Y. Bai’s research while affiliated with Technical University of Munich and other places

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Publications (903)


Fig. 1 | Transverse view of a Λ --Λ space-like separation event in the detector. The center of the detector corresponds to the e + e − interaction point, where the J/ψ is produced and decays instantaneously into a photon and the η c meson. The η c itself decays also instantaneously into a hyperon pair Λ Λ, and the Λð ΛÞ decays into the charged particles p and π − ( p and π + ). The trajectories of the charged tracks can be seen as black curves. The areas colored beige, yellow and light blue correspond to the MDC, TOF and EMC of the BESIII detector, respectively.
Fig. 2 | The distribution of CHðθ pp Þ=α 2 Λ = ½ 3 cos θ pp Àcosð3θ pp Þ 4 À 1 2 Š. The points with total error bars are the measurements, the solid line is the QM prediction, and the dashed line is the upper bound of the LHVT prediction. The shaded area above the dashed line indicates the violation of the CHðθ p p Þ inequality.
Fig. 3 | Illustration of helicity angles defined in each step of a decay chain. Helicity angles in J=ψ ! γη c , η c ! Λ Λ decays, and η c ! Λ Λ ! p pπ + π À decays.
Test of local realism via entangled ΛΛˉ\Lambda \bar{\Lambda } system
  • Article
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May 2025

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8 Reads

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1 Citation

M. Ablikim

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M. N. Achasov

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P. Adlarson

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J. Zu

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Observation of $\chi_{cJ}(J=0,1,2)\rightarrow p\bar{p}\eta\eta

May 2025

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1 Read

Using (2712.4±14.3)×106(2712.4\pm14.3)\times10^6 ψ(3686)\psi(3686) events collected by the BESIII detector operating at the BEPCII storage ring, the decays χcJ(J=0,1,2)ppˉηη\chi_{cJ}(J=0,1,2)\rightarrow p\bar{p}\eta\eta are observed for the first time through the radiative transition ψ(3686)γχcJ\psi(3686)\to\gamma\chi_{cJ}. The statistical significances for χcJ\chi_{cJ} signals are all larger than 5σ\sigma. The branching fractions of χc0,1,2ppˉηη\chi_{c0,1,2}\to p\bar{p} \eta\eta are determined to be (5.75±0.59±0.42)×105({5.75 \pm 0.59 \pm 0.42}) \times 10^{-5}, (1.40±0.33±0.17)×105({1.40 \pm 0.33 \pm 0.17}) \times 10^{-5}, and (2.64±0.40±0.27)×105({2.64 \pm 0.40 \pm 0.27}) \times 10^{-5}, respectively, where the first uncertainties are statistical and the second systematic. No evident resonant structures are found in the ppˉp\bar{p} and pη/pˉηp\eta/\bar{p}\eta systems.


FIG. 2. Distribution of M γ i Λ versus M γ j ¯ Λ in the data. Events are within the ω mass window. The red solid box indicates the signal region, the green dashed boxes denote the 1-D sideband regions, and the magenta long dashed box represents the Σ 0 − ¯ Σ 0 sideband region.
FIG. 3. Fit to the M π þ π − π 0 distribution. The dots with error bars are data, the grass green solid line denotes the fit result, the red long dashed line represents the signal component, the blue dashed line is smooth background, and the light blue shadowed area represents the smooth 2-D sideband of Σ 0 and ¯ Σ 0 .
Observation of the decay ψ ( 3686 ) → Σ 0 Σ ¯ 0 ω

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


Measurement of the branching fractions of D + → K + K − π + π + π − , ϕ π + π + π − , K S 0 K + π + π − π 0 , K S 0 K + η , and K S 0 K + ω decays

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


Figure 2. Fit to the M (K + K − ) distribution at √ s = 3096.986 MeV. The black dots with error bars are candidate events in the η mass window of M (γγ). The red solid curve is the fit result. The green dotted line is the fitted background shape. The blue histogram is the M (K + K − ) spectrum for candidate events in the sη sidebands of M (γγ).
Figure 3. Distribution of X ISR = s ′ /s in the signal MC sample at √ s = 3096.986 MeV. The red (blue) line shows the generated (reconstructed) events. The events in the green shaded region are used to obtain the efficiency.
Figure 5. 1D χ 2 -scan over a range of different values for ϕ γ,3g . The dashed blue box represents the interval where ∆χ 2 = χ 2 − χ 2 min = 1, which corresponds to a 1σ confidence interval.
Fit results of the lineshape e + e − → ϕη. The quoted uncertainties in the fit parameters include both statistical and systematic uncertainties.
Measurement of the phase between strong and electromagnetic amplitudes in the decay $J/\psi\to\phi\eta

May 2025

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8 Reads

The first direct measurement of the relative phase between the strong and electromagnetic amplitudes for a J/ψJ/\psi decaying into a vector-pseudoscalar final state is performed using 26 energy points of e+ee^+e^- annihilation data between 3.00 GeV3.00\ \text{GeV} and \mbox{3.12 GeV}. The data sets were collected by the BESIII detector with a total integrated luminosity of 452 pb1^{-1}. By investigating the interference pattern in the cross section lineshape of e+eϕηe^+e^-\to\phi\eta, the relative phase between the strong and electromagnetic amplitudes of J/ψJ/\psi decay is determined to be within [133,228][133^\circ,228^\circ] at 68\% confidence level. The result hints at interference between the strong and electromagnetic amplitudes of J/ψJ/\psi decay.


FIG. 1. Decay mechanism diagram of the D 0 → a 0 ð980Þ − e þ ν e decay. It illustrates a clear separation of the weak current, W þ → e þ ν e , and strong current, D 0 → a 0 ð980Þ − , in SL decay. The transition of D 0 → a 0 ð980Þ − is parametrized by the FF f a 0 þ ðq 2 Þ. The green region represents the hadronization process of the a 0 ð980Þ − , which may form either as a conventional d ¯ u state or an exotic d ¯ us¯ s state with the s¯ s generated from gluon interactions.
Study of the light scalar a 0 ( 980 ) through the decay D 0 → a 0 ( 980 ) − e + ν e with a 0 ( 980 ) − → η π

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


FIG. 1. The Feynman diagrams of the direct process η c → γγ (a), and the time-inversion process γγ → η c (b).
Observation of the Charmonium Decay η c → γ γ in J / ψ → γ η c

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


Future Circular Collider Feasibility Study Report: Volume 2, Accelerators, Technical Infrastructure and Safety

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.


Future Circular Collider Feasibility Study Report: Volume 1, Physics, Experiments, Detectors

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.


Future Circular Collider Feasibility Study Report: Volume 3, Civil Engineering, Implementation and Sustainability

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.


Citations (21)


... 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]). ...

Reference:

Reaching the Ultimate Quantum Precision Limit at Colliders: Conditions and Case Studies
Test of local realism via entangled ΛΛˉ\Lambda \bar{\Lambda } system

... 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)%, ...

Observation of the Charmonium Decay η c → γ γ in J / ψ → γ η c

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. ...

Observation of D → K ¯ 1 ( 1270 ) μ + ν μ and test of lepton flavor universality with D → K ¯ 1 ( 1270 ) ℓ + ν ℓ

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. ...

Partial-wave analysis of J / ψ → γ γ ϕ

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. ...

Observation of the singly Cabibbo-suppressed decay Λ c + → p π 0

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. ...

Measurement of the branching fractions of the decays Λ c + → Λ K S 0 K + , Λ c + → Λ K S 0 π + , and Λ c + → Λ K * +

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. ...

Search for a massless dark photon in c → u γ ′ decays

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. ...

Study of the decay D 0 → ρ ( 770 ) − e + ν e

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]. ...

Observation of D → a 0 ( 980 ) π in the decays D 0 → π + π − η and D + → π + π 0 η

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. ...

Study of the decay J / ψ → ϕ π 0 η

Physical Review D