Magill, S.
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Annihilation cross-sections of anti-neutrons on C, Al, Cu, Sn and Pb at low momenta (180-MeV/c - 280-MeV/c) with the OBELIX spectrometer

The OBELIX collaboration Ableev, V.G. ; Adamo, A. ; Agnello, M. ; et al.
Nuovo Cim.A 107 (1994) 943-953, 1994.
Inspire Record 384438 DOI 10.17182/hepdata.37841

Annihilation cross-sections σann for antineutrons on some nuclei (C, Al, Cu, Sn and Pb) at three antineutron momenta (180, 240 and 280 MeV/c) were measured at LEAR (CERN) with the OBELIX spectrometer. A behaviour σann=σ0Aν has been found withν≈2/3. The data are discussed following some models for antineutron-nucleus interaction.

3 data tables
Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.


Particle production in He Li collisions at 4.5-A/GeV/c

Al-Baaj, E. ; Al-Baaj, S. ; Besliu, C. ; et al.
Nuovo Cim.A 107 (1994) 1611-1623, 1994.
Inspire Record 384746 DOI 10.17182/hepdata.37842

In this paper the main experimental results on some significant physical quantities obtained in He−Li collisions at 4.5A GeV/c are presented. The experiments have been performed at the Syncrophasotron from JINR Dubna, in the frame of the SKM 200 Collaboration.

4 data tables
Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.

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Neutron halo in heavy nuclei from anti-proton absorption

Lubinski, P. ; Jastrzebski, J. ; Grochulska, A. ; et al.
Phys.Rev.Lett. 73 (1994) 3199-3202, 1994.
Inspire Record 384612 DOI 10.17182/hepdata.19678

A new method to study the nuclear periphery using antiproton annihilation was applied to nine isotopes with mass numbers between 58 and 238. The method makes use of the detection of the radioactive annihilation products one unit lower in mass number than the target. A clear neutron halo effect, strongly correlated with the neutron binding energy, was observed in some nuclei. The experimental results are in qualitative agreement with calculations of proton and neutron densities at the nuclear periphery based on either a simple asymptotic density model or a more complex Hartree-Fock approach.

3 data tables
Table 1

No description provided.

Table 2

No description provided.

Table 3

A(FRAGT)=A(TARGET)-1.


Some characteristics of high multiplicity (>= 45) proton AgBr interactions at 800-GeV

Soni, S.K. ; Malik, S. ; Shivpuri, R.K. ;
Z.Phys.A 348 (1994) 311-315, 1994.
Inspire Record 383019 DOI 10.17182/hepdata.16556

Experimental results on some characteristics of high multiplicity (≧45) proton-AgBr interactions at 800 GeV are presented. The results are compared with those in lower multiplicity regions as well as for CNO target. The various parameters investigated here are pseudorapidity distribution, mean normalised multiplicity, mean number of intranuclear collisions and normalised pseudorapidity.

2 data tables
Table 1

NUCLEUS IS AgBr (NUMBER(HTRACK) >= 9).

Table 2

NUCLEUS IS CNO (2 <= NUMBER(HTRACK) <= 5).


Inelastic interactions of Li-6 nuclei in emulsion at 4.5-A/GeV/c as a probe for Li-6 internal structure

El-Sharkawy, S. ;
Phys.Scripta 50 (1994) 97-101, 1994.
Inspire Record 383434 DOI 10.17182/hepdata.19309

The mean free path for inelastic interactions of 6Li in emulsion is measured and found not to be in systematic agreement with the different known theoretical parameterizations. This may be attributed to the loosely bound structure of 6Li nuclei. Possible internal structures of 6Li nuclei are investigated via the analysis of the shower particles multiplicity distributions for inclusive and central 6Li-Em interactions. In this analysis the experimental P-Em, d-Em and α-Em data are used as inputs for folding the corresponding distributions for 6Li-Em interactions. The results from central collisions favour the (α + d) cluster structure for the incident 6Li nuclei.

3 data tables
Table 1

INTERACTION WITH EMULSION NUCLEUS WAS MEASURED.

Table 2

INTERACTION WITH average AgBr NUCLEUS WAS MEASURED.

Table 3

INTERACTION WITH average AgBr NUCLEUS WAS MEASURED.


Forward - backward charge asymmetry of quark pairs produced at the KEK TRISTAN e+ e- collider

The AMY collaboration Stuart, D. ; Breedon, R.E. ; Chinitz, L.M. ; et al.
Phys.Rev.D 49 (1994) 3098-3105, 1994.
Inspire Record 378569 DOI 10.17182/hepdata.22552

We report on a measurement of the forward-backward charge asymmetry in e+e−→qq¯ at KEK TRISTAN, where the asymmetry is near maximum. We sum over all flavors and measure the asymmetry by determining the charge of the quark jets. In addition we exploit flavor dependencies in the jet charge determination to enhance the contributions of certain flavors. This provides a check on the asymmetries of individual flavors. The measurement agrees with the standard model expectations.

1 data table
Table 1

Forward--backward asymmetry summed over all flavours of quarks.


Measurements of cross-section and asymmetry for e+ e- ---> b anti-b and heavy quark fragmentation at KEK TRISTAN

The AMY collaboration Liu, F. ; Chinitz, L.M. ; Abe, K. ; et al.
Phys.Rev.D 49 (1994) 4339-4347, 1994.
Inspire Record 381324 DOI 10.17182/hepdata.22547

Using 773 muons found in hadronic events from 142 pb−1 of data at a c.m. energy of 57.8 GeV, we extract the cross section and forward-backward charge asymmetry for the e+e−→bb¯ process, and the heavy quark fragmentation function parameters for the Peterson model. For the analysis of the e+e−→bb¯ process, we use a method in which the behavior of the c quark and lighter quarks is assumed, with only that of the b quark left indeterminate. The cross section and asymmetry for e+e−→bb¯ are found to be Rb = 0.57 ± 0.06(stat) ± 0.08(syst) and Ab = −0.59 ± 0.09 ± 0.09, respectively. They are consistent with the standard model predictions. For the study of the fragmentation function we use the variable 〈xE〉, the fraction of the beam energy carried by the heavy hadrons. We obtain 〈xE〉c=0.56−0.05−0.03+0.04+0.03 and 〈xE〉b=0.65−0.04−0.06+0.06+0.05, respectively. These are in good agreement with previously measured values.

4 data tables
Table 1

No description provided.

Table 2

No description provided.

Table 3

Here X=E(hadron)/E(beam).

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A Study of single photon production in e+ e- annihilation at S**(1/2) = 58-GeV

The VENUS collaboration Hosoda, N. ; Abe, K. ; Amako, K. ; et al.
Phys.Lett.B 331 (1994) 211-216, 1994.
Inspire Record 371909 DOI 10.17182/hepdata.38390

We have studied single photon production in e + e − annihilation based on a data sample corresponding to an integrated luminosity of 164.1 pb −1 at s =58 GeV . The single photon yield is consistent with the prediction of the standard model with three light neutrino species. No anomalous signal has been observed. From this result left- and right-handed scalar electrons in the mass degenerate case are excluded at 90% CL below 44.4 GeV/ c 2 for the massless photino.

1 data table
Table 1

No description provided.


Hadron production in S + Ag and S + Au collisions at 200-GeV/nucleon

The NA35 collaboration Röhrich, Dieter ; Alber, T. ; Bächler, J. ; et al.
Nucl.Phys.A 566 (1994) 35C-44C, 1994.
Inspire Record 378631 DOI 10.17182/hepdata.36563

None

3 data tables
Table 1

No description provided.

Table 2

NET BARYON DENSITY D(N)/D(Y) HAS BEEN DETERMINED AT THE RAPIDITY OF NN C.M.S., FOR NET BARYON THE FORMULAR: 2*(P-PBAR)+1.6*(LAMBDA- LAMBDABAR) HAS BEEN USED.

Table 3

No description provided.


First measurement of the charged current cross-section at HERA

The H1 collaboration Ahmed, T. ; Andreev, V. ; Andrieu, B. ; et al.
Phys.Lett.B 324 (1994) 241-248, 1994.
Inspire Record 371597 DOI 10.17182/hepdata.45134

The cross section of the charged current process e − p → v e + hadrons is measured at HERA for transverse momenta of the hadron system larger than 25 GeV. The size of the cross section exhibits the W propagator.

1 data table
Table 1

No description provided.