cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.43332.v1/t14
title: "Table 14" of "Quasi-elastic p n scattering in Li-6_D and Li-6_H targets from 1.1-GeV to 2.4-GeV."

description: 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.
description: SACLAY-SATURNE-II. Measurement of the spin dependent observables, the analysing power and depolarization parameter DNN, in quasi-elastic scattering of a polarized proton beam on the Saclay polarized targets with Li compounds and an unpolarized CH2 target. Data cover the energy range 1.1 to 2.4 GeV. In table 1, the analysing power measurements, the first sets of results were obtained through the use of the forward outgoing protons and neutron charge- exchange in the carbon analyser. The second sets were obtained with protons scattered at large angles and correlated neutrons detected in the NC hodoscope.
DOI: 10.17182/hepdata.43332.v1/t15
title: "Table 15" of "Quasi-elastic p n scattering in Li-6_D and Li-6_H targets from 1.1-GeV to 2.4-GeV."

description: 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.
description: SACLAY-SATURNE-II. Measurement of the spin dependent observables, the analysing power and depolarization parameter DNN, in quasi-elastic scattering of a polarized proton beam on the Saclay polarized targets with Li compounds and an unpolarized CH2 target. Data cover the energy range 1.1 to 2.4 GeV. In table 1, the analysing power measurements, the first sets of results were obtained through the use of the forward outgoing protons and neutron charge- exchange in the carbon analyser. The second sets were obtained with protons scattered at large angles and correlated neutrons detected in the NC hodoscope.
DOI: 10.17182/hepdata.43332.v1/t9
title: "Table 9" of "Quasi-elastic p n scattering in Li-6_D and Li-6_H targets from 1.1-GeV to 2.4-GeV."

description: 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.
description: SACLAY-SATURNE-II. Measurement of the spin dependent observables, the analysing power and depolarization parameter DNN, in quasi-elastic scattering of a polarized proton beam on the Saclay polarized targets with Li compounds and an unpolarized CH2 target. Data cover the energy range 1.1 to 2.4 GeV. In table 1, the analysing power measurements, the first sets of results were obtained through the use of the forward outgoing protons and neutron charge- exchange in the carbon analyser. The second sets were obtained with protons scattered at large angles and correlated neutrons detected in the NC hodoscope.
DOI: 10.17182/hepdata.43332.v1/t16
title: "Table 16" of "Quasi-elastic p n scattering in Li-6_D and Li-6_H targets from 1.1-GeV to 2.4-GeV."

description: 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.
description: SACLAY-SATURNE-II. Measurement of the spin dependent observables, the analysing power and depolarization parameter DNN, in quasi-elastic scattering of a polarized proton beam on the Saclay polarized targets with Li compounds and an unpolarized CH2 target. Data cover the energy range 1.1 to 2.4 GeV. In table 1, the analysing power measurements, the first sets of results were obtained through the use of the forward outgoing protons and neutron charge- exchange in the carbon analyser. The second sets were obtained with protons scattered at large angles and correlated neutrons detected in the NC hodoscope.
DOI: 10.17182/hepdata.43332.v1/t17
title: "Table 17" of "Quasi-elastic p n scattering in Li-6_D and Li-6_H targets from 1.1-GeV to 2.4-GeV."

description: 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.
description: SACLAY-SATURNE-II. Measurement of the spin dependent observables, the analysing power and depolarization parameter DNN, in quasi-elastic scattering of a polarized proton beam on the Saclay polarized targets with Li compounds and an unpolarized CH2 target. Data cover the energy range 1.1 to 2.4 GeV. In table 1, the analysing power measurements, the first sets of results were obtained through the use of the forward outgoing protons and neutron charge- exchange in the carbon analyser. The second sets were obtained with protons scattered at large angles and correlated neutrons detected in the NC hodoscope.
DOI: 10.17182/hepdata.43333.v1/t1
title: "Table 1" of "A measurement of the transverse polarization of Lambda-hyperons produced in n C reactions in the EXCHARM experiment."

description: LAMBDA polarization as a function of PT for the whole XL region.
description: SERPUKHOV accelerator. . Measurement of the transverse polarization of LAMBDA hyperons produced in N Carbon interactions at energies up to 70 GeV. Data cover the XL range from 0.1 to 0.6 and PT from 0.2 to 1.2 GeV.
DOI: 10.17182/hepdata.43333.v1/t2
title: "Table 2" of "A measurement of the transverse polarization of Lambda-hyperons produced in n C reactions in the EXCHARM experiment."

description: LAMBDA polarization as a function of PT for three XL regions.
description: SERPUKHOV accelerator. . Measurement of the transverse polarization of LAMBDA hyperons produced in N Carbon interactions at energies up to 70 GeV. Data cover the XL range from 0.1 to 0.6 and PT from 0.2 to 1.2 GeV.
DOI: 10.17182/hepdata.43334.v1/t1
title: "Table 1" of "Determination of the total c anti-c production cross section in 340-GeV/c Sigma- nucleus interactions."

description: Fits to the DSIG/DXL and DSIG/DPT**2 distributions in the range XL &gt; 0. Theerrors shown are statistical only.. The fits are of the following form:. DSIG/DXL : Const*(1-X)**N. DSIG/DPT**2 : Const*EXP(-B*PT**2).
description: CERN-SPS. Measurement of the production of charmed particles in collisions of 340 GeV SIGMA- hyperons with copper and carbon targets using the OMEGA spectrometer. The data were taken during the 1993 and 1994 SPS running periods and correspond to an integrated luminosity of 1600 mub-1.The data from both targets arecombined and converted to a NUCLEON cross section using a linear dependence on the atomic mass of the target.
DOI: 10.17182/hepdata.43334.v1/t2
title: "Table 2" of "Determination of the total c anti-c production cross section in 340-GeV/c Sigma- nucleus interactions."

description: The production cross sections for anti-charmed and charmed hadrons in the range XL &gt; 0. The Errors are statistical only.
description: CERN-SPS. Measurement of the production of charmed particles in collisions of 340 GeV SIGMA- hyperons with copper and carbon targets using the OMEGA spectrometer. The data were taken during the 1993 and 1994 SPS running periods and correspond to an integrated luminosity of 1600 mub-1.The data from both targets arecombined and converted to a NUCLEON cross section using a linear dependence on the atomic mass of the target.
DOI: 10.17182/hepdata.43334.v1/t3
title: "Table 3" of "Determination of the total c anti-c production cross section in 340-GeV/c Sigma- nucleus interactions."

description: The total CQUARK+CQUARKBAR cross section in the range XL &gt; obtained as the weighted average of the sum of all the measured contributions to the charmed andanti-charmed hadron production in the previous table. second systematic (DSYS) error is due to the uncertainty in the contribution of XI/C production to the cross section.
description: CERN-SPS. Measurement of the production of charmed particles in collisions of 340 GeV SIGMA- hyperons with copper and carbon targets using the OMEGA spectrometer. The data were taken during the 1993 and 1994 SPS running periods and correspond to an integrated luminosity of 1600 mub-1.The data from both targets arecombined and converted to a NUCLEON cross section using a linear dependence on the atomic mass of the target.
DOI: 10.17182/hepdata.43334.v1/t4
title: "Table 4" of "Determination of the total c anti-c production cross section in 340-GeV/c Sigma- nucleus interactions."

description: The of the measured D+DBAR production cross section.
description: CERN-SPS. Measurement of the production of charmed particles in collisions of 340 GeV SIGMA- hyperons with copper and carbon targets using the OMEGA spectrometer. The data were taken during the 1993 and 1994 SPS running periods and correspond to an integrated luminosity of 1600 mub-1.The data from both targets arecombined and converted to a NUCLEON cross section using a linear dependence on the atomic mass of the target.
DOI: 10.17182/hepdata.43334.v1/t5
title: "Table 5" of "Determination of the total c anti-c production cross section in 340-GeV/c Sigma- nucleus interactions."

description: The ratio of the measured D to DBAR production cross sections.
description: CERN-SPS. Measurement of the production of charmed particles in collisions of 340 GeV SIGMA- hyperons with copper and carbon targets using the OMEGA spectrometer. The data were taken during the 1993 and 1994 SPS running periods and correspond to an integrated luminosity of 1600 mub-1.The data from both targets arecombined and converted to a NUCLEON cross section using a linear dependence on the atomic mass of the target.
DOI: 10.17182/hepdata.43334.v1/t6
title: "Table 6" of "Determination of the total c anti-c production cross section in 340-GeV/c Sigma- nucleus interactions."

description: The ratio of the measured D/S- to (D+DBAR) production cross sections.
description: CERN-SPS. Measurement of the production of charmed particles in collisions of 340 GeV SIGMA- hyperons with copper and carbon targets using the OMEGA spectrometer. The data were taken during the 1993 and 1994 SPS running periods and correspond to an integrated luminosity of 1600 mub-1.The data from both targets arecombined and converted to a NUCLEON cross section using a linear dependence on the atomic mass of the target.
DOI: 10.17182/hepdata.43392.v1/t1
title: "Table 1" of "Measurement of spin observables in neutron proton elastic scattering. I: Correlation parameters"

description: Values of the coefficients for the linear combinations of the spin correlation parameters Cpq measurements for the four different beam and target polarisation orientations. For the (z,z) and (y,y) configurations the coefficients are identical for all incident kinetic energies.
description: PSI. Measurement of the analysing power and spin correlation parameters CSS, CSL, CNN, and CLL in free neutron proton elastic scattering at kinetic energies of 260, 315, 380, 460 and 535 MeV in the c.m. angular range 60 to 164 degrees.The experiment uses a polarised neutron beam with a continuous energy incident on a polarised proton target. Pure measurements are made of the analysing power and the parameters CNN, and CLL. Linear combinations are measured for CSL and CSS.
DOI: 10.17182/hepdata.43392.v1/t2
title: "Table 2" of "Measurement of spin observables in neutron proton elastic scattering. I: Correlation parameters"

description: Measurement of the analysing power. Statistical errors only are shown. For the systematic errors see the systematics section above. Note that there are two overlapping angular settings.
description: PSI. Measurement of the analysing power and spin correlation parameters CSS, CSL, CNN, and CLL in free neutron proton elastic scattering at kinetic energies of 260, 315, 380, 460 and 535 MeV in the c.m. angular range 60 to 164 degrees.The experiment uses a polarised neutron beam with a continuous energy incident on a polarised proton target. Pure measurements are made of the analysing power and the parameters CNN, and CLL. Linear combinations are measured for CSL and CSS.
DOI: 10.17182/hepdata.43392.v1/t3
title: "Table 3" of "Measurement of spin observables in neutron proton elastic scattering. I: Correlation parameters"

description: Measurements of the spin correlation parameter CNN. Statistical errors onlyare shown. For the systematics see the systematic section above. Note the two overlapping angular settings.
description: PSI. Measurement of the analysing power and spin correlation parameters CSS, CSL, CNN, and CLL in free neutron proton elastic scattering at kinetic energies of 260, 315, 380, 460 and 535 MeV in the c.m. angular range 60 to 164 degrees.The experiment uses a polarised neutron beam with a continuous energy incident on a polarised proton target. Pure measurements are made of the analysing power and the parameters CNN, and CLL. Linear combinations are measured for CSL and CSS.
DOI: 10.17182/hepdata.43392.v1/t4
title: "Table 4" of "Measurement of spin observables in neutron proton elastic scattering. I: Correlation parameters"

description: 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.
description: PSI. Measurement of the analysing power and spin correlation parameters CSS, CSL, CNN, and CLL in free neutron proton elastic scattering at kinetic energies of 260, 315, 380, 460 and 535 MeV in the c.m. angular range 60 to 164 degrees.The experiment uses a polarised neutron beam with a continuous energy incident on a polarised proton target. Pure measurements are made of the analysing power and the parameters CNN, and CLL. Linear combinations are measured for CSL and CSS.
DOI: 10.5281/zenodo.17523485
title: PCR as an Amplification Tool, Not a Diagnostic Test: Technical, Historical, and Regulatory Evidence

description: The polymerase chain reaction (PCR) is a laboratory amplification technique designed to detect genetic material, not to diagnose infectious disease. During the COVID-19 era, PCR was repurposed as a mass diagnostic instrument, treated as synonymous with “infection” and “case count,” despite the absence of clinical correlation, viral culture, or standardized threshold criteria. This paper establishes, using peer-reviewed literature, MIQE reporting standards, and regulatory admissions, that PCR is technically incapable of confirming the presence of intact, infectious, replicating virus — and that the public, governments, and media were misled into interpreting amplification fragments as direct indicators of disease. The intention is not to discredit PCR as a method, but to separate scientific function from political misuse. The conclusion is simple: PCR is valid for detecting nucleic acid fragments, but invalid as a standalone diagnostic for clinical infection or contagiousness. Any claim beyond that is either ignorance or manipulation
DOI: 10.17182/hepdata.43392.v1/t5
title: "Table 5" of "Measurement of spin observables in neutron proton elastic scattering. I: Correlation parameters"

description: 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.
description: PSI. Measurement of the analysing power and spin correlation parameters CSS, CSL, CNN, and CLL in free neutron proton elastic scattering at kinetic energies of 260, 315, 380, 460 and 535 MeV in the c.m. angular range 60 to 164 degrees.The experiment uses a polarised neutron beam with a continuous energy incident on a polarised proton target. Pure measurements are made of the analysing power and the parameters CNN, and CLL. Linear combinations are measured for CSL and CSS.
DOI: 10.17182/hepdata.43392.v1/t6
title: "Table 6" of "Measurement of spin observables in neutron proton elastic scattering. I: Correlation parameters"

description: 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.
description: PSI. Measurement of the analysing power and spin correlation parameters CSS, CSL, CNN, and CLL in free neutron proton elastic scattering at kinetic energies of 260, 315, 380, 460 and 535 MeV in the c.m. angular range 60 to 164 degrees.The experiment uses a polarised neutron beam with a continuous energy incident on a polarised proton target. Pure measurements are made of the analysing power and the parameters CNN, and CLL. Linear combinations are measured for CSL and CSS.
DOI: 10.17182/hepdata.43393.v1/t1
title: "Table 1" of "Study of QED processes e+ e- --&gt; e+ e- gamma, e+ e- gamma gamma with the SND detector at VEPP-2M."

description: No statistical errors are given. 3.8 PCT is the total systematic error.
description: NOVO-VEPP-2M accelerator. STUDY OF QED PROCESSES E+ E- ---& gt; E+ E- GAMMA, E+ E- GAMMA GAMMA WITH THE SND DETECTOR AT VEPP-2M.
DOI: 10.17182/hepdata.43393.v1/t2
title: "Table 2" of "Study of QED processes e+ e- --&gt; e+ e- gamma, e+ e- gamma gamma with the SND detector at VEPP-2M."

description: No statistical errors are given. 5.8 PCT is the total systematic error.
description: NOVO-VEPP-2M accelerator. STUDY OF QED PROCESSES E+ E- ---& gt; E+ E- GAMMA, E+ E- GAMMA GAMMA WITH THE SND DETECTOR AT VEPP-2M.
DOI: 10.17182/hepdata.43394.v1/t1
title: "Table 1" of "Experimental study of the processes e+ e- --&gt; phi --&gt; eta gamma, pi0 gamma at VEPP-2M."

description: Results of energy scan of the cross section.
description: NOVO-VEPP-2M collider. Measurement of the cross section for the process E+ E- --& gt; PHI with decay into ETA GAMMA and PI0 GAMMA final states. The paper also gives the branching ratios determined from the cross sections.
DOI: 10.17182/hepdata.43394.v1/t2
title: "Table 2" of "Experimental study of the processes e+ e- --&gt; phi --&gt; eta gamma, pi0 gamma at VEPP-2M."

description: Cross sections for PHI production and decay into the two states from a fit to the data at the peak.
description: NOVO-VEPP-2M collider. Measurement of the cross section for the process E+ E- --& gt; PHI with decay into ETA GAMMA and PI0 GAMMA final states. The paper also gives the branching ratios determined from the cross sections.
DOI: 10.17182/hepdata.43397.v1/t1
title: "Table 1" of "Measurement of xF3 and F2 structure functions in low Q**2 region with the IHEP-JINR neutrino detector."

description: No description provided.
description: wide band beam (two configurations) with initial proton energy 67/70 GeV, the target non-isoscalarity (N-Z)/A is -4.6%.
DOI: 10.17182/hepdata.43397.v1/t2
title: "Table 2" of "Measurement of xF3 and F2 structure functions in low Q**2 region with the IHEP-JINR neutrino detector."

description: No description provided.
description: wide band beam (two configurations) with initial proton energy 67/70 GeV, the target non-isoscalarity (N-Z)/A is -4.6%.
DOI: 10.17182/hepdata.43398.v1/t1
title: "Table 1" of "Angular dependence of p p spin correlation and rescattering observables between 1.80-GeV and 2.10-GeV."

description: Spin correlation parameter CSL measured with the beam polarisation measuredalong the +-S direction and the target polarisation along the +-L axis. Additional 4.3 PCT systematic normalisation uncertainty.
description: SACLAY-SATURNE-II. Measurement of the spin correlation parameter CSL and the rescattering observables KSS, DLL HSNS and HSLN in proton proton elastic scattering at kinetic energies of 1.80 and 2.10 GeV. The Beam polarisation was oriented perpendicular to the beam direction in the horizontal scattering plane and the target polarisation was directed either along the vertical axis or longitudinally. Data are also given for measurements of DNN and KNN at 1.80, 1.85, 2.04 and2.10.
DOI: 10.17182/hepdata.43398.v1/t2
title: "Table 2" of "Angular dependence of p p spin correlation and rescattering observables between 1.80-GeV and 2.10-GeV."

description: Measurement of the rescattering parameter KSS with the beam polarisation inthe +- S direction. Additional 6.7 PCT systematic error.
description: SACLAY-SATURNE-II. Measurement of the spin correlation parameter CSL and the rescattering observables KSS, DLL HSNS and HSLN in proton proton elastic scattering at kinetic energies of 1.80 and 2.10 GeV. The Beam polarisation was oriented perpendicular to the beam direction in the horizontal scattering plane and the target polarisation was directed either along the vertical axis or longitudinally. Data are also given for measurements of DNN and KNN at 1.80, 1.85, 2.04 and2.10.
DOI: 10.17182/hepdata.43398.v1/t3
title: "Table 3" of "Angular dependence of p p spin correlation and rescattering observables between 1.80-GeV and 2.10-GeV."

description: Measurement of the rescattering parameter KSS with the beam polarisation inthe +- S direction. Additional 6.7 PCT systematic error.
description: SACLAY-SATURNE-II. Measurement of the spin correlation parameter CSL and the rescattering observables KSS, DLL HSNS and HSLN in proton proton elastic scattering at kinetic energies of 1.80 and 2.10 GeV. The Beam polarisation was oriented perpendicular to the beam direction in the horizontal scattering plane and the target polarisation was directed either along the vertical axis or longitudinally. Data are also given for measurements of DNN and KNN at 1.80, 1.85, 2.04 and2.10.
DOI: 10.17182/hepdata.43398.v1/t4
title: "Table 4" of "Angular dependence of p p spin correlation and rescattering observables between 1.80-GeV and 2.10-GeV."

description: 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.
description: SACLAY-SATURNE-II. Measurement of the spin correlation parameter CSL and the rescattering observables KSS, DLL HSNS and HSLN in proton proton elastic scattering at kinetic energies of 1.80 and 2.10 GeV. The Beam polarisation was oriented perpendicular to the beam direction in the horizontal scattering plane and the target polarisation was directed either along the vertical axis or longitudinally. Data are also given for measurements of DNN and KNN at 1.80, 1.85, 2.04 and2.10.
DOI: 10.17182/hepdata.43398.v1/t5
title: "Table 5" of "Angular dependence of p p spin correlation and rescattering observables between 1.80-GeV and 2.10-GeV."

description: 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.
description: SACLAY-SATURNE-II. Measurement of the spin correlation parameter CSL and the rescattering observables KSS, DLL HSNS and HSLN in proton proton elastic scattering at kinetic energies of 1.80 and 2.10 GeV. The Beam polarisation was oriented perpendicular to the beam direction in the horizontal scattering plane and the target polarisation was directed either along the vertical axis or longitudinally. Data are also given for measurements of DNN and KNN at 1.80, 1.85, 2.04 and2.10.
DOI: 10.17182/hepdata.43398.v1/t6
title: "Table 6" of "Angular dependence of p p spin correlation and rescattering observables between 1.80-GeV and 2.10-GeV."

description: 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.
description: SACLAY-SATURNE-II. Measurement of the spin correlation parameter CSL and the rescattering observables KSS, DLL HSNS and HSLN in proton proton elastic scattering at kinetic energies of 1.80 and 2.10 GeV. The Beam polarisation was oriented perpendicular to the beam direction in the horizontal scattering plane and the target polarisation was directed either along the vertical axis or longitudinally. Data are also given for measurements of DNN and KNN at 1.80, 1.85, 2.04 and2.10.