Arefev, A.
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SEARCH FOR EXOTIC BARYON RESONANCES WITH ISOSPIN I = 5/2 IN pi+ p REACTIONS AT 3.94-GeV/c pi+ MESON MOMENTA

Arefev, A.V. ; Bayukov, Yu.D. ; Grishuk, Yu.G. ; et al.
ITEP-86-150, 1986.
Inspire Record 234870 DOI 10.17182/hepdata.40112

None

1 data table match query
Table 1

No description provided.


STUDY OF THE BARYON EXCHANGE REACTION pi+ p ---> DELTA++ rho0 AT MOMENTUM 3.94-GeV/c

Arefev, A.V. ; Bayukov, Yu.D. ; Grishuk, Yu.G. ; et al.
ITEP-86-76, 1986.
Inspire Record 230667 DOI 10.17182/hepdata.40119

None

2 data tables match query
Table 1

No description provided.

Table 2

No description provided.


MEASUREMENT OF pi- d BACKWARD ELASTIC SCATTERING CROSS-SECTIONS IN THE pi- MESON MOMENTUM INTERVALS FROM 0.74-GeV/c TO 1.3-GeV/c

Arefev, A.V. ; Bayukov, Yu.D. ; Buklei, A.E. ; et al.
ITEP-49-1978, 1978.
Inspire Record 131151 DOI 10.17182/hepdata.40259

None

1 data table match query
Table 1

No description provided.


Estimate of cross section of elastic pi- d backward scattering at 3.7 gev/c momentum

Arefev, A.V. ; Bayukov, Yu.D. ; Efremenko, V.I. ; et al.
Pisma Zh.Eksp.Teor.Fiz. 19 (1974) 775-776, 1974.
Inspire Record 96877 DOI 10.17182/hepdata.39923

None

1 data table match query
Table 1

No description provided.


Anti-D0 meson production in interactions of neutrons with hydrogen, carbon, and aluminum nuclei at 37.5-GeV to 70-GeV

The BIS-2 collaboration Aleev, A.N. ; Arefev, V.A. ; Balandin, V.P. ; et al.
Phys.Atom.Nucl. 56 (1993) 1235-1240, 1993.
Inspire Record 364824 DOI 10.17182/hepdata.17203

None

6 data tables match query
Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.

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FORWARD PRODUCTION OF DELTA (1232) AND N* (1688) IN THE REACTION pi- d ---> N*0 pi- p(s) AT 3.65-GeV/c

Arefev, A.V. ; Leksin, G.A. ; Suchkov, D.A. ; et al.
Sov.J.Nucl.Phys. 35 (1982) 847, 1982.
Inspire Record 156015 DOI 10.17182/hepdata.17760

None

1 data table match query
Table 1

No description provided.


Study of rho n-interaction on basis of the data on incoherent rho-meson production on carbon nuclei by 3.72-GeV/c pi- mesons

Arefev, A.V. ; Bayukov, Yu.D. ; Efremenko, V.I. ; et al.
Sov.J.Nucl.Phys. 19 (1974) 304-307, 1974.
Inspire Record 95159 DOI 10.17182/hepdata.18240

None

2 data tables match query
Table 1

No description provided.

Table 2

No description provided.


Spin observables in neutron proton elastic scattering.

Ahmidouch, A. ; Arnold, J. ; van den Brandt, B. ; et al.
Eur.Phys.J.C 2 (1998) 627-641, 1998.
Inspire Record 471273 DOI 10.17182/hepdata.11376

The analyzing power,$A_{oono}$, and the polarization transfer observables$K_{onno}$,$K_{os''so}$

20 data tables match query
Table 1

Position 'A' (see text for explanation).

Table 2

Position 'A' (see text for explanation).

Table 3

Position 'A' (see text for explanation).

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rivet Analysis
QCD analyses and determinations of alpha(s) in e+ e- annihilation at energies between 35-GeV and 189-GeV.

The JADE & OPAL collaborations Pfeifenschneider, P. ; Biebel, O. ; Movilla Fernandez, P.A. ; et al.
Eur.Phys.J.C 17 (2000) 19-51, 2000.
Inspire Record 513337 DOI 10.17182/hepdata.12882

We employ data taken by the JADE and OPAL experiments for an integrated QCD study in hadronic e+e- annihilations at c.m.s. energies ranging from 35 GeV through 189 GeV. The study is based on jet-multiplicity related observables. The observables are obtained to high jet resolution scales with the JADE, Durham, Cambridge and cone jet finders, and compared with the predictions of various QCD and Monte Carlo models. The strong coupling strength, alpha_s, is determined at each energy by fits of O(alpha_s^2) calculations, as well as matched O(alpha_s^2) and NLLA predictions, to the data. Matching schemes are compared, and the dependence of the results on the choice of the renormalization scale is investigated. The combination of the results using matched predictions gives alpha_s(MZ)=0.1187+{0.0034}-{0.0019}. The strong coupling is also obtained, at lower precision, from O(alpha_s^2) fits of the c.m.s. energy evolution of some of the observables. A qualitative comparison is made between the data and a recent MLLA prediction for mean jet multiplicities.

80 data tables match query
Table 1

Overall result for ALPHAS at the Z0 mass from the combination of the ln R-matching results from the observables evolved using a three-loop running expression. The errors shown are total errors and contain all the statistics and systematics.

Table 2

Weighted mean for ALPHAS at the Z0 mass determined from the energy evolutions of the mean values of the 2-jet cross sections obtained with the JADE and DURHAMschemes and the 3-jet fraction for the JADE, DURHAM and CAMBRIDGE schemes evaluted at a fixed YCUT.. The errors shown are total errors and contain all the statistics and systematics.

Table 3

Combined results for ALPHA_S from fits of matched predicitions. The first systematic (DSYS) error is the experimental systematic, the second DSYS error isthe hadronization systematic and the third is the QCD scale error. The values of ALPHAS evolved to the Z0 mass using a three-loop evolution are also given.

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A Determination of alpha-s (M (Z0)) at LEP using resummed QCD calculations

The OPAL collaboration Acton, P.D. ; Alexander, G. ; Allison, John ; et al.
Z.Phys.C 59 (1993) 1-20, 1993.
Inspire Record 354188 DOI 10.17182/hepdata.14427

The strong coupling constant, αs, has been determined in hadronic decays of theZ0 resonance, using measurements of seven observables relating to global event shapes, energy correlatio

7 data tables match query
Table 1

Data corrected for finite acceptance and resolution of the detector and for intial state photon radiation. No corrections for hadronic effects are applied.. Errors include statistical and systematic uncertainties, added in quadrature.

Table 2

Data corrected for finite acceptance and resolution of the detector and for intial state photon radiation. No corrections for hadronic effects are applied.. Errors include statistical and systematic uncertainties, added in quadrature.

Table 3

Data corrected for finite acceptance and resolution of the detector and for intial state photon radiation. No corrections for hadronic effects are applied.. Errors include statistical and systematic uncertainties, added in quadrature.

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