Single Particle Inclusive Spectra Resulting from the Collision of Relativistic Protons, Deuterons, alpha Particles, and Carbon Ions with Nuclei

Papp, James ;
PhD Thesis, 1975.
Inspire Record 98718 DOI 10.17182/hepdata.9305
20 data tables

No description provided.

No description provided.

No description provided.

More…

Yield of Secondary Particles at an Angle of 188-Mrad at the ITEP Synchrotron

Belikov, Yu.E. ; Buklei, A.E. ; Gavrilov, V.B. ; et al.
ITEP-31-1977, 1977.
Inspire Record 121163 DOI 10.17182/hepdata.40348

None

2 data tables

No description provided.

No description provided.


Pions with Maximum Momenta in Proton-Nuclei Interaction at 8.8-GeV/c

Bayukov, Yu.D. ; Efremenko, V.I. ; Fedorov, V.B. ; et al.
ITEP-49-1977, 1977.
Inspire Record 121162 DOI 10.17182/hepdata.40390

None

4 data tables

No description provided.

No description provided.

No description provided.

More…

Protons and pi- Generation at 188-Mrad in Proton-Nucleus Interaction for 9-GeV/c

Belikov, Yu.E. ; Buklei, A.E. ; Gavrilov, V.B. ; et al.
ITEP-50-1977, 1977.
Inspire Record 121158 DOI 10.17182/hepdata.40275

None

2 data tables

No description provided.

No description provided.


Pion Production by Protons on a Thin Beryllium Target at 6.4, 12.3, and 17.5 GeV/c Incident Proton Momenta

The E910 collaboration Chemakin, I. ; Cianciolo, V. ; Cole, B.A. ; et al.
Phys.Rev.C 77 (2008) 015209, 2008.
Inspire Record 755923 DOI 10.17182/hepdata.51393

An analysis of inclusive pion production in proton-beryllium collisions at 6.4, 12.3, and 17.5 GeV/c proton beam momentum has been performed. The data were taken by Experiment 910 at the Alternating Gradient Synchrotron at the Brookhaven National Laboratory. The differential $\pi^+$ and $\pi^-$ production cross sections ($d^2\sigma/dpd\Omega$) are measured up to 400 mRad in $\theta_{\pi}$ and up to 6 GeV/c in $p_{\pi}$. The measured cross section is fit with a Sanford-Wang parameterization.

16 data tables

Pion production cross section for 6.4 GeV incident protons.

Pion production cross section for 6.4 GeV incident protons.

Pion production cross section for 6.4 GeV incident protons.

More…

Experimental Data on Cumulative Production of Positive and Negative Kaons in p-Pb Interaction

Baldin, A.M. ; Bondarev, V.K. ; Ghiordanescu, N. ;
JINR-1-80-488, 1980.
Inspire Record 1189877 DOI 10.17182/hepdata.34057

Cross sections of cumulative K exp + and K exp - -meson production in the 200-1000 MeV kinetic energy range at 90 deg, 120 deg, 168 deg (l.c.s.) are measured. The ranges of kinetic energies and emission angles mean that, according to the hypothesis of cum ...

50 data tables
More…

Production of Cumulative Protons at Momenta 0.6-{GeV}/$c$ to 1.83-{GeV}/$c$

Boyarinov, S.V. ; Gerzon, S.A. ; Kats, M.M. ; et al.
Sov.J.Nucl.Phys. 46 (1987) 871, 1987.
Inspire Record 233179 DOI 10.17182/hepdata.40173

None

3 data tables

Large-angle production of charged pions by 3 GeV/c - 12.9 GeV/c protons on beryllium, aluminium and lead targets

The HARP collaboration Catanesi, M.G. ; Radicioni, E. ; Edgecock, R. ; et al.
Eur.Phys.J.C 54 (2008) 37-60, 2008.
Inspire Record 761543 DOI 10.17182/hepdata.51357

Measurements of the double-differential $\pi^{\pm}$ production cross-section in the range of momentum $100 \MeVc \leq p < 800 \MeVc$ and angle $0.35 \rad \leq \theta < 2.15 \rad$ in proton--beryllium, proton--aluminium and proton--lead collisions are presented. The data were taken with the HARP detector in the T9 beam line of the CERN PS. The pions were produced by proton beams in a momentum range from 3 \GeVc to 12.9 \GeVc hitting a target with a thickness of 5% of a nuclear interaction length. The tracking and identification of the produced particles was performed using a small-radius cylindrical time projection chamber (TPC) placed inside a solenoidal magnet. Incident particles were identified by an elaborate system of beam detectors. Results are obtained for the double-differential cross-sections at six incident proton beam momenta (3 \GeVc, 5 \GeVc, 8 \GeVc, 8.9 \GeVc (Be only), 12 \GeVc and 12.9 \GeVc (Al only)) and compared to previously available data.

54 data tables

Double-differential cross section for PI+ production from BE in the LAB system for PI+ polar angle from 0.35 to 0.55 radians.

Double-differential cross section for PI+ production from BE in the LAB system for PI+ polar angle from 0.55 to 0.75 radians.

Double-differential cross section for PI+ production from BE in the LAB system for PI+ polar angle from 0.75 to 0.95 radians.

More…

Inclusive soft pion production from 12.3-GeV/c and 17.5-GeV/c protons on Be, Cu and Au.

Chemakin, I. ; Cianciolo, V. ; Cole, B.A. ; et al.
Phys.Rev.C 65 (2002) 024904, 2002.
Inspire Record 561173 DOI 10.17182/hepdata.31363

Differential cross-sections are presented for the inclusive production of charged pions in the momentum range 0.1 to 1.2 GeV/c in interactions of 12.3 and 17.5 GeV/c protons with Be, Cu, and Au targets. The measurements were made by Experiment 910 at the Alternating Gradient Synchrotron in Brookhaven National Laboratory. The cross-sections are presented as a function of pion total momentum and production polar angle $\theta$ with respect to the beam.

25 data tables

The pion production cross section of P-AU interactions at 17.5 GeV incidentmomentum.

The pion production cross section of P-AU interactions at 17.5 GeV incidentmomentum.

The pion production cross section of P-AU interactions at 17.5 GeV incidentmomentum.

More…

Pion yield from 450-GeV/c protons on beryllium.

The SPY collaboration Ambrosini, G. ; Arsenescu, R. ; Bernier, K. ; et al.
Phys.Lett.B 425 (1998) 208-214, 1998.
Inspire Record 470999 DOI 10.17182/hepdata.49490

This paper reports on the charged pion production yields measured by the SPY/NA56 experiment for 450 GeV/c proton interactions on beryllium targets. The present data cover a secondary momentum range from 7 GeV/c to 135 GeV/c in the forward direction. An experimental accuracy ranging from 5 to 10%, depending on the beam momentum, has been achieved, limited mainly by the knowledge of the beam acceptance. These results will be relevant in the calculation of neutrino fluxes in present and future neutrino beams.

2 data tables

No description provided.

No description provided.