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Semi-inclusive π0 multiplicity distributions for 2-14 charged prongs are obtained using a generating-function approach based on an expansion in terms of Mueller moments. The four-prong data require the explicit assumption of a two-component model. Under this assumption and the further assumption of no three-neutral-particle correlations, the total pion multiplicity is obtained. The total multiplicity shows peaking at even prongs, indicative of G-parity-conserving diffractive processes which dominate at lower multiplicities. The cross section for these processes is ∼4 mb.

1 data table

Table 1

TOTAL NO. EVENTS=21395.

TOTAL NEUTRON NUCLEUS CROSS-SECTIONS AT INTERMEDIATE-ENERGIES

Franz, J. ; Grotz, H.P. ; Lehmann, L. ; et al.

Nucl.Phys.A 490 (1988) 667-688, 1988.

Inspire Record 263460 DOI 10.17182/hepdata.37108

Total neutron cross sections have been measured for the nuclei Be, C, O, Al, V, Mn, Co, Cu, Ag, Ce, Ta, Pb, Bi and U at 22 energies from 160 MeV to 575 MeV by the transmission method. The energy region contains the threshold for pion production. Different parametrizations of the experimental results are discussed. A test of charge symmetry was obtained from the proton- and neutron-induced cross sections on C and O, yielding 〈 (σ p − σ n ) σ p 〉 = 0.0012 ± 0.0059 .

2 data tables

Table 1

No description provided.

Table 2

No description provided.

TOTAL, ELASTIC AND INCLUSIVE SINGLE DIFFRACTIVE CROSS-SECTIONS IN ALPHA-ALPHA COLLISIONS AT THE CERN INTERSECTING STORAGE RINGS

Lloyd Owen, D. ; Paternoster, G. ; Patricelli, S. ; et al.

Nucl.Phys.B 274 (1986) 685-706, 1986.

Inspire Record 227125 DOI 10.17182/hepdata.33694

We present measurements of the total interaction cross section and of the single-diffractive dissociation cross section in αα collisions at √ s = 126 GeV. The result obtained for the total cross section, σ tot = (315±18) mb, is a substantial improvement on the precision of earlier measurements. Earlier elastic data were re-analysed, incorporating, through the optical theorem, the present σ tot measurement, resulting in improved determinations of the forward slope, b − t <0.07 = (87±4) GeV −2 , and of the integrated elastic cross section, σ el = (58±6) mb. The single-diffractive differential cross section falls exponentially with momentum transfer at small values of t with a slope b sd = (19.3 ± 0.6) GeV −2 . The integrated single-diffractive cross section is σ sd = (16.6±2.5) mb. The topology of charged tracks resulting from the disintegration of the α in single-diffractive events reveals a two-component distribution. The cross section data are compared with multiple-scattering models.

2 data tables

Table 1

Total cross section by total rate method. Systematic errors included.

Table 2

Reanalysis using data from ISR experiments R-418, and R-807.

TRANSITION FORM-FACTOR OF THE VERTEX GAMMA P DELTA (1231) +. (IN RUSSIAN)

Akhmerov, R.V. ; Esaulov, A.S. ; Omelaenko, A.S. ; et al.

Yad.Fiz. 31 (1980) 156-166, 1980.

Inspire Record 157407 DOI 10.17182/hepdata.18229

None

4 data tables

Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.

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TRANSVERSAL MOMENTUM DISTRIBUTIONS OF pi0 MESONS PRODUCED IN THE pi- Xe INTERACTIONS AT 3.5-GeV/c

Ilina, A.N. ; Okhrimenko, L.S. ; Slowinski, B. ;

JINR-P1-82-543, 1982.

Inspire Record 180889 DOI 10.17182/hepdata.39128

None

1 data table

Table 1

No description provided.

TRANSVERSE SPIN DEPENDENCE OF THE P P TOTAL CROSS-SECTION DELTA sigma-t FROM 0.8-GEV/C TO 2.5-GEV/C

Madigan, W.P. ; Bell, D.A. ; Buchanan, J.A. ; et al.

Phys.Rev.D 31 (1985) 966-975, 1985.

Inspire Record 216906 DOI 10.17182/hepdata.23564

The difference ΔσT=σ(↓↑)-σ(↑↑) between the proton-proton total cross sections for protons in pure transverse-spin states, was measured at incident momenta 0.8 to 2.5 GeV/c in experiments performed at the Los Alamos Clinton P. Anderson Meson Physics Facility and the Argonne Zero Gradient Synchrotron. In agreement with other data, peaks were observed at center-of-mass energies of 2.14 and 2.43 GeV/c2, where D21 and G41 dibaryon resonances have been proposed.

2 data tables

Table 1

DATA FROM LAMPF EXPERIMENT.

Table 2

DATA FROM ARGONNE EXPERIMENT.