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Measured values of the P P analysing power at kinetic energy 2.035 GeV fromrun II. The relative and additive systematic errors are +- 0.050 and 0.001.

Measured values of the P P analysing power at kinetic energy 2.115 GeV. Therelative and additive systematic errors are +- 0.038 and 0.001.

Measured values of the P P analysing power at kinetic energy 2.155 GeV. Therelative and additive systematic errors are +- 0.030 and 0.001.

Measured values of the P P analysing power at kinetic energy 2.175 GeV. Therelative and additive systematic errors are +- 0.032 and 0.001.

Measured values of the P P analysing power at kinetic energy 2.215 GeV. Therelative and additive systematic errors are +- 0.028 and 0.001.

Measured values of the P P analysing power at kinetic energy 2.225 GeV. Therelative and additive systematic errors are +- 0.042 and 0.001.

Measured values of the P P analysing power at kinetic energy 2.235 GeV. Therelative and additive systematic errors are +- 0.034 and 0.001.

Measured values of the P P analysing power at kinetic energy 2.345 GeV. Therelative and additive systematic errors are +- 0.040 and 0.001.

Measured values of the P P analysing power at kinetic energy 2.395 GeV. Therelative and additive systematic errors are +- 0.039 and 0.002.

Measured values of the P P analysing power at kinetic energy 2.445 GeV. Therelative and additive systematic errors are +- 0.042 and 0.001.

Measured values of the P P analysing power at kinetic energy 2.495 GeV. Therelative and additive systematic errors are +- 0.034 and 0.002.

Measured values of the P P analysing power at kinetic energy 2.515 GeV. Therelative and additive systematic errors are +- 0.036 and 0.001.

Measured values of the P P analysing power at kinetic energy 2.565 GeV. Therelative and additive systematic errors are +- 0.036 and 0.001.

Measured values of the P P analysing power at kinetic energy 2.575 GeV. Therelative and additive systematic errors are +- 0.035 and 0.001.

Measured values of the P P analysing power at kinetic energy 2.595 GeV. Therelative and additive systematic errors are +- 0.034 and 0.001.

Measured values of the P P analysing power at kinetic energy 2.645 GeV. Therelative and additive systematic errors are +- 0.035 and 0.001.

Measured values of the P P analysing power at kinetic energy 2.795 GeV. Therelative and additive systematic errors are +- 0.061 and 0.001.

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.

Measurement values of the P P analysing power at kinetic energy 1.955 GeV. The relative and additive systematic errors are +- 0.082 and 0.003.

Measurement values of the P P analysing power at kinetic energy 1.975 GeV. The relative and additive systematic errors are +- 0.067 and 0.002.

Measurement values of the P P analysing power at kinetic energy 1.995 GeV. The relative and additive systematic errors are +- 0.098 and 0.002.

Measurement values of the P P analysing power at kinetic energy 2.015 GeV. The relative and additive systematic errors are +- 0.075 and 0.002.

Measurement values of the P P analysing power at kinetic energy 2.035 GeV from run I. The relative and additive systematic errors are +- 0.065 and 0.003.

Measurement values of the P P analysing power at kinetic energy 2.035 GeV from run II. The relative and additive systematic errors are +- 0.059 and 0.002.

Measurement values of the P P analysing power at kinetic energy 2.055 GeV. The relative and additive systematic errors are +- 0.065 and 0.003.

Measurement values of the P P analysing power at kinetic energy 2.075 GeV. The relative and additive systematic errors are +- 0.058 and 0.003.

Measurement values of the P P analysing power at kinetic energy 2.095 GeV from run I. The relative and additive systematic errors are +- 0.062 and 0.003.

Measurement values of the P P analysing power at kinetic energy 2.095 GeV from run II. The relative and additive systematic errors are +- 0.043 and 0.002.

Measurement values of the P P analysing power at kinetic energy 2.115 GeV. The relative and additive systematic errors are +- 0.066 and 0.003.

Measurement values of the P P analysing power at kinetic energy 2.135 GeV. The relative and additive systematic errors are +- 0.065 and 0.003.

Measurement values of the P P analysing power at kinetic energy 2.155 GeV. The relative and additive systematic errors are +- 0.062 and 0.004.

Measurement values of the P P analysing power at kinetic energy 2.175 GeV. The relative and additive systematic errors are +- 0.062 and 0.003.

Measurement values of the P P analysing power at kinetic energy 2.205 GeV. The relative and additive systematic errors are +- 0.068 and 0.003.

Measurement values of the P P analysing power at kinetic energy 2.215 GeV. The relative and additive systematic errors are +- 0.081 and 0.003.

Measurement values of the P P analysing power at kinetic energy 2.225 GeV. The relative and additive systematic errors are +- 0.065 and 0.003.

Measurement values of the P P analysing power at kinetic energy 2.235 GeV. The relative and additive systematic errors are +- 0.060 and 0.004.

Measurements of the spin correlation parameter CLL. Statistical errors onlyare shown. For the systematics see the systematic section above. Note the two overlapping angular settings.

Measurements of the combined spin observable Cpq measured in the (x,xz) position as a linear combination of CSS, CSL and CLL (see the table above for the coefficients). The errors are purely statistical. An extra 6 PCT uncertainty has to be added to the systematic errors shown in the systematic section above.

Measurements of the combined spin observable Cpq measured in the (x,z) position as a linear combination of CSL and CLL (see the table above for the coefficients). The errors are purely statistical. An extra 6 PCT uncertainty has to be added to the systematic errors shown in the systematic section above.

Measurements of DSL with statistical errors only.

Measurements of DSS with statistical errors only.

Measurements of KNN with statistical errors only.

Measurements of KSL with statistical errors only.

Measurements of KSS with statistical errors only.

Measurements of the triple spin parameter NNLL with statistical errors only.

Measurements of the triple spin parameter NSLN with statistical errors only.

Measurements of the triple spin parameter NSNS with statistical errors only.

Measurements of the triple spin parameter NSSN with statistical errors only.

Measurement of the rescattering parameter HSNS with the beam polarisation in the +- S direction and the target polarisation in the +- N direction. Additional 7.4 PCT systematic error.

Measurement of the rescattering parameter HSNS with the beam polarisation in the +- S direction and the target polarisation in the +- N direction. Additional 7.4 PCT systematic error.

Measurement of the rescattering parameter DLS with the beam polarisation inthe +- S direction and the target polarisation in the +- L direction. Additional 6.7 PCT systematic error.

Measurement of the rescattering parameter DLS with the beam polarisation inthe +- S direction and the target polarisation in the +- L direction. Additional 6.7 PCT systematic error.

Measurement of the rescattering parameter HSLN with the beam polarisation in the +- S direction and the target polarisation in the +- L or +- N directions. Additional 7.4 PCT systematic uncertainty.

Measurement of the rescattering parameter HSLN with the beam polarisation in the +- S direction and the target polarisation in the +- L or +- N directions. Additional 7.4 PCT systematic uncertainty.

Measurement of the rescattering parameters DNN and KNN for the beam and target polarisations in the +- N directions. Additional 6.7 PCT systematic error.

Measurement of the rescattering parameters DNN and KNN for the beam and target polarisations in the +- N directions. Additional 6.7 PCT systematic error.

Measurement of the rescattering parameters DNN and KNN for the beam and target polarisations in the +- N directions. Additional 6.7 PCT systematic error.

Measurement of the rescattering parameters DNN and KNN for the beam and target polarisations in the +- N directions. Additional 6.7 PCT systematic error.

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.

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.

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Analysing power measurements in P P elastic scattering LEN(C=CU) is the length of CU degrader thickness used in each group.

Analysing power measurements in P P elastic scattering LEN(C=CU) is the length of CU degrader thickness used in each group.

Analysing power measurements in P P elastic scattering LEN(C=CU) is the length of CU degrader thickness used in each group.

Data from 97.7 to 123.4 degrees are combined beam and target analyzing powers.

Data from 97.7 to 123.4 degrees are combined beam and target analyzing powers.

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Results of the analyzing power for n p scattering at 0.840 GeV.

Results of the analyzing power for n p scattering at 0.860 GeV.

Results of the analyzing power for n p scattering at 0.877 GeV. Data taken with the CH2 target.

Results of the analyzing power for n p scattering at 0.880 GeV.

Results of the analyzing power for n p scattering at 0.910 GeV.

Results of the analyzing power for n p scattering at 0.940 GeV.

Results of the analyzing power for n p scattering at 1.00 GeV.

Results of the analyzing power for n p scattering at 1.08 GeV.

Results of the analyzing power for n p scattering at 1.10 GeV.

Results of the analyzing power for n p scattering at 0.84 GeV measured with the additional CH2 target.

Results of the analyzing power for n p scattering at 0.86 GeV measured with the additional CH2 target.

Results of the analyzing power for n p scattering at 1.00 GeV measured with the additional CH2 target.

Results of the analyzing power for n p scattering at 1.10 GeV measured with the additional CH2 target.

Analyzing power for n p elastic and quasielastic scattering measured with the CH2 target at 0.363 GeV. Only recoil protons were detected.

Analyzing power for n p elastic and quasielastic scattering measured with the carbon target at 0.363 GeV. Only recoil protons were detected.

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Position 'A' (see text for explanation).

Position 'A' (see text for explanation).

Position 'B' (see text for explanation).

Position 'B' (see text for explanation).

Position 'B' (see text for explanation).

Position 'B' (see text for explanation).

Position 'B' (see text for explanation).

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Differential production cross-sections with respect to transverse momentum, dsigma / dp_T, of D*(2010)+ mesons or their charge conjugates in proton-proton collisions at center-of-mass (CM) energy sqrt(s) = 7 TeV. Measured in bins of hadron transverse momentum (p_T) and rapidity (y) with respect to the beam axis, where p_T and y are measured in the CM frame. Contributions of charm hadrons from the decays of b-hadrons have been removed.

Differential production cross-sections with respect to transverse momentum, dsigma / dp_T, of D_s+ mesons or their charge conjugates in proton-proton collisions at center-of-mass (CM) energy sqrt(s) = 7 TeV. Measured in bins of hadron transverse momentum (p_T) and rapidity (y) with respect to the beam axis, where p_T and y are measured in the CM frame. Contributions of charm hadrons from the decays of b-hadrons have been removed.

Combined cross section for c-cbar production. The second systematic error is the uncertainty due to the fragmentation functions.

Bin integrated production cross sections for prompt LAMBDA/C+ + CC baryons in YRAP bins integrated over PT from 2-8 GeV/c.

Single differential production cross sections of prompt J/PSI mesons and of J/PSI from B decay as a function of rapidity in the BACKWARD region. The errors shown are statistical and the uncorrelated and correlated components of the systematic uncertainties.

Double differential production cross sections of prompt J/PSI mesons as a function of transverse momentum and rapidity in the FORWARD region. The errors shown are statistical and the uncorrelated and correlated components of the systematic uncertainties.

Double differential production cross sections of J/PSI mesons from B decays as a function of transverse momentum and rapidity in the FORWARD region. The errors shown are statistical and the uncorrelated and correlated components of the systematic uncertainties.

The nuclear modification factor RpPB for PT < 14 GeV/c in the BACKWARD and FORWARD regions.

The FORWARD/BACKWARD production ratio R(FB) as a function of rapidity for PT < 14 GeV/c.

The FORWARD/BACKWARD production ratioo (R(FB) as a function of PT with |yrap|=2.5-4.0.

The product of the electronic width of the PHI(1020) and its branching fraction to KS KL.

Cross section measurement for PHI(1680).

Mass measurement for PHI(1680).

Measurement of the PHI(1680) width.

The product of the electronic width of the PHI(1680) and its branching fraction to KS KL.

The measured E+ E- --> KS KL cross section as a function of the centre-of-mass energy.

The measured E+ E- --> KS KL PI+ PI- cross section as a function of the centre-of-mass energy.

The measured E+ E- --> KS KS PI+ PI- cross section as a function of the centre-of-mass energy.

The measured E+ E- --> KS KS K+ K- cross section as a function of the centre-of-mass energy.

The product WIDTH(E+ E- --> J/PSI) * BR(J/PSI --> KS KL PI+ PI-) and the J/PSI branching fraction.

The product WIDTH(E+ E- --> J/PSI) * BR(J/PSI --> KS KS PI+ PI-) and the J/PSI branching fraction.

The product WIDTH(E+ E- --> J/PSI) * BR(J/PSI --> KS KS K+ K-) and the J/PSI branching fraction.

The product WIDTH(E+ E- --> J/PSI) * BR(J/PSI --> K*(892) KS PI) * BR(K*(892) --> KS PI) and the J/PSI branching fraction.

The product WIDTH(E+ E- --> J/PSI) * BR(J/PSI --> K2*(1430) KS PI) * BR(K2*(1430) --> KS PI) and the J/PSI branching fraction.

The product WIDTH(E+ E- --> J/PSI) * BR(J/PSI --> K*(892)+ K*(892)-) * (BR(K*(892) --> KS PI))**2 and the 90% C.L. J/PSI branching fraction.

The product WIDTH(E+ E- --> J/PSI) * BR(J/PSI --> K2*(1430) K*(892)) * BR(K2*(1430) --> KS PI) * BR(K*(892) --> KS PI) and the 90% C.L. J/PSI branching fraction.

The product WIDTH(E+ E- --> J/PSI) * BR(J/PSI --> KS KS PHI(1020)) * BR(PHI --> K+ K-) and the J/PSI branching fraction.

The product WIDTH(E+ E- --> J/PSI) * BR(J/PSI --> F2PRIME(1525) PHI(1020)) * BR(PHI --> K+ K-} * BR(F2PRIME(1525) --> KS KS) and the J/PSI branching fraction.

The product WIDTH(E+ E- --> J/PSI) * BR(J/PSI --> F2PRIME(1525) K+ K-) * BR(F2PRIME(1525) --> KS KS) and the J/PSI branching fraction.

Normalized differential cross-section $d\ln\sigma(pp\rightarrow J/\psi \Lambda_c^+ X)/dp_T(J/\psi)$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(\Lambda_c^+)<4$, $3<p_T(\Lambda_c^+) <12$ GeV/$c$ region.

Normalized differential cross-section $d\ln\sigma(pp\rightarrow J/\psi D^0 X)/dp_T(D^0)$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ region.

Normalized differential cross-section $d\ln\sigma(pp\rightarrow J/\psi D^+ X)/dp_T(D^+)$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $d\ln\sigma(pp\rightarrow J/\psi D_s^+ X)/dp_T(D_s^+)$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D_s^+)<4$, $3<p_T(D_s^+)<12$ GeV/$c$ region.

Normalized differential cross-section $d\ln\sigma(pp\rightarrow J/\psi \Lambda_c^+ X)/dp_T(\Lambda_c^+)$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(\Lambda_c^+)<4$, $3<p_T(\Lambda_c^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^0 X \right)}{dp_T( D^0 )}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^+ X \right)}{dp_T( D )}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D_s^+ X \right)}{dp_T( D )}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(D_s^+)<4$, $3<p_T(D_s^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D^+ X \right)}{dp_T( D^+ )}$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D_s^+ X \right)}{dp_T( D )}$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$, $2<y(D_s^+)<4$, $3<p_T(D_s^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 \bar{D}^0 X \right)}{dp_T( D )}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^- X \right)}{dp_T( D )}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12~GeV/c$, $2<y(D^-)<4$, $3<p_T(D^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D_s^- X \right)}{dp_T( D )}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(D_s^-)<4$, $3<p_T(D_s^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 \bar{\Lambda}_c^- X \right)}{dp_T( C )}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(\bar{\Lambda}_c^-)<4$, $3<p_T(\bar{\Lambda}_c^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D- X \right)}{dp_T( D )}$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D_s- X \right)}{dp_T( D )}$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$, $2<y(D_s^-)<4$, $3<p_T(D_s^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ \bar{\Lambda}_c^- X \right)}{dp_T( C )}$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$, $2<y(\bar{\Lambda}_c^-)<4$, $3<p_T(\bar{\Lambda}_c^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow J/\psi D^0 X \right)}{d \left| \Delta \phi/\pi \right|}$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow J/\psi D^+ X \right)}{d \left| \Delta \phi/\pi \right|}$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow J/\psi D_s^+ X \right)}{d \left| \Delta \phi/\pi \right|}$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D_s^+)<4$, $3<p_T(D_s^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow J/\psi D^0 X \right)}{d \Delta y }$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow J/\psi D^+ X \right)}{d \Delta y }$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow J/\psi D_s^+ X \right)}{d \Delta y}$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D_s^+)<4$, $3<p_T(D_s^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^0 X \right)}{d \left| \Delta \phi/\pi \right|}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^+ X \right)}{d \left| \Delta \phi/\pi \right|}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^0 X \right)}{d \left| \Delta y \right|}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12~GeV/c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^+ X \right)}{d \left| \Delta y \right|}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 \bar{D}^0 X \right)}{d \left| \Delta \phi/\pi \right|}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^- X \right)}{d \left| \Delta \phi/\pi \right|}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ , $2<y(D^-)<4$, $3<p_T(D^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D_s^- X \right)}{d \left| \Delta \phi/\pi \right|}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ , $2<y(D_s^-)<4$, $3<p_T(D_s^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D^- X \right)}{d \left| \Delta \phi/\pi \right|}$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D_s^- X \right)}{d \left| \Delta \phi/\pi \right|}$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$, $2<y(D_s^-)<4$, $3<p_T(D_s^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 \bar{D}^0 X \right)}{d \left| \Delta y \right|}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12~GeV/c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^- X \right)}{d \left| \Delta y \right|}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ , $2<y(D^-)<4$, $3<p_T(D^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D_s^- X \right)}{d \left| \Delta y \right|}$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(D_s^-)<4$, $3<p_T(D_s^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D^- X \right)}{d \left| \Delta y \right|}$ for $2<y(D^-)<4$, $3<p_T(D^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D_s^- X \right)}{d \left| \Delta y \right|}$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$, $2<y(D_s^-)<4$, $3<p_T(D_s^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow J/\psi D^0 X \right)}{d m_{J/\psi D^0} }$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow J/\psi D^+ X \right)}{d m_{J/\psi D^+} }$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow J/\psi D_s^+ X \right)}{d m_{J/\psi D_s^+} }$ for $2<y(J/\psi)<4$, $p_T(J/\psi)<12$ GeV/$c$, $2<y(D_s^+)<4$, $3<p_T(D_s^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^0 X \right)}{d m_{D^0 D^0} }$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^+ X \right)}{d m_{D^0 D^+} }$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 \bar{D}^0 X \right)}{d m_{D^0 \bar{D}^0} }$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D^- X \right)}{d m_{D^0 D^-} }$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(D^-)<4$, $3<p_T(D^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 D_s^- X \right)}{d m_{D^0 D_s^-} }$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(D_s^-)<4$, $3<p_T(D_s^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^0 \bar{\Lambda}_c^- X \right)}{d m_{D^0 D_s^-} }$ for $2<y(D^0)<4$, $3<p_T(D^0)<12$ GeV/$c$, $2<y(\bar{\Lambda}_c^-)<4$, $3<p_T(\bar{\Lambda}_c^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D^- X \right)}{d m_{D^+ D^-} }$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ D_s^- X \right)}{d m_{D^+ D_s^-} }$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$, $2<y(D_s^-)<4$, $3<p_T(D_s^-)<12$ GeV/$c$ region.

Normalized differential cross-section $\frac{d\ln\sigma\left(pp\rightarrow D^+ \bar{\Lambda}_c^- X \right)}{d m_{D^+ \bar{\Lambda}_c^-} }$ for $2<y(D^+)<4$, $3<p_T(D^+)<12$ GeV/$c$, $2<y(\bar{\Lambda}_c^-)<4$, $3<p_T(\bar{\Lambda}_c^-)<12$ GeV/$c$ region.

Distribution of the total energy outside the reconstructed jets for the completed data samples. Also tabulated is the estimated background.

Distribution of the total energy outside the reconstructed jets for the 'Dir' domain. Also tabulated is the estimated background.

Distribution of the total energy outside the reconstructed jets for the 'SR' domain. Also tabulated is the estimated background.

Distribution of the total energy outside the reconstructed jets for the 'DR' domain. Also tabulated is the estimated background.

Observed distribution of the charged particle multiplicity.

Observed distribution of the charged particle invariant mass.

Observed distribution of the mean of X(C=GAMMA-PLUS) and X(GAMMA-MINUS).

Observed mean number of particles in the reconstructed jets.