{ "metadata": { "title": "HFLAV Charm D0 Hadronic Branching Fractions", "description": "Averages of D0 -> K- pi+, D0 -> pi- pi+, and D0 -> K+ K- branching fractions including correlations among these averages from the fit. Also includes a derived DCS D0 -> K+ pi- branching fraction.", "version": "1.0.1", "date": "2026-02-19", "author": "HFLAV Collaboration", "schema": "1.1.0" }, "groups": [ { "name": "CF & CS D0 to hh branching fractions from fit", "fit": { "chi2": 35.98476, "ndf": 13, "p": 0.0005965862112060339 }, "averages": [ { "name": "BR_D0_K-_pi+", "latexname": "$\\mathcal{B}(D^0 \\to K^- \\pi^+)$", "PDGcode": "S032.1", "comment": "Averages after adjustments to ensure uniform treatment of final state radiation across all input measurements. See chapter 10.3 of https://arxiv.org/pdf/2411.18639", "average": { "value": { "central": 0.03999, "statistical": 5.5e-05, "systematic": 0.00044697203491941194 } } }, { "name": "BR_D0_pi+_pi-", "latexname": "$\\mathcal{B}(D^0 \\to \\pi^+ \\pi^-)$", "PDGcode": "S032.5", "comment": "Averages after adjustments to ensure uniform treatment of final state radiation across all input measurements. See chapter 10.3 of https://arxiv.org/pdf/2411.18639", "average": { "value": { "central": 0.00149, "statistical": 1.2e-05, "systematic": 2.4207436873820408e-05 } } }, { "name": "BR_D0_K+_K-", "latexname": "$\\mathcal{B}(D^0 \\to K^+ K^-)$", "PDGcode": "S032.7", "comment": "Averages after adjustments to ensure uniform treatment of final state radiation across all input measurements. See chapter 10.3 of https://arxiv.org/pdf/2411.18639", "average": { "value": { "central": 0.004113, "statistical": 1.7e-05, "systematic": 4.802082881417188e-05 } } } ], "averages_correlation": [ [ 1.0, 0.767, 0.755 ], [ 0.767, 1.0, 0.577 ], [ 0.755, 0.577, 1.0 ] ], "inputs": [ { "name": "BR_D0_K-_pi+", "latexname": "$\\mathcal{B}(D^0 \\to K^- \\pi^+)$", "comment": "Absolute branching fraction measurements", "sources": [ { "name": "BESIII:2018", "value": { "central": 0.03883, "statistical": 6e-05, "systematic": 0.00051 }, "references": { "bibtex": "BESIII:2018apz", "pub": "Phys. Rev. D 97 (2018) 072004", "doi": "10.1103/PhysRevD.97.072004", "arxiv": "1802.03119", "url": "https://doi.org/10.1103/PhysRevD.97.072004" } }, { "name": "CLEOc:2014", "value": { "central": 0.03934, "statistical": 0.00021, "systematic": 0.00061 }, "references": { "bibtex": "CLEO:2013rjc", "pub": "Phys. Rev. D 89 (2014) 072002", "doi": "10.1103/PhysRevD.89.072002", "arxiv": "1312.6775", "url": "https://doi.org/10.1103/PhysRevD.89.072002" } }, { "name": "BaBar:2008", "value": { "central": 0.04007, "statistical": 0.00037, "systematic": 0.00072 }, "references": { "bibtex": "BaBar:2007crr", "pub": "Phys. Rev. Lett. 100 (2008) 051802", "doi": "10.1103/PhysRevLett.100.051802", "arxiv": "0704.2080", "url": "https://doi.org/10.1103/PhysRevLett.100.051802" } }, { "name": "CLEOII:1998", "value": { "central": 0.0381, "statistical": 0.0015, "systematic": 0.0016 }, "references": { "bibtex": "CLEO:1997zun", "pub": "Phys. Rev. Lett. 80 (1998) 3193", "doi": "10.1103/PhysRevLett.80.3193", "arxiv": "hep-ex/9712023", "url": "https://doi.org/10.1103/PhysRevLett.80.3193" } }, { "name": "ALEPH:1997", "value": { "central": 0.039, "statistical": 0.0009, "systematic": 0.0012 }, "references": { "bibtex": "ALEPH:1997jyv", "pub": "Phys. Lett. B 403 (1997) 367", "doi": "10.1016/S0370-2693(97)00585-6", "url": "https://doi.org/10.1016/S0370-2693(97)00585-6" } }, { "name": "ARGUS:1994", "value": { "central": 0.0341, "statistical": 0.0012, "systematic": 0.0028 }, "references": { "bibtex": "ARGUS:1994onx", "pub": "Phys. Lett. B 340 (1994) 125", "doi": "10.1016/0370-2693(94)91308-0", "url": "https://doi.org/10.1016/0370-2693(94)91308-0" } }, { "name": "CLEOII:1993", "value": { "central": 0.0395, "statistical": 0.0008, "systematic": 0.0017 }, "references": { "bibtex": "CLEO:1993gww", "pub": "Phys. Rev. Lett. 71 (1993) 3070", "doi": "10.1103/PhysRevLett.71.3070", "url": "https://doi.org/10.1103/PhysRevLett.71.3070" } }, { "name": "ALEPH:1991", "value": { "central": 0.0362, "statistical": 0.0034, "systematic": 0.0044 }, "references": { "bibtex": "ALEPH:1991phy", "pub": "Phys. Lett. B 266 (1991) 218", "doi": "10.1016/0370-2693(91)90769-M", "url": "https://doi.org/10.1016/0370-2693(91)90769-M" } } ] }, { "name": "BR_D0_pi+_pi-", "latexname": "$\\mathcal{B}(D^0 \\to \\pi^+ \\pi^-)$", "comment": "Absolute branching fraction measurements", "sources": [ { "name": "BESIII:2018", "value": { "central": 0.001508, "statistical": 1.8e-05, "systematic": 3.2e-05 }, "references": { "bibtex": "BESIII:2018apz", "pub": "Phys. Rev. D 97 (2018) 072004", "doi": "10.1103/PhysRevD.97.072004", "arxiv": "1802.03119", "url": "https://doi.org/10.1103/PhysRevD.97.072004" } } ] }, { "name": "BR_D0_pi+_pi-..BR_D0_K-_pi+", "latexname": "$\\mathcal{B}(D^0 \\to \\pi^+ \\pi^-)/\\mathcal{B}(D^0 \\to K^- \\pi^+)$", "comment": "Ratio to D0 -> K- pi+ measurements", "sources": [ { "name": "CLEOc:2010", "value": { "central": 0.037, "statistical": 0.0006, "systematic": 0.0009 }, "references": { "bibtex": "CLEO:2009fiz", "pub": "Phys. Rev. D 81 (2010) 052013", "doi": "10.1103/PhysRevD.81.052013", "arxiv": "0906.3198", "url": "https://doi.org/10.1103/PhysRevD.81.052013" } }, { "name": "CDF:2005", "value": { "central": 0.03594, "statistical": 0.00054, "systematic": 0.0004 }, "references": { "bibtex": "CDF:2004ohx", "pub": "Phys. Rev. Lett. 94 (2005) 122001", "doi": "10.1103/PhysRevLett.94.122001", "arxiv": "hep-ex/0504006", "url": "https://doi.org/10.1103/PhysRevLett.94.122001" } }, { "name": "FOCUS:2003", "value": { "central": 0.0353, "statistical": 0.0012, "systematic": 0.0006 }, "references": { "bibtex": "FOCUS:2002qvx", "pub": "Phys. Lett. B 555 (2003) 167", "doi": "10.1016/S0370-2693(03)00053-4", "arxiv": "hep-ex/0212058", "url": "https://doi.org/10.1016/S0370-2693(03)00053-4" } } ] }, { "name": "BR_D0_K+_K-", "latexname": "$\\mathcal{B}(D^0 \\to K^+ K^-)$", "comment": "Absolute branching fraction measurements", "sources": [ { "name": "BESIII:2018", "value": { "central": 0.004233, "statistical": 2.1e-05, "systematic": 6.4e-05 }, "references": { "bibtex": "BESIII:2018apz", "pub": "Phys. Rev. D 97 (2018) 072004", "doi": "10.1103/PhysRevD.97.072004", "arxiv": "1802.03119", "url": "https://doi.org/10.1103/PhysRevD.97.072004" } } ] }, { "name": "BR_D0_K+_K-..BR_D0_K-_pi+", "latexname": "$\\mathcal{B}(D^0 \\to K^+ K^-)/\\mathcal{B}(D^0 \\to K^- \\pi^+)$", "comment": "Ratio to D0 -> K- pi+ measurements", "sources": [ { "name": "CLEOc:2010", "value": { "central": 0.1041, "statistical": 0.0011, "systematic": 0.0012 }, "references": { "bibtex": "CLEO:2009fiz", "pub": "Phys. Rev. D 81 (2010) 052013", "doi": "10.1103/PhysRevD.81.052013", "arxiv": "0906.3198", "url": "https://doi.org/10.1103/PhysRevD.81.052013" } }, { "name": "CDF:2005", "value": { "central": 0.0992, "statistical": 0.0011, "systematic": 0.0012 }, "references": { "bibtex": "CDF:2004ohx", "pub": "Phys. Rev. Lett. 94 (2005) 122001", "doi": "10.1103/PhysRevLett.94.122001", "arxiv": "hep-ex/0504006", "url": "https://doi.org/10.1103/PhysRevLett.94.122001" } }, { "name": "FOCUS:2003", "value": { "central": 0.0993, "statistical": 0.0014, "systematic": 0.0014 }, "references": { "bibtex": "FOCUS:2002qvx", "pub": "Phys. Lett. B 555 (2003) 167", "doi": "10.1016/S0370-2693(03)00053-4", "arxiv": "hep-ex/0212058", "url": "https://doi.org/10.1016/S0370-2693(03)00053-4" } } ] } ] }, { "name": "Derived DCS D0 to K+ pi- branching fraction", "fit": { "chi2": 0, "p": 1 }, "averages": [ { "name": "BR_D0_K+_pi-", "latexname": "$\\mathcal{B}(D^0 \\to K^+ \\pi^-)$", "PDGcode": "S032.362", "comment": "Derived DCS D0 to K+ pi- branching fraction. See chapter 10.3 of https://arxiv.org/pdf/2411.18639", "average": { "value": { "central": 0.0001375656, "uncertainty": 1.74345651577549e-06 } } } ], "averages_correlation": [ [ 1.0 ] ], "inputs": [ { "name": "BR_D0_K+_pi-..BR_D0_K-_pi+", "latexname": "$\\mathcal{B}(D^0 \\to K^+ \\pi^-)/\\mathcal{B}(D^0 \\to K^- \\pi^+)$", "comment": "DCS D0 to K+ pi- / CF D0 to K- pi+ branching fraction ratio as determined by HFLAV (includes DCS anti-D0 to K- pi+ in numerator and CF anti-D0 to K+ pi- in denominator). Otherwise known as R_D. See chapter 9.1 of https://arxiv.org/pdf/2411.18639 and compare to D0 to K+ pi- via via DCS Decay Mode Summary in the PDG (PDG ID: S032.362).", "sources": [ { "name": "HFLAV:2026Feb", "value": { "central": 0.00344, "uncertainty": 2e-05 }, "references": { "bibtex": "HeavyFlavorAveragingGroupHFLAV:2024ctg", "pub": "Phys. Rev. D 113 (2026) 012008", "doi": "10.1103/x87q-tld5", "arxiv": "2411.18639", "url": "https://doi.org/10.1103/x87q-tld5" } } ] }, { "name": "BR_D0_K-_pi+", "latexname": "$\\mathcal{B}(D^0 \\to K^- \\pi^+)$", "comment": "CF D0 to K- pi+ branching fraction as determined by HFLAV.", "sources": [ { "name": "HFLAV:2026Feb", "value": { "central": 0.03999, "statistical": 5.5e-05, "systematic": 0.00044697203491941194 }, "references": { "bibtex": "HeavyFlavorAveragingGroupHFLAV:2024ctg", "pub": "Phys. Rev. D 113 (2026) 012008", "doi": "10.1103/x87q-tld5", "arxiv": "2411.18639", "url": "https://doi.org/10.1103/x87q-tld5" } } ] } ] } ] }