cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.135471.v1/t41
title: "Table 41 (diHiggs obs 68%)" of "Constraining the Higgs boson self-coupling from single- and double-Higgs production with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

description: Observed constraints in the $\kappa_{2V}$–$\kappa_{V}$ plane from double-Higgs combination. The solid lines show the 68% (95%) CL contours.
description: Constraints on the Higgs boson self-coupling are set by combining double-Higgs boson analyses in the bbbb, bb$\tau\tau$ and bb$\gamma\gamma$ decay channels with single-Higgs boson analyses targeting the $\gamma\gamma$, $ZZ^{∗}$, $WW^{∗}$, $\tau\tau$ and bb decay channels. The data used in these analyses were recorded by the ATLAS detector at the LHC in proton−proton collisions at 13 TeV and correspond to an integrated luminosity of 126−139 fb$^{-1}$ . The combination of the double-Higgs analyses sets an upper limit of $\mu_{HH} &lt; 2.4$ at 95% confidence level on the double-Higgs production cross-section normalised to its Standard Model prediction. Combining the single-Higgs and double-Higgs analyses, with the assumption that new physics affects only the Higgs boson self-coupling ($\lambda_{HHH}$), values outside the interval $-0.4&lt; \kappa_\lambda &lt; 6.3$ are excluded at 95% confidence level. The combined single-Higgs and double-Higgs analyses provide results with fewer assumptions, by adding in the fit more coupling modifiers introduced to account for the Higgs boson interactions with the other Standard Model particles.
DOI: 10.17182/hepdata.135471.v1/t42
title: "Table 42 (diHiggs obs 95%)" of "Constraining the Higgs boson self-coupling from single- and double-Higgs production with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

description: Observed constraints in the $\kappa_{2V}$–$\kappa_{V}$ plane from double-Higgs combination. The dashed lines show the 68% (95%) CL contours.
description: Constraints on the Higgs boson self-coupling are set by combining double-Higgs boson analyses in the bbbb, bb$\tau\tau$ and bb$\gamma\gamma$ decay channels with single-Higgs boson analyses targeting the $\gamma\gamma$, $ZZ^{∗}$, $WW^{∗}$, $\tau\tau$ and bb decay channels. The data used in these analyses were recorded by the ATLAS detector at the LHC in proton−proton collisions at 13 TeV and correspond to an integrated luminosity of 126−139 fb$^{-1}$ . The combination of the double-Higgs analyses sets an upper limit of $\mu_{HH} &lt; 2.4$ at 95% confidence level on the double-Higgs production cross-section normalised to its Standard Model prediction. Combining the single-Higgs and double-Higgs analyses, with the assumption that new physics affects only the Higgs boson self-coupling ($\lambda_{HHH}$), values outside the interval $-0.4&lt; \kappa_\lambda &lt; 6.3$ are excluded at 95% confidence level. The combined single-Higgs and double-Higgs analyses provide results with fewer assumptions, by adding in the fit more coupling modifiers introduced to account for the Higgs boson interactions with the other Standard Model particles.
DOI: 10.17182/hepdata.135471.v1/t43
title: "Table 43 (diHiggs exp 68%)" of "Constraining the Higgs boson self-coupling from single- and double-Higgs production with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

description: Expected constraints in the $\kappa_{2V}$-$\kappa_{V}$ plane from double-Higgs combination. The solid lines show the 68% CL contours.
description: Constraints on the Higgs boson self-coupling are set by combining double-Higgs boson analyses in the bbbb, bb$\tau\tau$ and bb$\gamma\gamma$ decay channels with single-Higgs boson analyses targeting the $\gamma\gamma$, $ZZ^{∗}$, $WW^{∗}$, $\tau\tau$ and bb decay channels. The data used in these analyses were recorded by the ATLAS detector at the LHC in proton−proton collisions at 13 TeV and correspond to an integrated luminosity of 126−139 fb$^{-1}$ . The combination of the double-Higgs analyses sets an upper limit of $\mu_{HH} &lt; 2.4$ at 95% confidence level on the double-Higgs production cross-section normalised to its Standard Model prediction. Combining the single-Higgs and double-Higgs analyses, with the assumption that new physics affects only the Higgs boson self-coupling ($\lambda_{HHH}$), values outside the interval $-0.4&lt; \kappa_\lambda &lt; 6.3$ are excluded at 95% confidence level. The combined single-Higgs and double-Higgs analyses provide results with fewer assumptions, by adding in the fit more coupling modifiers introduced to account for the Higgs boson interactions with the other Standard Model particles.
DOI: 10.17182/hepdata.135471.v1/t44
title: "Table 44 (diHiggs exp 95%)" of "Constraining the Higgs boson self-coupling from single- and double-Higgs production with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

description: Expected constraints in the $\kappa_{2V}$-$\kappa_{V}$ plane from double-Higgs combination. The dashed lines show the 95% CL contours.
description: Constraints on the Higgs boson self-coupling are set by combining double-Higgs boson analyses in the bbbb, bb$\tau\tau$ and bb$\gamma\gamma$ decay channels with single-Higgs boson analyses targeting the $\gamma\gamma$, $ZZ^{∗}$, $WW^{∗}$, $\tau\tau$ and bb decay channels. The data used in these analyses were recorded by the ATLAS detector at the LHC in proton−proton collisions at 13 TeV and correspond to an integrated luminosity of 126−139 fb$^{-1}$ . The combination of the double-Higgs analyses sets an upper limit of $\mu_{HH} &lt; 2.4$ at 95% confidence level on the double-Higgs production cross-section normalised to its Standard Model prediction. Combining the single-Higgs and double-Higgs analyses, with the assumption that new physics affects only the Higgs boson self-coupling ($\lambda_{HHH}$), values outside the interval $-0.4&lt; \kappa_\lambda &lt; 6.3$ are excluded at 95% confidence level. The combined single-Higgs and double-Higgs analyses provide results with fewer assumptions, by adding in the fit more coupling modifiers introduced to account for the Higgs boson interactions with the other Standard Model particles.
DOI: 10.17182/hepdata.55768.v1/t1
title: "Table 1" of "Measurement of Spin-Density Matrix Elements for $\phi$-Meson Photoproduction from Protons and Deuterons Near Threshold"

description: Measurements of the spin density matrix element RHO(JJ=0,MM=00) for the GAMMA P --&gt; PHI P reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.
description: OSAKA. Measurements of the spin-density matrix elements for the reactions GAMMA P --&gt; PHI P, GAMMA DEUT --&gt; PHI P N and GAMMA DEUT --&gt; PHI DEUT at forward production angles. The experiment was performed at the laser-electron photon facility SPring-8 using a linearily polarized photon beam of energy 1.6 to 2.4 GeV. Numerical values were supplied by W.C.Chang.

UPDATE (23 OCT 2017): Changed erroneous headers RHO(JJ=0,MM=11) to RHO(JJ=1,MM=11); thanks to Vincent Mathieu for spotting the mistake.
DOI: 10.17182/hepdata.55768.v1/t2
title: "Table 2" of "Measurement of Spin-Density Matrix Elements for $\phi$-Meson Photoproduction from Protons and Deuterons Near Threshold"

description: Measurements of the spin density matrix element RE(RHO(JJ=0,MM=10)) for the GAMMA P --&gt; PHI P reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.
description: OSAKA. Measurements of the spin-density matrix elements for the reactions GAMMA P --&gt; PHI P, GAMMA DEUT --&gt; PHI P N and GAMMA DEUT --&gt; PHI DEUT at forward production angles. The experiment was performed at the laser-electron photon facility SPring-8 using a linearily polarized photon beam of energy 1.6 to 2.4 GeV. Numerical values were supplied by W.C.Chang.

UPDATE (23 OCT 2017): Changed erroneous headers RHO(JJ=0,MM=11) to RHO(JJ=1,MM=11); thanks to Vincent Mathieu for spotting the mistake.
DOI: 10.17182/hepdata.55768.v1/t3
title: "Table 3" of "Measurement of Spin-Density Matrix Elements for $\phi$-Meson Photoproduction from Protons and Deuterons Near Threshold"

description: Measurements of the spin density matrix element RHO(JJ=0,MM=1-1) for the GAMMA P --&gt; PHI P reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.
description: OSAKA. Measurements of the spin-density matrix elements for the reactions GAMMA P --&gt; PHI P, GAMMA DEUT --&gt; PHI P N and GAMMA DEUT --&gt; PHI DEUT at forward production angles. The experiment was performed at the laser-electron photon facility SPring-8 using a linearily polarized photon beam of energy 1.6 to 2.4 GeV. Numerical values were supplied by W.C.Chang.

UPDATE (23 OCT 2017): Changed erroneous headers RHO(JJ=0,MM=11) to RHO(JJ=1,MM=11); thanks to Vincent Mathieu for spotting the mistake.
DOI: 10.17182/hepdata.55768.v1/t4
title: "Table 4" of "Measurement of Spin-Density Matrix Elements for $\phi$-Meson Photoproduction from Protons and Deuterons Near Threshold"

description: Measurements of the spin density matrix element RHO(JJ=1,MM=11) for the GAMMA P --&gt; PHI P reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.
description: OSAKA. Measurements of the spin-density matrix elements for the reactions GAMMA P --&gt; PHI P, GAMMA DEUT --&gt; PHI P N and GAMMA DEUT --&gt; PHI DEUT at forward production angles. The experiment was performed at the laser-electron photon facility SPring-8 using a linearily polarized photon beam of energy 1.6 to 2.4 GeV. Numerical values were supplied by W.C.Chang.

UPDATE (23 OCT 2017): Changed erroneous headers RHO(JJ=0,MM=11) to RHO(JJ=1,MM=11); thanks to Vincent Mathieu for spotting the mistake.
DOI: 10.17182/hepdata.55768.v1/t5
title: "Table 5" of "Measurement of Spin-Density Matrix Elements for $\phi$-Meson Photoproduction from Protons and Deuterons Near Threshold"

description: Measurements of the spin density matrix element RHO(JJ=1,MM=00) for the GAMMA P --&gt; PHI P reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.
description: OSAKA. Measurements of the spin-density matrix elements for the reactions GAMMA P --&gt; PHI P, GAMMA DEUT --&gt; PHI P N and GAMMA DEUT --&gt; PHI DEUT at forward production angles. The experiment was performed at the laser-electron photon facility SPring-8 using a linearily polarized photon beam of energy 1.6 to 2.4 GeV. Numerical values were supplied by W.C.Chang.

UPDATE (23 OCT 2017): Changed erroneous headers RHO(JJ=0,MM=11) to RHO(JJ=1,MM=11); thanks to Vincent Mathieu for spotting the mistake.
DOI: 10.17182/hepdata.55768.v1/t6
title: "Table 6" of "Measurement of Spin-Density Matrix Elements for $\phi$-Meson Photoproduction from Protons and Deuterons Near Threshold"

description: Measurements of the spin density matrix element RE(RHO(JJ=1,MM=10)) for the GAMMA P --&gt; PHI P reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.
description: OSAKA. Measurements of the spin-density matrix elements for the reactions GAMMA P --&gt; PHI P, GAMMA DEUT --&gt; PHI P N and GAMMA DEUT --&gt; PHI DEUT at forward production angles. The experiment was performed at the laser-electron photon facility SPring-8 using a linearily polarized photon beam of energy 1.6 to 2.4 GeV. Numerical values were supplied by W.C.Chang.

UPDATE (23 OCT 2017): Changed erroneous headers RHO(JJ=0,MM=11) to RHO(JJ=1,MM=11); thanks to Vincent Mathieu for spotting the mistake.
DOI: 10.17182/hepdata.55768.v1/t7
title: "Table 7" of "Measurement of Spin-Density Matrix Elements for $\phi$-Meson Photoproduction from Protons and Deuterons Near Threshold"

description: Measurements of the spin density matrix element RHO(JJ=1,MM=1-1) for the GAMMA P --&gt; PHI P reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.
description: OSAKA. Measurements of the spin-density matrix elements for the reactions GAMMA P --&gt; PHI P, GAMMA DEUT --&gt; PHI P N and GAMMA DEUT --&gt; PHI DEUT at forward production angles. The experiment was performed at the laser-electron photon facility SPring-8 using a linearily polarized photon beam of energy 1.6 to 2.4 GeV. Numerical values were supplied by W.C.Chang.

UPDATE (23 OCT 2017): Changed erroneous headers RHO(JJ=0,MM=11) to RHO(JJ=1,MM=11); thanks to Vincent Mathieu for spotting the mistake.
DOI: 10.17182/hepdata.55768.v1/t8
title: "Table 8" of "Measurement of Spin-Density Matrix Elements for $\phi$-Meson Photoproduction from Protons and Deuterons Near Threshold"

description: Measurements of the spin density matrix element IM(RHO(JJ=2,MM=10)) for the GAMMA P --&gt; PHI P reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.
description: OSAKA. Measurements of the spin-density matrix elements for the reactions GAMMA P --&gt; PHI P, GAMMA DEUT --&gt; PHI P N and GAMMA DEUT --&gt; PHI DEUT at forward production angles. The experiment was performed at the laser-electron photon facility SPring-8 using a linearily polarized photon beam of energy 1.6 to 2.4 GeV. Numerical values were supplied by W.C.Chang.

UPDATE (23 OCT 2017): Changed erroneous headers RHO(JJ=0,MM=11) to RHO(JJ=1,MM=11); thanks to Vincent Mathieu for spotting the mistake.
DOI: 10.17182/hepdata.55768.v1/t9
title: "Table 9" of "Measurement of Spin-Density Matrix Elements for $\phi$-Meson Photoproduction from Protons and Deuterons Near Threshold"

description: Measurements of the spin density matrix element IM(RHO(JJ=2,MM=1-1)) for the GAMMA P --&gt; PHI P reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.
description: OSAKA. Measurements of the spin-density matrix elements for the reactions GAMMA P --&gt; PHI P, GAMMA DEUT --&gt; PHI P N and GAMMA DEUT --&gt; PHI DEUT at forward production angles. The experiment was performed at the laser-electron photon facility SPring-8 using a linearily polarized photon beam of energy 1.6 to 2.4 GeV. Numerical values were supplied by W.C.Chang.

UPDATE (23 OCT 2017): Changed erroneous headers RHO(JJ=0,MM=11) to RHO(JJ=1,MM=11); thanks to Vincent Mathieu for spotting the mistake.
DOI: 10.17182/hepdata.55768.v1/t10
title: "Table 10" of "Measurement of Spin-Density Matrix Elements for $\phi$-Meson Photoproduction from Protons and Deuterons Near Threshold"

description: Measurements of the spin density matrix element RHO(JJ=0,MM=00) for the GAMMA P --&gt; PHI P reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.
description: OSAKA. Measurements of the spin-density matrix elements for the reactions GAMMA P --&gt; PHI P, GAMMA DEUT --&gt; PHI P N and GAMMA DEUT --&gt; PHI DEUT at forward production angles. The experiment was performed at the laser-electron photon facility SPring-8 using a linearily polarized photon beam of energy 1.6 to 2.4 GeV. Numerical values were supplied by W.C.Chang.

UPDATE (23 OCT 2017): Changed erroneous headers RHO(JJ=0,MM=11) to RHO(JJ=1,MM=11); thanks to Vincent Mathieu for spotting the mistake.
DOI: 10.17182/hepdata.55768.v1/t11
title: "Table 11" of "Measurement of Spin-Density Matrix Elements for $\phi$-Meson Photoproduction from Protons and Deuterons Near Threshold"

description: Measurements of the spin density matrix element RE(RHO(JJ=0,MM=10)) for the GAMMA P --&gt; PHI P reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.
description: OSAKA. Measurements of the spin-density matrix elements for the reactions GAMMA P --&gt; PHI P, GAMMA DEUT --&gt; PHI P N and GAMMA DEUT --&gt; PHI DEUT at forward production angles. The experiment was performed at the laser-electron photon facility SPring-8 using a linearily polarized photon beam of energy 1.6 to 2.4 GeV. Numerical values were supplied by W.C.Chang.

UPDATE (23 OCT 2017): Changed erroneous headers RHO(JJ=0,MM=11) to RHO(JJ=1,MM=11); thanks to Vincent Mathieu for spotting the mistake.
DOI: 10.17182/hepdata.55768.v1/t12
title: "Table 12" of "Measurement of Spin-Density Matrix Elements for $\phi$-Meson Photoproduction from Protons and Deuterons Near Threshold"

description: Measurements of the spin density matrix element RHO(JJ=0,MM=1-1) for the GAMMA P --&gt; PHI P reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.
description: OSAKA. Measurements of the spin-density matrix elements for the reactions GAMMA P --&gt; PHI P, GAMMA DEUT --&gt; PHI P N and GAMMA DEUT --&gt; PHI DEUT at forward production angles. The experiment was performed at the laser-electron photon facility SPring-8 using a linearily polarized photon beam of energy 1.6 to 2.4 GeV. Numerical values were supplied by W.C.Chang.

UPDATE (23 OCT 2017): Changed erroneous headers RHO(JJ=0,MM=11) to RHO(JJ=1,MM=11); thanks to Vincent Mathieu for spotting the mistake.
DOI: 10.17182/hepdata.55768.v1/t13
title: "Table 13" of "Measurement of Spin-Density Matrix Elements for $\phi$-Meson Photoproduction from Protons and Deuterons Near Threshold"

description: Measurements of the spin density matrix element RHO(JJ=1,MM=11) for the GAMMA P --&gt; PHI P reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.
description: OSAKA. Measurements of the spin-density matrix elements for the reactions GAMMA P --&gt; PHI P, GAMMA DEUT --&gt; PHI P N and GAMMA DEUT --&gt; PHI DEUT at forward production angles. The experiment was performed at the laser-electron photon facility SPring-8 using a linearily polarized photon beam of energy 1.6 to 2.4 GeV. Numerical values were supplied by W.C.Chang.

UPDATE (23 OCT 2017): Changed erroneous headers RHO(JJ=0,MM=11) to RHO(JJ=1,MM=11); thanks to Vincent Mathieu for spotting the mistake.
DOI: 10.17182/hepdata.55768.v1/t14
title: "Table 14" of "Measurement of Spin-Density Matrix Elements for $\phi$-Meson Photoproduction from Protons and Deuterons Near Threshold"

description: Measurements of the spin density matrix element RHO(JJ=1,MM=00) for the GAMMA P --&gt; PHI P reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.
description: OSAKA. Measurements of the spin-density matrix elements for the reactions GAMMA P --&gt; PHI P, GAMMA DEUT --&gt; PHI P N and GAMMA DEUT --&gt; PHI DEUT at forward production angles. The experiment was performed at the laser-electron photon facility SPring-8 using a linearily polarized photon beam of energy 1.6 to 2.4 GeV. Numerical values were supplied by W.C.Chang.

UPDATE (23 OCT 2017): Changed erroneous headers RHO(JJ=0,MM=11) to RHO(JJ=1,MM=11); thanks to Vincent Mathieu for spotting the mistake.
DOI: 10.17182/hepdata.55768.v1/t15
title: "Table 15" of "Measurement of Spin-Density Matrix Elements for $\phi$-Meson Photoproduction from Protons and Deuterons Near Threshold"

description: Measurements of the spin density matrix element RE(RHO(JJ=1,MM=10)) for the GAMMA P --&gt; PHI P reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.
description: OSAKA. Measurements of the spin-density matrix elements for the reactions GAMMA P --&gt; PHI P, GAMMA DEUT --&gt; PHI P N and GAMMA DEUT --&gt; PHI DEUT at forward production angles. The experiment was performed at the laser-electron photon facility SPring-8 using a linearily polarized photon beam of energy 1.6 to 2.4 GeV. Numerical values were supplied by W.C.Chang.

UPDATE (23 OCT 2017): Changed erroneous headers RHO(JJ=0,MM=11) to RHO(JJ=1,MM=11); thanks to Vincent Mathieu for spotting the mistake.
DOI: 10.17182/hepdata.55768.v1/t16
title: "Table 16" of "Measurement of Spin-Density Matrix Elements for $\phi$-Meson Photoproduction from Protons and Deuterons Near Threshold"

description: Measurements of the spin density matrix element RHO(JJ=1,MM=1-1) for the GAMMA P --&gt; PHI P reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.
description: OSAKA. Measurements of the spin-density matrix elements for the reactions GAMMA P --&gt; PHI P, GAMMA DEUT --&gt; PHI P N and GAMMA DEUT --&gt; PHI DEUT at forward production angles. The experiment was performed at the laser-electron photon facility SPring-8 using a linearily polarized photon beam of energy 1.6 to 2.4 GeV. Numerical values were supplied by W.C.Chang.

UPDATE (23 OCT 2017): Changed erroneous headers RHO(JJ=0,MM=11) to RHO(JJ=1,MM=11); thanks to Vincent Mathieu for spotting the mistake.
DOI: 10.17182/hepdata.55768.v1/t17
title: "Table 17" of "Measurement of Spin-Density Matrix Elements for $\phi$-Meson Photoproduction from Protons and Deuterons Near Threshold"

description: Measurements of the spin density matrix element IM(RHO(JJ=2,MM=10)) for the GAMMA P --&gt; PHI P reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.
description: OSAKA. Measurements of the spin-density matrix elements for the reactions GAMMA P --&gt; PHI P, GAMMA DEUT --&gt; PHI P N and GAMMA DEUT --&gt; PHI DEUT at forward production angles. The experiment was performed at the laser-electron photon facility SPring-8 using a linearily polarized photon beam of energy 1.6 to 2.4 GeV. Numerical values were supplied by W.C.Chang.

UPDATE (23 OCT 2017): Changed erroneous headers RHO(JJ=0,MM=11) to RHO(JJ=1,MM=11); thanks to Vincent Mathieu for spotting the mistake.
DOI: 10.17182/hepdata.55768.v1/t18
title: "Table 18" of "Measurement of Spin-Density Matrix Elements for $\phi$-Meson Photoproduction from Protons and Deuterons Near Threshold"

description: Measurements of the spin density matrix element IM(RHO(JJ=2,MM=1-1)) for the GAMMA P --&gt; PHI P reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.
description: OSAKA. Measurements of the spin-density matrix elements for the reactions GAMMA P --&gt; PHI P, GAMMA DEUT --&gt; PHI P N and GAMMA DEUT --&gt; PHI DEUT at forward production angles. The experiment was performed at the laser-electron photon facility SPring-8 using a linearily polarized photon beam of energy 1.6 to 2.4 GeV. Numerical values were supplied by W.C.Chang.

UPDATE (23 OCT 2017): Changed erroneous headers RHO(JJ=0,MM=11) to RHO(JJ=1,MM=11); thanks to Vincent Mathieu for spotting the mistake.
DOI: 10.17182/hepdata.55768.v1/t19
title: "Table 19" of "Measurement of Spin-Density Matrix Elements for $\phi$-Meson Photoproduction from Protons and Deuterons Near Threshold"

description: Measurements of the spin density matrix element RHO(JJ=0,MM=00) for the GAMMA P --&gt; PHI P reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.
description: OSAKA. Measurements of the spin-density matrix elements for the reactions GAMMA P --&gt; PHI P, GAMMA DEUT --&gt; PHI P N and GAMMA DEUT --&gt; PHI DEUT at forward production angles. The experiment was performed at the laser-electron photon facility SPring-8 using a linearily polarized photon beam of energy 1.6 to 2.4 GeV. Numerical values were supplied by W.C.Chang.

UPDATE (23 OCT 2017): Changed erroneous headers RHO(JJ=0,MM=11) to RHO(JJ=1,MM=11); thanks to Vincent Mathieu for spotting the mistake.
DOI: 10.17182/hepdata.55768.v1/t20
title: "Table 20" of "Measurement of Spin-Density Matrix Elements for $\phi$-Meson Photoproduction from Protons and Deuterons Near Threshold"

description: Measurements of the spin density matrix element RE(RHO(JJ=0,MM=10)) for the GAMMA P --&gt; PHI P reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.
description: OSAKA. Measurements of the spin-density matrix elements for the reactions GAMMA P --&gt; PHI P, GAMMA DEUT --&gt; PHI P N and GAMMA DEUT --&gt; PHI DEUT at forward production angles. The experiment was performed at the laser-electron photon facility SPring-8 using a linearily polarized photon beam of energy 1.6 to 2.4 GeV. Numerical values were supplied by W.C.Chang.

UPDATE (23 OCT 2017): Changed erroneous headers RHO(JJ=0,MM=11) to RHO(JJ=1,MM=11); thanks to Vincent Mathieu for spotting the mistake.