Distler, M.O.
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K0(L) p Charge Exchange Scattering from 550-MeV/c to 1000-MeV/c

Edelstein, R.M. ; Fisk, H.E. ; Joseph, P. ; et al.
Phys.Rev.D 14 (1976) 702-707, 1976.
Inspire Record 115726 DOI 10.17182/hepdata.24674

Employing a neutral kaon beam at the Argonne Zero Gradient Synchrotron, a high-resolution magnetic spectrometer, and a neutron detector, differential cross sections have been obtained in the forward direction [0.045<|t|<0.18 (GeV/c)2] for the reaction KL0p→K+n. Previous studies of the time-reversed process in deuterium, K+d→K0p(p), have not yielded direct cross-section measurements in the forward direction because there is an inhibition of the non-spin-flip process in deuterium due to the Pauli exclusion principle. Nevertheless, our data are in agreement with the extracted free-neutron cross sections of deuterium studies as determined from the impulse and closure approximations.

3 data tables
Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.


MEASUREMENT OF K0 TOTAL CROSS-SECTIONS ON NUCLEI. (IN RUSSIAN)

Berezin, V.M. ; Bogdanov, E.T. ; Vishnevsky, M.E. ; et al.
Yad.Fiz. 43 (1986) 358-365, 1986.
Inspire Record 231531 DOI 10.17182/hepdata.17514

None

1 data table
Table 1

Axis error includes +- 1/1 contribution (DUE TO BACKGROUND).


Search for an H dibaryon

Alekseev, A.N. ; Berezin, V.M. ; Bogdanov, E.T. ; et al.
Sov.J.Nucl.Phys. 52 (1990) 1016-1018, 1990.
Inspire Record 310395 DOI 10.17182/hepdata.17311

None

1 data table
Table 1

The cross-section obtained in the paper is the model dependent estimation.


Production of a Lambda K0 pair in neutron nucleus interactions

Alekseev, A.N. ; Berezin, V.M. ; Bogdanov, E.T. ; et al.
Sov.J.Nucl.Phys. 54 (1991) 977-981, 1991.
Inspire Record 326672 DOI 10.17182/hepdata.40022

None

1 data table
Table 1

ABSENT OF AN ABSOLUTE NEUTRON FLUX NORMALIZATION DIDN'T ALLOWED TO DEFINE THE CROSS-SECTION OF LAMBDA-K0-PARE PRODUCTION,SO IT WAS DEFINED THE RELATION OF CARBON AND CUPRUM CROSS-SECTION.


Polarization of Lambda hyperons in n C and n Pb interactions at initial momenta of 4-GeV/c to 10-GeV/c

Vishnevsky, M.E. ; Vlasova, M.O. ; Galanina, N.D. ; et al.
Phys.Atom.Nucl. 57 (1994) 985-990, 1994.
Inspire Record 383446 DOI 10.17182/hepdata.17186

None

2 data tables
Table 1

No description provided.

Table 2

No description provided.


Precise pion electroproduction in the p (e, e-prime pi+) n reaction at W = 1125-MeV

Blomqvist, K.I. ; Boeglin, W.U. ; Böhm, R. ; et al.
Z.Phys.A 353 (1996) 415-421, 1996.
Inspire Record 428951 DOI 10.17182/hepdata.16502

The reactione+p →> e+π++n at c.m. energyW=1125MeV and momentum transfer Q2=0.117GeV2/c2 has been measured. The transverse and longitudinal structure functions have been separated by varying the polarization of the virtual photon (Rosenbluth plot) with a 3 to 4% error. In addition the longitudinal-transverse interference term has been determined measuring the right-left asymmetry with an accuracy of 3%. The experimental data are compared to model calculations, and the sensitivity of the results to the axial and pion formfactors is discussed.

6 data tables
Table 1

Angle PHI(P=4) is the angle between the scattering plane (defined by 1 and 3 particles) and the reaction plane (defined by 4 and 5 particles).

Table 2

Angle PHI(P=4) is the angle between the scattering plane (defined by 1 and 3 particles) and the reaction plane (defined by 4 and 5 particles).

Table 3

Angle PHI(P=4) is the angle between the scattering plane (defined by 1 and 3 particles) and the reaction plane (defined by 4 and 5 particles).

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Features of leading Lambda hyperons produced by neutrons on nuclei.

Bulekov, O.V. ; Vishnevsky, M.E. ; Vlasova, M.O. ; et al.
Phys.Atom.Nucl. 61 (1998) 74-78, 1998.
Inspire Record 444255 DOI 10.17182/hepdata.17150

None

1 data table
Table 1

No description provided.


Virtual Compton scattering under pi0 threshold at Q**2 = 0.33-GeV**2: Preliminary results.

Roche, J. ; Bartsch, P. ; Berthot, J. ; et al.
Nucl.Phys.A 654 (1999) 547c-551c, 1999.
Inspire Record 500668 DOI 10.17182/hepdata.31223

We have measured the absolute unpolarized cross sections for photon electro-production off the proton ep → epγ with the Three-Spectrometer-Setup at MAMI at a momentum transfer q=600 MeV/c and a virtual photon polarization ɛ=0.62. The momentum q ′ of the outgoing real photon range from 33 to 111 MeV/c. We extracted two combinations of the recently introduced generalized polarizabilities [1,2].

1 data table
Table 1

No description provided.


Coherent pi0 threshold production from the deuteron at Q**2 = 0.1-GeV**2/c**2.

Ewald, Ingo ; Bartsch, Peter ; Baumann, Dagmar ; et al.
Phys.Lett.B 499 (2001) 238-244, 2001.
Inspire Record 534929 DOI 10.17182/hepdata.31443

First data on coherent threshold \pi^0 electroproduction from the deuteron taken by the A1 Collaboration at the Mainz Microtron MAMI are presented. At a four-momentum transfer of q^2=-0.1 GeV^2/c^2 the full solid angle was covered up to a center-of-mass energy of 4 MeV above threshold. By means of a Rosenbluth separation the longitudinal threshold s wave multipole and an upper limit for the transverse threshold s wave multipole could be extracted and compared to predictions of Heavy Baryon Chiral Perturbation Theory.

3 data tables
Table 1

Differential cross-section d(SIG(PI0))/d(OMEGA) is related to electron-deuteron one by the relation as follows: d(SIG)/d(OMEGA_e)/d(E_e)/d(OMEGA) = Gamma *d(SIG)/d(OMEGA), where the virtual photon flux is give by: Gamma = (alpha/2*pi**2) * (E'/E) * (k_gamma/Q2) / (1-epsilon). Here epsilon is transverse degree of polarization of the virtual photon. See article for details.

Table 2

Differential cross-section d(SIG(PI0))/d(OMEGA) is related to electron-deuteron one by the relation as follows: d(SIG)/d(OMEGA_e)/d(E_e)/d(OMEGA) = Gamma *d(SIG)/d(OMEGA), where the virtual photon flux is give by: Gamma = (alpha/2*pi**2) * (E'/E) * (k_gamma/Q2) / (1-epsilon). Here epsilon is transverse degree of polarizatiuon of the virtual photon. See article for details.

Table 3

Differential cross-section d(SIG(PI0))/d(OMEGA) is related to electron-deuteron one by the relation as follows: d(SIG)/d(OMEGA_e)/d(E_e)/d(OMEGA) = Gamma *d(SIG)/d(OMEGA), where the virtual photon flux is give by: Gamma = (alpha/2*pi**2) * (E'/E) * (k_gamma/Q2) / (1-epsilon). Here epsilon is transverse degree of polarizatiuon of the virtual photon. See article for details.


Polarization transfer in the He-4(e(pol.),e' p(pol.)H-3 reaction.

Dieterich, S. ; Bartsch, P. ; Baumann, D. ; et al.
Phys.Lett.B 500 (2001) 47-52, 2001.
Inspire Record 536853 DOI 10.17182/hepdata.31423

Polarization transfer in the 4He(e,e'p)3H reaction at a Q^2 of 0.4 (GeV/c)^2 was measured at the Mainz Microtron MAMI. The ratio of the transverse to the longitudinal polarization components of the ejected protons was compared with the same ratio for elastic ep scattering. The results are consistent with a recent fully relativistic calculation which includes a predicted medium modification of the proton form factor based on a quark-meson coupling model.

2 data tables
Table 1

No description provided.

Table 2

No description provided.