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INCLUSIVE STUDY OF NEUTRINO AND ANTI-NEUTRINO INTERACTIONS WITH NUCLEI AT ENERGIES E anti-neutrino <= 30-GeV

Ammosov, V.V. ; Baranov, D.S. ; Bugorsky, A.P. ; et al.
Z.Phys.C 30 (1986) 175, 1986.
Inspire Record 215974 DOI 10.17182/hepdata.15918

None

6 data tables
Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.

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ASYMMETRY OF CROSS-SECTIONS FOR THE REACTION GAMMA HE-3 ---> P D WITH LINEARLY POLARIZED GAMMA RAYS

Belyaev, A.A. ; Getman, V.A. ; Gorbenko, V.G. ; et al.
JETP Lett. 40 (1984) 1275-1277, 1984.
Inspire Record 220217 DOI 10.17182/hepdata.16924

None

2 data tables
Table 1

No description provided.

Table 2

No description provided.


POSSIBLE OBSERVATION OF NARROW TWO PROTON RESONANCES IN HADRON NUCLEUS INTERACTIONS

Azimov, S.A. ; Allaberdin, M.L. ; Edgorov, S.O. ; et al.
JETP Lett. 40 (1984) 1109-1111, 1984.
Inspire Record 218921 DOI 10.17182/hepdata.16927

None

2 data tables
Table 1

No description provided.

Table 2

No description provided.


NONCONSERVATION OF PARITY IN ATOMIC BISMUTH

Birich, G.N. ; Bogdanov, Yu.V. ; Kanorsky, S.I. ; et al.
Sov.Phys.JETP 60 (1984) 442-449, 1984.
Inspire Record 221351 DOI 10.17182/hepdata.16986

None

1 data table
Table 1

No description provided.


MEASUREMENT OF POLARIZATION OF PROTONS FROM THE REACTION GAMMA P ---> P PI0 AT THETA (PI) = 110-DEGREES C.M. IN THE RANGE OF THE SECOND AND THIRD RESONANCES. (IN RUSSIAN)

Bratashevsky, A.S. ; Zybalov, A.A. ; Karasev, S.P. ; et al.
Yad.Fiz. 42 (1985) 658-663, 1985.
Inspire Record 221959 DOI 10.17182/hepdata.17612

None

1 data table
Table 1

No description provided.


RESTRAINTS ON PARAMETERS OF OSCILLATIONS OF MUON NEUTRINOS FROM QUASIELASTIC SCATTERING DATA. (IN RUSSIAN)

Belikov, S.V. ; Volkov, A.A. ; Kochetkov, V.I. ; et al.
Yad.Fiz. 41 (1985) 919-924, 1985.
Inspire Record 219091 DOI 10.17182/hepdata.17585

None

1 data table
Table 1

Axis error includes +- 0.0/0.0 contribution (?////DUE TO UNCERTAINTY IN NU SPECTRUM).


ELASTIC SCATTERING OF 1-GEV PROTONS BY HE ISOTOPES. (IN RUSSIAN)

Alkhazov, G.D. ; Belostotsky, S.L. ; Dotsenko, Yu.V. ; et al.
Yad.Fiz. 41 (1985) 561-572, 1985.
Inspire Record 217236 DOI 10.17182/hepdata.17630

None

1 data table
Table 1

No description provided.


PI+ MESON PHOTOPRODUCTION ON CR, FE, AND NI ISOTOPES. (IN RUSSIAN)

Tonapetian, S.G. ; Khvorostian, V.M. ; Vinokurov, E.A. ; et al.
Yad.Fiz. 40 (1984) 728-730, 1984.
Inspire Record 215362 DOI 10.17182/hepdata.17633

None

1 data table
Table 1

No description provided.


DETERMINATION OF CROSS-SECTIONS OF INELASTIC INTERACTION OF PIONS AND NUCLEONS WITH FE NUCLEI IN THE ENERGY INTERVAL 0.5-TEV - 5-TEV. (IN RUSSIAN)

Avakian, V.V. ; Garyaka, A.P. ; Gevorkian, S.R. ; et al.
Yad.Fiz. 40 (1984) 949-959, 1984.
Inspire Record 218762 DOI 10.17182/hepdata.17632

None

4 data tables
Table 1

No description provided.

Table 2

No description provided.

Table 3

No description provided.

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STUDY OF THE MECHANISM OF THE He-3 p ---> p p d REACTION AT He-3 MOMENTUM OF 5-GeV/c

Blinov, A.V. ; Chuvilo, I.V. ; Drobot, V.V. ; et al.
Nucl.Phys.A 451 (1986) 701-727, 1986.
Inspire Record 214108 DOI 10.17182/hepdata.17644

The mechanism of the reaction 3 He + p → p + p + d is studied by making use of the ITEP 80 cm liquid-hydrogen bubble chamber exposed to a beam of 5 GeV/ c 3 He nuclei. The reaction cross section is equal to 20.6 ± 0.3 mb. The phase-space regions associated with quasifree scattering (QFS) and final-state interactions (FSI) are selected. Angular, mass and momentum distributions of the reaction products are obtained in the entire kinematically allowed range. The experimental data in the QFS region are compared with theoretical calculations based on the simplest pole-diagram approximation. The 3 He and deuteron wave functions (WF) correspond to the realistic RSC potential. The D-wave components of these WF are taken into account. The absolute value of the cross section and shape of the distributions are described as a whole reasonably well within the frame of the model considered in the kinematical region where FSI may be neglected. But at large spectator momenta there is an essential disagreement. The possible reasons for this are discussed.

2 data tables
Table 1

No description provided.

Table 2

No description provided.