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Polarization at Small Angles in Anti-proton - Carbon Elastic Scattering at {LEAR} Energies

The SING collaboration
Nucl.Phys. A487 (1988) 563-590, 1988

Abstract (data abstract)
POLARIZED BEAM, A DOUBLE-SCATTERING EXPERIMENT. THE AZIMUTHAL ASYMMETRY GIVEN IN TABELS IS DEFINED AS FOLLOWS. AFTER THE SECOND SCATTERING, THE ANGULAR DISTRIBUTION OF PBAR IS GIVEN BY: N(THETA2,FI)=NO(THETA2)*(1+ASYM*COS FI), WHERE THETA1 IS THE FIRST (ELASTIC) SCATTERING ANGLE. THETA2 FI IS THE ANGLE BETWEEN THE FIRST AND THE SECOND SCATTERING PLANES.

  • Table 1

    Data from T 4

    10.17182/hepdata.37001.v1/t1

    THETA1(RF=LAB)=8 DEG, THETA POINTED IN TABLE IS THE SECOND SCATTERING ANGLE.

  • Table 2

    Data from T 4

    10.17182/hepdata.37001.v1/t2

    THETA1(RF=LAB)=5 DEG, THETA POINTED IN TABLE IS THE SECOND SCATTERING ANGLE.

  • Table 3

    Data from T 4

    10.17182/hepdata.37001.v1/t3

    THETA1(RF=LAB)=8 DEG, THETA POINTED IN TABLE IS THE SECOND SCATTERING ANGLE.

  • Table 4

    Data from T 5

    10.17182/hepdata.37001.v1/t4

    THETA1(RF=LAB)=8 DEG, THETA POINTED IN TABLE IS THE SECOND SCATTERING ANGLE.

  • Table 5

    Data from T 5

    10.17182/hepdata.37001.v1/t5

    THETA1(RF=LAB)=5 DEG, THETA POINTED IN TABLE IS THE SECOND SCATTERING ANGLE.

  • Table 6

    Data from T 5

    10.17182/hepdata.37001.v1/t6

    THETA1(RF=LAB)=8 DEG, THETA POINTED IN TABLE IS THE SECOND SCATTERING ANGLE.

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