Analysing power measurements in the scattering of polarized protons from either hydrogen in the LiH target or on bound protons in the LiD target. The three sets of results are independent.

Analysing power measurements in the scattering of polarized protons from either hydrogen in the LiH target or on bound protons in the LiD target. The three sets of results are independent.

Analysing power measurements in the scattering of polarized protons from either hydrogen in the LiH target or on bound protons in the LiD target. The three sets of results are independent.

Analysing power measurements in the scattering of polarized protons from either hydrogen in the LiH target or on bound protons in the LiD target. The three sets of results are independent.

The P P analysing power in elastic and quasi-elastic scattering on free (C=H) and strongly bound (C=C) protons in the CH2 target. All results are independent.

The P P analysing power in elastic and quasi-elastic scattering on free (C=H) and strongly bound (C=C) protons in the CH2 target. All results are independent.

The P P analysing power in elastic and quasi-elastic scattering on free (C=H) and strongly bound (C=C) protons in the CH2 target. All results are independent.

The P P analysing power in elastic and quasi-elastic scattering on free (C=H) and strongly bound (C=C) protons in the CH2 target. All results are independent.

The P P analysing power in elastic and quasi-elastic scattering on free (C=H) and strongly bound (C=C) protons in the CH2 target. All results are independent.

The P P analysing power in elastic and quasi-elastic scattering on free (C=H) and strongly bound (C=C) protons in the CH2 target. All results are independent.

The P P analysing power in elastic and quasi-elastic scattering on free (C=H) and strongly bound (C=C) protons in the CH2 target. All results are independent.

The spin correlation parameter CNN in the scattering of polarized protons from polarized hydrogen in the LiH target (C=H). At 1.095 GeV to uncertainty in the target polarization is 4 PCT.

The spin correlation parameter CNN in the scattering of polarized protons from polarized bound protons in the LiD target (Li+D(+H)). At 1.095 GeV to uncertainty in the target polarization is 4 PCT.

The spin correlation parameter CNN in the scattering of polarized protons from polarized bound protons in the LiD target (Li+D(+H)). At 1.095 GeV to uncertainty in the target polarization is 4 PCT.

The depolarization parameter DNN from elastic scattering of polarized protons on the polarized LiH target. The relative systematic error provided by the normalization uncertainty in the P-C analysing power is +- 6 PCT. There is also a +- 15 PCT uncertainty due to the relative normalization of measurements with the two opposite, (and small) target polarization values.

The polarization transfer parameter KNN measured with polarized protons on the polarized LiH and LiD targets. The relative uncertainty due to the P-C analysing power is +- 6 PCT.

The polarization transfer parameter KNN measured with polarized protons on the polarized LiD target. The relative uncertainty due to the P-C analysing power is +- 6 PCT.

The polarization transfer parameter KNN measured with polarized protons on the polarized LiD target. The relative uncertainty due to the P-C analysing power is +- 6 PCT.

The polarization transfer parameter KNN measured with polarized protons on the polarized LiH and LiD targets. The relative uncertainty due to the P-C analysing power is +- 6 PCT.

The polarization transfer parameter KNN measured with polarized protons on the polarized LiH and LiD targets. The relative uncertainty due to the P-C analysing power is +- 6 PCT.

The polarization transfer parameter KNN measured with polarized protons on the polarized LiH and LiD targets. The relative uncertainty due to the P-C analysing power is +- 6 PCT.

The polarization transfer parameter KNN measured with polarized protons on the polarized LiH and LiD targets. The relative uncertainty due to the P-C analysing power is +- 6 PCT.

The PN analysing power of polarized protons scattered on the polarized and/or unpolarized LiD and LiH targets.

The PN analysing power of polarized protons scattered on the polarized and/or unpolarized LiD and LiH targets.

The PN analysing power of polarized protons scattered on the polarized and/or unpolarized LiD and LiH targets.

The PN analysing power of polarized protons scattered on the polarized and/or unpolarized LiD and LiH targets.

The PN analysing power of polarized protons scattered on neutrons bound in carbon nuclei in the CH2 target.

The PN spin correlation parameter CNN of polarized protons scattered on polarized neutrons bound in the LiD target. The target polarization uncertainty is 4 PCT at 1.095 GeV and 10 PCT at 1.595 GeV.

The PN spin correlation parameter CNN of polarized protons scattered on polarized neutrons bound in the LiD target. The target polarization uncertainty is 4 PCT at 1.095 GeV and 10 PCT at 1.595 GeV.

The depolarization parameter DNN for quasi-elastic PN scattering of polarized protons on LiD and LiH targets. The relative systematic error provided by thenormalization uncertainty in the P-C analysing power is 6 PCT.

The depolarization parameter DNN for quasi-elastic PN scattering of polarized protons on LiD and LiH targets. The relative systematic error provided by thenormalization uncertainty in the P-C analysing power is 6 PCT.

The depolarization parameter DNN for quasi-elastic PN scattering of polarized protons on LiD and LiH targets. The relative systematic error provided by thenormalization uncertainty in the P-C analysing power is 6 PCT.

The depolarization parameter DNN for quasi-elastic PN scattering of polarized protons on LiD and LiH targets. The relative systematic error provided by thenormalization uncertainty in the P-C analysing power is 6 PCT.

The depolarization parameter DNN for quasi-elastic PN scattering of polarized protons on LiD and LiH targets. The relative systematic error provided by thenormalization uncertainty in the P-C analysing power is 6 PCT.

The depolarization parameter DNN for quasi-elastic PN scattering of polarized protons on LiD and LiH targets. The relative systematic error provided by thenormalization uncertainty in the P-C analysing power is 6 PCT.

The depolarization parameter DNN for quasi-elastic PN scattering of polarized protons on LiD and LiH targets. The relative systematic error provided by thenormalization uncertainty in the P-C analysing power is 6 PCT.

No description provided.

Axis error includes +- 5/5 contribution (DUE TO ANALYZING POWER UNCERTAINTY).