Precision study of the eta-3He system using the d+p->3He+eta reaction

Mersmann, T. ; Khoukaz, A. ; Buscher, M. ; et al.
Phys.Rev.Lett. 98 (2007) 242301, 2007.
Inspire Record 743387 DOI 10.17182/hepdata.31493

The differential and total cross sections for the d+p->3He+eta reaction have been measured in a high precision high statistics COSY-ANKE experiment near threshold using a continuous beam energy ramp up to an excess energy Q of 11.3 MeV with essentially 100% acceptance. The kinematics allowed the mean value of Q to be determined to about 9 keV. Evidence is found for the effects of higher partial waves for Q>4 MeV. The very rapid rise of the total cross section to its maximum value within 0.5 MeV of threshold implies a very large eta-3He scattering length and hence the presence of a quasi-bound state extremely close to threshold.

2 data tables

Total cross section measurements.

Angular distribution asymmetry parameter defined as:. SIG(TOTAL)*(1+ASYM*COS(THETA(CM))/4*PI.


Near threshold eta meson production in the d d --> He-4 eta reaction.

Wrońska, A. ; Hejny, V. ; Wilkin, C. ; et al.
Eur.Phys.J.A 26 (2005) 421-428, 2005.
Inspire Record 695766 DOI 10.17182/hepdata.43489

The d+d->alpha+eta reaction has been investigated near threshold using the ANKE facility at COSY-Juelich. Both total and differential cross sections have been measured at two excess energies, Q=2.6 MeV and 7.7 MeV, with a subthreshold measurement being undertaken at Q=-2.6 MeV to study the physical background. While consistent with isotropy at the lower energy, the angular distribution reveals a pronounced anisotropy at the higher one, indicating the presence of higher partial waves. Options for the decomposition into partial amplitudes and their consequences for determination of the s-wave eta-alpha scattering length are discussed.

3 data tables

Measured cross sections. Systematic (DSYS) error does not include the luminosity uncertainty.

Experimental angular distribution at excess energy 2.6 MeV.

Experimental angular distribution at excess energy 7.7 MeV.


Threshold enhancement in eta photoproduction from 2H and 4He

Hejny, V. ; Weiss, J. ; Achenbach, P. ; et al.
Eur.Phys.J.A 13 (2002) 493-499, 2002.
Inspire Record 588187 DOI 10.17182/hepdata.43669

The photoproduction of eta-mesons from 2H and 4He has been studied for energies close to the production thresholds. The experiments were carried out with the tagged photon beam of the Mainz MAMI accelerator. The eta-mesons were detected via their two photon decays with the electromagnetic calorimeter TAPS. Total cross sections, angular and momentum distributions of the eta-mesons have been determined for both reactions. The total cross sections in the threshold region show a large enhancement over the predictions of a participant - spectator model, indicating significant final state interaction effects. The results are compared to recent model calculations taking into account nucleon-nucleon and nucleon-eta final state interaction effects on different levels of sophistication.

9 data tables

Total inclusive photoproduction cross sections. Statistical errors only.

Angular distributions of ETA mesons from the Deuterium target in the photon-nucleus cm system. Statistical errors only.

Angular distributions of ETA mesons from the Deuterium target in the photon-nucleus cm system. Statistical errors only.

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Near threshold photoproduction of eta mesons from He-4.

Hejny, V. ; Achenbach, P. ; Ahrens, J. ; et al.
Eur.Phys.J.A 6 (1999) 83-89, 1999.
Inspire Record 509583 DOI 10.17182/hepdata.43494

None

1 data table

SIG(Q=N) and SIG(Q=P) ratio is extracted from the data of scattering on HE4.


Multistep production of eta and hard pi0 mesons in subthreshold Au Au collisions.

Wolf, A.R. ; Appenheimer, M. ; Averbeck, R. ; et al.
Phys.Rev.Lett. 80 (1998) 5281-5284, 1998.
Inspire Record 471975 DOI 10.17182/hepdata.41989

The neutral π0 and η mesons are studied in 197Au−197Au collisions at an incident energy of 800AMeV, substantially below the threshold for η production in N−N collisions. While the gross π0 multiplicity increases almost linearly with the number of participant nucleons, the multiplicities of η and hard π0 mesons show a stronger than linear dependence. The nonlinearity is governed by the average transverse-mass excess 〈mt〉−(s−2mN) of the mesons and is insensitive to their final-state interaction in the nuclear medium.

4 data tables

No description provided.

No description provided.

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Near threshold photoproduction of eta mesons from complex nuclei

Röbig-Landau, M. ; Ahrens, J. ; Anton, G. ; et al.
Phys.Lett.B 373 (1996) 45-50, 1996.
Inspire Record 429457 DOI 10.17182/hepdata.28390

Total and differential cross sections for photoproduction of η mesons from 12 C, 40 Ca, 93 Nb, and nat Pb have been obtained up to 790 MeV incident photon energy at the Mainz Microtron (MAMI) with the TAPS spectrometer. The absorption cross section σ ηN abs = (30 ± 2.5 ± 6)mb of η mesons in nuclear matter and the absorption length λ η = (2.0 ± 0.2 ± 0.4) fm are extracted. No significant depletion of the S 11 (1535) strength in the η photoproduction on nuclei is observed.

1 data table

THE TOTAL SIG WAS PARAMETRIZED BY A**POWER.


Near threshold photoproduction of $\eta$-mesons from the deuteron

Krusche, B. ; Ahrens, J. ; Annand, J.R.M. ; et al.
Phys.Lett.B 358 (1995) 40-46, 1995.
Inspire Record 406946 DOI 10.17182/hepdata.28490

The first measurement of incoherent η-photoproduction from the deuteron in the threshold region is reported. The experiment was carried out at the MAMI accelerator with the TAPS spectrometer. Total and differential inclusive cross sections have been obtained between 627 and 790 MeV. It is found that the reaction is completely dominated by the incoherent part. An upper limit for coherent η-photoproduction on the deuteron is deduced, which is substantially lower than the result from an earlier measurement. The incoherent cross section is reproduced in a participant-spectator approach under the assumption of an energy-independent ratio between the neutron and proton cross sections. Best agreement is found for the ratio σ n σ p ≈ 2 3 . The implications for the isospin components of the electromagnetic excitation of the S 11 (1535) resonance are discussed.

1 data table

The helicity amplitudes A(1/2) = <S11|j(em)|nucleon> are measured.