Search for double-Lambda hypernuclei and the H dibaryon in the (K-,K+) reaction on C-12.

The E885 collaboration Yamamoto, K. ; Alburger, D.E. ; Barnes, P.D. ; et al.
Phys.Lett.B 478 (2000) 401-407, 2000.
Inspire Record 528779 DOI 10.17182/hepdata.28030

A search for double- Λ hypernuclei ( 12 ΛΛ Be) and H -dibaryons using the 12 C( K − , K + ) reaction was performed at the BNL-AGS using a high-intensity 1.8 GeV/ c K − beam. A missing-mass analysis below the end point of the quasi-free Ξ − production was used to investigate these S =−2 systems. The upper limit obtained for the forward-angle cross section of 12 ΛΛ Be production is 6 to 10 nb/sr. This is the first search for the direct production of double- Λ hypernuclei to reach the sensitivity required to observe the signal predicted by theoretical calculations. For the H -production cross section, we have obtained an upper limit in the range of a few nb/sr to 10 nb/sr for the H mass below 2100 MeV/ c 2 . This upper limit is the most sensitive H search result to date for a tightly bound H .

2 data tables

Upper limit is given.

The production of the H-dibaryon could occur via the (K-, K+) reaction on two protons in a nucleus: K- (PP) --> K+ H-dibaryon. Upper limit is given.


Isospin resolved double pion production in the reaction p + d --> He-3 + 2pi.

Andersson, M. ; Bargholtz, C. ; Fransson, K. ; et al.
Phys.Lett.B 485 (2000) 327-333, 2000.
Inspire Record 532724 DOI 10.17182/hepdata.28016

Neutral and charged two-pion production in p+d→ 3 He+2 π reactions has been studied at CELSIUS at a proton beam energy of 477 MeV. The total cross section for double pion production is 0.22±0.03 μ b. The ratio of the cross sections for the production of charged pion pairs with isospin T =1 and T =0 was determined to be σ ( π + π − ; T =1)/ σ ( π + π − ; T =0)=1.4±0.4.

1 data table

(I=1, I=0) stands for isospin of PI+ PI- system.


Antiproton neon annihilation at 57-MeV/c.

Bianconi, A. ; Bonomi, G. ; Bussa, M.P. ; et al.
Phys.Lett.B 481 (2000) 194-198, 2000.
Inspire Record 529624 DOI 10.17182/hepdata.28015

The p ̄ Ne annihilation cross section is measured for the first time in the momentum interval (53÷63) MeV/c. About 9000 pictures collected by the Streamer Chamber Collaboration (PS179) at LEAR-CERN have been scanned. Four events are found, corresponding to σ ann =2210±1105 mb. The result is compared to the set of measurements presently available in the region of low p̄ momentum.

1 data table

No description provided.


Antineutron proton total cross section from 50-MeV/c to 400-MeV/c.

The OBELIX collaboration Iazzi, F. ; Feliciello, A. ; Agnello, M. ; et al.
Phys.Lett.B 475 (2000) 378-385, 2000.
Inspire Record 527242 DOI 10.17182/hepdata.28048

The antineutron–proton total cross section has been measured in the low momentum range 50–400 MeV/ c (below 100 MeV/ c for the first time). The measurement was performed at LEAR (CERN) by the OBELIX experiment, thanks to its unique antineutron beam facility. A thick target transmission technique has been used. The measured total cross section shows an anomalous behaviour below 100 MeV/ c . A dominance of the isospin I =0 channel over the I =1 one at low energy is clearly deduced.

1 data table

Measured values of the total cross section.


Energy dependence of the near-threshold total cross-section for the p p --> p p eta' reaction.

Moskal, P. ; Adam, H.H. ; Balewski, J.T. ; et al.
Phys.Lett.B 474 (2000) 416-422, 2000.
Inspire Record 522744 DOI 10.17182/hepdata.28036

Total cross sections for the pp --> pp eta' reaction have been measured in the excess energy range from Q = 1.53 MeV to Q = 23.64 MeV. The experiment has been performed at the internal installation COSY-11 using a stochastically cooled proton beam of the COoler SYnchrotron COSY and a hydrogen cluster target. The determined energy dependence of the total cross section weakens the hypothesis of the S-wave repulsive interaction between the eta' meson and the proton. New data agree well with predictions based on the phase-space distribution modified by the proton-proton final-state-interaction (FSI) only.

1 data table

Total cross sections w.r.t the excess energy in the CM system. Statistical errors only are given. As well as the 15 PCT overall systematic uncertainty there is an uncertainty on the energy of 0.44 MeV.


New analysis of the radiative decay omega --> eta gamma in proton - anti-proton annihilation at rest

Case, T. ; Crowe, K.M. ; Heinsius, F.H. ; et al.
Phys.Rev.D 61 (2000) 032002, 2000.
Inspire Record 522711 DOI 10.17182/hepdata.22247

We report on a measurement of the branching ratio of the rare decay ω→ηγ relative to the well known decay ω→π0γ. The ω’s are produced in pp¯→ηω and pp¯→π0ω. Eigenstate mixing and interference effects of the ω and ρ0 are taken into account, as well as coherent interference with the background. We find evidence for the non-resonant annihilation channel B(pp¯→ηηγ)=(3.5±1.3)×10−5 and limit the value of B(ω→ηγ) to the range of (0.7to5.5)×10−4 depending on the degree of coherence with the background.

1 data table

No description provided.


Measurement of spin observables in neutron proton elastic scattering. I: Correlation parameters

Arnold, J. ; van den Brandt, B. ; Daum, M. ; et al.
Eur.Phys.J.C 17 (2000) 67-81, 2000.
Inspire Record 537914 DOI 10.17182/hepdata.43392

The spin correlation parameters$A_{oonn}, A_{ooss}, A_{oosk}, A_{ookk}$and the analyzing power$A_{oono}$have been measured i

6 data tables

Values of the coefficients for the linear combinations of the spin correlation parameters Cpq measurements for the four different beam and target polarisation orientations. For the (z,z) and (y,y) configurations the coefficients are identical for all incident kinetic energies.

Measurement of the analysing power. Statistical errors only are shown. For the systematic errors see the systematics section above. Note that there are two overlapping angular settings.

Measurements of the spin correlation parameter CNN. Statistical errors onlyare shown. For the systematics see the systematic section above. Note the two overlapping angular settings.

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Measurement of spin observables in neutron proton elastic scattering. II: Rescattering parameters

Arnold, J. ; van den Brandt, B. ; Daum, M. ; et al.
Eur.Phys.J.C 17 (2000) 83-95, 2000.
Inspire Record 537915 DOI 10.17182/hepdata.43295

A double scattering experiment, performed at the Paul-Scherrer-Institut (PSI), has measured a large variety of spin observables for free np elastic scattering from 260 to 535 MeV in the c.m. angle ran

12 data tables

Relative uncertainties on the carbon polarimeter analysing power (AC).

Relative uncertainty in the beam polarisation (PB).

Measurements of DNN with statistical errors only.

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Near-threshold eta production in the p d --> p d eta reaction.

Hibou, F. ; Wilkin, Colin ; Bergdolt, A.M. ; et al.
Eur.Phys.J.A 7 (2000) 537-541, 2000.
Inspire Record 523315 DOI 10.17182/hepdata.43410

The total cross section of the p d -> p d eta reaction has been measured at two energies near threshold by detecting the final proton and deuteron in a magneti spectrometer. The values are somewhat larger than expected on the basis of two simple theoretical estimates.

1 data table

The first quoted error includes statistical and normalization uncertainties, the scond is that induced by the uncertainty in the excess energy.


Measurement of tensor polarization elastic electron deuteron scattering at large momentum transfer.

The JLAB t(20) collaboration Abbott, D. ; Ahmidouch, A. ; Anklin, H. ; et al.
Phys.Rev.Lett. 84 (2000) 5053-5057, 2000.
Inspire Record 523086 DOI 10.17182/hepdata.40433

Tensor polarization observables (t20, t21 and t22) have been measured in elastic electron-deuteron scattering for six values of momentum transfer between 0.66 and 1.7 (GeV/c)^2. The experiment was performed at the Jefferson Laboratory in Hall C using the electron HMS Spectrometer, a specially designed deuteron magnetic channel and the recoil deuteron polarimeter POLDER. The new data determine to much larger Q^2 the deuteron charge form factors G_C and G_Q. They are in good agreement with relativistic calculations and disagree with pQCD predictions.

5 data tables

No description provided.

No description provided.

No description provided.

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