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Production of fast deuterons in proton nucleus interactions at 2.5-GeV to 9.2-GeV.

Safronov, G.A. ; Baranov, M.V. ; Voronin, S.V. ; et al.
Sov.J.Nucl.Phys. 47 (1988) 966-969, 1988.
Inspire Record 272212 DOI 10.17182/hepdata.17350

None

2 data tables
Table 1

No description provided.

Table 2

No description provided.


SPECTRA OF DEUTERONS EMITTED WITH LARGE TRANSVERSAL MOMENTA IN COLLISIONS OF 9-GeV/c DEUTERONS WITH HYDROGEN, DEUTERIUM AND CARBON NUCLEI

Azhgirei, L.S. ; Vzorov, I.K. ; Zhmyrov, V.N. ; et al.
Sov.J.Nucl.Phys. 48 (1988) 1058, 1988.
Inspire Record 261915 DOI 10.17182/hepdata.17354

None

3 data tables
Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.


Elastic p d scattering at small angles in the energy range 700-MeV to 1000-MeV.

Velichko, G.N. ; Vorobev, A.A. ; Grebenyuk, O.G. ; et al.
Sov.J.Nucl.Phys. 47 (1988) 755-759, 1988.
Inspire Record 273536 DOI 10.17182/hepdata.17377

None

4 data tables
Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.

More…

Mass-number dependence of proton, pi+, and K+ production in interactions between 10.1-GeV/c protons and nuclei.

Sibirtsev, A.A. ; Baranov, M.V. ; Voronin, S.V. ; et al.
Sov.J.Nucl.Phys. 47 (1988) 662-664, 1988.
Inspire Record 272924 DOI 10.17182/hepdata.17411

None

2 data tables
Table 1

No description provided.

Table 2

No description provided.


PION AND KAON PRODUCTION IN COLLISIONS OF RELATIVISTIC NUCLEI WITH AN ENERGY OF 3.65-GEV/NUCLEON

Kurepin, A.B. ; Pantuev, V.S. ; Filippov, S.N. ;
JETP Lett. 47 (1988) 17-22, 1988.
Inspire Record 271432 DOI 10.17182/hepdata.16889

None

1 data table
Table 1

No description provided.


OBSERVATION OF SLOW PION PRODUCTION IN NUCLEUS NUCLEUS INTERACTIONS

Dubinina, A.I. ; Kolganova, E.D. ; Pozharova, E.A. ; et al.
JETP Lett. 48 (1988) 251-253, 1988.
Inspire Record 271948 DOI 10.17182/hepdata.16886

None

4 data tables
Table 1

BEAM NUCLEUS ARE MIXTURE OF NE AND MG.

Table 2

BEAM NUCLEUS ARE MIXTURE OF NE AND MG.

Table 3

BEAM NUCLEUS ARE MIXTURE OF NE AND MG.

More…

DETERMINATION OF THE PROBABILITY FOR THE DECAY RHO0 ---> MU+ MU-

Antipov, Yu.M. ; Batarin, V.A. ; Bezzubov, V.A. ; et al.
JETP Lett. 48 (1988) 561-565, 1988.
Inspire Record 271950 DOI 10.17182/hepdata.16898

None

2 data tables
Table 1

No description provided.

Table 2

No description provided.


Electromagnetic Dissociation for High $Z$ Projectiles and at Ultrarelativistic Energies

Hill, J.C. ; Wohn, F.K. ; Winger, J.A. ; et al.
Phys.Rev.Lett. 60 (1988) 999-1001, 1988.
Inspire Record 264182 DOI 10.17182/hepdata.20156

Experiments to determine the characteristics of electromagnetic dissociation (ED) has been extended to high projectile charge and ultrarelativistic energies using La139 and O16 projectiles on Au197 targets. The gross features are reproduced in a Weizsäcker-Williams calculation but significant systematic deviations appear. The results are used as a guide in extending the calculations to the regime of energies and projectiles expected for planned heavy-ion colliders where Ed effects should comprise a major fraction of the total cross section.

2 data tables
Table 1

ESTIMATED CROSS SECTION OF THIS REACTION FROM ELECTROMAGNETIC DISSOCIATION IS 1.99+-.12 B.

Table 2

ESTIMATED CROSS SECTION OF THIS REACTION FROM ELECTROMAGNETIC DISSOCIATION IS .28+-.03 B AND .44+-.04 AT 60 AND 200 GEV/N,RESPECTIVELY.


Detector for the Antiproton Annihilation

Kuzichev, V.F. ;
ITEP-88-112, 1988.
Inspire Record 1498393 DOI 10.17182/hepdata.75414

None

1 data table
Table 1

No description provided.


rivet Analysis
Study of the Reaction $e^+ e^- \to K^+ K^-$ in the Energy Range 1350 $\le \sqrt{s} \le$ 2400-{MeV}

The DM2 collaboration Bisello, D. ; Busetto, G. ; Castro, A. ; et al.
Z.Phys.C 39 (1988) 13, 1988.
Inspire Record 262690 DOI 10.17182/hepdata.15622

Thee+e−→K+K− cross section has been measured from about 750 events in the energy interval\(1350 \leqq \sqrt s\leqq 2400 MeV\) with the DM2 detector at DCI. TheK± form factor |FF±| cannot be explained by the ρ, ω, ϕ and ρ′(1600). An additional resonant amplitude at 1650 MeV has to be added as suggested by a previous experiment.

2 data tables
Table 1

No description provided.

Table 2

No description provided.