Date

Collaboration

Phrases

Reactions

Cmenergies

K0 and Lambda Production at the CERN ISR

Busser, F.W. ; Camilleri, L. ; Di Lella, L. ; et al.
Phys.Lett. B61 (1976) 309-312, 1976.
Inspire Record 101076 DOI 10.17182/hepdata.5534
3 data tables

No description provided.

No description provided.

No description provided.


Charge exchange and production of eta mesons and multiple neutral pions in pi- p reactions between 654 and 1247 mev/c

Bulos, F. ; Lanou, R.E. ; Piper, A.E. ; et al.
Phys.Rev. 187 (1969) 1827-1844, 1969.
Inspire Record 62084 DOI 10.17182/hepdata.5293
34 data tables

No description provided.

No description provided.

No description provided.

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Backward elastic scattering from 875 to 1580 mev/c

Abillon, J.M. ; Borg, A. ; Crozon, M. ; et al.
Phys.Lett. B32 (1970) 712-715, 1970.
Inspire Record 63081 DOI 10.17182/hepdata.5883
30 data tables

No description provided.

No description provided.

No description provided.

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DIJET PRODUCTION CROSS-SECTION AND FRAGMENTATION OF JETS PRODUCED IN P P COLLISIONS AT S**(1/2) = 63-GEV

The AXIAL FIELD SPECTROMETER collaboration Akesson, T. ; Albrow, M.G. ; Almehed, S. ; et al.
Z.Phys. C30 (1986) 27-43, 1986.
Inspire Record 221571 DOI 10.17182/hepdata.16017

We present stdies of events triggered on two high-pT jets, produced inpp collisions at the CERN Intersecting Storage Rings (ISR) at\(\sqrt s \)=63 GeV, using a large solid angle calorimeter. The cross-section for producing two jets is measured in the dijet mass range 17–50 GeV/c2. A high-statistics sample of dijet events, where each jet has transverse energy above 10 GeV, is used to study the structure of jets and the associated event. We find the longitudinal fragmentation function to be similar to that of jets emerging frome+e− collisions but considerably harder than that observed at the Super Proton Synchrotron (SPS)\(p\bar p\) Collider. A steepening of the fragmentation function is observed when increasing the jet energy. Studies of the charge distribution in jets show that these predominantly originate from fragmenting valence quarks. The transverse energy and particle flows are presented as functions of the azimuthal distance from the jet axis.

3 data tables

No description provided.

No description provided.

FRAGMENTATION FUNCTION FOR ET(JET) > 10 GEV.


ERRORS ARE PURELY STATISTICAL.

ERRORS ARE PURELY STATISTICAL.

ERRORS ARE PURELY STATISTICAL.

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LEADING PROTON AND ANTI-PROTON DISTRIBUTIONS IN PROTON NUCLEUS AND ANTI-PROTON NUCLEUS INTERACTIONS

Bailey, R. ; Blanar, G. ; Bosman, M. ; et al.
Z.Phys. C29 (1985) 1-8, 1985.
Inspire Record 221966 DOI 10.17182/hepdata.15989
1 data table

No description provided.


No description provided.

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No description provided.

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Inclusive Pion and eta Production in K- p Interactions at 14.3-GeV/c

Borg, A.C. ; Bardadin-Otwinowska, M. ; Barloutaud, R. ; et al.
Nucl.Phys. B106 (1976) 430-450, 1976.
Inspire Record 100813 DOI 10.17182/hepdata.8392
27 data tables

No description provided.

No description provided.

No description provided.

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Production Spectra of pi+-, K+-, rho+- at Large Angles in Proton Proton Collisions in the CERN Intersecting Storage Rings

The British-Scandinavian collaboration Alper, B. ; Boggild, H. ; Booth, P.S.L. ; et al.
Nucl.Phys. B100 (1975) 237-290, 1975.
Inspire Record 99735 DOI 10.17182/hepdata.8506
168 data tables

Axis error includes +- 15.0/15.0 contribution (NORMALIZATION ERROR - THE LARGEST SYSTEMATICS).

Axis error includes +- 15.0/15.0 contribution (NORMALIZATION ERROR - THE LARGEST SYSTEMATICS).

Axis error includes +- 15.0/15.0 contribution (NORMALIZATION ERROR - THE LARGEST SYSTEMATICS).