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The Λ p å Λ p cross section has been measured in the Λ-momentum range of 120 to 320 MeV/ c using 238 events. A comparison with the effective range approximation yielded the values a s = −2.46, a t = −2.07, r s = 3.87 and r t = 4.50 in fm.

1 data table

Table 1

No description provided.

Experimental results on the annihilation $\bar{p} p \to \bar{K} K\pi$ at rest; $K^{*}$ production

Armenteros, R. ; Edwards, D.N. ; Jacobsen, T. ; et al.

Phys.Lett. 17 (1965) 170-171, 1965.

Inspire Record 1389661 DOI 10.17182/hepdata.30259

None

1 data table

Table 1

No description provided.

Observation of the heavy nucleon isobar $N^{∗}_\frac1{2}(3690)$

Bartke, J. ; Czyżewski, O. ; Danysz, J.A. ; et al.

Phys.Lett.B 24 (1967) 118-120, 1967.

Inspire Record 1389636 DOI 10.17182/hepdata.29588

The analysis of the eight-prong interactions of 8 GeV/ c π + with protons indicates the existence of the new heavy nucleon isobar with the mass M = 3.69 GeV and the isospin T = 1 2 .

1 data table

Table 1

No description provided.

Phase shift analysis of K+p elastic scattering at 780 MeV/c

Focardi, S. ; Minguzzi-Ranzi, A. ; Monari, L. ; et al.

Phys.Lett.B 24 (1967) 90461 314-317, 1967.

Inspire Record 1389646 DOI 10.17182/hepdata.29618

A phase shift analysis of the K+p elastic scattering at 780 MeV/c has been performed. The experimental differential cross section is best explained by a solution with dominant s wave, negative s wave phase shift (−42.7 ± 1 deg.) and small contributions of p and d waves.

1 data table

Table 1

Corrected for PI+ P events and scanning efficiency.

Backward Kp elastic scattering at 3.55 GeV/c

Banaigs, J. ; Berger, J. ; Bonnel, C. ; et al.

Phys.Lett.B 24 (1967) 90462 317-320, 1967.

Inspire Record 1389626 DOI 10.17182/hepdata.29619

Backward elastic K+p and K−p scattering has been measured in the angular interval 168o <θc.m. < 177o. We find <math altimg="si1.gif">(<rm>d</rm>σ/<rm>d</rm>Ω) <inf loc="post"><rm>K</rm>+<rm>p</rm> → <rm>pK</rm>+</inf> = 17 ± 4 μ<rm>b</rm>/<rm>sr</rm></math> and <math altimg="si2.gif">(<rm>d</rm>σ/<rm>d</rm>Ω)<inf loc="post"><rm>K</rm>−<rm>p</rm> → <rm>pK</rm>−</inf> < 0.6 μ<rm>b</rm>/<rm>sr</rm></math>. K+p elastic scattering exhibits a backward peak.

2 data tables

Table 1

The data for cos(theta) = 1 is the extrapolation.

Table 2

The data for cos(theta) = 1 is the extrapolation.

Study of the $e^+ e^-\to\mu^+ \mu^- \gamma$ reaction at center-of-mass energies between 54 and 64 GeV

The VENUS collaboration Yonezawa, Y. ; Abe, K. ; Amako, K. ; et al.

Phys.Lett.B 264 (1991) 212-218, 1991.

Inspire Record 1389624 DOI 10.17182/hepdata.29359

The cross section and forward-backward muon charge asymmetry for the e + e − → μ + μ − γ reaction were measured to be σ =2.82±0.35 pb and A =−0.34±0.10 with the VENUS detector at TRISTAN at 〈√ s 〉=59.2GeV for an integrated luminosity of 53.5 pb −1 . The measured cross section agrees with the theoretical prediction. The asymmetry result is consistent with the electroweak prediction but not with the QED prediction at the level of 2 σ .

2 data tables

Table 1

No description provided.

Table 2

No description provided.

Neutrons from the breakup of $^{19}$C

Marqués, F.M. ; Liegard, E. ; Orr, N.A. ; et al.

Phys.Lett.B 381 (1996) 407-412, 1996.

Inspire Record 1389647 DOI 10.17182/hepdata.55047

Neutrons arising from the breakup of a 30 MeV/nucleon 19 C beam on a tantalum target have been measured using the 98 element array DEMON. A narrow, forward peaked neutron angular distribution, with a corresponding momentum spread considerably smaller than those measured simultaneously for 21 N, 22 O and 24 F, was observed for charged fragments with Z < Z proj . Interpreted in terms of the core-breakup reaction model, the results support the existence of a one neutron halo in 19 C.

2 data tables

Table 1

No description provided.

Table 2

No description provided.

Total charge-changing cross sections for neutron-deficient isotopes from $^{58}$Ni fragmentation

Blank, B. ; Andriamonje, S. ; Del Moral, R. ; et al.

Z.Phys.A 352 (1995) 69-75, 1995.

Inspire Record 1389077 DOI 10.17182/hepdata.16503

At the projectile-fragment separator FRS of GSI, relativistic secondary beams of about 520 MeV/nucleon were produced by fragmentation of a primary beam of58Ni at 650 MeV/nucleon in a beryllium target. By means of aΔE—Bρ—TOF measurement, the fragments have been identified and their charge-changing probabilities in targets of CH2, C, Al, and Pb have been determined. We describe the results for the total charge-changing cross sections in this first paper, whereas a second article deals with the partial charge-changing cross sections. At the drip line, the measured charge-changing cross sections exhaust close to 100% of the total interaction cross sections as calculated with semiempirical models. The measurements at the proton drip line with low-Z targets indicate that only a very small increase of the cross sections may be observed, whereas the measurements with a lead target show that no significant increase of the total charge-changing cross sections is present which would be a hint for low-lying dipole strength. Our experimental data are compared to Glauber-type calculations.

24 data tables

Table 1

Nucleus is C H2.

Table 2

Nucleus is C H2.

Table 3

Nucleus is C H2.

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The charge exchange $K^- + p \to K^0 + n$ at 9.50 GeV/c

Low-momentum interactions of Σ hyperons with protons

Low energy $\Lambda p \to \Lambda p$ cross section measurement and determination of S-wave scattering lengths

Experimental results on the annihilation $\bar{p} p \to \bar{K} K\pi$ at rest; $K^{*}$ production

Observation of the heavy nucleon isobar $N^{∗}_\frac1{2}(3690)$

Phase shift analysis of K+p elastic scattering at 780 MeV/c

Backward Kp elastic scattering at 3.55 GeV/c

Study of the $e^+ e^-\to\mu^+ \mu^- \gamma$ reaction at center-of-mass energies between 54 and 64 GeV

Neutrons from the breakup of $^{19}$C

Total charge-changing cross sections for neutron-deficient isotopes from $^{58}$Ni fragmentation