High p(T) inclusive hadron production in pi- p collisions at 40-GeV and angles 49-degrees <= theta(cm) <= 93-degrees

Turchanovich, L.K. ; Abramov, V.V. ; Baldin, B.Yu. ; et al.
Phys.Atom.Nucl. 56 (1993) 1367-1377, 1993.
Inspire Record 356443 DOI 10.17182/hepdata.40547

None

6 data tables

Only statistical errors are given.

Only statistical errors are given.

Only statistical errors are given.

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Inclusive neutral pion production at forward angles at 4.5-GeV/c per nucleon in nucleus nuclei reactions

Abraamian, Kh.U. ; Izyurov, V.M. ; Khachaturian, M.N. ; et al.
Phys.Lett.B 323 (1994) 1-6, 1994.
Inspire Record 342328 DOI 10.17182/hepdata.39401

Distributions for transverse momentum P ⊥ and cumulative number X of inclusive neutral pions are measured with a lead glass calorimeter in α +C→ π 0 +x and α +Cu→ π 0 +x reactions at 4.5 GeV/ c per nucleon. The target-mass dependence for π 0 production is presented.

4 data tables

No description provided.

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CUMULATIVE NUMBER XL IS EQUAL TO: XL=(2*M(N)*E(PI0)-M(PI0)**2)/ (2*(E(N)*M(N)-E(N)*E(PI0)-M(N)**2+P(N)*P(PI0)*COS(THETA(PI0))).

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Cross-sections of backward proton production in 40-GeV/c pi- (K-, anti-p) A interactions

Antipov, Yu.M. ; Batarin, V.A. ; Bezzubov, V.A. ; et al.
Nucl.Phys.A 536 (1992) 637-647, 1992.
Inspire Record 337176 DOI 10.17182/hepdata.36704

The inclusive cross sections of backward proton production in π − ( K − , p ) -Be, Al, Cu, Pb interactions at 40 GeV/ c are presented. Protons have been detected in the angular range 150°–165° and kinetic energy region 0.1–0.3 GeV. The invariant cross-section ratios for various beam particles are independent of the values of kinetic energy and of the nuclear target type: 〈ƒ K − /ƒ π − 〉= 0.87 ± 0.03 stat ± 0.03 syst , 〈ƒ p /ƒ π − 〉 = 1.82 ± 0.10 stat ± 0.05 syst . The A -dependence of the cross-section slope parameter for A ⩾27 is less than ∼2%.

22 data tables

CYCLE N1.

CYCLE N1.

CYCLE N1.

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Cumulative production of pi- mesons in pi C interactions at 40-GeV/c

Baatar, Ts. ; Batsaikhan, Ts. ; Ivanovskaya, I.A. ; et al.
Sov.J.Nucl.Phys. 52 (1990) 504-508, 1990.
Inspire Record 299082 DOI 10.17182/hepdata.38727

None

7 data tables

HERE XL IS CUMULATIVE NUMBER, DEFINED AS FOLLOWS: (E-PL)/M(NUCLEON). THE DISTRIBUTION (1/N)*D(N)/D(XL) WAS FITTED BY THE SUM: CONST(1)* EXP(-SLOPE(1)*XL)+CONST(2)*EXP(-SLOPE(2)*XL).

HERE XL IS CUMULATIVE NUMBER, DEFINED AS FOLLOWS: (E-PL)/M(NUCLEON). THE DISTRIBUTION (XL/N)*D(N)/D(XL) WAS FITTED BY THE SUM: CONST(1)* EXP(-SLOPE(1)*XL)+CONST(2)*EXP(-SLOPE(2)*XL).

HERE XL IS CUMULATIVE NUMBER, DEFINED AS FOLLOWS: (E-PL)/M(NUCLEON).

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Subthreshold anti-proton production in nucleon nucleus and nucleus-nucleus collisions

Baldin, A.A. ; Gavrilov, Yu.K. ; Guber, F.F. ; et al.
Nucl.Phys.A 519 (1990) 407C-411C, 1990.
Inspire Record 306204 DOI 10.17182/hepdata.36821

New experimental data on antiproton production by carbon and deutron ions on copper and carbon nuclei at 3.65 GeV/nucleon and by proton at 3.65–8.1 GeV incident energy were obtained. Production angle is 24° and antiproton momentum is 0.8 GeV/c in the laboratory system.

5 data tables

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Cumulative A(1232,P33) Production in p A Interactions at 7.5 GeV/c

Vorobev, L.S. ;
ITEP-90-5, 1990.
Inspire Record 1395347 DOI 10.17182/hepdata.40035

None

3 data tables

No description provided.

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RESULTS OF ELECTRONIC EXPERIMENTS IN STUDYING THE REACTION alpha (pi+-, p) + A (C, Al, Cu, Cd, Pb) ---> LAMBDA0 + X

Vorobev, L.S. ; Gavrilov, V.B. ; Goryainov, N.A. ; et al.
ITEP-89-27, 1989.
Inspire Record 278858 DOI 10.17182/hepdata.40114

None

26 data tables

No description provided.

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PRODUCTION OF SOFT PIONS IN H A INTERACTIONS

Vorobev, L.S. ; Gavrilov, V.B. ; Goryainov, N.A. ; et al.
JETP Lett. 49 (1989) 670-674, 1989.
Inspire Record 287792 DOI 10.17182/hepdata.16848

None

2 data tables

No description provided.

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EMISSION OF RIGID GAMMA QUANTA IN pi- Xe INTERACTIONS AT 3.5-GeV/c

Abdurakhimov, A.U. ; Okhrimenko, L.S. ; Slowinski, B. ;
JINR-P1-88-903, 1988.
Inspire Record 270995 DOI 10.17182/hepdata.38832

None

3 data tables

No description provided.

INDEPENDENTLY OF THE NUMBER OF PI0 PRODUCED IN THE REACTION.

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