Spectra and correlations of Lambda and Lambda produced in 340-GeV/c Sigma -+C and 260-GeV/c n+C interactions

Adamovich, M.I. ; Alexandrov, Yu.A. ; Baranov, S.P. ; et al.
Phys.Rev.C 65 (2002) 042202, 2002.
Inspire Record 585235 DOI 10.17182/hepdata.25354

We have measured the production of strange baryons and antibaryons in 340-GeV/c Σ−+C and 260-GeV/c n+C interactions. The single xF distributions show the expected leading particle effect, and the single pt2 distributions show a distinct nonthermal behavior. The xF distributions of Λ-Λ pairs indicate two different phase space distributions for the two coincident baryons. On the other hand two Λ¯’s show identical distributions. Momentum conservation during the formation process may represent a significant source for the observed behavior.

4 data tables

Total inclusive LAMBDA and LAMBDABAR production cross sections for the SIGMA- beam on the Carbon target.

Total inclusive LAMBDA and LAMBDABAR production cross sections for the Neutron beam on the Carbon target.

Total inclusive LAMBDA LAMBDA and LAMBDABAR LAMBDABAR pair production crosssections for the SIGMA- beam on the Carbon target.

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Nuclear Compton scattering from 12C and bound-nucleon polarizabilities

Warkentin, B. J. ; Hornidge, D. L. ; Igarashi, R. ; et al.
Phys.Rev.C 64 (2001) 014603, 2001.
Inspire Record 557785 DOI 10.17182/hepdata.25395

Compton scattering cross sections from 12C have been measured at scattering angles of θγ=35°−150° using tagged photons of Eγ=84−105 MeV. Attempts to extract nucleon polarizabilities from the data were hampered by model ambiguities. These included uncertainties in the strength of the electric quadrupole and quasideuteron total photon absorption channels, and in the parametrizations of meson-exchange effects and nuclear form factors. These ambiguities led to large variations in the extracted values of the effective polarizabilities of the bound nucleon. Inelastic Compton scattering cross sections from the 4.44 MeV first-excited state were also obtained.

2 data tables

No description provided.

C12* is 4.44 MeV state.


Loss of memory of target nucleus deformation axis in heavy ion fusion fission

Hinde, D. J. ; Pan, W. ; Berriman, A. C. ; et al.
Phys.Rev.C 62 (2000) 024615, 2000.
Inspire Record 530771 DOI 10.17182/hepdata.25429

Fission fragment cross sections and angular anisotropies have been measured to high accuracy following fusion of 16O with the strongly deformed nucleus 182W, at bombarding energies spanning the fusion barrier region. Together with existing evaporation residue data, they show that at all the beam energies, the statistical transition state model adequately describes the fission properties measured. No significant evidence was found for a memory of the different configurations at fusion resulting from the target nucleus deformation, in contrast with previous measurements for deformed actinide nuclei.

1 data table

No description provided.


Determination of the γ - π - ρ coupling constant from the −/+ ratio for photoproduction from deuterium

Pine, J. ; Bazin, M. ;
Phys.Lett. 5 (1963) 168-170, 1963.
Inspire Record 1388798 DOI 10.17182/hepdata.27961

None

3 data tables

No description provided.

No description provided.

No description provided.


The Real Part of the Forward Scattering Amplitude in pi+- p Elastic Scattering Below 2-GeV/c

Baillon, P. ; Bricman, C. ; Eberhard, P. ; et al.
Phys.Lett.B 50 (1974) 387-390, 1974.
Inspire Record 89683 DOI 10.17182/hepdata.27947

The differential cross section for π ± p elastic scattering below 2 GeV/ c has been measured at small forward pion angles by an electronics experiment. The interference effects observed between the Coulomb and the nuclear interaction have been used to determine the magnitude and sign of the real parts of the π ± p forward scattering amplitude. The latter are compared to the values predicted by the dispersion relations.

7 data tables
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A measurement of elastic pion-proton scattering at 50 gev

Derevchekov, A.A. ; Golovin, N.I. ; Khodirev, Y.C. ; et al.
Phys.Lett.B 48 (1974) 367-370, 1974.
Inspire Record 95356 DOI 10.17182/hepdata.27998

We have measured elastic pion-proton scattering in a 50 GeV/ c π − beam at the 76 GeV proton synchrotron in Serpukhov. Data are presented for four-momenta transfer squared in the range 0.03 < t < 0.4 (GeV/ c ) 2 .

1 data table

SLOPE IS 9.1, +0.2, -0.4 GEV**-2 (INCLUDING SYSTEMATIC ERRORS).


Anti-proton helium-3 annihilation at 55-MeV/c

Bianconi, A. ; Bonomi, G. ; Bussa, M.P. ; et al.
Phys.Lett.B 492 (2000) 254-258, 2000.
Inspire Record 538722 DOI 10.17182/hepdata.27999

The p̄ 3 He annihilation cross section is measured for the first time in the momentum interval (50÷60) MeV/ c . About 9000 pictures collected by the Streamer Chamber Collaboration (PS179) at LEAR–CERN have been scanned. Six events are found, corresponding to σ ann =1850±700 mb. The result is compared to the set of measurements presently available in the region of low p̄ momentum.

1 data table

The mean beam momentum at the center of the fiducial volume = 55 MeV.


Differential cross-sections for anti-p p ---> pi- pi+, k- k+ between 0.8 and 2.4 gev/c

Eisenhandler, E. ; Gibson, W.R. ; Hojvat, C. ; et al.
Phys.Lett.B 47 (1973) 531-535, 1973.
Inspire Record 95394 DOI 10.17182/hepdata.28034

We present measurements from a spark chamber experiment of the differential cross-sections for p p → π − π + , K − K + at 20 momenta in the range 0.8–2.4 GeV/ c (c.m. energy 2.02 to 2.57 GeV). The c.m. angular range was −0.95 < cos θ ∗ < 0.95 . There are about 2000π − π + events and about 300 K − K + events at each momentum.

1 data table

ALL ANGLES.


Pionic fusion to a halo state, the d(alpha,Li-6*)pi0 reaction studied close to threshold.

Andersson, M. ; Bargholtz, C. ; Fransson, K. ; et al.
Phys.Lett.B 481 (2000) 165-170, 2000.
Inspire Record 529623 DOI 10.17182/hepdata.28018

The d( α , 6 Li ∗ 3.56 ) π 0 reaction has been studied at E c.m. =1.2 and 1.9 MeV above threshold with an alpha-particle beam incident on a deuterium cluster-jet target in CELSIUS. Complete differential cross sections were measured at both energies, integrated to σ =228±6+70 nb and 141±12+42 nb respectively. Observed large anisotropies are discussed in relation to the cluster structure of the 6 Li ∗ halo.

1 data table

The excited LI6* level has E=3.56 mev (at the highest beam energy the second T=1 state in LI6 at 5.37 mev is possible to populate).


Isospin resolved double pion production in the reaction p + d --> He-3 + 2pi.

Andersson, M. ; Bargholtz, C. ; Fransson, K. ; et al.
Phys.Lett.B 485 (2000) 327-333, 2000.
Inspire Record 532724 DOI 10.17182/hepdata.28016

Neutral and charged two-pion production in p+d→ 3 He+2 π reactions has been studied at CELSIUS at a proton beam energy of 477 MeV. The total cross section for double pion production is 0.22±0.03 μ b. The ratio of the cross sections for the production of charged pion pairs with isospin T =1 and T =0 was determined to be σ ( π + π − ; T =1)/ σ ( π + π − ; T =0)=1.4±0.4.

1 data table

(I=1, I=0) stands for isospin of PI+ PI- system.