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INCLUSIVE PRODUCTION OF MESONS IN n p INTERACTIONS AT 3.83-GeV/c

Abdivaliev, A. ; Besliu, K. ; Gasparian, A.P. ; et al.
No Journal Information, 1981.
Inspire Record 167522 DOI 10.17182/hepdata.39060
7 data tables
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Comparison between hadronic final states produced in $\mu p$ and $e^+ e^-$ interactions

The European Muon collaboration Arneodo, M. ; Arvidson, A. ; Aubert, J.J. ; et al.
Z.Phys. C35 (1987) 417, 1987.
Inspire Record 233424 DOI 10.17182/hepdata.16655
23 data tables

With respect to the virtual photon axis.

With respect to the sphericity axis.

With respect to the thrust axis.

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Observation and Study of a Narrow State in a $\Sigma^-$ (1385) $K^+$ System

The Berlin-Budapest-Dubna-Moscow-Prague-Sofiya-Tbilisi collaboration Aleev, A.N. ; Arefev, V.A. ; Balandin, V.P. ; et al.
Z.Phys. C25 (1984) 205, 1984.
Inspire Record 201523 DOI 10.17182/hepdata.39601
5 data tables

YN IS IN ARBITRARY UNITS.

ARBITRARY UNITS FOR YN.

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Differential cross-sections, charge production asymmetry, and spin density matrix elements for D*+-(2010) produced in 500-GeV/c pi- nucleon interactions

The Fermilab E791 collaboration Aitala, E.M. ; Amato, S. ; Anjos, J.C. ; et al.
Phys.Lett. B539 (2002) 218-226, 2002.
Inspire Record 587686 DOI 10.17182/hepdata.42892

We report differential cross sections for the production of D*(2010) produced in 500 GeV/c pi^- nucleon interactions from experiment E791 at Fermilab, as functions of Feynman-x (x_F) and transverse momentum squared (p_T^2). We also report the D* +/- charge asymmetry and spin-density matrix elements as functions of these variables. Investigation of the spin-density matrix elements shows no evidence of polarization. The average values of the spin alignment are \eta= 0.01 +- 0.02 and -0.01 +- 0.02 for leading and non-leading particles, respectively.

8 data tables

Acceptance corrected differential cross sections for D*+- production as a function of XL, Feynman X.

Acceptance corected differential cross sections for D*+- production as a function of PT**2.

Charge production asymmetry as a function of Feynman X.

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A Study of strange particle production in muon-neutrino charged current interactions in the NOMAD experiment

The NOMAD collaboration Astier, P. ; Autiero, D. ; Baldisseri, A. ; et al.
Nucl.Phys. B621 (2002) 3-34, 2002.
Inspire Record 566751 DOI 10.17182/hepdata.48925

A study of strange particle production in muon neutrino charged current interactions has been performed using the data from the NOMAD experiment. Yields of neutral strange particles K0s, Lambda, AntiLambda have been measured. Mean multiplicities are reported as a function of the event kinematic variables Enu, W2 and Q2 as well as of the variables describing particle behaviour within a hadronic jet: xF, z and pT2. Decays of resonances and heavy hyperons with identified K0s and Lambda in the final state have been analyzed. Clear signals corresponding to K*+-, Sigma*+-, Xi- and Sigma0 have been observed.

20 data tables

Measured yields of the neutral strange particles measured in this analysis.The second line (marked *) is a recalculation taking into account contributions from both primary and secondary V0. The values for K0 are the K0S rates multipl ied by 2.

Measured yields as a function of E, the neutrino energy.

Measured yields as a function of W**2.

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Study of D*+ production in nu/mu charged current interactions in the NOMAD experiment

The NOMAD collaboration Astier, P. ; Autiero, D. ; Baldisseri, A. ; et al.
Phys.Lett. B526 (2002) 278-286, 2002.
Inspire Record 567771 DOI 10.17182/hepdata.49701
5 data tables

Distribution in Feynman X.

Distribution in transverse momentum.

Distribution in fractional energy Z.

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Hadron production in diffractive deep inelastic scattering

The H1 collaboration Adloff, C. ; Aid, S. ; Anderson, M. ; et al.
Phys.Lett. B428 (1998) 206-220, 1998.
Inspire Record 468748 DOI 10.17182/hepdata.44324

Characteristics of hadron production in diffractive deep-inelastic positron-proton scattering are studied using data collected in 1994 by the H1 experiment at HERA. The following distributions are measured in the centre-of-mass frame of the photon dissociation system: the hadronic energy flow, the Feynman-x (x_F) variable for charged particles, the squared transverse momentum of charged particles (p_T^{*2}), and the mean p_T^{*2} as a function of x_F. These distributions are compared with results in the gamma^* p centre-of-mass frame from inclusive deep-inelastic scattering in the fixed-target experiment EMC, and also with the predictions of several Monte Carlo calculations. The data are consistent with a picture in which the partonic structure of the diffractive exchange is dominated at low Q^2 by hard gluons.

6 data tables

Energy flow distributions in the gamma*-pomeron CM frame.. Positive etarap corresponds to the direction of the incoming photon.

Energy flow distributions in the gamma*-pomeron CM frame.. Positive etarap corresponds to the direction of the incoming photon.

Energy flow distributions in the gamma*-pomeron CM frame.. Positive etarap corresponds to the direction of the incoming photon.

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Charged particles and neutral kaons in photoproduced jets at HERA

The ZEUS collaboration Breitweg, J. ; Derrick, M. ; Krakauer, D. ; et al.
Eur.Phys.J. C2 (1998) 77-93, 1998.
Inspire Record 451528 DOI 10.17182/hepdata.44362

Charged particles ($h^\pm$) and \kz mesons have been studied in photoproduced events containing at least one jet of $E_T > 8$ GeV in a pseudorapidity interval (--0.5, 0.5) in the ZEUS laboratory frame. Distributions are presented in terms of transverse momentum, pseudorapidity and distance of the particle from the axis of a jet. The properties of \hpm within the jet are described well using the standard settings of PYTHIA, but the use of the multiparton interaction option improves the description outside the jets. A reasonable overall description of the \kz behaviour is possible with PYTHIA using a reduced value of the strangeness suppression parameter. The numbers of $h^\pm$ and \kz within a jet as defined above are measured to be $3.25\pm0.02\pm0.28$ and $0.431\pm0.013\pm0.088$ respectively. Fragmentation functions are presented for $h^\pm$ and \kz in photoproduced jets; agreement is found with calculations of Binnewies et al. and, at higher momenta, with $p\bar p$ scattering and with standard PYTHIA. Fragmentation functions in direct photoproduced events are extracted, and at higher momenta give good agreement with data from related processes in $e^+e^-$ annihilation and deep inelastic $ep$ scattering.

11 data tables

Corrected multiplicities of charged particles and neutral K0 mesons per photoproduced jet.

Corrected distribution of charged particles per jet in events containing a hadron jet.

Corrected distribution of charged particles per jet in events containing a hadron jet.

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Proton dissociative $\rho$ and elastic $\phi$ electroproduction at HERA

The H1 collaboration Adloff, C. ; Aid, S. ; Anderson, M. ; et al.
Z.Phys. C75 (1997) 607-618, 1997.
Inspire Record 443293 DOI 10.17182/hepdata.44590

The electroproduction of rho mesons with proton diffractive dissociation for Q^2 > 7 GeV^2 and the elastic electroproduction of Phi mesons for Q^2 > 6 Gev^2 are studied in e^+ p collisions at HERA with the H1 detector, for an integrated luminosity of 2.8 pb-1. The dependence of the cross sections on P_t^2 and Q^2 is measured, and the vector meson polarisation obtained. The cross section ratio between proton dissociative and elastic production of rho mesons is measured and discussed in the framework of the factorisation hypothesis of diffractive vertices. The ratio of the elastic cross section for Phi and rho meson production is investigated as a function of Q^2.

11 data tables

Corrected PT**2 distribution for RHO production from the proton dissociative sample. Statistical errors only.

Cross sections and ratio of proton dissociative to elastic cross sections.

Cross sections and ratio of proton dissociative to elastic cross sections.

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Nuclear target diffraction dissociation in pi+ and K+ collisions with Au and Al at 250-GeV/c

The EHS/NA22 collaboration Agababyan, N.M. ; Ataian, M.R. ; Charlet, M. ; et al.
Z.Phys. C72 (1996) 65-70, 1996.
Inspire Record 419049 DOI 10.17182/hepdata.14252
6 data tables

For target-diffractive cross-section.

For target-diffractive cross-section.

Multiplicities for the diffractive system.

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Transverse momentum distributions for meson resonances at central rapidity and P(t) >= 2-GeV/c

The WA77 collaboration Belogianni, A. ; Benayoun, Maurice ; Beusch, W. ; et al.
Z.Phys. C59 (1993) 35-46, 1993.
Inspire Record 354486 DOI 10.17182/hepdata.48468
6 data tables

No description provided.

Acceptance corrected tranverse momentum distribution.

Acceptance corrected tranverse momentum distribution.

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Neutral strange particle production in deep inelastic scattering at HERA

The ZEUS collaboration Derrick, M. ; Krakauer, D. ; Magill, S. ; et al.
Z.Phys. C68 (1995) 29-42, 1995.
Inspire Record 395196 DOI 10.17182/hepdata.44998

This paper presents measurements of \k\ and \lam\ production in neutral current, deep inelastic scattering of 26.7 GeV electrons and 820 GeV protons in the kinematic range $ 10 < Q~{2} < 640 $ GeV$~2$, $0.0003 < x < 0.01$, and $y > 0.04$. Average multiplicities for \k\ and \lam\ production are determined for transverse momenta \ \ptr\ $> 0.5 $ GeV and pseudorapidities $\left| \eta \right| < 1.3$. The multiplicities favour a stronger strange to light quark suppression in the fragmentation chain than found in $e~+ e~-$ experiments. The production properties of \k's in events with and without a large rapidity gap with respect to the proton direction are compared. The ratio of neutral \k's to charged particles per event in the measured kinematic range is, within the present statistics, the same in both samples.

12 data tables

No description provided.

No description provided.

No description provided.

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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
6 data tables

No description provided.

No description provided.

No description provided.

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Inclusive Characteristics of $\pi^-$ Mesons Produced in $p$ C and $p$ Ta Interactions at 10-{GeV}/$c$ Proton Momentum

Armutliisky, D.D. ; Akhababian, N.O. ; Grishin, V.G. ; et al.
Sov.J.Nucl.Phys. 48 (1988) 101-107, 1988.
Inspire Record 251090 DOI 10.17182/hepdata.9502
8 data tables

No description provided.

No description provided.

MOMENTUM SPECTRA IN THE WINDOW P=0.1-6.0 HAVE BEEN FITTED BY THE FORMULA: (1/N)*D(N)/D(P)=CONST(Q=1)*EXP(-SLOPE(Q=1)*P)+CONST(Q=2)*EXP (-SLOPE(Q=2)*P).

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Study of charm photoproduction mechanisms

The NA14/2 collaboration Alvarez, M.P. ; Barate, R. ; Bloch, D. ; et al.
Z.Phys. C60 (1993) 53-62, 1993.
Inspire Record 333271 DOI 10.17182/hepdata.14331
10 data tables

D0 cross section assuming branching ratio of D0 --> K- PI+ of 3.65 +- 0.21 PCT.

D+(-) cross section assuming branching ratio of D+ --> K- PI+ PI+ of 8.0 +0.8,-0.7 PCT.

Total non diffractive open charm production cross section allowing for contributions for other charmed particles (D/S and LAMBDA/C). Comparison of data with first order QCD leads to a predicted charm quark mass of 1.5 +0.2,-0.1 GeV.

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Neutral strange particle production in anti-neutrino - neon charged current interactions

The WA59 collaboration Willocq, Stephane ; Marage, P. ; Aderholz, M. ; et al.
Z.Phys. C53 (1992) 207-218, 1992.
Inspire Record 319235 DOI 10.17182/hepdata.14768
20 data tables

No description provided.

No description provided.

No description provided.

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No description provided.

No description provided.

No description provided.

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Distributions of charged hadrons observed in deep inelastic muon - deuterium scattering at 490-GeV

The E-665 collaboration Adams, M.R. ; Aid, S. ; Anthony, P.L. ; et al.
Phys.Lett. B272 (1991) 163-168, 1991.
Inspire Record 318993 DOI 10.17182/hepdata.29288
5 data tables

No description provided.

No description provided.

No description provided.

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Comparison of Light Quark and Charm Quark Fragmentation

Kesten, P. ; Akerlof, C. ; Bonvicini, G. ; et al.
Phys.Lett. B161 (1985) 412-416, 1985.
Inspire Record 17116 DOI 10.17182/hepdata.30349
3 data tables

Charm Quark Jet Trigger. Characteristics of Jet Opposite the Trigger Jet.

Light Quark Jet Trigger. Characteristics of Jet Opposite the Trigger Jet.

No description provided.


Evidence for Anomalous Prompt Photons in Deep Inelastic Muon Scattering at 200-{GeV}

The European Muon collaboration Aubert, J.J. ; Bassompierre, G. ; Becks, K.H. ; et al.
Phys.Lett. B218 (1989) 248-256, 1989.
Inspire Record 261250 DOI 10.17182/hepdata.29855
2 data tables

Z distribution of anomalous direct photons.

PT distribution of anomalous direct photons.


Production Cross-section and Electroweak Asymmetry of $D^*$ and $D$ Mesons Produced in $e^+ e^-$ Annihilations at 29-{GeV}

Baringer, Philip S. ; Bylsma, B.G. ; DeBonte, R. ; et al.
Phys.Lett. B206 (1988) 551-556, 1988.
Inspire Record 23360 DOI 10.17182/hepdata.6192
11 data tables

No description provided.

No description provided.

No description provided.

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HADRONS AND GAMMAS ASSOCIATED TO DIMUONS AND J / psi PARTICLES IN pi- C INTERACTIONS AT 38-GeV/c

The RISK collaboration Jani, J. ; Mihalyi, Z. ; Nyitrai, G. ; et al.
Conference Paper, 1987.
Inspire Record 251044 DOI 10.17182/hepdata.9973
7 data tables

No description provided.

No description provided.

No description provided.

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Production of anti-D0 and D- Mesons in Neutron - Carbon Interactions at 40-GeV to 70-GeV

The BIS-2 collaboration Aleev, A.N. ; Arefev, V.A. ; Balandin, V.P. ; et al.
Z.Phys. C37 (1988) 243, 1988.
Inspire Record 248611 DOI 10.17182/hepdata.9960
4 data tables

No description provided.

No description provided.

No description provided.

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No description provided.

No description provided.

No description provided.

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Evidence for Planar Events and a Forward Double Jet Structure in Deep Inelastic Muon Scattering

The European Muon collaboration Aubert, J.J. ; Bassompierre, G. ; Becks, K.H. ; et al.
Phys.Lett. B100 (1981) 433-438, 1981.
Inspire Record 164536 DOI 10.17182/hepdata.31213
2 data tables

PTIN**2 is the sum of the PTIN components squared.

PTOUT**2 is the sum of the PTOUT components squared.