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MEASUREMENT OF THE DIFFERENTIAL CROSS-SECTIONS OF THE REACTION gamma p ---> pi0 p IN THE RESONANCE REGION

Roderburg, Eduard ;
BONN-IR-78-7, 1978.
Inspire Record 129738 DOI 10.17182/hepdata.50152

None

1 data table
Table 1

No description provided.


Measurement of the Differential Cross-Section in Photoproduction of pi- Mesons

Sternemann, Klaus-Peter ;
BONN-IR-76-45, 1976.
Inspire Record 111853 DOI 10.17182/hepdata.50171

None

19 data tables
Table 1

No description provided.

Table 2

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Table 3

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Differential Cross-Sections for the pi0 Photoproduction at Theta (CM) = 90-Degrees and K (Lab) = 380-MeV-820-MeV

Jung, M. ; Kattein, J. ; Leu, P. ; et al.
BONN-HE-76-15, 1976.
Inspire Record 111677 DOI 10.17182/hepdata.50235

None

1 data table
Table 1

No description provided.


Photoeinfacherzeugung geladener $\pi$-Mesonen bei kleinen Impulsüberträgen im Energiebereich zwischen 2.6 und 6.0 GeV

Heide, Peter ;
DESY-F-35-69-01, 1969.
Inspire Record 917751 DOI 10.17182/hepdata.21701

None

6 data tables
Table 1

No description provided.

Table 2

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Table 3

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$\pi^+$ Photoproduction Between 1.2 and 3 GeV at Very Small Angles

Buschhorn, G. ; Carroll, J. ; Eandi, R.D. ; et al.
Phys.Rev.Lett. 18 (1967) 571-574, 1967.
Inspire Record 52312 DOI 10.17182/hepdata.21767

The reaction γ+p→π++n has been investigated for photon energies between 1.2 and 3 GeV and pion c.m. angles from 2.5 to 15°. The cross section is strongly peaked in the forward direction and shows resonance structure in the region of the N32*(1920) and N12*(2190).

10 data tables
Table 1

No description provided.

Table 2

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Table 3

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Photoproduction of $\pi^0$ in the Backward Direction

Buschhorn, G. ; Heide, P. ; Kotz, U. ; et al.
Phys.Rev.Lett. 20 (1968) 230-232, 1968.
Inspire Record 54459 DOI 10.17182/hepdata.21735

None

1 data table
Table 1

No description provided.


Photoproduction of Single Positive Pions Between 1.2 and 3 GeV

Buschhorn, G. ; Carroll, J. ; Eandi, R.D. ; et al.
Phys.Rev.Lett. 17 (1966) 1027-1030, 1966.
Inspire Record 50803 DOI 10.17182/hepdata.21795

Differential cross sections for the reaction γ+p→n+π+ are presented for incident photon energies between 1.2 and 3 GeV and pion center-of-mass production angles of 15 to 50 deg.

11 data tables
Table 1

No description provided.

Table 2

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Table 3

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Elastic electron - Proton Scattering at Large Four Momentum Transfer

Kirk, Paul N. ; Breidenbach, Martin ; Friedman, Jerome I. ; et al.
Phys.Rev.D 8 (1973) 63-91, 1973.
Inspire Record 73424 DOI 10.17182/hepdata.21999

Electron-proton elastic-scattering cross sections have been measured at the Stanford Linear Accelerator Center for four-momentum transfers squared q 2 from 1.0 to 25.0 (GeVc)2. The electric (GEp) and magnetic (GMp) form factors of the proton were not separated, since angular distributions were not measured at each q 2. However, values for GMp were derived assuming various relations between GEp and GMp. Several theoretical models for the behavior of the proton magnetic form factor at high values of q 2 are compared with the data.

22 data tables
Table 1

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Table 2

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Table 3

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Strange-particle production in {8-BeV/c} proton-proton interactions

Firebaugh, M. ; Ascoli, G. ; Goldwasser, E.L. ; et al.
Phys.Rev. 172 (1968) 1354-1369, 1968.
Inspire Record 53978 DOI 10.17182/hepdata.26501

A systematic survey of strange-particle final states produced by 8−BeVc protons was made in the BNL 80-in. hydrogen bubble chamber. Cross sections were measured for some 33 reactions. The ratio of the cross section for the KK¯ channels to the total strange-particle cross section was measured to be 0.12 and appears to be rising in this momentum region. The total cross section for strange-particle production is estimated as 1.8±0.2 mb. Comparison is made of the data with the predictions of the one-pion-exchange model, and at least partial agreement occurs for the K+pΛ and πKNΣ final states. The KpΣ states appear to contain N*(1924)→KΣ, and the πKNΛ states all include Y*(1385) production with the π+K0pΛ state also containing N*(1236) and K*(890) production. An examination of the five- and six-body K, Λ states indicates strong Y*(1385) and N*(1236) production. Finally, all final states containing a K and a Λ show a dependence on M(K,Λ) which is well parametrized by a Breit-Wigner shape with M0=1777 MeV and Γ=345 MeV. This behavior is interpreted as being consistent with one-pion exchange as the dominant mechanism for these reactions.

1 data table
Table 1

'1'. '2'.


Pion production in $\pi^-$ - $p$ interactions at energies 790, 830, and 870 {MeV}

Cason, N.M. ; Derado, I. ; Lamsa, J.W. ; et al.
Phys.Rev. 150 (1966) 1134-1140, 1966.
Inspire Record 50370 DOI 10.17182/hepdata.26587

Single-pion production has been studied in the reactions π−p→π−π+n and π−p→π−π0p at 790, 830, and 870 MeV. A total of 4193 events in these two channels, divided approximately equally between the three energies, have been identified. The most interesting feature of the data is the tendency for events to concentrate at high values of mππ and low values of four-momentum transfer. These effects are discussed in terms of conventional isobar models and a model involving two-pion exchange. Partial cross sections for the reactions studied are reported for each energy.

1 data table
Table 1

No description provided.