n p elastic analyzing power A(NO) and spin transfer K(NN)

McNaughton, M.W. ; Johnston, K. ; Swenson, D. ; et al.
Phys.Rev.C 48 (1993) 256-265, 1993.
Inspire Record 34401 DOI 10.17182/hepdata.51045

We have measured the analyzing power ANO and the spin transfer KNN for np-elastic scattering from about 60° to 170° c.m. at 485, 635, and 788 MeV. The new data clarify previous discrepancies and complete the first-order determination of nucleon-nucleon elastic scattering at these energies.

6 data tables

For definition of the POL(NAME=SPIN-TRANSFER) see text.

For definition of the POL(NAME=SPIN-TRANSFER) see text.

For definition of the POL(NAME=SPIN-TRANSFER) see text.

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Precision measurement of charge symmetry breaking in n p elastic scattering at 347-MeV

Zhao, J. ; Abegg, R. ; Berdoz, A.R. ; et al.
Phys.Rev.C 57 (1998) 2126-2141, 1998.
Inspire Record 484066 DOI 10.17182/hepdata.25692

A nonzero difference of the analyzing powers due to charge symmetry breaking has been measured with high precision in np elastic scattering at a neutron beam energy of 347 MeV. The neutron beam and proton target were alternately polarized for the measurements of An and Ap. A mirror-symmetric detection system was used to cancel geometry-related systematic errors. From fits of the measured asymmetry angular distributions over the range of 53.4°<~θcm<~86.9°, the difference in the zero-crossing angles of the analyzing powers was determined to be 0.438°±0.054°(stat.)±0.051°(syst.) in the center-of-mass system. Using the experimentally determined slope of the analyzing power dA/dθ=(−1.35±0.05)×10−2 deg−1 (c.m.), this is equivalent to ΔA≡An−Ap=[59±7(stat.)±7(syst.)±2(syst.)]×10−4. The shape of ΔA(θ) in the vicinity of the zero-crossing angle has also been extracted. Predictions of nucleon-nucleon interaction models based on meson exchange agree well with the results.

1 data table

(C=N) or (C=P) stands for polarized beam or target.


Differential cross-section for n p elastic scattering in the angular region 50-degrees < Theta* < 180-degrees at 459-MeV

Northcliffe, L.C. ; Jain, M. ; Evans, M.L. ; et al.
Phys.Rev.C 47 (1993) 36-46, 1993.
Inspire Record 358672 DOI 10.17182/hepdata.26016

The differential cross section for n-p elastic scattering at 459 MeV in the c.m. angular region 50°<θ*<180° has been measured with high statistical precision and good relative accuracy. The uncertainty in the absolute normalization (based on the simultaneously measured yield of deuterons from the np→dπ0 reaction) was initially estimated to be ∼7%. The results agree well with back-angle data obtained independently at LAMPF but less well with results from Saclay and the Princeton-Pennsylvania Accelerator and, except for a normalization difference of 10%, are fairly well represented by a phase-shift fit. The pole-extrapolation method of Chew was used to extract the pion-nucleon coupling constant f2 from the back-angle portion of the data. The value obtained, f2=0.069, is somewhat smaller than the values 0.0735–0.0790 obtained from analyses of pion-nucleon scattering, tending to confirm the need for an upward renormalization of the angular distribution by ∼10%.

1 data table

No description provided.


The Zero crossing angle of the n - p analyzing power

Davis, C.A. ; Abegg, R. ; Berdoz, A.R. ; et al.
Phys.Rev.C 53 (1996) 2052-2067, 1996.
Inspire Record 402498 DOI 10.17182/hepdata.26459

The angles at which the n-p elastic scattering neutron analyzing power A00n0 crosses zero were measured with precision at four TRIUMF energies below 300 MeV. The mean interaction energies are also measured with greater precision than in previous experiments. The results are En=175.26±0.23 MeV, θzx=98.48°±0.28°; En=203.15±0.20 MeV, θzx=91.31°±0.18°; En=217.24±0.19 MeV, θzx=87.64°±0.18°; and En=261.00±0.16 MeV, θzx=80.18°±0.19°. After correction for charge symmetry breaking effects, the energy where the averaged neutron-proton analyzing power crosses zero at θzx=90° is found to be En=206.8±0.6 MeV. © 1996 The American Physical Society.

4 data tables

Polarized beam and target.

Polarized beam and target.

Polarized beam and target.

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Neutron-Proton Charge Exchange Scattering from 8-GeV/c to 29-GeV/c

Kreisler, Michael N. ; Davis, Michael B. ; Longo, Michael J. ; et al.
Nucl.Phys.B 84 (1975) 3-54, 1975.
Inspire Record 90302 DOI 10.17182/hepdata.32178

The differential cross sections for neutron-proton charge-exchange scattering have been measured for incident neutron momenta between 8 and 29 GeV /c and for four-momentum transfers | t | between 0.002 and 1.0 (GeV/ c ) 2 . A neutron beam with a broad momentum spectrum was scattered from a liquid hydrogen target. The momenta and scattering angles of the forward-scattered protons were measured by a spark-chamber magnet spectrometer. The flight times and scattering angles of the recoil neutrons were measured by a bank of thick scintillation counters. The efficiencies of the neutron counters were determined in a separate measurement. Absolute normalization of the data was obtained from a measurement of the diffraction dissociation of neutrons from carbon nuclei. Differential cross sections, based on ∼ 23 000 events, are presented for 9 different momenta. The shape of the differential cross sections and the momentum dependence are examined in detail.

9 data tables

No description provided.

No description provided.

No description provided.

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Neutron-Proton Charge Exchange Scattering from 9-GeV/c to 23-GeV/c

Bohmer, V. ; Engler, J. ; Flauger, W. ; et al.
Nucl.Phys.B 110 (1976) 205-213, 1976.
Inspire Record 108523 DOI 10.17182/hepdata.35731

The differential cross sections for neutron-proton charge-exchange scattering have been measured with high statistics in the region of momentum transfer squared 0.002 < | t | ⩽ 0.400 (GeV/ c ) 2 and for incident neutron momenta 9 < p ⩽ 23 GeV/ c .

1 data table

No description provided.


Neutron-Proton Charge-Exchange Scattering from 22-GeV/c to 65-GeV/c

Babaev, A. ; Brachman, E. ; Eliseev, G. ; et al.
Nucl.Phys.B 110 (1976) 189-204, 1976.
Inspire Record 100178 DOI 10.17182/hepdata.35776

The differential cross sections for neutron-proton elastic charge-exchange scattering have been measured with a two-arm technique for incident neutron momenta between 22 and 65 GeV/ c and for values of the momentum transfer squared between 0.002 and 0.8 (GeV/ c ) 2 . The sharp forward peak observed previously at lower energies is also present at momenta up to 65 GeV/ c ; however the s dependence of the cross section is slowing down.

9 data tables

No description provided.

No description provided.

No description provided.

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Neutron-proton differential cross-section measurements for En from 28 to 75 MeV

Benck, S. ; Slypen, I. ; Meulders, J-P. ; et al.
Nucl.Phys.A 615 (1997) 220-228, 1997.
Inspire Record 459311 DOI 10.17182/hepdata.36360

Experimental measurements of differential cross-sections for neutron-proton scattering are reported for 12 incident neutron energies between 28 and 75 MeV. Data are compared with predictions of different theoretical models and with other experimental results.

6 data tables

No description provided.

No description provided.

No description provided.

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MEASUREMENT OF DEPOLARIZATION PARAMETERS D IN CHARGE EXCHANGE n p SCATTERING AT 600-MeV

Bagaturiya, Yu.Sh. ; Kazarinov, Yu.M. ; Kazarinov, M.Yu. ; et al.
Sov.J.Nucl.Phys. 33 (1981) 659, 1981.
Inspire Record 160829 DOI 10.17182/hepdata.9878

None

4 data tables

DATA AVERAGED FOR TWO DIRECTIONS OF TARGET POLARIZATION.

No description provided.

No description provided.

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N p Charge Exchange Scattering at Fermilab

Barton, H.R., Jr. ; Reay, N.W. ; Reibel, K. ; et al.
Phys.Rev.Lett. 37 (1976) 1656, 1976.
Inspire Record 112288 DOI 10.17182/hepdata.21058

We have measured the neutron-proton charge-exchange differential cross section in the momentum interval 60 to 300 GeV/c, with squared four-momentum transfers 0.002 to 0.8 (GeV/c)2. Independent of incident momentum, the data are characterized by a sharp forward peak of width 0.02 (GeV/c)2, followed by a shoulder and gentler falloff at higher momentum transfers.

1 data table

No description provided.