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Evidence for Local Compensation of Baryon Number in $e^+ e^-$ Annihilation

The TASSO collaboration Althoff, M. ; Braunschweig, W. ; Kirschfink, F.J. ; et al.
Phys.Lett.B 139 (1984) 126-132, 1984.
Inspire Record 199469 DOI 10.17182/hepdata.27109

We have studied at CM energies of 14, 22 and 30–36.7 GeV e + e − annihilation events in which the hadronic final state contains both a proton and an antiproton in the momentum range 1.0 < p < GeV/ c . We find that such pairs are produced predominantly in the same jet and conclude that baryon-antibaryon production is dominated by a mechanism involving local compensation of baryon number.

2 data tables
Table 1

BACKGROUND SUBTRACTED DATA.

Table 2

BACKGROUND SUBTRACTED DATA.


PHENOMENOLOGICAL MULTIPOLAR ANALYSIS OF THE REACTION GAMMA p---> p pi0 IN ENERGY INTERVALS FROM THRESHOLD TO e (gamma) = 1200-MeV

Konovalov, O.G. ; Omelaenko, A.S. ; Sorokin, P.V. ;
KhFTI-84-23, 1984.
Inspire Record 211003 DOI 10.17182/hepdata.38330

None

1 data table
Table 1

No description provided.


SMALL ANGLE CORRELATIONS OF IDENTICAL PARTICLES IN CARBON CARBON INTERACTIONS AT P = 4.2-GEV/C PER NUCLEON

Akhababian, N. ; Bartke, J. ; Grishin, V.G. ; et al.
Z.Phys.C 26 (1984) 245-248, 1984.
Inspire Record 200208 DOI 10.17182/hepdata.39586

Two-particle small-angle correlations between negative pions and between protons in carbon-carbon collisions atP=4.2 GeV/c per nucleon have been studied, both for an unbiased sample and for “central” events. A comparison of experimental π− π− andpp correlation functions with theoretical predictions has been made. A possible evidence for the existence of two fireballs in C+C interactions atP=4.2 GeV/c per nucleon is presented.

5 data tables
Table 1

THE SECOND REACTION IS TAKEN TO BE 'CENTRAL'.

Table 2

THE SECOND REACTION IS TAKEN TO BE 'CENTRAL' AND P OF PROTONS < 0.3 GEV FOR BOTH REACTIONS.

Table 3

THE SECOND REACTION IS TAKEN TO BE 'CENTRAL' AND E(P=3-4,RF=LAB) < 0.3 GEV ,(P(P=3-4,RF=LAB))**2 < 0.2 GEV**2 FOR ALL REACTIONS.

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SEARCH FOR NARROW SINGULARITIES IN EFFECTIVE MASS SPECTRA OF TWO AND THREE PROTONS WITH THE 2-METER PROPANE CHAMBER

Agakishiev, G.N. ; Gasparian, A.P. ; Kvatadze, R.A. ;
JINR-1-84-103, 1984.
Inspire Record 210407 DOI 10.17182/hepdata.39657

None

10 data tables
Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.

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HIGHER TWIST EFFECTS IN SEMIINCLUSIVE ANTI-NEUTRINO N ---> mu+ h- X REACTIONS

Ammosov, V.V. ; Asratian, A.E. ; Denisov, A.G. ; et al.
JETP Lett. 39 (1984) 537, 1984.
Inspire Record 200138 DOI 10.17182/hepdata.40969

None

6 data tables
Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.

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PROTON YIELDS AT AN ANGLE OF 132-DEGREES ON LI-6, C, CU AND PB NUCLEI IN REACTIONS PI+- A ---> P X AT A PI MESON MOMENTUM OF 1.5-GEV/C. (IN RUSSIAN)

Buklei, A.E. ; Burgov, N.A. ; Vlasov, M.K. ; et al.
Moscow Inst. Theor. Exp. Phys. Gkae - ITEF-84-056 (84,REC.JUN.) 12p, 1984.
Inspire Record 205430 DOI 10.17182/hepdata.40145

None

2 data tables
Table 1

No description provided.

Table 2

No description provided.


pi+ MESON PRODUCTION AT 137-degree ANGLE IN THE INCLUSIVE REACTIONS pi+- A ---> pi+ X AT MOMENTA OF 1.5-GeV/c INCIDENT PIONS

Burgov, N.A. ; Buklei, A.E. ; Vlasov, M.K. ; et al.
ITEP-82-1984, 1984.
Inspire Record 204552 DOI 10.17182/hepdata.40189

None

2 data tables
Table 1

No description provided.

Table 2

No description provided.


STUDY OF CHARMED STRANGE VECTOR MESON PRODUCTION BY ANTI-NEUTRINOS

Asratian, A.E. ; Fedotov, A.V. ; Gorichev, P.A. ; et al.
Moscow Inst. Theor. Exp. Phys. Gkae - ITEF-84-099 (84,REC.AUG.) 7p, 1984.
Inspire Record 210786 DOI 10.17182/hepdata.40174

None

1 data table
Table 1

ERROR DUE TO ERROR IN BRANCHING VALUE IS 0.008.


ELECTROPRODUCTION OF ETA MESONS IN THE REGION OF THE RESONANCE S11 (1535) AT MOMENTUM TRANSFERS OF 2-GEV**2 AND 3-GEV**2

Brasse, F.W. ; Flauger, W. ; Gayler, Joerg ; et al.
Z.Phys.C 22 (1984) 33-38, 1984.
Inspire Record 203579 DOI 10.17182/hepdata.16229

We report on results of η-electroproduction in the resonance region at momentum transfers ofQ2=2 GeV2 and 3 GeV2. The differential cross sections obtained in the region of the second nucleon resonance strongly support the dominance of theS11(1535) in this channel. The total transverse virtual photoproduction cross section of theS11(1535) shows a flatQ2-dependence ∼e−0.39·Q2. Comparison with the total resonant γvp cross section in the second resonance region aroundW=1.5 GeV shows that theD13(1520) production decreases much faster (∼e−1.6·Q2). The data are not compatible with the simple harmonic oscillator quark model with spin and orbit excitation of a quark only.

23 data tables
Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.

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EVIDENCE FOR A NONTENSOR (Q ANTI-Q) MESON AT 1410-MEV PRODUCED IN THE REACTION PI- P ---> K0(S) K0(S) N AT 63-GEV

The ACCMOR collaboration Daum, C. ; Hertzberger, L.O. ; Hoogland, W. ; et al.
Z.Phys.C 23 (1984) 339-347, 1984.
Inspire Record 204305 DOI 10.17182/hepdata.16225

We present an analysis of theKs0Ks0 system produced in the reaction π−p→Ks0Ks0n at 63 GeV based on ∼700 events in the kinematical region of |t|<0.5 GeV2. We concentrate on masses between 1,200 and 1,600 MeV where a double maximum structure is observed. Performing an amplitude analysis in this mass interval we find thatS,D0 andD+ waves contribute to the mass spectrum at approximately equal strength. The peaks are attributed to spin 2 waves. However, we failed to explained them by interferingf(1270),A2(1310) andf′(1520) resonances alone. While the first peak can be associated withf(1270)−A2(1310) production, an additional tensor meson is needed with mass of ∼1410 MeV and a narrow width for a description of the second one. The analysis as well as the energy dependence deduced from some publishedKs0Ks0 mass spectra suggests this object to be dominantly produced by a natural parity exchange. Because the 2++\(q\bar q\) nonet is already complete the nature of the new tensor meson is an open question.

1 data table
Table 1

No description provided.