Measured values of CNN at EKIN 2035 Mev (from run period IV).. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.056.

Measured values of CNN at EKIN 2115 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.046.

Measured values of CNN at EKIN 2155 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.039.

Measured values of CNN at EKIN 2175 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.041.

Measured values of CNN at EKIN 2215 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.038.

Measured values of CNN at EKIN 2225 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.049.

Measured values of CNN at EKIN 2235 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.043.

Measured values of CNN at EKIN 2245 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.048.

Measured values of CNN at EKIN 2395 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.047.

Measured values of CNN at EKIN 2445 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.049.

Measured values of CNN at EKIN 2495 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.043.

Measured values of CNN at EKIN 2515 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.044.

Measured values of CNN at EKIN 2565 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.044.

Measured values of CNN at EKIN 2575 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.044.

Measured values of CNN at EKIN 2595 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.042.

Measured values of CNN at EKIN 2645 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.043.

Measured values of CNN at EKIN 2795 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.066.

Measured values of CNN at EKIN 1955 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.086.

Measured values of CNN at EKIN 1975 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.072.

Measured values of CNN at EKIN 1995 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.101.

Measured values of CNN at EKIN 2015 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.079.

Measured values of CNN at EKIN 2035 Mev (from run period I).. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.070.

Measured values of CNN at EKIN 2035 Mev (from run period II).. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.065.

Measured values of CNN at EKIN 2055 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.070.

Measured values of CNN at EKIN 2075 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.064.

Measured values of CNN at EKIN 2095 Mev (from run period I).. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.068.

Measured values of CNN at EKIN 2095 Mev (from run period II).. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.050.

Measured values of CNN at EKIN 2115 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.071.

Measured values of CNN at EKIN 2135 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.070.

Measured values of CNN at EKIN 2155 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.067.

Measured values of CNN at EKIN 2175 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.067.

Measured values of CNN at EKIN 2205 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.073.

Measured values of CNN at EKIN 2215 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.085.

Measured values of CNN at EKIN 2225 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.070.

Measured values of CNN at EKIN 2235 Mev.. Fractional systematic uncertainty in the absolute beam and target polarization is +-0.066.

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.