May 2025
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8 Reads
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1 Citation
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May 2025
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8 Reads
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1 Citation
May 2025
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1 Read
Using events collected by the BESIII detector operating at the BEPCII storage ring, the decays are observed for the first time through the radiative transition . The statistical significances for signals are all larger than 5. The branching fractions of are determined to be , , and , respectively, where the first uncertainties are statistical and the second systematic. No evident resonant structures are found in the and systems.
May 2025
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14 Reads
Physical Review D
Using a dataset of ( 27.12 ± 0.14 ) × 10 8 ψ ( 3686 ) events collected by the BESIII detector operating at the BEPCII collider, we report the first observation of the decay ψ ( 3686 ) → Σ 0 Σ ¯ 0 ω with a statistical significance of 8.9 σ . The measured branching fraction is ( 1.24 ± 0.1 6 stat ± 0.1 1 sys ) × 10 − 5 , where the first uncertainty is statistical and the second is systematic. Additionally, we investigate potential intermediate states in the invariant mass distributions of Σ 0 ω , Σ ¯ 0 ω and Σ 0 Σ ¯ 0 . A hint of a resonance is observed in the invariant mass distribution of M Σ 0 ( Σ ¯ 0 ) ω , located around 2.06 GeV / c 2 , with a significance of 2.5 σ . Published by the American Physical Society 2025
May 2025
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5 Reads
Physical Review D
Using 20.3 fb − 1 of e + e − collision data collected at a center-of-mass energy of 3.773 GeV with the BESIII detector operating at the BEPCII collider, the branching fractions of three hadronic charm meson decays, D + → ϕ π + π + π − , D + → K S 0 K + π + π − π 0 , and D + → K S 0 K + ω , are measured for the first time to be ( 0.54 ± 0.19 ± 0.02 ) × 10 − 4 , ( 2.51 ± 0.34 ± 0.14 ) × 10 − 4 , and ( 2.02 ± 0.35 ± 0.10 ) × 10 − 4 , respectively. Futhermore, the branching fractions of D + → K + K − π + π + π − and D + → K S 0 K + η are measured with improved precision, yielding values of ( 0.66 ± 0.11 ± 0.03 ) × 10 − 4 and ( 2.27 ± 0.22 ± 0.05 ) × 10 − 4 , respectively. Published by the American Physical Society 2025
May 2025
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8 Reads
The first direct measurement of the relative phase between the strong and electromagnetic amplitudes for a decaying into a vector-pseudoscalar final state is performed using 26 energy points of annihilation data between and \mbox{3.12 GeV}. The data sets were collected by the BESIII detector with a total integrated luminosity of 452 pb. By investigating the interference pattern in the cross section lineshape of , the relative phase between the strong and electromagnetic amplitudes of decay is determined to be within at 68\% confidence level. The result hints at interference between the strong and electromagnetic amplitudes of decay.
May 2025
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6 Reads
Physical Review D
Using 7.93 fb − 1 of e + e − collision data collected at a center-of-mass energy of 3.773 GeV with the BESIII detector, we present an analysis of the decay D 0 → η π − e + ν e . The branching fraction of the decay D 0 → a 0 ( 980 ) − e + ν e with a 0 ( 980 ) − → η π − is measured to be ( 0.86 ± 0.1 7 stat ± 0.0 5 syst ) × 10 − 4 . The decay dynamics of this process is studied with a single-pole parametrization of the hadronic form factor and the Flatté formula describing the a 0 ( 980 ) line shape in the differential decay rate. The product of the form factor f + a 0 ( 0 ) and the Cabibbo-Kobayashi-Maskawa matrix element | V c d | is determined for the first time with the result f + a 0 ( 0 ) | V c d | = 0.126 ± 0.01 3 stat ± 0.00 3 syst . Published by the American Physical Society 2025
May 2025
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10 Reads
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1 Citation
Physical Review Letters
Using ( 2712.4 ± 14.3 ) × 10 6 ψ ( 3686 ) events collected with the BESIII detector at the BEPCII collider, the decay η c → γ γ in J / ψ → γ η c is observed. We determine the product branching fraction B ( J / ψ → γ η c ) × B ( η c → γ γ ) = ( 5.23 ± 0.2 6 stat ± 0.3 0 syst ) × 10 − 6 . This result is consistent with the lattice QCD calculation ( 5.34 ± 0.16 ) × 10 − 6 from HPQCD in 2023. By using the world-average values of B ( J / ψ → γ η c ) and the total decay width of η c , the partial decay width Γ ( η c → γ γ ) is determined to be ( 11.30 ± 0.5 6 stat ± 0.6 6 syst ± 1.1 4 ref ) keV , which deviates from the corresponding world-average value by 3.4 σ . Published by the American Physical Society 2025
April 2025
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107 Reads
In response to the 2020 Update of the European Strategy for Particle Physics, the Future Circular Collider (FCC) Feasibility Study was launched as an international collaboration hosted by CERN. This report describes the FCC integrated programme, which consists of two stages: an electron-positron collider (FCC-ee) in the first phase, serving as a high-luminosity Higgs, top, and electroweak factory; followed by a proton-proton collider (FCC-hh) at the energy frontier in the second phase. FCC-ee is designed to operate at four key centre-of-mass energies: the Z pole, the WW production threshold, the ZH production peak, and the top/anti-top production threshold - delivering the highest possible luminosities to four experiments. Over 15 years of operation, FCC-ee will produce more than 6 trillion Z bosons, 200 million WW pairs, nearly 3 million Higgs bosons, and 2 million top anti-top pairs. Precise energy calibration at the Z pole and WW threshold will be achieved through frequent resonant depolarisation of pilot bunches. The sequence of operation modes remains flexible. FCC-hh will operate at a centre-of-mass energy of approximately 85 TeV - nearly an order of magnitude higher than the LHC - and is designed to deliver 5 to 10 times the integrated luminosity of the HL-LHC. Its mass reach for direct discovery extends to several tens of TeV. In addition to proton-proton collisions, FCC-hh is capable of supporting ion-ion, ion-proton, and lepton-hadron collision modes. This second volume of the Feasibility Study Report presents the complete design of the FCC-ee collider, its operation and staging strategy, the full-energy booster and injector complex, required accelerator technologies, safety concepts, and technical infrastructure. It also includes the design of the FCC-hh hadron collider, development of high-field magnets, hadron injector options, and key technical systems for FCC-hh.
April 2025
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151 Reads
Volume 1 of the FCC Feasibility Report presents an overview of the physics case, experimental programme, and detector concepts for the Future Circular Collider (FCC). This volume outlines how FCC would address some of the most profound open questions in particle physics, from precision studies of the Higgs and EW bosons and of the top quark, to the exploration of physics beyond the Standard Model. The report reviews the experimental opportunities offered by the staged implementation of FCC, beginning with an electron-positron collider (FCC-ee), operating at several centre-of-mass energies, followed by a hadron collider (FCC-hh). Benchmark examples are given of the expected physics performance, in terms of precision and sensitivity to new phenomena, of each collider stage. Detector requirements and conceptual designs for FCC-ee experiments are discussed, as are the specific demands that the physics programme imposes on the accelerator in the domains of the calibration of the collision energy, and the interface region between the accelerator and the detector. The report also highlights advances in detector, software and computing technologies, as well as the theoretical tools /reconstruction techniques that will enable the precision measurements and discovery potential of the FCC experimental programme. This volume reflects the outcome of a global collaborative effort involving hundreds of scientists and institutions, aided by a dedicated community-building coordination, and provides a targeted assessment of the scientific opportunities and experimental foundations of the FCC programme.
April 2025
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132 Reads
Volume 3 of the FCC Feasibility Report presents studies related to civil engineering, the development of a project implementation scenario, and environmental and sustainability aspects. The report details the iterative improvements made to the civil engineering concepts since 2018, taking into account subsurface conditions, accelerator and experiment requirements, and territorial considerations. It outlines a technically feasible and economically viable civil engineering configuration that serves as the baseline for detailed subsurface investigations, construction design, cost estimation, and project implementation planning. Additionally, the report highlights ongoing subsurface investigations in key areas to support the development of an improved 3D subsurface model of the region. The report describes development of the project scenario based on the 'avoid-reduce-compensate' iterative optimisation approach. The reference scenario balances optimal physics performance with territorial compatibility, implementation risks, and costs. Environmental field investigations covering almost 600 hectares of terrain - including numerous urban, economic, social, and technical aspects - confirmed the project's technical feasibility and contributed to the preparation of essential input documents for the formal project authorisation phase. The summary also highlights the initiation of public dialogue as part of the authorisation process. The results of a comprehensive socio-economic impact assessment, which included significant environmental effects, are presented. Even under the most conservative and stringent conditions, a positive benefit-cost ratio for the FCC-ee is obtained. Finally, the report provides a concise summary of the studies conducted to document the current state of the environment.
... where |q ± ⟩ are the spin states based on the pion directions in each τ rest frame. These operatorsÊ are rank-one projectors onto separable states, reflecting the independent τ decay amplitudes in Eq. (9) (see the exclusion of decay dependence on local variables [47,48]). ...
May 2025
... Recently, BESIII reported a direct measurement of η c → γγ in the decay channel J/ψ → γη c , yielding the product branching fraction (BF) of B(J/ψ → γη c )×B(η c → γγ) = (5.23±0.40)×10 −6 [30]. By using the word-average value of B(J/ψ → γη c ) = (1.41±0.14)%, ...
May 2025
Physical Review Letters
... Recently first experimental data on the semileptonic D ðsÞ decays to orbitally excited strange and light mesons became available [14][15][16][17][18][19][20]. The branching fractions of the semielectronic D decays into the axial-vector K 1 ð1270Þ meson were measured in Refs. ...
April 2025
Physical Review D
... GeV. In Ref. [40], the BW mass of ηð1405=1475Þ in the γϕ spectrum is located at around 1.475 GeV, and in the latest analysis of the same decay channel but with higher statistics [41], the mass is found to be 1422 AE 2.1 þ5.9 −7.8 MeV. This could be an indication that there must be controversial issues among these existing data. ...
March 2025
Physical Review D
... Different from the hadronic weak decays of bottomed baryons where contributions of the nonfactorizable processes can be neglected [2], in the charm sector various measurements seem to indicate the nontrivial role played by the nonfactorizable processes. Note that more and more data have been accumulated in recent years by different experiments, such as BESIII Collaboration [3][4][5][6][7][8][9][10], LHCb Collaboration [11][12][13][14][15][16], and Belle and Belle II Collaborations [17][18][19][20][21]. Benefiting from this, a combined study of these transitions should allow us to gain more insights into the mechanism for the hadronic weak decay of charmed baryons. ...
March 2025
Physical Review D
... The measured BF of the decay Λ + c → ΛK 0 S K + is consistent with the PDG value (2.80 ± 0.55) × 10 −3 with improved precision. This result is also consistent with the previous BESIII measurement [51] and the theoretical predictions [11,28]. The combination with the previous BESIII measurement [51] gives the average BF of the decay Λ + c → ΛK 0 S K + , (3.07 ± 0.26 ± 0.13) × 10 −3 , taking into account the small overlap between the signal samples in the two analyses. ...
January 2025
Physical Review D
... Previous searches associated to sub-GeV invisible particles have been performed using many data samples from high intensity facilities [12][13][14][15][16][17][18][19][20][21][22]. However, there are fewer searches for sub-GeV invisible particles in the hadronic decays of intermediate states, where the strong interaction dominates. ...
January 2025
Physical Review D
... It should be emphasized that the FFs involved in the D l4 decays depend not only on the momentum transfer squared q 2 but also on the P 1 P 2 invariant mass squared k 2 . Furthermore, the D l4 decays provide access to multiple angular observables [8,9], such as the forward-backward asymmetry and other differential distributions, enabling more sensitive tests of the SM. ...
December 2024
Physical Review D
... The decay ϕ → γa 0 ð980Þ 0 , which violates both charge conjugation and parity conservation, is also observed with an anomalously large branching fraction (BF) [3,4]. In addition, the BESIII Collaboration measured the BFs of the D þ s → a 0 ð980Þ 0ðþÞ π þð0Þ [5], D þ s → a 0 ð980Þ 0ðþÞ ρ þð0Þ [6] and D 0ðþÞ → a 0 ð980Þ þ π −ð0Þ [7] decays to be much larger than the expectations based on the naive two-quark model [8][9][10]. ...
December 2024
Physical Review D
... The systematic search for such states, and their subsequent investigation, will supplement our knowledge about the h 1 family and improve our understanding of the strangeonium spectrum [15]. Recently, BESIII observed the 1 þ− state, which is a candidate for the h 1 ð2PÞ state [16]. However, the h 1 ð3PÞ still remains unobserved by experiments. ...
December 2024
Physical Review D