Giulia Casarosa
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Giulia Casarosa has a total of 1000 co-authors. Here are the top co-authors by number of shared publications:
- Stefano Bettarini
The Belle II Collaboration)
287 shared publications - Lorenzo Vitale
The Belle II Collaboration)
277 shared publications - J. A. McKenna
The Belle II Collaboration)
269 shared publications - Roberto Stroili
INFN Sezione di Padova, I-35131 Padova, Italy
267 shared publications - Giuliana Rizzo
The Belle II Collaboration)
262 shared publications - Robert Kowalewski
University of Victoria
259 shared publications
Latest Publications
- Open Access
- 4 November 2026
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 137 (19)
First Measurement of the Masses of the ϒ 1 ( 1 D ) and ϒ 3 ( 1 D ) States and the Energy Dependence of the Cross Sections for e + e − → ϒ J ( 1 D ) η and e + e − → ϒ J <mo...
We study the processes e + e − → ϒ J ( 1 D ) η and e + e − → ϒ J ( 1 D ) π + π − at center-of-mass energies s = ( 10.73 − 11.02 ) GeV using a 142.5 fb − 1 data sample, including 122 fb − 1 near the ϒ ( 10860 ) peak ( s = 10.866 GeV ), collected with the Belle detector at the KEKB asymmetric-energy e + e − collider. From the peak sample, the products of Born cross section times branching fraction are obtained for σ Born ( e + e − → ϒ J ( 1 D ) η ) or σ Born ( e + e − → ϒ J ( 1 D ) π + π − ) and B ( ϒ J ( 1 D ) → χ b 1 γ ) or B ( ϒ J ( 1 D ) → χ b 2 γ ) for each ϒ J ( 1 D ) state. The corresponding branching fractions for ϒ ( 10860 ) decays are also obtained. The significances of the ϒ 1 ( 1 D ) , ϒ 2 ( 1 D ) , and ϒ 3 ( 1 D ) signals are 4.8 σ , > 10 σ , and 3.0 σ , respectively, including systematic uncertainties. The mass for ϒ 2 ( 1 D ) is measured to be ( 10167.0 ± 1.0 ± 0.2 ) MeV / c 2 , where the first and second uncertainties are statistical and systematic. The mass splittings Δ m 12 = m ( ϒ 2 ( 1 D ) ) − m ( ϒ 1 ( 1 D ) ) and Δ m 23 = m ( ϒ 3 ( 1 D ) ) − m ( ϒ 2 ( 1 D ) ) are ( 11.8 ± 1.5 ± 0.4 ) MeV / c 2 and ( 7.6 ± 2.4 ± 0.6 ) MeV / c 2 , respectively. We determine the energy dependence of the cross sections for e + e − → ϒ J ( 1 D ) η and e + e − → ϒ J ( 1 D ) π + π − for the ϒ 1 ( 1 D ) , ϒ 2 ( 1 D ) , and ϒ 3 ( 1 D ) states, combined.
- 4 November 2026
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 137 (19)
Open AccessFirst Measurement of the Masses of the ϒ 1 ( 1 D ) and ϒ 3 ( 1 D ) States and the Energy Dependence of the Cross Sections for e + e − → ϒ J ( 1 D ) η and e + e − → ϒ J <mo...
We study the processes e + e − → ϒ J ( 1 D ) η and e + e − → ϒ J ( 1 D ) π + π − at center-of-mass energies s = ( 10.73 − 11.02 ) GeV using a 142.5 fb − 1 data sample, including 122 fb − 1 near the ϒ ( 10860 ) peak ( s = 10.866 GeV ), collected with the Belle detector at the KEKB asymmetric-energy e + e − collider. From the peak sample, the products of Born cross section times branching fraction are obtained for σ Born ( e + e − → ϒ J ( 1 D ) η ) or σ Born ( e + e − → ϒ J ( 1 D ) π + π − ) and B ( ϒ J ( 1 D ) → χ b 1 γ ) or B ( ϒ J ( 1 D ) → χ b 2 γ ) for each ϒ J ( 1 D ) state. The corresponding branching fractions for ϒ ( 10860 ) decays are also obtained. The significances of the ϒ 1 ( 1 D ) , ϒ 2 ( 1 D ) , and ϒ 3 ( 1 D ) signals are 4.8 σ , > 10 σ , and 3.0 σ , respectively, including systematic uncertainties. The mass for ϒ 2 ( 1 D ) is measured to be ( 10167.0 ± 1.0 ± 0.2 ) MeV / c 2 , where the first and second uncertainties are statistical and systematic. The mass splittings Δ m 12 = m ( ϒ 2 ( 1 D ) ) − m ( ϒ 1 ( 1 D ) ) and Δ m 23 = m ( ϒ 3 ( 1 D ) ) − m ( ϒ 2 ( 1 D ) ) are ( 11.8 ± 1.5 ± 0.4 ) MeV / c 2 and ( 7.6 ± 2.4 ± 0.6 ) MeV / c 2 , respectively. We determine the energy dependence of the cross sections for e + e − → ϒ J ( 1 D ) η and e + e − → ϒ J ( 1 D ) π + π − for the ϒ 1 ( 1 D ) , ϒ 2 ( 1 D ) , and ϒ 3 ( 1 D ) states, combined.
- Open Access
- 30 September 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 114 (5)
Observation of the decays B + → Σ c ( 2455 ) + + Ξ ¯ c ′ − and B 0 → Σ c ( 2455 ) ...
We report the first observation of the decays B + → Σ c ( 2455 ) + + Ξ ¯ c ′ − and B 0 → Σ c ( 2455 ) 0 Ξ ¯ c ′ 0 , with significances of 6.4 σ and 5.3 σ , respectively, including systematic uncertainties. This analysis is based on data samples containing 771.6 × 10 6 ϒ ( 4 S ) decays collected with the Belle detector at the KEKB collider and 520.6 × 10 6 ϒ ( 4 S ) decays collected with the Belle II detector at the SuperKEKB collider. The branching fractions are measured to be B ( B + → Σ c ( 2455 ) + + Ξ ¯ c ′ − ) = ( 1.69 ± 0.31 ± 0.1 2 − 0.56 + 1.39 ) × 10 − 3 and B ( B 0 → Σ c ( 2455 ) 0 Ξ ¯ c ′ 0 ) = ( 1.28 ± 0.32 ± 0.1 0 − 0.22 + 0.26 ) × 10 − 3 , where the first and second uncertainties are statistical and systematic, respectively, and the third arises from the uncertainties in the absolute branching fractions of Ξ ¯ c − and Ξ ¯ c 0 decays. This result represents the first observation of B -meson decays into a pair of charmed baryon-antibaryon states belonging to the same S U ( 3 ) flavor sextet.
- 30 September 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 114 (5)
Open AccessObservation of the decays B + → Σ c ( 2455 ) + + Ξ ¯ c ′ − and B 0 → Σ c ( 2455 ) ...
We report the first observation of the decays B + → Σ c ( 2455 ) + + Ξ ¯ c ′ − and B 0 → Σ c ( 2455 ) 0 Ξ ¯ c ′ 0 , with significances of 6.4 σ and 5.3 σ , respectively, including systematic uncertainties. This analysis is based on data samples containing 771.6 × 10 6 ϒ ( 4 S ) decays collected with the Belle detector at the KEKB collider and 520.6 × 10 6 ϒ ( 4 S ) decays collected with the Belle II detector at the SuperKEKB collider. The branching fractions are measured to be B ( B + → Σ c ( 2455 ) + + Ξ ¯ c ′ − ) = ( 1.69 ± 0.31 ± 0.1 2 − 0.56 + 1.39 ) × 10 − 3 and B ( B 0 → Σ c ( 2455 ) 0 Ξ ¯ c ′ 0 ) = ( 1.28 ± 0.32 ± 0.1 0 − 0.22 + 0.26 ) × 10 − 3 , where the first and second uncertainties are statistical and systematic, respectively, and the third arises from the uncertainties in the absolute branching fractions of Ξ ¯ c − and Ξ ¯ c 0 decays. This result represents the first observation of B -meson decays into a pair of charmed baryon-antibaryon states belonging to the same S U ( 3 ) flavor sextet.
- Open Access
- 21 September 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (9) , 216
Measurement of time-dependent CP violation parameters in ${B}^{0}\to {K}_{\text{S}}^{0}{\pi }^{0}\gamma $ decays at Belle and Belle IIA bstract: We perform a measurement of time-dependent CP violation parameters in $${B}^{0}\to {K}_{\text{S}}^{0}{\pi }^{0}\gamma $$ decays using a dataset of approximately 772 × 10 6 and 521 × 10 6 Υ(4 S ) decays collected by the Belle and Belle II experiments, respectively. The measured parameters for the combined dataset in the K *0 (892) dominated region ( $${M}_{{K}_{\text{S}}^{0}{\pi }^{0}}\in \left[{0.8,1.0}\right]$$ GeV/ c 2 ) are S = 0.09 ± 0.16 ± 0.02 and C = − 0.09 ± 0.08 ± 0.04. For the non- K *0 (892) region ( $${M}_{{K}_{\text{S}}^{0}{\pi }^{0}}\in \left({1.0,1.8}\right]$$ GeV/ c 2 ), the corresponding values are S = −0.32 ± 0.33 ± 0.09 and C = −0.07 ± 0.17 ± 0.08. The first quoted uncertainties are statistical, while the second ones are systematic. These results are consistent with Standard Model predictions and more precise than previous measurements.- 21 September 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (9) , 216
Open AccessMeasurement of time-dependent CP violation parameters in ${B}^{0}\to {K}_{\text{S}}^{0}{\pi }^{0}\gamma $ decays at Belle and Belle IIA bstract: We perform a measurement of time-dependent CP violation parameters in $${B}^{0}\to {K}_{\text{S}}^{0}{\pi }^{0}\gamma $$ decays using a dataset of approximately 772 × 10 6 and 521 × 10 6 Υ(4 S ) decays collected by the Belle and Belle II experiments, respectively. The measured parameters for the combined dataset in the K *0 (892) dominated region ( $${M}_{{K}_{\text{S}}^{0}{\pi }^{0}}\in \left[{0.8,1.0}\right]$$ GeV/ c 2 ) are S = 0.09 ± 0.16 ± 0.02 and C = − 0.09 ± 0.08 ± 0.04. For the non- K *0 (892) region ( $${M}_{{K}_{\text{S}}^{0}{\pi }^{0}}\in \left({1.0,1.8}\right]$$ GeV/ c 2 ), the corresponding values are S = −0.32 ± 0.33 ± 0.09 and C = −0.07 ± 0.17 ± 0.08. The first quoted uncertainties are statistical, while the second ones are systematic. These results are consistent with Standard Model predictions and more precise than previous measurements. - Open Access
- 12 August 2026
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 137 (7) , 071803
Searches for Charged-Lepton-Flavor Violation in χ b J ( 1 P ) Decays
We report the first searches for charged-lepton-flavor violation in decays of χ b J ( 1 P ) ( J = 0 , 1, and 2) to a pair of charged leptons using 158 million ϒ ( 2 S ) decays collected with the Belle detector in e + e − collisions at the KEKB collider. No significant signal is observed, and we set upper limits on the branching fractions for χ b J ( 1 P ) decays to e ± μ ∓ at the level of 10 − 6 and to e ± τ ∓ or μ ± τ ∓ at the level of 10 − 5 . Limits on χ b 0 ( 1 P ) decays are translated into bounds on the corresponding Wilson coefficients of scalar operators that mediate charged-lepton-flavor violation.
- 12 August 2026
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 137 (7) , 071803
Open AccessSearches for Charged-Lepton-Flavor Violation in χ b J ( 1 P ) Decays
We report the first searches for charged-lepton-flavor violation in decays of χ b J ( 1 P ) ( J = 0 , 1, and 2) to a pair of charged leptons using 158 million ϒ ( 2 S ) decays collected with the Belle detector in e + e − collisions at the KEKB collider. No significant signal is observed, and we set upper limits on the branching fractions for χ b J ( 1 P ) decays to e ± μ ∓ at the level of 10 − 6 and to e ± τ ∓ or μ ± τ ∓ at the level of 10 − 5 . Limits on χ b 0 ( 1 P ) decays are translated into bounds on the corresponding Wilson coefficients of scalar operators that mediate charged-lepton-flavor violation.
- Top Cited Papers
- 5 August 2026
- Published by World Scientific Pub Co Pte Ltd in International Journal of Modern Physics A
- Vol. 41 (22)
Review of Particle Physics *
The Review summarizes much of particle physics and cosmology. Using data from previous editions, plus 3,200 new measurements from 903 papers, we list, evaluate, and average measured properties of gauge bosons and the recently discovered Higgs boson, leptons, quarks, mesons, and baryons. We summarize searches for hypothetical particles such as supersymmetric particles, heavy bosons, axions, dark photons, etc. Particle properties and search limits are listed in Summary Tables. We give numerous tables, figures, formulae, and reviews of topics such as Higgs Boson Physics, Supersymmetry, Grand Unified Theories, Neutrino Mixing, Dark Energy, Dark Matter, Cosmology, Particle Detectors, Colliders, Probability and Statistics. Most of the 118 reviews are updated, including many that are heavily revised. The Review is divided into two volumes. Volume 1 includes the Summary Tables and 96 review articles. Volume 2 consists of the Particle Listings and contains also 22 reviews that address specific aspects of the data presented in the Listings. The complete Review (both volumes) is published online on the website of the Particle Data Group ( pdg.lbl.gov ) and in a journal. Volume 1 is available in print as the PDG Book. A Particle Physics Booklet with the Summary Tables and essential tables, figures, and equations from selected review articles is available in print, as a web version optimized for use on phones, and as an Android app. The PDG API (Application Programming Interface) provides access to the data published in the Review in machine-readable format.
- 5 August 2026
- Published by World Scientific Pub Co Pte Ltd in International Journal of Modern Physics A
- Vol. 41 (22)
Top Cited PapersReview of Particle Physics *
The Review summarizes much of particle physics and cosmology. Using data from previous editions, plus 3,200 new measurements from 903 papers, we list, evaluate, and average measured properties of gauge bosons and the recently discovered Higgs boson, leptons, quarks, mesons, and baryons. We summarize searches for hypothetical particles such as supersymmetric particles, heavy bosons, axions, dark photons, etc. Particle properties and search limits are listed in Summary Tables. We give numerous tables, figures, formulae, and reviews of topics such as Higgs Boson Physics, Supersymmetry, Grand Unified Theories, Neutrino Mixing, Dark Energy, Dark Matter, Cosmology, Particle Detectors, Colliders, Probability and Statistics. Most of the 118 reviews are updated, including many that are heavily revised. The Review is divided into two volumes. Volume 1 includes the Summary Tables and 96 review articles. Volume 2 consists of the Particle Listings and contains also 22 reviews that address specific aspects of the data presented in the Listings. The complete Review (both volumes) is published online on the website of the Particle Data Group ( pdg.lbl.gov ) and in a journal. Volume 1 is available in print as the PDG Book. A Particle Physics Booklet with the Summary Tables and essential tables, figures, and equations from selected review articles is available in print, as a web version optimized for use on phones, and as an Android app. The PDG API (Application Programming Interface) provides access to the data published in the Review in machine-readable format.
- Open Access
- 26 June 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (6) , 278
Study of e+e− → π+π−Υ(1D) at Belle II
A bstract: The bottomonium spectrum, consisting of bound states of a b quark and an anti- b quark, provides an excellent laboratory for probing quantum chromodynamics in the non-perturbative regime. While S and P-wave bottomonium states are well studied experimentally, information on D-wave states remains scarce. We search for the D-wave bottomonium states Υ 2 (1 D ) and Υ 3 (1 D ) via the decay of a vector bottomonium-like state Υ(10753) in the reaction e + e − → π + π − Υ(1 D ), using 19 . 6 fb − 1 of data collected with the Belle II detector at center-of-mass energies $$\sqrt{s}=10.653$$ , 10.701, 10.745, and 10.805 GeV, in the vicinity of the Υ(10753) resonance. No significant signals are observed. We set upper limits at the 90% credibility level on the products of the cross sections and branching fractions, σ [ e + e − → π + π − Υ 2 (1 D )] × ℬ(Υ 2 (1 D ) → γχ b 1 ) and σ [ e + e − → π + π − Υ 3 (1 D )] × ℬ(Υ 3 (1 D ) → γχ b 2 ), at each center-of-mass energy.- 26 June 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (6) , 278
Open AccessStudy of e+e− → π+π−Υ(1D) at Belle II
A bstract: The bottomonium spectrum, consisting of bound states of a b quark and an anti- b quark, provides an excellent laboratory for probing quantum chromodynamics in the non-perturbative regime. While S and P-wave bottomonium states are well studied experimentally, information on D-wave states remains scarce. We search for the D-wave bottomonium states Υ 2 (1 D ) and Υ 3 (1 D ) via the decay of a vector bottomonium-like state Υ(10753) in the reaction e + e − → π + π − Υ(1 D ), using 19 . 6 fb − 1 of data collected with the Belle II detector at center-of-mass energies $$\sqrt{s}=10.653$$ , 10.701, 10.745, and 10.805 GeV, in the vicinity of the Υ(10753) resonance. No significant signals are observed. We set upper limits at the 90% credibility level on the products of the cross sections and branching fractions, σ [ e + e − → π + π − Υ 2 (1 D )] × ℬ(Υ 2 (1 D ) → γχ b 1 ) and σ [ e + e − → π + π − Υ 3 (1 D )] × ℬ(Υ 3 (1 D ) → γχ b 2 ), at each center-of-mass energy. - Open Access
- 23 June 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 113 (11)
Study of e + e − → h + h − J / ψ ( h = π , K , p ) via initial-state radiation at Belle II
Using a data sample of 427.9 fb − 1 collected by the Belle II detector at or near the ϒ ( 4 S ) and ϒ ( 10753 ) resonances, the cross sections for e + e − → h + h − J / ψ ( h = π / K / p ) at center-of-mass energies ranging from 3.8 GeV or the production threshold to 5.5 / 6.0 / 7.0 GeV have been measured via initial-state radiation. The cross sections for the processes e + e − → π + π − J / ψ and e + e − → K + K − J / ψ are consistent with previously published results. The cross sections for these channels obtained by combining with previous Belle results are also given. The process e + e − → p p ¯ J / ψ is investigated for the first time. The yields are small and no significant structure is observed in the cross section versus energy. Searches for vector charmoniumlike states in the h + h − J / ψ systems, and for associated intermediate states in the h ± J / ψ systems, are also presented.
- 23 June 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 113 (11)
Open AccessStudy of e + e − → h + h − J / ψ ( h = π , K , p ) via initial-state radiation at Belle II
Using a data sample of 427.9 fb − 1 collected by the Belle II detector at or near the ϒ ( 4 S ) and ϒ ( 10753 ) resonances, the cross sections for e + e − → h + h − J / ψ ( h = π / K / p ) at center-of-mass energies ranging from 3.8 GeV or the production threshold to 5.5 / 6.0 / 7.0 GeV have been measured via initial-state radiation. The cross sections for the processes e + e − → π + π − J / ψ and e + e − → K + K − J / ψ are consistent with previously published results. The cross sections for these channels obtained by combining with previous Belle results are also given. The process e + e − → p p ¯ J / ψ is investigated for the first time. The yields are small and no significant structure is observed in the cross section versus energy. Searches for vector charmoniumlike states in the h + h − J / ψ systems, and for associated intermediate states in the h ± J / ψ systems, are also presented.
- Open Access
- 22 June 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 113 (11)
Study of B + → μ + ν μ decays at Belle and Belle II
We report a measurement of the branching fraction for the leptonic decay B + → μ + ν μ . This work presents the first B + → μ + ν μ result using Belle II data, an updated Belle measurement that supersedes the previous result, and their combination, which yields the most precise search to date. The analysis is based on 1076 fb − 1 of e + e − collision data collected at a center-of-mass energy of 10.58 GeV with the Belle and Belle II detectors at the KEKB and SuperKEKB colliders, respectively. We measure B ( B + → μ + ν μ ) = ( 4.4 ± 1.9 ± 1.0 ) × 10 − 7 , where the first uncertainty is statistical and the second systematic. The observed significance relative to the background-only hypothesis is 2.4 standard deviations. We set a 90% confidence level upper limit of B ( B + → μ + ν μ ) < 6.7 × 10 − 7 using a frequentist approach and a 90% credibility level upper limit of B ( B + → μ + ν μ ) < 7.2 × 10 − 7 using a Bayesian approach. These are the most stringent limits to date. The result is interpreted as an exclusion region in the parameter space of type II and type III two-Higgs-doublet models. We search for stable sterile neutrinos with masses m N ∈ [ 0 , 1.5 ] GeV . No signal is observed, and the resulting exclusion on the squared mixing parameter | U μ N | 2 provides improvement over previous limits. We report a measurement of the partial branching fraction of semileptonic B → X u ℓ ν ℓ decays with p μ B > 2.2 GeV , obtaining Δ B ( B → X u ℓ ν ℓ ) = ( 2.72 ± 0.05 ± 0.29 ) × 10 − 4 . We present a model-dependent study of weak annihilation decays using the muon momentum spectrum. We observe a signal of 2.4 standard deviations above the background-only hypothesis in regions where the distribution resembles that of B → X u ℓ ν ℓ decays.
- 22 June 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 113 (11)
Open AccessStudy of B + → μ + ν μ decays at Belle and Belle II
We report a measurement of the branching fraction for the leptonic decay B + → μ + ν μ . This work presents the first B + → μ + ν μ result using Belle II data, an updated Belle measurement that supersedes the previous result, and their combination, which yields the most precise search to date. The analysis is based on 1076 fb − 1 of e + e − collision data collected at a center-of-mass energy of 10.58 GeV with the Belle and Belle II detectors at the KEKB and SuperKEKB colliders, respectively. We measure B ( B + → μ + ν μ ) = ( 4.4 ± 1.9 ± 1.0 ) × 10 − 7 , where the first uncertainty is statistical and the second systematic. The observed significance relative to the background-only hypothesis is 2.4 standard deviations. We set a 90% confidence level upper limit of B ( B + → μ + ν μ ) < 6.7 × 10 − 7 using a frequentist approach and a 90% credibility level upper limit of B ( B + → μ + ν μ ) < 7.2 × 10 − 7 using a Bayesian approach. These are the most stringent limits to date. The result is interpreted as an exclusion region in the parameter space of type II and type III two-Higgs-doublet models. We search for stable sterile neutrinos with masses m N ∈ [ 0 , 1.5 ] GeV . No signal is observed, and the resulting exclusion on the squared mixing parameter | U μ N | 2 provides improvement over previous limits. We report a measurement of the partial branching fraction of semileptonic B → X u ℓ ν ℓ decays with p μ B > 2.2 GeV , obtaining Δ B ( B → X u ℓ ν ℓ ) = ( 2.72 ± 0.05 ± 0.29 ) × 10 − 4 . We present a model-dependent study of weak annihilation decays using the muon momentum spectrum. We observe a signal of 2.4 standard deviations above the background-only hypothesis in regions where the distribution resembles that of B → X u ℓ ν ℓ decays.
- Open Access
- 16 June 2026
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 136 (24) , 241901
Observation of the Radiative Decay D s 0 * ( 2317 ) + → D s * + γ
We report the first observation of the radiative decay D s 0 * ( 2317 ) + → D s * + γ with a statistical significance exceeding 10 standard deviations. The signal is observed in the continuum e + e − → c c ¯ process, using combined data samples of 980.4 fb − 1 from Belle and 427.9 fb − 1 from Belle II, collected at the KEKB and SuperKEKB asymmetric-energy e + e − colliders, respectively. The branching fraction ratio B [ D s 0 * ( 2317 ) + → D s * + γ ] / B [ D s 0 * ( 2317 ) + → D s + π 0 ] is measured to be [ 7.13 ± 0.70 ( stat ) ± 0.26 ( syst ) ] % . This result provides crucial discrimination between theoretical models of the D s 0 * ( 2317 ) + structure.
- 16 June 2026
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 136 (24) , 241901
Open AccessObservation of the Radiative Decay D s 0 * ( 2317 ) + → D s * + γ
We report the first observation of the radiative decay D s 0 * ( 2317 ) + → D s * + γ with a statistical significance exceeding 10 standard deviations. The signal is observed in the continuum e + e − → c c ¯ process, using combined data samples of 980.4 fb − 1 from Belle and 427.9 fb − 1 from Belle II, collected at the KEKB and SuperKEKB asymmetric-energy e + e − colliders, respectively. The branching fraction ratio B [ D s 0 * ( 2317 ) + → D s * + γ ] / B [ D s 0 * ( 2317 ) + → D s + π 0 ] is measured to be [ 7.13 ± 0.70 ( stat ) ± 0.26 ( syst ) ] % . This result provides crucial discrimination between theoretical models of the D s 0 * ( 2317 ) + structure.