in the range of Λ = 350 − 550 MeV. Given the abundance of np spin-observables available at the energies around E lab ∼ 260 MeV and coming from the recent experiments of [94][95][96], we decided to set E max lab = 260 MeV at this chiral order. We will address the sensitivity of our results on the choice of E max lab in section VII E. At N 3 LO, we fit up to E lab = 200 MeV while the maximum energy of included scattering data at LO, NLO and N 2 LO is chosen to be E lab = 25, 100 and 125 MeV.…”
Section: Fitting Proceduresmentioning
confidence: 99%