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pi+ + d --> p + p reaction between 18-MeV and 44-MeV.

Pasyuk, E.A. ; Alexakhin, V.Yu. ; Gogolev, S.I. ; et al.
Phys.Rev.C 55 (1997) 1026-1032, 1997.
Inspire Record 425528 DOI 10.17182/hepdata.25740

A study of the reaction pi+ + d --> p + p has been performed in the energy range of 18 - 44 MeV. Total cross sections and differential cross sections at six angles have been measured at 15 energies with an energy increment of 1 - 2 MeV. This is the most systematic data set in this energy range. No structure in the energy dependence of the cross section has been observed within the accuracy of this experiment.

16 data tables
Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.

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Study of the pi0 pi0 eta-prime final state in anti-p p annihilation at rest

The Crystal Barrel collaboration Abele, A. ; Adomeit, J. ; Amsler, C. ; et al.
Phys.Lett.B 404 (1997) 179-186, 1997.
Inspire Record 457856 DOI 10.17182/hepdata.28292

A partial wave analysis of p̄p → π 0 π 0 η ′ has been performed using the η′ → π 0 π 0 η and η ′ → γγ decay modes. The data are dominated by an η ′ recoiling against the ( ππ ) S-wave. In addition, α 2 (1320) → η′π 0 is needed. There is evidence for contributions from α 0 (1450) → η′π 0 . The branching ratio of α 0 (1450) → η′π 0 with respect to ηπ 0 is consistent with the prediction of SU(3).

1 data table
Table 1

No description provided.


A comparison of pi+ and pi- total cross-sections of light nuclei near the 3-3 resonance

Wilkin, Colin ; Cox, C.R. ; Domingo, J.J. ; et al.
Nucl.Phys.B 62 (1973) 61-85, 1973.
Inspire Record 83895 DOI 10.17182/hepdata.32488

The total cross sections of 4 He, 6 Li, 7 Li, 9 Be, 12 C and 32 S for positive and negative pions have been measured in the energy range 80 to 260 MeV in a transmission experiment. Coulomb corrections were applied using real parts of the forward nuclear amplitudes as determined from dispersion relations. At the lower energies there remain large residual differences between the π + and π − scattering on the isoscalar nuclei. These can be largely understood in terms of the Coulomb distortion.

6 data tables
Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.

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Second generation leptoquark search in p anti-p collisions at S**(1/2) = 1.8-TeV

The D0 collaboration Abachi, S. ; Abbott, B. ; Abolins, M. ; et al.
Phys.Rev.Lett. 75 (1995) 3618-3623, 1995.
Inspire Record 397099 DOI 10.17182/hepdata.42373

We report on a search for second generation leptoquarks with the D\O\ detector at the Fermilab Tevatron $p\overline{p}$ collider at $\sqrt{s}$ = 1.8 TeV. This search is based on 12.7 pb$~{-1}$ of data. Second generation leptoquarks are assumed to be produced in pairs and to decay into a muon and quark with branching ratio $\beta$ or to neutrino and quark with branching ratio $(1-\beta)$. We obtain cross section times branching ratio limits as a function of leptoquark mass and set a lower limit on the leptoquark mass of 111 GeV/c$~{2}$ for $\beta = 1 $ and 89 GeV/c$~{2}$ for $\beta = 0.5 $ at the 95\%\ confidence level.

1 data table
Table 1

The cross section times branching ratios.


Measurements of the total cross-section for the scattering of polarized neutrons from polarized He-3

Keith, C.D. ; Gould, C.R. ; Haase, D.G. ; et al.
Phys.Rev.C 54 (1996) 477-486, 1996.
Inspire Record 433949 DOI 10.17182/hepdata.31350

Measurements of polarized-neutron–polarized−3He scattering are reported. The target consisted of cryogenically polarized solid He3, with thickness 0.04 atom/b and polarization ∼0.4. Polarized neutrons were produced via the H3(p→,n→)3He or H2(d→,n→)3He polarization-transfer reactions. The longitudinal and transverse total cross-section differences ΔσL and ΔσT were measured for incident neutron energies 2–8 MeV. The results are compared to phase-shift predictions based on four different analyses of n−3He scattering. The best agreement is obtained with a recent R-matrix analysis of A=4 scattering and reaction data, lending strong support to the He4 level scheme obtained in that analysis. Discrepancies with other phase-shift parametrizations of n−3He scattering exist, attributable in most instances to one or two particular partial waves. © 1996 The American Physical Society.

1 data table
Table 1

SIG(C=L-...) and SIG(C=T-...) correspond to longitudinal and transverse polarization, respectively.


Total photoabsorption cross-section for He-4 from 200-MeV to 800-MeV

MacCormick, M. ; Habermann, J. ; Ahrens, J. ; et al.
Phys.Rev.C 55 (1997) 1033-1038, 1997.
Inspire Record 457684 DOI 10.17182/hepdata.25723

The total photoabsorption cross section for 4He has been measured for the first time over a wide photon energy range (200 MeV<~Eγ<~800 MeV). By using the large acceptance detector DAPHNE at the tagged photon facility of the MAMI microtron in Mainz high precision results with small systematic errors were obtained. This measurement shows that 4He has a behavior similar to heavy nuclei and, in particular, a reduction of the cross section with respect to the lighter nuclei is found for Eγ>600 MeV.

1 data table
Table 1

No description provided.


The Search for heavy pentaquark exotic baryons with hidden strangeness in the p + N ---> (p Phi) + N and p + N ---> (Lambda (1520) K+) + N reactions at E(p) = 70-GeV

The SPHINX collaboration Dorofeev, V.A. ; Golovkin, S.V. ; Kozhevnikov, A.P. ; et al.
Phys.Atom.Nucl. 57 (1994) 227-237, 1994.
Inspire Record 385732 DOI 10.17182/hepdata.40688

None

2 data tables
Table 1

No description provided.

Table 2

The upper limits for production of EXOTIC-NUCLEON with narrow width (<50 MeV). Linear A-dependence of the cross section is assumed.


$\Lambda$ and $\bar{\Lambda}$ Polarization in $K^\pm p$ Interactions at 32-{GeV}/$c$

The French-Soviet & CERN-Soviet collaborations Faccini-Turluer, M.L. ; Barloutaud, R. ; Cochet, C. ; et al.
Z.Phys.C 1 (1979) 19, 1979.
Inspire Record 132913 DOI 10.17182/hepdata.19291

Data on Λ and\(\bar \Lambda \) polarization inK±p interactions at 32 GeV/c are presented. A comparison is made between the results of these two experiments as well as with the data at lower energies. The contribution of the different production mechanisms to the Λ(\(\bar \Lambda \)) polarization are discussed.

2 data tables
Table 1

Data are presented on figures only. DATA NOT ENCODED.

Table 2

No description provided.


Integral cross-sections for pi+ p interactions at low-energies

Friedman, E. ; Goldring, A. ; Wagner, G.J. ; et al.
Nucl.Phys.A 514 (1990) 601-612, 1990.
Inspire Record 296987 DOI 10.17182/hepdata.36853

Integral cross sections for the elastic scattering of π + by protons into angles greater than 20° or 30° (lab) have been measured by the beam-attenuation technique over the energy range of 45–126MeV. The measurements are aimed at providing independent checks on the absolute normalization of differential cross sections, where discrepancies exist between different data sets. Comparisons with predictions made with existing phase shifts show very good agreement with the dispersion-relation constrained phase shifts of the Karlsruhe group.

1 data table
Table 1

Two targets (C=THIN) and (C=THICK) are used.


Search for magnetic monopoles at the 70 gev iphe proton synchrotron

Gurevich, I.I. ; Khakimov, S.K. ; Martemyanov, V.P. ; et al.
Phys.Lett.B 38 (1972) 549-550, 1972.
Inspire Record 75823 DOI 10.17182/hepdata.28325

The result of a search for magnetic charged particles at 70 GeV IPHE proton synchrotron is presented. Using the ferromagnetic trap method the upper limit of the magnetic monopole production cross-section in proton-nucleon collisions was found to be α (95%) ⩾ × 10 −43 cm 2 .

1 data table
Table 1

No description provided.