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Collaboration

BIS-2 1
WA89 1

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Phrases Reset

Cross Section 2
Inclusive 2
Integrated Cross Section 2
Single Differential Cross Section 2
Strange production 2
Transverse Momentum Dependence 2
Exclusive 1

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Reactions Reset

N C --> SIGMA(1385P13)+ X 2
N C --> SIGMA(1385P13)- X 2
N NUCLEUS --> SIGMA(1385P13)+ X 2
N NUCLEUS --> SIGMA(1385P13)- X 2
N C --> LAMBDA X 1
N C --> LAMBDABAR X 1
N C --> OMEGA- X 1
N C --> SIGMABAR(1385P13)+ X 1
N C --> XI(1530P13)0 X 1
N C --> XI- X 1

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Observables Reset

DSIG/DPT**2 2
POWER 2
SIG 2
DSIG/DXL 1
E*DSIG/DXL 1
SLOPE 1

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CM Energies (GeV)

0.0 ≤ √s < 1.0
1.0 ≤ √s < 2.0
2.0 ≤ √s < 5.0
5.0 ≤ √s < 10.0
10.0 ≤ √s < 100.0
100.0 ≤ √s < 1000.0
1000.0 ≤ √s < 7000.0
7000.0 ≤ √s < 8000.0
8000.0 ≤ √s < 13000.0
√s ≥ 13000.0

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Authors

Chudakov, E.A. 2
Adamovich, M.I. 1
Aleev, A.N. 1
Aleksandrov, Yu.A. 1
Arefev, V.A. 1
Balandin, V.P. 1
Baranov, S.P. 1
Barberis, D. 1
Beck, M. 1
Belousov, A.S. 1

A study of Sigma+-, Sigma*+- and anti-Sigma(1385)- production in the hyperon beam experiment WA89 at CERN

The WA89 collaboration Adamovich, M.I. ; Aleksandrov, Yu.A. ; Baranov, S.P. ; et al.

Eur.Phys.J.C 22 (2001) 255-267, 2001.

https://inspirehep.net/literature/570717 Inspire Record 570717 DOI 10.17182/hepdata.43263 https://doi.org/10.17182/hepdata.43263

None

26 data tables

Table 1

Total inclusive production cross sections for the SIGMA- beam on the Coppertarget.

Table 2

Total inclusive production cross sections for the SIGMA- beam on the Carbontarget.

Table 3

Total inclusive production cross sections per nucleon for the SIGMA- beam, and the exponent in the cross section parametrization of the form A**POWER.

Table 4

Inclusive SIGMA(1660) production cross sections, times the < LAMBDA PI> branching ratio, in the XL range 0.3 to 1.0 for the SIGMA- beam on the Copper target.

Table 5

Inclusive SIGMA(1660) production cross sections, times the < LAMBDA PI> branching ratio, in the XL range 0.3 to 1.0 for the SIGMA- beam on the Carbon target.

Table 6

Inclusive SIGMA(1660) production cross sections per nucleon, times the < LAMBDA PI> branching ratio, in the XL range 0.3 to 1.0 for the SIGMA- beam on the Carbon target, and the exponent in the cross section parametrization of the formA**POWER.

Table 7

Inclusive SIGMA(1385) production cross sections for the PI- beam with a Copper target, times the < LAMBDA PI> branching ratio., RE = PI- CU --> SIGMA(1385)- X. PI- CU --> SIGMA(1385)+ X.

Table 8

Inclusive SIGMA(1385) production cross sections for the PI- beam with a Carbon target, times the < LAMBDA PI> branching ratio., RE = PI- C --> SIGMA(1385)-X. PI- C --> SIGMA(1385)+ X.

Table 9

Inclusive SIGMA(1385) production cross sections per nucleon, times the < LAMBDA PI> branching ratio, for the PI- beam, and the exponent in the cross section parametrization of the form A**POWER.

Table 10

Inclusive SIGMA(1385) production cross sections for the Neutron beam with aCopper target, times the < LAMBDA PI> branching ratio.

Table 11

Inclusive SIGMA(1385) production cross sections for the Neutron beam with aCarbon target, times the < LAMBDA PI> branching ratio.

Table 12

Inclusive SIGMA(1385) production cross sections per nucleon, times the < LAMBDA PI> branching ratio, for the Neutron beam, and the exponent in the cross section parametrization of the form A**POWER.

Table 13

Differential cross sections as a function of XL for SIGMA+- production in CU and C with the SIGMA- beam.

Table 14

Differential cross sections as a function of PT**2 for SIGMA+- production in CU and C with the SIGMA- beam.

Table 15

Differential cross sections as a function of XL for SIGMA(1385)- productionin CU and C with the PI- and SIGMA- beams.

Table 16

Differential cross sections as a function of XL for SIGMA(1385)- productionin CU and C with the Neutron beam.

Table 17

Differential cross sections as a function of PT**2 for SIGMA(1385)- production in CU and C with the PI- and SIGMA- beams.

Table 18

Differential cross sections as a function of PT**2 for SIGMA(1385)- production in CU and C with the Neutron beam.

Table 19

Differential cross sections as a function of XL for SIGMA(1385)+ productionin CU and C with the PI- and SIGMA- beams.

Table 20

Differential cross sections as a function of XL for SIGMA(1385)+ productionin CU and C with the Neutron beam.

Table 21

Differential cross sections as a function of PT**2 for SIGMA(1385)+ production in CU and C with the PI- and SIGMA- beams.

Table 22

Differential cross sections as a function of PT**2 for SIGMA(1385)+ production in CU and C with the Neutron beam.

Table 23

Differential cross sections as a function of XL for SIGMABAR(1385)- production in CU and C with the SIGMA- beam.

Table 24

Differential cross sections as a function of PT**2 for SIGMABAR(1385)- production in CU and C with the SIGMA- beam.

Table 25

Differential cross sections as a function of XL for SIGMA(1660)+- production in CU and C with the SIGMA- beam.

Table 26

Differential cross sections as a function of PT**2 for SIGMA(1660)+- production in CU and C with the SIGMA- beam.

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Inclusive Production of Hyperons and Anti-hyperons in $N$ C Collisions at an Energy of About 40-{GeV} (In Russian)

The BIS-2 collaboration Aleev, A.N. ; Arefev, V.A. ; Balandin, V.P. ; et al.

Yad.Fiz. 44 (1986) 661-670, 1986.

https://inspirehep.net/literature/239304 Inspire Record 239304 DOI 10.17182/hepdata.17456 https://doi.org/10.17182/hepdata.17456

None

4 data tables

Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.

Table 4

MODEL DEPENDENT CALCULATION FROM SIG FOR XL>.2.

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