Yoshida, H.
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Results on pi- p Backward Elastic Scattering and Search for pi- p --> d anti-p at 9-GeV/c and 12-GeV/c

Jacholkowski, A. ; Bouquet, B. ; D'Almagne, B. ; et al.
Nucl.Phys.B 126 (1977) 1-10, 1977.
Inspire Record 125076 DOI 10.17182/hepdata.35368

From an experiment done with the CERN Omega spectrometer, triggered by a fast forward proton device, we present results on the differential cross section d σ d u for π − p backward elastic scattering. The d σ d u distribution agrees with an A e Bu law. The compilation of existing results shows a discrepancy between results but the ( d σ d u ) u=0 data fit perfectly an s 2 α 0 −2 dependence, as predicted by a single Δδ Regge trajectory exchange. A search for the reaction π − p → d p , with a fast forward deuteron, which can be produced by a double-baryon exchange mechanism, gives cross-section upper limits of ∼1% of the backward elastic cross section.

4 data tables
Table 1

UMIN IS 0.0446 GEV**2.

Table 2

UMIN IS 0.0333 GEV**2.

Table 3

D(SIG)/DU FITTED FOR 0 < -U < 0.75 GEV**2 TO GIVE SLOPE/INTERCEPT.

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Baryon Exchange in the Reaction pi- p --> n*0 pi0 at 9-GeV/c and 12-GeV/c

Rouge, A. ; de Rosny, G. ; Fleury, P. ; et al.
Phys.Lett.B 69 (1977) 115-118, 1977.
Inspire Record 5224 DOI 10.17182/hepdata.27540

In π − p interactions at 9 GeV/ c and 12 GeV/ c , the forward production of N ∗ 1680 and N ∗ 1520 has been observed with features of nucleon exchange. The production of Δ1232 is strongly suppressed.

2 data tables
Table 1

No description provided.

Table 2

SLOPE ABOUT 6 GEV**-2 FOR SMALL U AND EVIDENCE FOR CHANGE OF SLOPE NEAR -U = 0.15 GEV**2.


Production of Fast Protons in the Forward Direction by a 12-GeV/c pi Beam at the omega Spark Chamber Spectrometer

Yoshida, H. ;
LAL-1292, 1977.
Inspire Record 122328 DOI 10.17182/hepdata.807

None

2 data tables
Table 1

No description provided.

Table 2

No description provided.


Anti-proton Proton Annihilation at Rest Into $\pi^0$ M and $\gamma$ M With M = $\phi$, $\eta^\prime$, $\omega$, $\rho^0$, $\eta$, and $\pi^0$

The Fukui-KEK-Kyoto Sangyo-Osaka-Tokyo Metropolitan collaboration Chiba, M. ; Fujitani, T. ; Iwahori, J. ; et al.
Phys.Rev.D 38 (1988) 2021, 1988.
Inspire Record 263258 DOI 10.17182/hepdata.23277

We have carried out high-statistics measurements of inclusive π0 and γ-ray spectra from p¯p annihilation at rest. From the monochromatic peaks in the π0 spectra, we derive the yield (or its upper limit) of the reaction p¯p→π0M for M=φ, η’, ω, ρ0, η, and π0. The same quantity was independently obtained from the γ-ray spectra, which included some π0’s that were mistaken as single γ rays due to the limited granularity of the γ detector. Taking the monochromatic peaks in the γ-ray spectra as being due to prompt γ rays, we also derive the upper limit for p¯p→γM.

2 data tables
Table 1

No description provided.

Table 2

No description provided.


Pontecorvo reactions in antiproton annihilation at rest in deuterium to pi0 n, pi0 Delta0, eta n and eta Delta0.

The Fukui-KEK-Kyoto Sangyo-Osaka-Tokyo Metropolitan collaboration Chiba, M. ; Fujitani, T. ; Iwahori, J. ; et al.
Phys.Rev.D 55 (1997) 2577-2583, 1997.
Inspire Record 424916 DOI 10.17182/hepdata.41181

Using modularized NaI(Tl) detectors, we carried out a high statistics measurement of inclusive γ-ray, π0, and η spectra, and determined the branching ratios or upper limits of Pontecorvo reactions p¯d→π0n, π0Δ0, ηn, and ηΔ0 from the corresponding monochromatic peaks in them. The obtained branching ratios are B(p¯d→π0n)=(1.03±0.41)×10−5, B(p¯d→π0Δ0)=(4.67±1.66)×10−5, B(p¯d→ηn)<8.94×10−6 (95% C.L.), and B(p¯d→ηΔ0)<6.49×10−5 (95% C.L.).

1 data table
Table 1

No description provided.


Backward rho- Production in the Reaction pi- p --> p pi- pi0 at 9-GeV/c and 12-GeV/c

Benkheiri, P. ; Eisenstein, Bob I. ; Fleury, P. ; et al.
Lett.Nuovo Cim. 20 (1977) 297, 1977.
Inspire Record 5542 DOI 10.17182/hepdata.37385

None

1 data table
Table 1

SIG(C=BACKWARD) = SIG(-UP<1 GEV**2)/(1-EXP(-SLOPE)). UP DISTRIBUTION OF EVENTS HAS A PERFECT EXPONENTIAL SHAPE.


Measurement of monochromatic pi0 and eta mesons in antiproton deuterium annihilation at rest.

Chiba, M. ; Fujitani, T. ; Iwahori, J. ; et al.
KEK-PREPRINT-97-247, 1998.
Inspire Record 467591 DOI 10.17182/hepdata.38331

None

2 data tables
Table 1

No description provided.

Table 2

No description provided.


Negative Pion Production from Neutrons by Polarized gamma Rays

Nishikawa, T. ; Hiramatsu, S. ; Kimura, Y. ; et al.
Phys.Rev.Lett. 21 (1968) 1288-1291, 1968.
Inspire Record 944914 DOI 10.17182/hepdata.38534

The differential asymmetry ratio for the process γ+n→p+π− was measured at 90° in the center-of-mass system and for incident photon energies from 352 to 550 MeV. The observed asymmetries are larger than the values predicted from the theory by Berends, Donnachie, and Weaver. A smaller M1- amplitude gives better agreement between the experiment and the theory.

2 data tables
Table 1

No description provided.

Table 2

No description provided.


Negative-pion photoproduction from neutrons by linearly polarized photons in the first resonance region

Kondo, K. ; Miyachi, T. ; Ukai, K. ; et al.
Phys.Rev.D 9 (1974) 529-533, 1974.
Inspire Record 93115 DOI 10.17182/hepdata.21954

The angular dependence of the asymmetry for negative-pion photoproduction on neutrons by linearly polarized photons has been measured for photon energies 260, 300, 350, 400, 450, and 500 MeV at center-of-mass angles 60°, 75°, 90°, 150°, and 120°. The results are compared with theoretical models of low-energy single-pion photoproduction. The observed asymmetry below 400 MeV shows good agreement with predictions of dispersion-theoretical models by Berends, Donnachie, and Weaver and by Schwela. The asymmetry values in the 400-500 MeV energy region suggest that smaller M1− amplitude is more favorable.

6 data tables
Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.

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Backward Production in $\pi^- p \to p_f \pi^+ \pi^- \pi^-$ Reaction at 9-{GeV}/$c$ and 12-{GeV}/$c$

Ferrer, A. ; Bouquet, B. ; D'Almagne, B. ; et al.
Nucl.Phys.B 142 (1978) 77-107, 1978.
Inspire Record 130740 DOI 10.17182/hepdata.34939

We have analyzed backward meson production in the reaction π − p → p f π + π − π − at 9 GeV/ c and 12 GeV/ c incident π − momenta, from an experiment performed at the CERN Ω Spectrometer using a fast proton (p f ) trigger device. We find strong production of quasi-two-body processes N ∗ ϱ and N ∗ f with a production mechanism consistent with u -channel nucleon exchange. At a lower level, we observe N ∗ π processes with a 3-body baryon decay through Δ(1232)π. In the (3π) − system, we find evidence for A 1 − and clear A 2 − backward production with similar cross sections (≈0.5 μb).

3 data tables
Table 1

No description provided.

Table 2

U-HELICITY JACKSON FRAME.

Table 3

U-HELICITY JACKSON FRAME.