CHARGED PARTICLE MULTIPLICITY IN K+ p INTERACTIONS AT 70-GeV/c

Chliapnikov, P.V. ; Fenyuk, A.B. ; Gritsaenko, I.A. ; et al.
1984.
Inspire Record 201293 DOI 10.17182/hepdata.40967
2 data tables

No description provided.

No description provided.


Polarization in pi--p Scattering between 500 and 940 Mev

Beall, E.F. ; Cork, B. ; Murphy, P.G. ; et al.
Phys.Rev. 126 (1962) 1554-1560, 1962.
Inspire Record 944982 DOI 10.17182/hepdata.26812
10 data tables

No description provided.

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Experimental Study of the Magnetic Structure of the Neutron

Friedman, J.I. ; Kendall, H.W. ; Gram, P.A.M. ;
Phys.Rev. 120 (1960) 992-999, 1960.
Inspire Record 944988 DOI 10.17182/hepdata.26815
7 data tables

No description provided.

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Photoproduction of Negative and Positive Pions from Deuterium for Photon Energies 500 to 1000 Mev

Neugebauer, Gerry ; Wales, Walter ; Walker, R.L. ;
Phys.Rev. 119 (1960) 1726-1735, 1960.
Inspire Record 47757 DOI 10.17182/hepdata.26818
7 data tables

No description provided.

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Photoproduction of pi0 Mesons from Hydrogen in the Region 900 to 1200 Mev

Jackson, H.E. ; DeWire, J.W. ; Littauer, R.M. ;
Phys.Rev. 119 (1960) 1381-1384, 1960.
Inspire Record 944989 DOI 10.17182/hepdata.26849
1 data table

No description provided.


Angular Distributions of Photopions from Hydrogen

Knapp, Edward A. ; Kenney, Robert W. ; Perez-Mendez, Victor ;
Phys.Rev. 114 (1959) 605-611, 1959.
Inspire Record 944992 DOI 10.17182/hepdata.26850
2 data tables

No description provided.

No description provided.


A Measurement of Direct Photon Production at Large P(T) at the CERN ISR

Diakonou, M. ; Kourkoumelis, C. ; Resvanis, L.K. ; et al.
Phys.Lett. B91 (1980) 296-300, 1980.
Inspire Record 152520 DOI 10.17182/hepdata.27234
1 data table

No description provided.


Characteristics of J/psi and Upsilon production at the CERN intersecting storage rings

Kourkoumelis, C. ; Resvanis, L. ; Filippas, T.A. ; et al.
Phys.Lett. B91 (1980) 481-486, 1980.
Inspire Record 152744 DOI 10.17182/hepdata.27235
2 data tables

No description provided.

UPSILON HERE = UPSILON+UPSILON PRIME.


Production of Pions and Light Fragments at Large Angles in High-Energy Nuclear Collisions

Nagamiya, S. ; Lemaire, M.C. ; Moller, E. ; et al.
Phys.Rev. C24 (1981) 971-1009, 1981.
Inspire Record 169971 DOI 10.17182/hepdata.26341

Inclusive cross sections for production of π+, π−, p, d, H3, He3, and He4 have been measured at laboratory angles from 10° to 145° in nuclear collisions of Ne + Naf, Ne + Cu, and Ne + Pb at 400 MeV/nucleon, C + C, C + Pb, Ne + NaF, Ne + Cu, Ne + Pb, Ar + KCl, and Ar + Pb at 800 MeV/nucleon, and Ne + NaF and Ne + Pb at 2.1 GeV/nucleon. The production of light fragments in proton induced collisions at beam energies of 800 MeV and 2.1 GeV has also been measured in order to allow us to compare these processes. For equal-mass nuclear collisions the total integrated yields of nuclear charges are well explained by a simple participant-spectator model. For 800 MeV/nucleon beams the energy spectra of protons at c.m. 90° are characterized by a "shoulder-arm" type of spectrum shape with an exponential falloff at high energies, whereas those of pions are of a simple exponential type. The inverse of the exponential slope, E0, for protons is systematically larger than that for pions. This value of E0 is larger for heavier-mass projectiles and targets. It also increases monotonically with the beam energy. The angular anisotropy of protons is larger than that of pions. The yield ratio of π− to total nuclear charge goes up with the beam energy, whereas the yields of composite fragments decrease. The ratio of low-energy π− to π+, as well as that of H3 to He3, is larger than the neutron to proton ratio of the system. The spectrum shape of the composite fragments with mass number A is explained very well by the Ath power of the observed proton spectra. The sizes of the interaction region are evaluated from the observed coalescence coefficients. The radius obtained is typically 3-4 fm. The yield ratio of composite fragments to protons strongly depends on the projectile and target masses and the beam energy, but not on the emission angle of the fragments. These results are compared with currently available theoretical models. NUCLEAR REACTIONS Ne + NaF, Ne + Cu, Ne + Pb, EA=400 MeV/nucleon; C + C, C + Pb, Ne + NaF, Ne + Cu, Ne + Pb, Ar + KCl, Ar + Pb, EA=800 MeV/nucleon; Ne + NaF, Ne + Pb, EA=2100 MeV/nucleon; p + C, p+ NaF, p + KCl, p + Cu, p + Pb, E=800 MeV; p + C, p + NaF, p + KCl, p + Cu, p + Pb, E=2100 MeV; measured σ(p,θ) for π+, π−, p, d, H3, He3, and He4.

5 data tables

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Spectra of p, d, and t from relativistic nuclear collisions

Sandoval, A. ; Gutbrod, H.H. ; Meyer, W.G. ; et al.
Phys.Rev. C21 (1980) 1321-1343, 1980.
Inspire Record 147669 DOI 10.17182/hepdata.26366

Inclusive energy spectra of protons, deuterons, and tritons were measured with a telescope of silicon and germanium detectors with a detection range for proton energies up to 200 MeV. Fifteen sets of data were taken using projectiles ranging from protons to Ar40 on targets from Al27 to U238 at bombarding energies from 240 MeV/nucleon to 2.1 GeV/nucleon. Particular attention was paid to the absolute normalization of the cross sections. For three previously reported reactions, He fragment cross sections have been corrected and are presented. To facilitate a comparison with theory the sum of nucleonic charges emitted as protons plus composite particles was estimated and is presented as a function of fragment energy per nucleon in the interval from 15 to 200 MeV/nucleon. For low-energy fragments at forward angles the protons account for only 25% of the nucleonic charges. The equal mass Ar40 plus Ca systems were examined in the center of mass. Here at 0.4 GeV/nucleon Ar40 plus Ca the proton spectra appear to be nearly isotropic in the center of mass over the region measured. Comparisons of some data with firestreak, cascade, and fluid dynamics models indicate a failure of the first and a fair agreement with the latter two. In addition, associated fast charged particle multiplicities (where the particles had energies larger than 25 MeV/nucleon) and azimuthal correlations were measured with an 80 counter array of plastic scintillators. It was found that the associated multiplicities were a smooth function of the total kinetic energy of the projectile. NUCLEAR REACTIONS U(Ne20,X), EA=240 MeV/nucleon; U(Ar40,X), Ca(Ar40,X), U(Ne20,X), Au(Ne20,X), Ag(Ne20,X), Al(Ne20,X), U(He4,X), Al(He4,X), EA=390 MeV/nucleon; U(Ar40,X), Ca(Ar40,X), U(Ne20,X), U(He4,X), U(p,X), EA=1.04 GeV/nucleon; U(Ne20,X), EA=2.1 GeV/nucleon; measured σ(E,θ), X=p,d,t.

5 data tables

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Inclusive $\pi^0$ Electroproduction in the Deep Inelastic Region

McPharlin, T.P. ; Caldwell, David O. ; Cumalat, John P. ; et al.
Phys.Lett. B90 (1980) 479-484, 1980.
Inspire Record 143042 DOI 10.17182/hepdata.27245
4 data tables

No description provided.

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Photoproduction of Neutral Pions at Energies 500 to 940 Mev

Vette, J.I. ;
Phys.Rev. 111 (1958) 622-631, 1958.
Inspire Record 944995 DOI 10.17182/hepdata.26859
1 data table

No description provided.


Photoproduction of pi+ Mesons from Hydrogen in the Region 350-900 Mev

Heinberg, M. ; McClelland, W.M. ; Turkot, F. ; et al.
Phys.Rev. 110 (1958) 1211-1212, 1958.
Inspire Record 46812 DOI 10.17182/hepdata.26860
1 data table

No description provided.


Polarization and Differential Cross Sections in Proton-Proton and Proton-Nucleus Scatterings at 725 MeV

McManigal, Paul G. ; Eandi, Richard D. ; Kaplan, Selig N. ; et al.
Phys.Rev. 137 (1965) B620-B629, 1965.
Inspire Record 49431 DOI 10.17182/hepdata.26687

The polarization and angular distribution of protons scattered from protons, helium, beryllium, carbon, aluminum, calcium, iron, and tantalum were measured as functions of angle at 725 MeV. A variation of the usual double-elastic-scattering method was used, in that the sense of the first scattering angle was reversed in finding asymmetries, rather than the second angle. Energy analysis of the scattered beam was accomplished by means of a 102-degree magnetic spectrometer allowing a total resolution of ±10 MeV. The data were fitted with an optical model. In the proton-nucleus scattering the polarization reaches a maximum value of about 40% at angles less than the diffraction minimum. Results in proton-proton scatterings are more interesting; however, because of an uncertainty in the analyzing power of carbon, a definite statement cannot be made. One can say, however, that either the polarization in proton-proton scatterings is above 50% at this energy or the analyzing power of carbon at 6 deg and 600 MeV is more than 40%, which is considerably greater than the 30% measured at 725 MeV.

7 data tables

No description provided.

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Photoproduction of Neutral Pions at Energies 600 to 800 Mev

Worlock, R.M. ;
Phys.Rev. 117 (1960) 537-543, 1960.
Inspire Record 944990 DOI 10.17182/hepdata.26862
3 data tables

No description provided.

No description provided.

No description provided.


Photoproduction of Low-Energy Charged Pions from Deuterium

Burq, J.P. ; Walker, J.K. ;
Phys.Rev. 132 (1963) 447-454, 1963.
Inspire Record 944972 DOI 10.17182/hepdata.26772
1 data table

No description provided.


Proton-Proton Elastic Scattering Involving Large Momentum Transfers

Cocconi, G. ; Cocconi, V.T. ; Krisch, A.D. ; et al.
Phys.Rev. 138 (1965) B165-B172, 1965.
Inspire Record 49634 DOI 10.17182/hepdata.26688

Twenty-nine proton-proton differential elastic cross sections for lab momenta p0 from 11 to 31.8 BeV/c, at four-momentum transfers squared, −t, from 2.3 to 24.4 (BeV/c)2, have been measured at the Brookhaven alternating gradient synchrotron. The circulating proton beam impinged upon a thin CH2 internal target. Both scattered protons from p−p elastic events were detected by scintillation-counter telescopes which were placed downstream from deflection magnets set at the appropriate angles to the incident beam. The angular correlation of the protons, their momenta, and the coplanarity of the events were determined by the detection system. The results show that at high momentum transfers the differential cross section, dσdt, depends strongly upon the energy; for −t=10 (BeV/c)2, the value of dσdt at p0=30 BeV/c is smaller by a factor∼1000 than at p0=10 BeV/c. At all energies, dσdt falls rapidly with increasing |t| for scattering angles up to about 65° (c.m.), while in the range from 65 to 90° the cross section falls only by a factor of about 2. The smallest cross section measured was 9×10−37 cm2 sr−1 (c.m.), at p0=31.8 BeV/c and −t=20.4 (BeV/c)2; this is about 3×10−12 of the zero-degree cross section at the same energy.

1 data table

'1'. '2'.


pi--p Elastic Scattering at 1.44 Bev

Chretien, M. ; Leitner, J. ; Samios, N.P. ; et al.
Phys.Rev. 108 (1957) 383-389, 1957.
Inspire Record 45962 DOI 10.17182/hepdata.26863
1 data table

No description provided.


Absolute Positive Pion Photoproduction Cross Sections from Hydrogen

Walker, R.J. ; Palfrey, T.R. ; Haxby, R.O. ; et al.
Phys.Rev. 132 (1963) 2656-2663, 1963.
Inspire Record 944973 DOI 10.17182/hepdata.26773
1 data table

No description provided.


Proton form factors from elastic electron-proton scattering

Janssens, T. ; Hofstadter, R. ; Hughes, E.B. ; et al.
Phys.Rev. 142 (1966) 922-931, 1966.
Inspire Record 49127 DOI 10.17182/hepdata.26698
27 data tables

Axis error includes +- 2./2. contribution (RANDOM ERROR).

Axis error includes +- 2./2. contribution (RANDOM ERROR).

Axis error includes +- 2./2. contribution (RANDOM ERROR).

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Elastic Proton-Proton Scattering at 2.24, 4.40, and 6.15 Bev

Cork, Bruce ; Wenzel, William A. ; Causey, Charles W. ;
Phys.Rev. 107 (1957) 859-867, 1957.
Inspire Record 944998 DOI 10.17182/hepdata.26883
1 data table

'ALL'.


Photoproduction of Neutral Pions from Hydrogen at Forward Angles from 240 to 480 Mev

McDonald, W.S. ; Peterson, V.Z. ; Corson, D.R. ;
Phys.Rev. 107 (1957) 577-585, 1957.
Inspire Record 48187 DOI 10.17182/hepdata.26895
1 data table

Axis error includes +- 7.3/7.3 contribution.


Photoproduction of Single Neutral Pions from Hydrogen at Energies 0.6 to 1.2 BeV

Diebold, R. ;
Phys.Rev. 130 (1963) 2089-2097, 1963.
Inspire Record 944976 DOI 10.17182/hepdata.26774
1 data table

No description provided.


Photoproduction of pi0 Mesons from Hydrogen at 500-900 Mev

Stein, P.C. ; Rogers, K.C. ;
Phys.Rev. 110 (1958) 1209-1211, 1958.
Inspire Record 944996 DOI 10.17182/hepdata.26898
1 data table

No description provided.


High-Energy Proton Scattering from Carbon and Deuterium

Cocconi, G. ; Diddens, A.N. ; Lillethun, E. ; et al.
Phys.Rev. 126 (1962) 277-278, 1962.
Inspire Record 944981 DOI 10.17182/hepdata.26781

The momentum spectra of protons scattered from carbon and deuterium at angles close to 60 mrad and for incident proton momenta between 12 and 27 Gev/c have been measured. The data show good agreement with calculations based on plural quasi-elastic proton-nucleon scattering within the nucleus.

2 data tables

No description provided.

No description provided.