cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.74247.v1/t38
title: "Table 38" of "Angular analysis of the $B^{0}\rightarrow K^{*0}\mu^{+}\mu^{-}$ decay"

description: Likelihood correlation matrix $15.0
description: CERN-LHC. An angular analysis of the $B^{0} \rightarrow K^{*0}(\rightarrow K^{+}\pi^{-})\mu^{+}\mu^{-}$ decay is presented. The dataset corresponds to an integrated luminosity of $3.0$ fb$^{-1}$ of $pp$ collision data collected at the LHCb experiment. The complete angular information from the decay is used to determine $C\!P$-averaged observables and $C\!P$ asymmetries, taking account of possible contamination from decays with the $K^{+}\pi^{-}$ system in an S-wave configuration. The angular observables and their correlations are reported in bins of $q^2$, the invariant mass squared of the dimuon system. The observables are determined both from an unbinned maximum likelihood fit and by using the principal moments of the angular distribution. In addition, by fitting for $q^2$-dependent decay amplitudes in the region $1.1 &lt; q^{2} &lt; 6.0 \mathrm{\,GeV}^{2}/c^{4}$, the zero-crossing points of several angular observables are computed. A global fit is performed to the complete set of $C\!P$-averaged observables obtained from the maximum likelihood fit. This fit indicates differences with predictions based on the Standard Model at the level of 3.4 standard deviations. These differences could be explained by contributions from physics beyond the Standard Model, or by an unexpectedly large hadronic effect that is not accounted for in the Standard Model predictions.
DOI: 10.17182/hepdata.74247.v1/t39
title: "Table 39" of "Angular analysis of the $B^{0}\rightarrow K^{*0}\mu^{+}\mu^{-}$ decay"

description: Bootstrap correlation matrix $0.10 &lt; q^2 &lt; 0.98~{\rm GeV}^2/c^4$.
description: CERN-LHC. An angular analysis of the $B^{0} \rightarrow K^{*0}(\rightarrow K^{+}\pi^{-})\mu^{+}\mu^{-}$ decay is presented. The dataset corresponds to an integrated luminosity of $3.0$ fb$^{-1}$ of $pp$ collision data collected at the LHCb experiment. The complete angular information from the decay is used to determine $C\!P$-averaged observables and $C\!P$ asymmetries, taking account of possible contamination from decays with the $K^{+}\pi^{-}$ system in an S-wave configuration. The angular observables and their correlations are reported in bins of $q^2$, the invariant mass squared of the dimuon system. The observables are determined both from an unbinned maximum likelihood fit and by using the principal moments of the angular distribution. In addition, by fitting for $q^2$-dependent decay amplitudes in the region $1.1 &lt; q^{2} &lt; 6.0 \mathrm{\,GeV}^{2}/c^{4}$, the zero-crossing points of several angular observables are computed. A global fit is performed to the complete set of $C\!P$-averaged observables obtained from the maximum likelihood fit. This fit indicates differences with predictions based on the Standard Model at the level of 3.4 standard deviations. These differences could be explained by contributions from physics beyond the Standard Model, or by an unexpectedly large hadronic effect that is not accounted for in the Standard Model predictions.
DOI: 10.17182/hepdata.74247.v1/t40
title: "Table 40" of "Angular analysis of the $B^{0}\rightarrow K^{*0}\mu^{+}\mu^{-}$ decay"

description: Bootstrap correlation matrix $1.1 &lt; q^2 &lt; 2.0~{\rm GeV}^2/c^4$.
description: CERN-LHC. An angular analysis of the $B^{0} \rightarrow K^{*0}(\rightarrow K^{+}\pi^{-})\mu^{+}\mu^{-}$ decay is presented. The dataset corresponds to an integrated luminosity of $3.0$ fb$^{-1}$ of $pp$ collision data collected at the LHCb experiment. The complete angular information from the decay is used to determine $C\!P$-averaged observables and $C\!P$ asymmetries, taking account of possible contamination from decays with the $K^{+}\pi^{-}$ system in an S-wave configuration. The angular observables and their correlations are reported in bins of $q^2$, the invariant mass squared of the dimuon system. The observables are determined both from an unbinned maximum likelihood fit and by using the principal moments of the angular distribution. In addition, by fitting for $q^2$-dependent decay amplitudes in the region $1.1 &lt; q^{2} &lt; 6.0 \mathrm{\,GeV}^{2}/c^{4}$, the zero-crossing points of several angular observables are computed. A global fit is performed to the complete set of $C\!P$-averaged observables obtained from the maximum likelihood fit. This fit indicates differences with predictions based on the Standard Model at the level of 3.4 standard deviations. These differences could be explained by contributions from physics beyond the Standard Model, or by an unexpectedly large hadronic effect that is not accounted for in the Standard Model predictions.
DOI: 10.17182/hepdata.74247.v1/t41
title: "Table 41" of "Angular analysis of the $B^{0}\rightarrow K^{*0}\mu^{+}\mu^{-}$ decay"

description: Bootstrap correlation matrix $2.0 &lt; q^2 &lt; 3.0~{\rm GeV}^2/c^4$.
description: CERN-LHC. An angular analysis of the $B^{0} \rightarrow K^{*0}(\rightarrow K^{+}\pi^{-})\mu^{+}\mu^{-}$ decay is presented. The dataset corresponds to an integrated luminosity of $3.0$ fb$^{-1}$ of $pp$ collision data collected at the LHCb experiment. The complete angular information from the decay is used to determine $C\!P$-averaged observables and $C\!P$ asymmetries, taking account of possible contamination from decays with the $K^{+}\pi^{-}$ system in an S-wave configuration. The angular observables and their correlations are reported in bins of $q^2$, the invariant mass squared of the dimuon system. The observables are determined both from an unbinned maximum likelihood fit and by using the principal moments of the angular distribution. In addition, by fitting for $q^2$-dependent decay amplitudes in the region $1.1 &lt; q^{2} &lt; 6.0 \mathrm{\,GeV}^{2}/c^{4}$, the zero-crossing points of several angular observables are computed. A global fit is performed to the complete set of $C\!P$-averaged observables obtained from the maximum likelihood fit. This fit indicates differences with predictions based on the Standard Model at the level of 3.4 standard deviations. These differences could be explained by contributions from physics beyond the Standard Model, or by an unexpectedly large hadronic effect that is not accounted for in the Standard Model predictions.
DOI: 10.17182/hepdata.74247.v1/t42
title: "Table 42" of "Angular analysis of the $B^{0}\rightarrow K^{*0}\mu^{+}\mu^{-}$ decay"

description: Bootstrap correlation matrix $3.0 &lt; q^2 &lt; 4.0~{\rm GeV}^2/c^4$.
description: CERN-LHC. An angular analysis of the $B^{0} \rightarrow K^{*0}(\rightarrow K^{+}\pi^{-})\mu^{+}\mu^{-}$ decay is presented. The dataset corresponds to an integrated luminosity of $3.0$ fb$^{-1}$ of $pp$ collision data collected at the LHCb experiment. The complete angular information from the decay is used to determine $C\!P$-averaged observables and $C\!P$ asymmetries, taking account of possible contamination from decays with the $K^{+}\pi^{-}$ system in an S-wave configuration. The angular observables and their correlations are reported in bins of $q^2$, the invariant mass squared of the dimuon system. The observables are determined both from an unbinned maximum likelihood fit and by using the principal moments of the angular distribution. In addition, by fitting for $q^2$-dependent decay amplitudes in the region $1.1 &lt; q^{2} &lt; 6.0 \mathrm{\,GeV}^{2}/c^{4}$, the zero-crossing points of several angular observables are computed. A global fit is performed to the complete set of $C\!P$-averaged observables obtained from the maximum likelihood fit. This fit indicates differences with predictions based on the Standard Model at the level of 3.4 standard deviations. These differences could be explained by contributions from physics beyond the Standard Model, or by an unexpectedly large hadronic effect that is not accounted for in the Standard Model predictions.
DOI: 10.17182/hepdata.74247.v1/t43
title: "Table 43" of "Angular analysis of the $B^{0}\rightarrow K^{*0}\mu^{+}\mu^{-}$ decay"

description: Bootstrap correlation matrix $4.0 &lt; q^2 &lt; 5.0~{\rm GeV}^2/c^4$.
description: CERN-LHC. An angular analysis of the $B^{0} \rightarrow K^{*0}(\rightarrow K^{+}\pi^{-})\mu^{+}\mu^{-}$ decay is presented. The dataset corresponds to an integrated luminosity of $3.0$ fb$^{-1}$ of $pp$ collision data collected at the LHCb experiment. The complete angular information from the decay is used to determine $C\!P$-averaged observables and $C\!P$ asymmetries, taking account of possible contamination from decays with the $K^{+}\pi^{-}$ system in an S-wave configuration. The angular observables and their correlations are reported in bins of $q^2$, the invariant mass squared of the dimuon system. The observables are determined both from an unbinned maximum likelihood fit and by using the principal moments of the angular distribution. In addition, by fitting for $q^2$-dependent decay amplitudes in the region $1.1 &lt; q^{2} &lt; 6.0 \mathrm{\,GeV}^{2}/c^{4}$, the zero-crossing points of several angular observables are computed. A global fit is performed to the complete set of $C\!P$-averaged observables obtained from the maximum likelihood fit. This fit indicates differences with predictions based on the Standard Model at the level of 3.4 standard deviations. These differences could be explained by contributions from physics beyond the Standard Model, or by an unexpectedly large hadronic effect that is not accounted for in the Standard Model predictions.
DOI: 10.17182/hepdata.74247.v1/t44
title: "Table 44" of "Angular analysis of the $B^{0}\rightarrow K^{*0}\mu^{+}\mu^{-}$ decay"

description: Bootstrap correlation matrix $5.0 &lt; q^2 &lt; 6.0~{\rm GeV}^2/c^4$.
description: CERN-LHC. An angular analysis of the $B^{0} \rightarrow K^{*0}(\rightarrow K^{+}\pi^{-})\mu^{+}\mu^{-}$ decay is presented. The dataset corresponds to an integrated luminosity of $3.0$ fb$^{-1}$ of $pp$ collision data collected at the LHCb experiment. The complete angular information from the decay is used to determine $C\!P$-averaged observables and $C\!P$ asymmetries, taking account of possible contamination from decays with the $K^{+}\pi^{-}$ system in an S-wave configuration. The angular observables and their correlations are reported in bins of $q^2$, the invariant mass squared of the dimuon system. The observables are determined both from an unbinned maximum likelihood fit and by using the principal moments of the angular distribution. In addition, by fitting for $q^2$-dependent decay amplitudes in the region $1.1 &lt; q^{2} &lt; 6.0 \mathrm{\,GeV}^{2}/c^{4}$, the zero-crossing points of several angular observables are computed. A global fit is performed to the complete set of $C\!P$-averaged observables obtained from the maximum likelihood fit. This fit indicates differences with predictions based on the Standard Model at the level of 3.4 standard deviations. These differences could be explained by contributions from physics beyond the Standard Model, or by an unexpectedly large hadronic effect that is not accounted for in the Standard Model predictions.
DOI: 10.17182/hepdata.74247.v1/t45
title: "Table 45" of "Angular analysis of the $B^{0}\rightarrow K^{*0}\mu^{+}\mu^{-}$ decay"

description: Bootstrap correlation matrix $6.0 &lt; q^2 &lt; 7.0~{\rm GeV}^2/c^4$.
description: CERN-LHC. An angular analysis of the $B^{0} \rightarrow K^{*0}(\rightarrow K^{+}\pi^{-})\mu^{+}\mu^{-}$ decay is presented. The dataset corresponds to an integrated luminosity of $3.0$ fb$^{-1}$ of $pp$ collision data collected at the LHCb experiment. The complete angular information from the decay is used to determine $C\!P$-averaged observables and $C\!P$ asymmetries, taking account of possible contamination from decays with the $K^{+}\pi^{-}$ system in an S-wave configuration. The angular observables and their correlations are reported in bins of $q^2$, the invariant mass squared of the dimuon system. The observables are determined both from an unbinned maximum likelihood fit and by using the principal moments of the angular distribution. In addition, by fitting for $q^2$-dependent decay amplitudes in the region $1.1 &lt; q^{2} &lt; 6.0 \mathrm{\,GeV}^{2}/c^{4}$, the zero-crossing points of several angular observables are computed. A global fit is performed to the complete set of $C\!P$-averaged observables obtained from the maximum likelihood fit. This fit indicates differences with predictions based on the Standard Model at the level of 3.4 standard deviations. These differences could be explained by contributions from physics beyond the Standard Model, or by an unexpectedly large hadronic effect that is not accounted for in the Standard Model predictions.
DOI: 10.17182/hepdata.74247.v1/t46
title: "Table 46" of "Angular analysis of the $B^{0}\rightarrow K^{*0}\mu^{+}\mu^{-}$ decay"

description: Bootstrap correlation matrix $7.0 &lt; q^2 &lt; 8.0~{\rm GeV}^2/c^4$.
description: CERN-LHC. An angular analysis of the $B^{0} \rightarrow K^{*0}(\rightarrow K^{+}\pi^{-})\mu^{+}\mu^{-}$ decay is presented. The dataset corresponds to an integrated luminosity of $3.0$ fb$^{-1}$ of $pp$ collision data collected at the LHCb experiment. The complete angular information from the decay is used to determine $C\!P$-averaged observables and $C\!P$ asymmetries, taking account of possible contamination from decays with the $K^{+}\pi^{-}$ system in an S-wave configuration. The angular observables and their correlations are reported in bins of $q^2$, the invariant mass squared of the dimuon system. The observables are determined both from an unbinned maximum likelihood fit and by using the principal moments of the angular distribution. In addition, by fitting for $q^2$-dependent decay amplitudes in the region $1.1 &lt; q^{2} &lt; 6.0 \mathrm{\,GeV}^{2}/c^{4}$, the zero-crossing points of several angular observables are computed. A global fit is performed to the complete set of $C\!P$-averaged observables obtained from the maximum likelihood fit. This fit indicates differences with predictions based on the Standard Model at the level of 3.4 standard deviations. These differences could be explained by contributions from physics beyond the Standard Model, or by an unexpectedly large hadronic effect that is not accounted for in the Standard Model predictions.
DOI: 10.17182/hepdata.74247.v1/t47
title: "Table 47" of "Angular analysis of the $B^{0}\rightarrow K^{*0}\mu^{+}\mu^{-}$ decay"

description: Bootstrap correlation matrix $11.00
description: CERN-LHC. An angular analysis of the $B^{0} \rightarrow K^{*0}(\rightarrow K^{+}\pi^{-})\mu^{+}\mu^{-}$ decay is presented. The dataset corresponds to an integrated luminosity of $3.0$ fb$^{-1}$ of $pp$ collision data collected at the LHCb experiment. The complete angular information from the decay is used to determine $C\!P$-averaged observables and $C\!P$ asymmetries, taking account of possible contamination from decays with the $K^{+}\pi^{-}$ system in an S-wave configuration. The angular observables and their correlations are reported in bins of $q^2$, the invariant mass squared of the dimuon system. The observables are determined both from an unbinned maximum likelihood fit and by using the principal moments of the angular distribution. In addition, by fitting for $q^2$-dependent decay amplitudes in the region $1.1 &lt; q^{2} &lt; 6.0 \mathrm{\,GeV}^{2}/c^{4}$, the zero-crossing points of several angular observables are computed. A global fit is performed to the complete set of $C\!P$-averaged observables obtained from the maximum likelihood fit. This fit indicates differences with predictions based on the Standard Model at the level of 3.4 standard deviations. These differences could be explained by contributions from physics beyond the Standard Model, or by an unexpectedly large hadronic effect that is not accounted for in the Standard Model predictions.
DOI: 10.17182/hepdata.74247.v1/t48
title: "Table 48" of "Angular analysis of the $B^{0}\rightarrow K^{*0}\mu^{+}\mu^{-}$ decay"

description: Bootstrap correlation matrix $11.75
description: CERN-LHC. An angular analysis of the $B^{0} \rightarrow K^{*0}(\rightarrow K^{+}\pi^{-})\mu^{+}\mu^{-}$ decay is presented. The dataset corresponds to an integrated luminosity of $3.0$ fb$^{-1}$ of $pp$ collision data collected at the LHCb experiment. The complete angular information from the decay is used to determine $C\!P$-averaged observables and $C\!P$ asymmetries, taking account of possible contamination from decays with the $K^{+}\pi^{-}$ system in an S-wave configuration. The angular observables and their correlations are reported in bins of $q^2$, the invariant mass squared of the dimuon system. The observables are determined both from an unbinned maximum likelihood fit and by using the principal moments of the angular distribution. In addition, by fitting for $q^2$-dependent decay amplitudes in the region $1.1 &lt; q^{2} &lt; 6.0 \mathrm{\,GeV}^{2}/c^{4}$, the zero-crossing points of several angular observables are computed. A global fit is performed to the complete set of $C\!P$-averaged observables obtained from the maximum likelihood fit. This fit indicates differences with predictions based on the Standard Model at the level of 3.4 standard deviations. These differences could be explained by contributions from physics beyond the Standard Model, or by an unexpectedly large hadronic effect that is not accounted for in the Standard Model predictions.
DOI: 10.17182/hepdata.74247.v1/t49
title: "Table 49" of "Angular analysis of the $B^{0}\rightarrow K^{*0}\mu^{+}\mu^{-}$ decay"

description: Bootstrap correlation matrix $15.0
description: CERN-LHC. An angular analysis of the $B^{0} \rightarrow K^{*0}(\rightarrow K^{+}\pi^{-})\mu^{+}\mu^{-}$ decay is presented. The dataset corresponds to an integrated luminosity of $3.0$ fb$^{-1}$ of $pp$ collision data collected at the LHCb experiment. The complete angular information from the decay is used to determine $C\!P$-averaged observables and $C\!P$ asymmetries, taking account of possible contamination from decays with the $K^{+}\pi^{-}$ system in an S-wave configuration. The angular observables and their correlations are reported in bins of $q^2$, the invariant mass squared of the dimuon system. The observables are determined both from an unbinned maximum likelihood fit and by using the principal moments of the angular distribution. In addition, by fitting for $q^2$-dependent decay amplitudes in the region $1.1 &lt; q^{2} &lt; 6.0 \mathrm{\,GeV}^{2}/c^{4}$, the zero-crossing points of several angular observables are computed. A global fit is performed to the complete set of $C\!P$-averaged observables obtained from the maximum likelihood fit. This fit indicates differences with predictions based on the Standard Model at the level of 3.4 standard deviations. These differences could be explained by contributions from physics beyond the Standard Model, or by an unexpectedly large hadronic effect that is not accounted for in the Standard Model predictions.
DOI: 10.17182/hepdata.74247.v1/t50
title: "Table 50" of "Angular analysis of the $B^{0}\rightarrow K^{*0}\mu^{+}\mu^{-}$ decay"

description: Bootstrap correlation matrix $16.0
description: CERN-LHC. An angular analysis of the $B^{0} \rightarrow K^{*0}(\rightarrow K^{+}\pi^{-})\mu^{+}\mu^{-}$ decay is presented. The dataset corresponds to an integrated luminosity of $3.0$ fb$^{-1}$ of $pp$ collision data collected at the LHCb experiment. The complete angular information from the decay is used to determine $C\!P$-averaged observables and $C\!P$ asymmetries, taking account of possible contamination from decays with the $K^{+}\pi^{-}$ system in an S-wave configuration. The angular observables and their correlations are reported in bins of $q^2$, the invariant mass squared of the dimuon system. The observables are determined both from an unbinned maximum likelihood fit and by using the principal moments of the angular distribution. In addition, by fitting for $q^2$-dependent decay amplitudes in the region $1.1 &lt; q^{2} &lt; 6.0 \mathrm{\,GeV}^{2}/c^{4}$, the zero-crossing points of several angular observables are computed. A global fit is performed to the complete set of $C\!P$-averaged observables obtained from the maximum likelihood fit. This fit indicates differences with predictions based on the Standard Model at the level of 3.4 standard deviations. These differences could be explained by contributions from physics beyond the Standard Model, or by an unexpectedly large hadronic effect that is not accounted for in the Standard Model predictions.
DOI: 10.3886/e222742v1
title: Code for: Explaining Variation in Child SSI Receipt: The Role of Medical CDRs

description: The administrative processes that govern the delivery of social safety net benefits have important implications for beneficiaries. We use variation in the occurrence of medical continuing disability reviews (CDRs) to explain trends of children receiving Supplemental Security Income (SSI) payments. CDR frequency is a major driver of SSI caseload dynamics, significantly influencing both program growth and decline. The percent of caseload changes that can be explained by CDRs varied substantially by geography. Understanding these regional variations in a federal program with a uniform set of rules across the entire country is critical to ensuring equitable access to the program.
DOI: 10.17182/hepdata.74247.v1/t51
title: "Table 51" of "Angular analysis of the $B^{0}\rightarrow K^{*0}\mu^{+}\mu^{-}$ decay"

description: Bootstrap correlation matrix $17.0
description: CERN-LHC. An angular analysis of the $B^{0} \rightarrow K^{*0}(\rightarrow K^{+}\pi^{-})\mu^{+}\mu^{-}$ decay is presented. The dataset corresponds to an integrated luminosity of $3.0$ fb$^{-1}$ of $pp$ collision data collected at the LHCb experiment. The complete angular information from the decay is used to determine $C\!P$-averaged observables and $C\!P$ asymmetries, taking account of possible contamination from decays with the $K^{+}\pi^{-}$ system in an S-wave configuration. The angular observables and their correlations are reported in bins of $q^2$, the invariant mass squared of the dimuon system. The observables are determined both from an unbinned maximum likelihood fit and by using the principal moments of the angular distribution. In addition, by fitting for $q^2$-dependent decay amplitudes in the region $1.1 &lt; q^{2} &lt; 6.0 \mathrm{\,GeV}^{2}/c^{4}$, the zero-crossing points of several angular observables are computed. A global fit is performed to the complete set of $C\!P$-averaged observables obtained from the maximum likelihood fit. This fit indicates differences with predictions based on the Standard Model at the level of 3.4 standard deviations. These differences could be explained by contributions from physics beyond the Standard Model, or by an unexpectedly large hadronic effect that is not accounted for in the Standard Model predictions.