International Workshop on e+e- collisions from Phi to Psi

25 Feb 2019, 08:00 → 1 Mar 2019, 18:00 Asia/Novosibirsk

Budker INP

During a Workshop you can join us remotely with ZOOM: https://www.zoom.us/j/7788996655

The aim of the Workshop is to discuss in detail the state of the art of various problems in hadroni.

2nd Bulleten PhiPsi19Bulleten2nd.pdf

Photo PhiPsi.JPG PhiPsi-s.JPG

Monday, 25 February

08:30 → 09:30 Registration

09:30 → 09:40 Welcome speech

09:40 → 13:00 Status of facilities and new projects

Conveners: Prof. Eugeny Levichev (BINP) , Prof. Yury KUDENKO (Institute for Nuclear Research of RAS)

09:40 Super Charm-Tau project at Novosibirsk

The Super Charm–Tau factory at the Budker Institute of Nuclear Physics (Novosibirsk, Russia) is an electron-positron collider that will operate in the center-of-mass energy range from 2 to 5-6 GeV with the peak luminosity of about $10^{35}$ cm$^{−2}$s$^{−1}$. The main goal of experiments is to study processes with c quark or τ leptons in the final state. The experiments at Super Charm-tau factory are complementary to experiments at LHCb and Belle-II. We'll discuss the physics case for the Super Charm–Tau factory, the conceptual design of the collider and the detector and the status of the project.

Speaker: Ivan Logashenko (BINP)

Slides SCTF_Logashenko.pdf

10:10 LHCb status and plans

This talk will present a status overview of ongoing LHCb upgrade. The new detector is designed to operate at the instantaneous luminosity of 2·10^33 cm-2s-1, more than five times higher than in Run 2. A crucial part of the upgrade is the software-only trigger, which should be able to select the desired events at 30MHz input rate with up to six visible interactions per bunch crossing. Current upgrade status and highlight performance results will be shown. In addition, the LHCb physics program and preparation for future challenges will be presented.

Speaker: Dr Pavel Krokovny (BINP)

Slides lhcb_status_plans_v3.pdf

10:40 Low-energy electron-positron collider to search and study (mu+ mu- ) bound state

From six leptonic atoms (e^+ e^- ), (μ^+ e^- ), (μ^+ μ^- ), (τ^+ e^- ), (τ^+ μ^- ), (τ^+ τ^- ) only positronium (e^+ e^- ) and muonium (μ^+ e^- ) were observed. Observation and study of dimuonium (μ^+ μ^- ) will test QED and quantum mechanics computations in the new regime. Dimuonium radius is 200 times smaller than positronium; therefore, it has a higher new-physics reach potential in comparison with other exotic atoms. We propose a low energy e^+ e^- collider for production of the not yet observed (μ^+ μ^- ) bound system. Low beam energy E_beam≈400 MeV and small circumference Π≈30 m of the machine make it inexpensive to manufacture and operate. Large angle (〖75〗^∘) crossing of e^+ e^- beams produces dimuonium with non-zero momentum shifting decay point from beams collision area and providing effective suppression of the main source of background  elastic e^+ e^- scattering. The peak luminosity at μ^+ μ^- production threshold is 8×〖10〗^31 cm^(-2) s^(-1). Reversing one of the beams direction allows to study π^± and η  mesons with high luminosity.

Speaker: Dr Anton Bogomyagkov (Budker Institute of Nuclear Physics)

Slides Bogomyagkov-Phi-Psi-2019.pptx

11:10 Coffee break

11:30 Super KEKB and Belle2 status and plans

Speaker: Prof. Xiaolong Wang (Fudan University)

Slides Belle2_Exp.pdf

12:00 BINP electron-positron facilities

The overview of two running BINP electron-positron colliders VEPP-4M (1-5 GeV/beam) and VEPP-2000 (0.15-1 GeV/beam) is presented. Since 2016 both colliders are joint to the single accelerator complex via common injector of high quality intensive beams. In 2017 VEPP-2000 resumed data taking after 3 years of upgrade. The luminosity was increased in a factor of 3-5 in a whole energy range.

Speaker: Dmitry Shwartz (BINP)

Slides BINP_facilities

12:30 BEPCII and BESIII Status and Plans

The BESIII detector and BEPCII accelerator represent major upgrades over the previous version of BES and BEPC; the facility is used for studies of hadron spectroscopy and ?-charm physics. The design luminosity was reached in 2016, setting a new world record for the accelerator in this energy regime. After opertaing for more than ten years, BESIII has achieved great success. In my this report, I review current status of BEPCII and BESIII, and also will show the future plan for the upgrade.

Speaker: Prof. Chengping SHEN (Beihang University)

Slides BESIII-shen.pdf

13:00 → 13:10 Conference photo

13:10 → 14:30 Lunch

14:30 → 18:00 Status of facilities and new projects

Conveners: Prof. Achim DENIG (JGU Mainz) , Dr Jens Soeren LANGE (University Giessen)

14:30 The KLOE-2 experiment at DAΦNE

The KLOE-2 experiment at the INFN Laboratori Nazionali di Frascati has finished its data-taking campaign at the DAΦNE ϕ-factory with the collection of 5.5 fb$^{-1}$ of integrated luminosity. A peak luminosity of $2.4\times 10^{32} cm^{-2}s^{-1}$ and a maximum daily integrated of 14 pb$^{-1}$ were achieved with the crab waist scheme of beam collisions. KLOE-2 represents the continuation of the KLOE experiment with a improved physics program mainly focused on the study of K$_S$, η rare decays as well as on kaon interferometry, test of discrete symmetries, and search for physics beyond the Standard Model. The collected data sample will allow to perform CPT symmetry and quantum coherence tests using entangled neutral kaons, studies of pseudoscalar mesons produced in γγ-physics collisions, and the search for signals of a hidden dark-matter sector, among the fields to be addressed. The general purpose KLOE detector, composed by one of the biggest Drift Chamber ever built surrounded by a lead-scintillating fiber Electromagnetic Calorimeter among the best ones for energy and timing performance at low energies, undergone several upgrades including an Inner Tracker made of cylindrical GEMs, to improve vertex reconstruction capabilities near the interaction region, a tagging system for scattered electrons in γγ processes, and small angle calorimeters to inprove the acceptance for particles coming from the Interaction Point. An overview of the KLOE-2 experiment will be given including present status and achievements together with physics plans.

Speakers: Dr Elena Perez del Rio (LNF-INFN) , Prof. Paolo Gauzzi (La Sapienza University of Rome (Italy))

Slides kloe-2-novosibirsk.pdf

15:00 Progress of Super Tau-Charm Facility (STCF) in China

The super tau-charm facility is of rich in the physics program, is an unique platform for the physics with charmed quark and tau lepton, and provide a great opportunity for study of QCD, exotic hadrons as well as search for new physics. BEPCII/BESIII, which is the only one machine running at the tau-charm region at present, is producing fruitful physics results, but will end its mission in 5-8 years. A STCF in China is a nature extension of BEPCII/BESIII, and the R&D process is ongoing in China. In this talk, we will introduce you the progress of STCF in China.

Speaker: Dr Haiping Peng PENG (University of Science and Technology, China)

Slides stcf-phi2psi2019.pdf

15:30 New Muonium Hyperfine Structure Measurement at J-PARC KEK IMSS

High precision measurements of the ground state hyperfine structure (HFS) of muonium, a leptonic system made of a bound state of a positive muon with an electron, is a stringent tool for testing bound-state quantum electrodynamics (QED) theory, determining fundamental constants of the muon magnetic moment and mass, and searches for new physics. Muonium is the most suitable system to test QED because both theoretical and experimental values can be precisely determined. At the J-PARC Muon Science Facility (MUSE), the MuSEUM collaboration is planing complementary measurements of muonium HFS both at zero field and at high magnetic field. The new high-intensity muon beam that will soon be available at MUSE H-Line will provide an opportunity to improve the precision of these measurements by one order of magnitude. The previous measurements at zero field [1] and high field [2] were performed decades ago at LAMPF with experimental uncertainties mostly dominated by statistical errors. An overview of the different aspects of these new muonium HFS measurements, the current status of the preparation for high -field measurements, and the latest measurements at zero field will be presented. [1] D. E. Casperson et al., Physics Letters 59B (1975) 397. [2] W. Liu et al., Physical Review Letters 82 (1999) 711.

Speaker: Prof. Koichioro Shimomura (KEK IMSS)

Slides phipsi19shimomura.pptx

15:50 J-PARC muon g-2/EDM experiment

The J-PARC muon $g-2$/EDM experiment (E34 experiment) aims to measure the muon anomalous magnetic moment with a precision of 0.5 ppm and search for muon electric dipole moment with a sensitivity of $10^{-21}~e\cdot$cm. The method of this experiment is independent of Fermilab's experiment, and a low-emittance muon beam and a factor of 20 smaller muon storage magnet are utilized. A new muon beam line (H-line) at J-PARC and dedicated muon LINAC to reaccelerate ultra-slow muons are under construction to supply a low-emittance muon beam. The latest update and current status of this experiment will be reported.

Speaker: Takayuki Yamazaki (KEK)

Slides 190225_PHIPSI19_yamazaki.pdf

16:10 Coffee break

16:30 MUonE status and plans

The MUonE experiment aims to measure with very high-precision the hadronic contribution to the running of alpha $\Delta\alpha_{had}(t)$, for space-like transferred momenta $t = q^2 < 0$. This measurement has to be performed by means the elastic scattering of high-energetic muons (160 GeV) on electrons target at rest. The precise knowledge of $\Delta\alpha_{had}(t)$ will allow to calculate the Leading Order Hadronic contribution $a_{\mu}^{HLO}$ to the muon g-2, by means of the dispersive technique, with an estimated precision comparable to the time-like traditional approach. MUonE is meant therefore as a new, complementary approach to $a_{\mu}^{HLO}$. To achieve the required luminosity MUonE plans to exploit the high-intensity muon beam M2 at CERN, with an expected muon rate of about 70 MHz, and low Z material targets. The envisaged detector is segmented in about 50 identical modules, each equipped with a Beryllium 1cm thick target element and 3 to 4 silicon strip tracking planes. The module length is set to 0.5m, with transverse dimensions of $10\times10$cm$^2$, in order to get the required tracking angular resolution and the geometrical acceptance. MUonE will be equipped with state of art available detector technology. The detector is being optimized to select suitable tracking elements, to define the trigger strategy and design the DAQ system. Detailed simulation studies based on GEANT4 and fast MC are ongoing to develop the analysis strategy in the LO and NLO approximations. MUonE has been proposed to CERN in the context of the Physics Beyond Collider initiative. The plan is to be ready for data taking, with a full scale prototype, already at the restart of LHC after the LS2. I will report on the MUonE project status and plans.

Speaker: Dr Umberto Marconi (INFN)

Slides MUonE_PsiPhi19.pdf

16:50 Precision Hadron Physics at the future MESA accelerator

Based on the expertise in high-intensity electron accelerator technology at the Mainz Microtron MAMI, a new accelerator MESA (Mainz Energy-Recovering Superconducting Accelerator) is currently under construction at the Institute for Nuclear Physics at Johannes Gutenberg University Mainz. MESA will be operated at low beam energies below 155 MeV, but at high inensities of at least 1 mA of beam current. The high intensity will provide the basis for a series of precision experiments in the fields of hadron and low-energy particle physics. In this talk, highlights of the research programme at MESA will be discussed including a new measurement of the electroweak mixing angle at low momentum transfer (P2 experiment), measurements of the electromagnetic form factors of the nucleons (MAGIX experiment) as well as searches for dark sector particles (the MAGIX and the beam dump experiment BDX). These experiments will be operated either in the extracted beam mode of MESA (P2 and BDX) or in the energy-recovering mode (MAGIX) of the accelerator, in which for the first time a high-intensity energy-recovering beam will be operated in conjunction with a gas internal target.

Speaker: Mr Denig Achim (JGU Mainz)

Slides Phipsi19_Denig_pdf.pdf

17:10 MEG2 and Mu3E status and plans

The status of the MEG II experiment, the upgrade of MEG, whose goal is to search for the forbidden decay mu -> e+ gamma with increased precision, is presented. After a brief review of the motivations behind such a search and the current limit due to MEG, we present the design of the detector in detail. The motivations of the upgrade of each subdetector is presented with the resolution improvements expected and measured. Novel subdetectors and calibration hardware are introduced. Results from beam tests on the subdetectors are presented. The schedule of the forthcoming years is presented. We conclude with the expected sensitivity of the MEGII experiment.

Speaker: Prof. Paolo Walter Cattaneo (INFN Pavia)

Slides Mu3e_PhiPsi19.pdf PhiPsi2019Cattaneo.pdf

17:40 New results and perspectives in neutrino physics

The review of the present status and futures perspectives of study neutrino oscillations in accelerator and reactor experiments will be presented. The results obtained in current long baseline accelerator experiments T2K and NOvA are discussed. An emphasis is put on a search for CP violation in neutrino oscillations. The brief overview and status of the next generation accelerator based experiments T2HK (Japan) with 260 kt Hyper-Kamiokande far neutrino detector and DUNE (USA) with 40 kt LAr TPCs will be given. The recent progress and results obtained in searches for light sterile neutrinos in accelerator and reactor experiments will be also discussed. Finally, the direct measurement of the neutrino mass and status of neutrinoless double beta decays experiments will be presented.

Speaker: Prof. YURY KUDENKO (INR, MOSCOW)

Slides kudenko_binp_2019.pdf

18:00 → 19:00 Excursion over BINP

19:00 → 21:30 Reception

Tuesday, 26 February

09:00 → 13:00 Mesons of heavy quarks

Conveners: Prof. Feng-Kun Guo (Institute of Theoretical Physics, Chinese Academy of Sciences) , Prof. Stephen Lars OLSEN (University of Chinese Academy of Sciences)

09:00 XYZ states at BESIII

BESIII has observed a lot of unclassified states which don't suit the standard quark model. These states are named as XYZ states, such as X(3872), Y(4260), $Z_c(3900)$... Some of these states are candidates of exotic tetra-quark states, molecular states, hybrid and so on. I'll report the recent experimental results from BESIII about these XYZ states.

Speaker: Dr Zhentian Sun (Institute of High Energy Physics, CAS)

Slides PhiPsi2019-Sunzt2.pdf

09:20 XYZ at Belle

New results and present status of exotic, narrow states with heavy quarks, often referred to as "XYZ states", at the Belle experiment will be presented. Not only observations, but also results of negative searches will be reviewed. Interpretation in view of the landscape of so far observed conventional and exotic states will be attempted, with comparison to theory expectations.

Speaker: Dr Jens Soeren Lange (University Giessen)

Slides lange_phipsi19_xyz_v2.pdf

09:40 XYZ at LHCb

The LHCb experiment is designed to study properties and decays of heavy hadrons produced in proton-proton collisions at the LHC. The large statistics collected by the LHCb experiment enables precision spectroscopy studies of beauty hadrons. The recent results on spectroscopy of conventional and exotic hadrons based on the data collected in Run-1 and Run-2 of LHC will be presented.

Speaker: Viacheslav Matiunin (Institute for Theoretical and Experimental Physics)

Slides PHIPSI19_Matiunin

10:00 XYZ search at Belle II

The Belle II experiment has successfully concluded Phase-2 of data taking in July 2018, and soon will start Phase-III, with the complete detector setup, planned in April 2019. Great perspectives and unique physics cases are enhanced in the Belle II physics program. In the sector of charmonium and spectroscopy, Belle II will investigate several physics processes: ISR physics for the vector states and bottomonium search are some examples where the contribution of the this experiment will help in better understanding QCD, for which several open questions still remain. First simulations and data analyses will be shown, with the first available dataset (2018), and the plan for spectroscopy search at Belle II will be discussed.

Speaker: Dr Elisabetta Prencipe (Forschungszentrum Juelich)

Slides Prencipe_PhiPsi2019_XYZ_v2.pdf

10:20 Theoretical Aspects of XYZ states

Selected theoretical aspects of the XYZ states, including different structure models and effects from kinematical singularities, will be discussed.

Speaker: Prof. Feng-Kun Guo (Institute of Theoretical Physics, Chinese Academy of Sciences)

Slides PsiPsi_FKGuo.pdf

10:40 Exotic molecular states in the decays of vector bottomonia

The most recent experimental data for the decays of the vector bottomonium Upsilon(10860) proceeding through the formation of the states Zb(10610) and Zb(10650) are analysed simultaneously using solutions of the Lippmann-Schwinger equations which respect constraints from unitarity and analyticity. The interaction potential in the open-bottom channels B(*)-anti-B* contains short-range interactions as well as the one-pion exchange; both types of the interaction are taken into account fully nonperturbatively. This way, all parameters of the interaction are fixed directly from the data and the pole positions for the Zb's are determined as a prediction. In particular, both Zb states are found to be described by poles located on the unphysical Riemann sheets in the vicinity of the corresponding thresholds: the Zb(10610) is associated with a virtual state residing just below the B-anti-B* threshold while the Zb(10650) state is most likely located just above the B*-anti-B* threshold. The heavy quark spin symmetry is employed to predict, in a parameter-free way, the pole positions and the line shapes in the elastic and inelastic channels for the Zbs' spin partner states W_bJ with the quantum numbers J++ (J=0,1,2). Such spin partners can be produced in radiative decays of the Upsilon(10860) state and, if they exist, are expected to be detected in the Belle-II experiment.

Speaker: Dr Alexey Nefediev (Lebedev Physical Institute)

Slides nefediev-phipsi-2019.pdf

11:00 Coffee break

11:20 Prospects of precision XYZ spectroscopy at PANDA/FAIR

The PANDA experiment at the new FAIR facility under construction at GSI/Darmstadt (Germany) is dedicated to a broad hadron physics programme addressing various different aspects of QCD. The multi-purpose PANDA detector will especially be best suited for charmonium spectroscopy. In combination with an intense and high-quality antiproton beam, PANDA will be able to perform precision spectroscopy via the method of resonance energy scan measurements. The uniqueness of PANDA to contribute to the field will be discussed.

Speaker: Dr Frank Nerling (GU Frankfurt, GSI Darmstadt)

Slides nerling_PANDA_PhiToPsi2019_web.pdf

11:40 The XYZ mesons: what aren’t they?

The list of XYZ mesons, which was initiated 16 years ago, continues to expand. Although these states have a number of common properties, including: large branching fractions to hidden-quarkonium states (in spite of kinematically accessible open-flavor, fall-apart decay channels); relatively narrow widths; and preferences for $J^{P(C)} =1^{+(+)}$ quantum numbers, no single theoretical model can provide a comprehensive description for them. Since the models that have been proposed: molecules, tetraquarks, QCD-hybrids, hadro-quarkonium, etc., can, at best, provide adequate descriptions for only a small subset of the observations, a concise exposition of what are they? is a Sisyphean task that I have given up on. Instead, I restrict myself to the easier question: what aren’t they?

Speaker: Prof. Stephen Lars OLSEN (University of Chinese Academy of Sciences)

Slides Phi_2_Psi2019_solsen.pdf

12:00 Charmonium studies at LHCb

A large set of data collected by the LHCb experiment in proton-proton collisions at sqrt{s}=7,8 and 13TeV allows many precise measurements for charmonia production and properties, in particular, the precise determination of the masses and the natural widths of several charmonium states.

Speaker: Dr Ivan Belyaev (Instriotute for Theoretical and Experimental Physics. ITEP)

Slides 20190216-PhiPsi19-QuarkoniumAtLHCb.pdf

12:20 Charmonium at BESIII

BESIII is an ideal laboratory to study charmonium decays, due to it's largest sample on J/psi, psi(2S) etc. Its achieved luminosity has reached the design luminosity. Recently, a lot of interesting studies are performed by BESIII, such as study of psi(2S)-> e+ e- chi_cJ, chi_cJ->e+ e- J/psi, J/psi -> Lambda_c+ e- + c.c. etc. This talk will introduce a few of them briefly.

Speaker: Mr Lianjin Wu (Institute of High Energy Physics, Beijing)

Slides CharmoniumAtBESIII.pdf

12:40 Charmonium studies at Belle

We present an overview of conventional charmonium studies at Belle. It includes the observation of the $\chi_{c0}(3860)$, the measurement of the absolute branching fractions of $B^+ \rightarrow X_{c\bar{c}} K^+$, the observation of $e^+e^- \rightarrow \chi_{c1}\gamma$, and other new results.

Speaker: Kirill Chilikin (LPI RAS)

Slides belle_charmonium.pdf

13:00 → 14:30 Lunch

14:30 → 14:50 Status of facilities and new projects

Convener: Dr Elisabetta Prencipe (Forschungszentrum Juelich)

14:30 COMET status and plans

Lepton Flavour Violation in the charged lepton sector (CLFV) is forbidden in the Standard Model. Therefore, the observation of CLFV process would be clear evidence of physics beyond the Standard Model. The COMET (COherent Muon to Electron Transitions) experiment will measure one of these processes: $\mu N \rightarrow eN$ at the Japan Proton Accelerator Research Complex (J-PARC) in Tokai, Japan. The COMET experiment will be conducted in two phases. Phase-I of the experiment is aiming at a signal sensitivity of $3.1 \times 10^{−15}$. Phase-II will use much more intense beam and a more complex detection system to achieve a single-event sensitivity of ~ $3 \times 10^{−17}$. This report gives an overview of construction and status of the COMET experiment.

Speaker: Dzmitry Shoukavy (B.I.Stepanov Institute of Physics of the National Academy of Sciences of Belarus)

Slides COMET_status_and_plans_PhiPsi.pdf

14:50 → 16:30 Mesons of heavy quarks

Convener: Dr Elisabetta Prencipe (Forschungszentrum Juelich)

14:50 Measurements of the J/ψ and ψ(2S) leptonic widths with KEDR detector

We report latest precise results on J/ψ and ψ(2S) parameters based on the data collected with the KEDR detector at the VEPP-4M e+e- collider. Leptonic width of J/ψ meson and its composition to hadronic and electronic branching fractions have been measured directly with the processes e+e- →hadrons and e+e- →e+e- at J/ψ resonance energy range. The obtained accuracy is less than 2%. The product of the electronic width of the ψ(2S) meson and the branching fraction of its decay to the muon pair has been measured in the e+e−→ψ(2S)→μ+μ− process with the world best accuracy about 3%. Leptonic width of ψ(2S) meson was calculated, using the previous KEDR measurements with the lepton universality assumption and without it.

Speaker: Tatyana Kharlamova (BINP, NSU)

Slides PhiPsi_Kharlamova.pdf

15:10 Charm Physics

Understanding  charm hadrons structures and dynamics motivates many studies within QCD. In particular Lattice QCD can provide us with precise calculation of the hadronic inputs required in  the   extraction of the CKM matrix elements as well as  leads to understanding of the exotic QCD structure as tertraquarks.  In the electroweak sector  B meson anomalies and muon anomalous magnetic moments initiated many studies of physics beyond the Standard Model. The question is whether  charm sector can be affected by the same New Physics. Intensive studies of Dark Matter stimulated a number of studies aimed to constrain or observe its presence in charm meson decays with the invisible particles in the final state.

Speaker: Prof. Svjetlana Fajfer (Department of Theoretical Physics, Jožef Stefan Institute)

Slides Fajfer-charm-19-Nosvosibirsk-.pdf

15:30 Electro-weak production of pseudovector C-even heavy quarkonia in electron-positron collisions on Belle II and BES III

It is shown that the $e^+e^-\to Z\to\chi_{c1}/\chi_{b1}$ and $e^+e^-\to\gamma^{\ast}\gamma^{\ast}\to\chi_{c1}/\chi_{b1}$ contributions do not interfere in the total cross sections. That is, the creation of longitudinally polarized electron-positron beams allows to study separately the $e^+e^-\to Z\to\chi_{c1}/\chi_{b1}$ and $e^+e^-\to\gamma^{\ast}\gamma^{\ast}\to\chi_{c1}/\chi_{b1}$. In the discussed energy region the weak interaction grows with energy increase $\propto G_FE^2$, where $G_F=10^{-5}m_p^{-2}$ is the Fermi constant. $G_FE^2=1.4\times 10^{-4}$ for $\chi_{c1}(1P)$ and $G_FE^2=1.7\times 10^{-4}$ for $\chi_{c1}(3872)$. That is, $G_FE^2\sim \alpha^2$ in the BES III energy region. $G_FE^2=1.1\times 10^{-3}$ for $\chi_{b1}(1P)$ and $G_FE^2=1.2\times 10^{-3}$ for $\chi_{b1}(2P)$. That is, $G_FE^2\gg\alpha^2$ in the Belle II energy region. The BESS III luminosity $10^{33} cm^{-2}s^{-1}$ gives possibilities to register near hundred of events $e^+e^-\to Z\to\chi_{c1}(1P)$ per day and near thirty of them in the well-known channel $\chi_{c1}(1P)\to\gamma\psi(1S)$. If $\chi_{c1}(3872)=\chi_{c1}(2P)$, then also near hundred of events $e^+e^-\to Z\to\chi_{c1}(3872)$ per day may be registered and several of them in the channel $\chi_{c1}(3872)\to\gamma\psi(2S)$, several tens of them in the channel $\chi_{c1}(3872)\to D^0\bar D^{0\ast}+c.c$. The huge Belle II luminosity $8\times 10^{35} cm^{-2}s^{-1}$ gives possibilities to register near hundred thousand of events each $e^+e^-\to Z\to\chi_{b1}(1P)$ and $e^+e^-\to Z\to\chi_{b1}(1P)$ per day and several tens of thousands of them in the well-known channels $\chi_{b1}(1P)\to\gamma\Upsilon(1S)$ and $\chi_{b1}(2P)\to\gamma\Upsilon(2S)$.

Speaker: Prof. Nikolay Achasov (Sobolev Institute for Mathematics)

Slides Achasov_26.02.2019.pdf

15:50 Review of bottomonium studies at Belle

We review recent Belle results on bottomonium. They include Y(2S) --> gamma eta_b(1S) with measurement of the eta_b(1S) mass; Y(4S) --> eta' Y(1S); energy scan of e+e- --> omega chi_bJ(1P); and updated result on energy scan of e+e- --> pi+pi- Y(1,2,3S) (new for this conference).

Speaker: Dr Romen Mizuk (Lebedev Physical Institute)

Slides mizuk_phipsi2019.pdf

16:10 Methods of parameterization of amplitudes and extraction of resonances, D-decay amplitudes

Various necessary conditions which two-body amplitudes (e.g. FSI) must meet will be presented and discussed. Methods of extraction of resonances from these amplitudes will be studied and examples of different results will be presented. The advantages and disadvantages of these methods will be analyzed and the methods that meet the necessary mathematical conditions and are convenient to describe the data will be shown. Example of Dalitz plot analysis for three body D decay with unitary two body amplitudes will be presented.

Speaker: Dr Robert Kaminski (Institute of Nuclear Physics PAS)

Slides TalkNovosibirskII2019RKaminski.pdf

16:30 → 17:00 Coffee break

17:00 → 20:00 Trip to opera house

Wednesday, 27 February

09:00 → 12:40 Mesons of light quarks

Conveners: Prof. Andrej Arbuzov (Joint Institute for Nuckear Research) , Prof. Jose Pelaez (Universidad Complutense de Madrid)

09:00 Light mesons from JPAC analyses

Identifying properties of excited hadronic states in the light meson sector remains an ongoing challenge, due to large widths, significant overlaps, and multiple decay channels of the resonances. A systematic approach using the unitarity-based coupled channel frameworks is required; for the reaction-independent determination of the resonance parameters, the pole positions of the resonances need to be extracted. As will be shown in the talk, several works in this direction have been performed by the Joint Physics Analysis Center (JPAC) in the past year in the tensor ($J^{PC}=2^{++}$) and exotic ($J^{PC}=1^{-+}$) waves of $\eta(')\pi$ system measured by the COMPASS experiment ([PLB 779 (2018)](http://inspirehep.net/record/1609260) and [arXiv:1810.04171](http://inspirehep.net/record/1697661)). The spin-exotic sector $J^{PC}=1^{-+}$ is also accessible from the partial wave analysis of the three pions system measured in diffractive reaction $\pi\,p \to 3\pi\,p$, however, the studies are hampered by the presence of a large, coherent, non-resonant background, known as the Deck process. I will highlight ongoing work on a comparison of the various models for this non-resonant production and show its influence found in the data. As the first steps in the route of understanding interaction in the $J^{PC}=1^{++}$ sector and the Deck process, we have built a model based on the approximate three-body unitary, fixed the free parameters by fitting it to the clean ALEPH data on $\tau\to 3\pi\,\nu_\tau$ decay. The pole position of the $a_1(1260)$ has been extracted for the first time using the unitary model ([PRD 98 (2018), 096021](http://inspirehep.net/record/1696497)).

Speaker: Mikhail Mikhasenko (HISKP, Universität Bonn)

Slides mikhasenko-light_meson_JPAC-2019-02-05.pdf

09:20 The updated status of the pseudoscalar glueball studies

The present theoretical and experimental status of the pseudoscalar glueball studies will be reviewed. We'd show that a converged picture from both theoretical and experimental evidences does not support the eta(1405) to be the so-far broadly quoted pseudoscalar glueball candidate.

Speaker: Prof. Qiang Zhao (Institute of High Energy Physics, Chinese Academy of Sciences)

Slides zhao-2019-02-phipsi-novosibirsk.pdf

09:40 Semileptonic D0 and D+ decays as a probe of the a0(980) nature

The decays $D^0\to d\bar u\,e^+\nu\to a^-_0(980)\, e^+\nu\to\pi^-\eta\, e^+\nu$ and $D^+\to d\bar d\,e^+\nu\to a^0_0(980)\, e^+\nu\to\pi^0\eta\, e^+\nu$ (and the charge conjugated ones) are the direct probe of the constituent two-quark components in the $a^\pm_0(980)$ and $a^0_0(980)$ wave functions. Recent BESIII experiment is the first step in experimental study of these decays. We suggest adequate formulas for the data analysis and present a variant of $\eta\pi$ invariant mass distribution when $a_0(980)$ has no constituent two-quark component at all.

Speaker: Dr Alexey Kiselev (Sobolev Institute for Mathematics)

Slides PhiPsi2019.pdf

10:00 New information on the strong isospin symmetry breaking in the reactions of the a0(980) and f0(980) resonance production

The strong isospin symmetry breaking is discussed as a tool for studying the production mechanisms and nature of light scalar mesons. The review considers various reactions in which it can be detected and in which the mixing of a00(980) and f0(980) resonances that breaks the isotopic invariance due to the mass dierence of K+ and K0 mesons has already been observed experimentally.

Speakers: Dr Georgii Shestakov (Sobolev Institute for Mathematics) , Prof. Nikolay Achasov (Sobolev Institute for Mathematics)

Slides AS-Slides-phi-psi-2019.pdf

10:20 Strange Light Resonances

I will review recent work on the determination of strange resonance parameters from meson-meson scattering data, using dispersion relations and other techniques based on analytic properties of amplitudes. Although I will discuss resonances below 1.7 GeV, I will pay particular attention to the lightest strange resonance K*(800) or kappa meson and the dispersive determination of its existence and its pole paramters as well as its possible non-ordinary nature.

Speaker: Prof. Jose Pelaez (Universidad Complutense de Madrid)

Slides

• 2019-02-Novosibirsk-PhiPsi2019-2003_format.ppt
• 2019-02-Novosibirsk-PhiPsi2019.pdf
• 2019-02-Novosibirsk-PhiPsi2019.pptx

10:40 Meson Decay Studies from MAMI A2

Decays of the light mesons $\pi^0\$, $\eta$, $\omega$, and $\eta'$ provide a unique laboratory to test fundamental aspects of hadron physics. Precision studies of such diverse topics as the light quark mass ratio, $\pi-\pi$ scattering lengths, and searches for physics beyond the Standard Model are possible. Additionally, their Dalitz decays provide a way of measuring the electromagnetic meson Transition Form Factors (TFFs) in the time-like region. Precise knowledge of pseudoscalar TFFs is vital for the precision frontier of the Standard Model as they are needed as experimental input in calculations of the hadronic Light-by-Light contribution to the anomalous magnetic moment of the muon. The A2 tagged photon facility at the Mainz Microtron (MAMI) provides a high yield of light mesons produced by photo-induced reactions on protons. It makes the experiment ideal for high precision measurements of meson decays. The experimental setup utilises the Bremsstrahlung distribution of the A2 photon beam, produced from the MAMI electron beam, along with a system of detectors that nearly covers the full solid angle. This talk will highlight the recent contributions as well as ongoing studies by the A2 collaboration in the field of light meson interactions.

Speaker: Dr Lena Heijkenskjöld (Institut für Kernphysik, Johannes Gutenberg Universität Mainz)

Slides PhiPsi19_Heijkenskjold_em.pdf

11:00 Coffee break

11:20 Light Hadron Spectroscopy at BESIII

Light Hadron Spectroscopy at BESIII

Speaker: Dr Tianjue Min (Nanjing University)

Slides Light_Hadron_Spectroscopy_at_BESIII_PhiPsi2019.pdf

11:40 The decay J/ψ→γX(Jᴾ)→γϕϕ: Dynamical analysis of X(Jᴾ)→ϕϕ resonance contributions.

The dynamics of the $J^{PC}=0^{-+}$, $0^{++}$, and $2^{++}$ resonance contributions to the decay $J/\psi\to\gamma X(J^{PC})\to\gamma\phi\phi$ is analysed using the data obtained by BESIII collaboration. The effective coupling constants parameterising invariant amplitudes of the transitions $J/\psi\to\gamma X(J^{PC})$ and $X(J^{PC})\to\phi\phi$ and masses of $X(J^{PC})$ resonances are found from the fits. They are used for evaluation of the branching fractions $B_{X(J^{PC})\to\phi\phi}$, relative branching fractions $B_{J/\psi\to\gamma X(J^{PC})\to\gamma\phi\phi}$, and for obtaining the photon angular distributions.

Speaker: Dr Arkadii Kozhevnikov (S.L. Sobolev Institute for Mathematics)

Slides Kozhevnikov_PhiPsi_2019.pdf

12:00 Isoscalar and isovector kaon form factors from e+e− and τ data

The recent precise measurements of the $e^+e^-\to K_SK_L$ and $e^+e^-\to K^+K^-$ cross sections and the hadronic spectral function of the $\tau^-\to K^-K_S\nu_\tau$ decay are used to extract the isoscalar and isovector electromagnetic form ractors and their relative phase in a model independent way. The experimental results are compared with a fit based on the vector-meson-dominance model.

Speaker: Dr Konstantin Beloborodov (Budker Institute of Nuclear Physics)

Slides beloborodov.pptx

12:20 Meson production in e+e- annihilation and tau-lepton decays within extended NJL model

The extended Nambu–Jona-Lasinio model is briefly described and various ways of its application are demonstrated. Theoretical treatment of low-energy meson production processes in colliding e+e- beams and tau lepton decays is reviewed. The processes considered occur via intermediate scalar, vector, and axial-vector mesons in the ground state and in the first radial excited one. The model employed uses the concept of spontaneous chiral symmetry breaking to describe such states. Experimental and theoretical comparisons with other phenomenological strong interaction models are presented. The talk is based on the review [M.K. Volkov, A.B. Arbuzov, Phys. Usp. 60 (2017) 643] and a few later articles.

Speaker: Prof. Andrej Arbuzov (Joint Institute for Nuckear Research)

Slides arbuzov_PhiPsi_2019.pdf

12:40 → 13:00 tau-lepton

12:40 Recent results on tau lepton from BaBar

We present measurements of the branching fractions of tau- to K- (pi-) n pi0 nu_tau, and the branching fraction and spectral function of tau- to K- K0 nu_tau, obtained with the full data sample collected by the BaBar experiment at PEP-II. Implications on the determination of Vus with tau decays will be discussed.

Speaker: Dr Alberto Lusiani (Scuola Normale Superiore)

Slides lusiani-phipsi19-v2.pdf

13:00 → 14:30 Lunch

14:30 → 18:10 e+e– annihilation and gamma–gamma physics

Conveners: Dr Frank Nerling (GU Frankfurt, GSI Darmstadt) , Dr Simon Eidelman (Budker Institute of Nuclear Physics)

14:30 Recent results from CMD-3

Speaker: Dr Fedor Ignatov (BINP)

Slides CMD3Ignatov_PhiPsi19.pdf

14:50 Recent results from SND detector at VEPP-2000 collider.

Recent results on e+e- annihilation to hadrons from SND experimnet at VEPP-2000 collider are presented. Corresponding data set is about 80 pb-1 of integrated luminosity collected at sqrt{s} below 2 GeV.

Speaker: Prof. Mikhail Achasov (BINP)

Slides phipsi19.pdf

15:10 Recent results on hadronic Physics at KLOE-2

The KLOE-2 experiment at the Frascati φ−factory ended last year collecting more than 5 fb$^{−1}$ at the φ peak. The new data sample together with the KLOE one corresponds to $2.4 ×10^{10}$ φ and $3.1 × 10^8$ η meson events. It represents the largest sample ever collected at the φ peak in $e^+ e^-$ colliders allowing to study light mesons with unprecedented statistics. Recent results obtained with KLOE data on hadron physics e.g. rare η meson decays, combination of hadron cross section measurements and determination of $a^{\pi\pi}_{\mu}$ , measurement of the running of the fine structure constant below 1 GeV and progress in γγ studies will be reviewed.

Speaker: Dr Francesca Curciarello (INFN-Laboratori Nazionali di Frascati)

Slides PhiPsi19_Curciarello.pdf

15:30 Two-photon physics at Belle

The Belle experiment has measured various two-photon physics processes, mostly using a no-tag method, and for a few of them also a single-tag technique. This way to analyze physics processes is useful to investigate transition form factors, as well as search for XYZ exotic states and baryons. A review of the main achievements at Belle will be given, and recent results will be shown.

Speaker: Dr Elisabetta Prencipe (Forschungszentrum Juelich)

Slides Prencipe_PhiPsi2019_TwoPhotons_v2.pdf

15:50 Hadronic and Transition Form Factor Measurements at BESIII

Motivated by the need of experimental input to improve the Standard Model prediction of the anomalous magnetic moment of the muon $a_\mu$, the BESIII collaboration started a dedicated program to measure hadronic cross sections as well as transition form factors (TFF) with high accuracy. In this presentation we will focus on the two-photon physics program, which is dedicated to the measurement of TFFs. The data acquired at BESIII allow to study the momentum dependence of the TFFs of light pseudoscalar mesons dominating the hadronic Light-by-Light contribution to $a_\mu$ in the relevant kinematic region. The current status and ongoing investigations of will be discussed.

Speaker: Dr Christoph Florian Redmer (Institute for Nuclear Physics, Johannes Gutenberg-University Mainz)

Slides CFR190227.pdf

16:10 Coffee break

16:30 R measurement at KEDR

KEDR measured the R values at twenty two center-of-mass energies between 1.84 and 3.72 GeV. This result provides the most precise information about R in this energy range. We present results mentioned above as well as prospects for R measurement with VEPP-4M collider at KEDR experiment.

Speaker: Korneliy Todyshev (BINP)

Slides PhiPsi2019todyshev.pdf

16:50 R value measurement at BESIII

Using data samples collected with BESIII detector operating at BEPCII storage ring, the R value is measured at 14 energy points from the center-of-mass energies 2.2324 to 3.671 GeV. This talk gives the descriptions and information for the data analysis, the calculations of the initial state radiations and generators simulations. (The average uncertainty of 14 R values is about 3%, which is dominated by the systematic uncertainty.)

Speaker: Prof. Haiming Hu (IHEP， CAS)

Slides Huhm_Rvalue_phipsi2019v2.pdf

17:10 Recent BaBar results in light hadron spectroscopy

A program of measuring the light hadrons production in exclusive e+e− \to hadrons processes is in place at BABAR, with the aim to improve the calculation of the hadronic contribution to the muon g−2. We present the most recent results obtained by using the full data set of about 470 fb−1 collected by the BABAR experiment at the PEP-II e+e− collider at a center-of-mass energy of about 10.6 GeV. In particular, we report the results on the channels e+e−→π+π−π0π0, pi+pi-pi0pi0pi0(η), e+e−→π+π−η. Additionally, we present the study of the two-photon process e+e−→e+e−η′ in the double-tag mode. The results for the form factor are compared with the predictions based on pQCD and VMD.

Speaker: Mr Evgeny Kozyrev (BINP)

Slides PHIPSI2019.pdf

17:30 Light exotic mesons at COMPASS

In recent years, the spectroscopy of hadrons containing heavy quarks has brought forward a plethora of new and unexpected resonance-like signals. Many of these so-called $X$, $Y$,$Z$ states are candidates for states beyond the quark-antiquark configurations of mesons, which have been sought after since the introduction of the quark model. Similar studies in the light-quark sector are more challenging due to the wide and overlapping nature of known resonances. Recent high-quality data samples, collected by the COMPASS experiment at CERN, open the possibility to search for exotics also at masses below 2.5 GeV. In particular, access to hadrons with explicit gluonic degrees of freedom is expected to be easier in this mass region. Recently, lattice QCD started to make predictions on the multiplet structure of exotic hadrons, which may be used as a guideline in the experimental searches. The COMPASS experiment at CERN uses a high-energy pion beam scattered off protons and heavier nuclei to produce mesonic excitations, which are observed in multi-particle final states subjected to partial-wave analyses. In addition to studying the properties of established mesons with unprecedented accuracy, the large existing data samples allow us to detect possibly exotic states. These either do not fit current theoretical expectations, like the recently observed $a_1(1420)$, or carry spin-exotic quantum numbers, like the $\pi_1(1600)$. The talk will give an update on ongoing studies of these states involving novel analysis techniques and discuss possible interpretations. Future plans concerning hadron spectroscopy in the strange and charm quark sector, envisaged at AMBER/COMPASS++, a new fixed-target QCD facility at CERN, will be presented.

Speaker: Prof. Bernhard Ketzer (University of Bonn)

Slides ketzer_phipsi2019_sub.pdf

17:50 Meson spectroscopy at VES and COMPASS

Diffractive production of $\pi^+\pi^-\pi^-$ and $\pi^-\pi^0\pi^0$ final states are subjects of comprehensive studies performed recently by VES and COMPASS experiments. The $3\pi$ states are produced at VES by 29 GeV/c $\pi^-$ beam on Be target ( $87x10^6$ $\pi^+\pi^-\pi^-$ events and $32x10^6$ $\pi^-\pi^0\pi^0$ events analyzed at 0 < t' < 1 GeV/c$^2$). At COMPASS $3\pi$ states are produced by 160 GeV/c $\pi^-$ beam impinging on liquid hydrogen target ( 50x10$^6$ $\pi^+\pi^-\pi^-$ events and $3.5x10^6$ $\pi^-\pi^0\pi^0$ events analyzed at 0.1 < t' < 1 GeV/c$^2$). The COMPASS collaboration pioneered the application of novel methods of partial-wave analysis: mass-independent PWA in multiple (m,t')-cells, mass-dependent analysis performed at-once for density matrices measured in all t' regions, the analysis with free shapes of $\pi^+\pi^-$ isobars. The COMPASS observed new narrow state: a_1(1420). The VES has leading world statistics of $\pi^+\pi^-\pi^-$ and $\pi^-\pi^0\pi^0$ events, compatible in two final states. This makes perspective the comparison of isospin relations between two states, using both: PWA with established shapes of isobars and PWA with freed $\pi\pi$ isobars.

Speaker: Dr Dmitry Ryabchikov (Institute for High Energy Physics)

Slides ryabchikov_phi_psi.pdf

Thursday, 28 February

09:00 → 11:40 g-2

Conveners: Ivan Logashenko (BINP) , Dr Roman Lee (The Budker Institute of Nuclear Physics, Novosibirsk)

09:00 Dispersive approach to the hadronic light-by-light contribution to the muon g-2

I will summarize the status of the dispersive approach to the hadronic light-by-light contribution to the muon $g-2$, and in particular report on recent progress, in particular concerning the role of short-distance constraints.

Speaker: Prof. Gilberto Colangelo (University of Bern)

Slides lbl-novosibirsk.pdf

09:20 Muon g-2: a new data-based analysis

This work presents a complete re-evaluation of the hadronic vacuum polarization contributions to the anomalous magnetic moment of the muon from the combination of e+ e- --> hadrons cross section data. Focus has been placed on the development of a new data combination method, which fully incorporates all correlated statistical and systematic uncertainties in a bias free approach. All available e+ e- --> hadrons cross section data have been analyzed and included, where the new data compilation has yielded the full hadronic R-ratio and its covariance matrix in the energy range $m_{\pi} < \sqrt{s} < 11.2 GeV$. Using these combined data and perturbative QCD above that range results in estimates of the hadronic vacuum polarization contributions to g-2 of the muon of $a_{\mu}^{had, LO VP} = (693.27 \pm 2.46 ) x 10^{-10}$ and $a_{\mu}^{had,NLO VP} = ( -9.82 \pm 0.04 ) x 10^{-10}$. The new estimate for the Standard Model prediction is found to be $a_{\mu}^{SM} = (11 659 182.05 \pm 3.56) x10^{-10}$, which is $3.7\sigma$ below the current experimental measurement.

Speaker: Dr Daisuke Nomura (KEK)

Slides nomura-Phipsi19.pdf

09:40 Axial-vector meson LbL contribution to g-2 of muon in nonlocal quark model

The light-by-light contribution to muon anomalous magnetic moment from axial-vector meson exchanges is estimated in the framework of nonlocal quark model. The full kinematic dependence of the transition form-factor is taken into account. The comparison with existed parametrizations based on the experimental data on the transition form factor is performed. The corresponding contribution to the hyperfine splitting in muonic hydrogen is discussed.

Speaker: Mr Andrei Radzhabov (Matrosov Institute for System Dynamics and Control Theory)

Slides RadzhabovPhitoPsiV2.pdf

10:00 The MUonE project: theory progress

QED radiative corrections to µe → µe: NNLO calculation; Theory status and progress.

Speaker: Prof. Massimo Passera (INFN Padova)

Slides Passera_PhiPsi2019.pdf

10:20 Muon-electron scattering at NLO

In this talk, based on arXiv:1811.06743, I will review the NLO electro-weak radiative corrections to the $\mu^\pm e^-\to\mu^\pm e^-$ process and discuss their relevance for the MUonE experiment, proposed at CERN. The aim of MUonE is the high precision measurement of the QED running coupling constant in the space-like region, from which the full hadronic contribution can be extracted and used to provide a new and independent determination of the leading-order hadronic correction to the muon $g-2$. In this context, the required accuracy demands that radiative corrections are accounted for at the the highest level of precision and implemented into a Monte Carlo event generator for data analysis. The first step towards the final goal of theoretical precision, which will require the full set of NNLO corrections and resummation of higher orders, is the inclusion of NLO electro-weak corrections.

Speaker: Dr Carlo M. Carloni Calame (INFN, Sezione di Pavia - Pavia, Italy)

Slides carloni.pdf

10:40 Dispersive analysis of the two-pion contribution to the hadronic vacuum polarization to the (g−2)μ

I will present the results of a dispersive analysis of the pion vector form factor, which determines the two-pion contribution to the $(g-2)_\mu$ below 1 GeV. As a by-product, both the $P$-wave $\pi \pi$ phase shift as well as the pion charge radius have been determined with higher precision than before.

Speaker: Prof. Gilberto Colangelo (University of Bern)

Slides hvp-novosibirsk.pdf

11:00 Coffee break

11:20 The Muon g-2 experiment at Fermilab

The study of the anomalous magnetic moment of the muon, Muon g-2, stands as an enduring and stringent test of the Standard Model (SM), where the current 3.5 standard deviations (or higher) discrepancy between the theoretical prediction and the experimental measurement could be an indication of new physics beyond the SM. The E989 Muon g?2 experiment at Fermilab aims to measure the muon anomaly to an unprecedented precision of 140 parts-per-billion, with an aim to either resolve or confirm this discrepancy. In this talk, I will discuss the current status of the analysis of Run-1 data taken during the spring of 2018 and give an update on overall progress as we enter a new data-taking period.

Speaker: Dr Keshavarzi Alex (University of Mississippi)

Slides AKeshavarzi_PhiPsi2019_Novosibirsk_28-02-10_compressed.pdf

11:40 → 13:00 Dark sector

Convener: Ivan Logashenko (BINP)

11:40 Search for the dark gauge vector and scalar bosons, the axion-like pseudo-scalar, and the dark matter at lepton colliders

Since 1933, cosmological anomalies are reported at different scales and ages of the Universe. These anomalies could be due to a non-luminous mass ("dark matter"), change of the laws of gravity, or a combination of both.  Lepton colliders can investigate the non-luminous mass scenario by searching for different dark matter candidates (millicharged dark matter, axion-like, or very stable multi-quark states) and new force carriers (dark vector, dark scalar, or axion-like). We will review the new results of BABAR and Belle, and the expected Belle II sensitivities to these searches.

Speaker: Mr Igal Jaegle (University of Florida)

Slides igal_jaegle_psi-phi_2019.pdf

12:00 Searching for dark sector with missing mass technique in fixed target experiments

Currently, the existence of a dark sector almost completely decoupled from the Standard Model is a viable solution for numerous long-standing problems in physics, including the nature of dark matter and the muon anomalous magnetic moment. A new gauge mediator, the dark photon, could be the portal to this hidden sector. The most general probe to its existence is the missing mass technique which requires a precise knowledge of the initial state of the process but does not put constraints on the dark photon final states. The experimental approaches to the search for dark photons in positron-on-target annihilation and in mesons decay in flight will be presented and the physics reach will be discussed.

Speaker: Venelin Kozhuharov (LNF-INFN &amp; University of Sofia)

Slides 2019-02-28-Venelin-DarkPhoton-short.pdf

12:20 Search for dark forces at KLOE-2

During the last years several Dark Sector Models have been proposed in order to address striking and pluzzing astrophysical observations which fail standard interpretations. In the minimal case a new vector particle, the so called dark photon or U-boson, is introduced, with small coupling with Standard Model particles. Also, the existence of a dark Higgs boson h’ is postulated, in analogy with the Standard Model, to give mass to the U-boson through the Spontaneous Symmetry Breaking mechanism. The discovery of such a Dark Force Mediator would belong to a new field of Physics Beyond the Standard Model. The KLOE experiment, working on the DAΦNE e+e- collider in Frascati, searched for the existence of the U-boson in a quite complete way, investigating several different processes and final states. Tight limits on the model parameters have been set at 90%CL. Further improvements are expected in terms of sensitivity and discovery potential with the new KLOE-2 detector working on the improved DAFNE e+e- collider, which has collected more than 5 fb−1.

Speaker: Dr Elena Perez del Rio (LNF-INFN)

Slides PhiPsi19_ElenaPerez.pdf

12:40 Search for highly ionizing particles with the Belle II pixel detector

The Belle II experiment, located at the SuperKEKB collider at the high-energy research facility KEK in Tsukuba, Japan, started operation in 2018. Compared to the predecessor experiment Belle, Belle II plans to increase the peak luminosity by a factor of <40, by employing nano-beam technology in the interaction region. In particular the new, innermost sub-detector of Belle II - the Pixel Vertex Detector (PXD) - is in close proximity to the interaction point. This allows for the detection of particles, which do not leave a signal in the outer sub-detectors. Among these, Highly Ionizing Particles (HIPs) encounter a characteristically high energy loss, limiting their penetration depth into the detector. Anti-deuterons, magnetic monopoles and stable tetraquarks as possible HIPs are considered. Without a signal in the outer sub-detectors, no track trigger is issued, resulting in possible non-observation. Therefore, in this talk, the possibility of identifying HIPs solely with information provided by the PXD is presented, by using neural network algorithms operating in a multidimensional parameter space of e.g. PXD cluster data. Most notably, the application of unsupervised learning in the form of Self-Organizing Maps (SOM) is presented.

Speaker: Ms Katharina Dort (Justus Liebig University Giessen)

Slides slides_phipsi19.pdf

13:00 → 14:30 Lunch

14:30 → 15:30 Dark sector

Convener: Dr Jan Friedrich (TU München)

14:30 QCD effects in searches for GeV-scale new physics.

The Standard Model of particle physics fails to explain several important phenomena like neutrino oscillations, matter-antimatter asymmetry of the Universe, cosmological dark matter. While we definitely need some new physics capable of explaining the phenomena above, the absence of any new particles at colliders implies that they are either very heavy or feebly interacting with the known particles. In the latter case they can be at GeV mass range, produced by and/or decaying to hadrons. We discuss the associated with QCD difficulties in obtaining the accurate predictions for the new particle production and decay rates, concentrating on the singlet scalar, fermion and vector messengers to the hidden sector.

Speaker: Prof. Dmitry Gorbunov (INR RAS)

Slides PhiPsi-2019.pdf

14:50 New Physics Beyond the SM at BESIII

Numerous astrophysical observations strongly suggest the existence of Dark Matter, which provides a hint of dark sector physics. There could exist many dark candidates predicted by theories BSM, such as dark photons and invisible things, that communicate with the Standard Model sector. The masses and decay modes of these particles are expected to be accessible at the BESIII experiment which is the only currently running tau-charm factory with the largest threshold charm samples and some other unique datasets. We have recently performed searches of dark photons and invisible things in several decay modes. Besides, light Higgs, FCNC processes, BNV/LNV processes are also investigated. This talk will summarize the recent results at BESIII on these searches for new physics BSM.

Speaker: Dr Ming-Gang Zhao (Nankai University)

Slides BESIII_28Feb2019_zhaomg.pdf

15:10 Recent results of the NA64 experiment at the CERN SPS

We report the recent results of the NA64 experiment at CERN on the search for a hypothetical X-boson which could explain the 8Be* anomaly. The results of the search for the dark photon A' which could mediate a new interaction between the visible and dark sectors and future NA64 research program will be also discussed.

Speaker: Dr Mikhail Kirsanov (INR RAS Moscow)

Slides PhiPsi2019.pdf

15:30 → 15:50 Flavour: violations

Convener: Dr Jan Friedrich (TU München)

15:30 Recent results on Kaon Physics at KLOE-2

KLOE-2 extends the physics program of the forerunner KLOE experiment, especially in the field of discrete symmetries tests with neutral kaons. KLOE and KLOE-2 have collected together the largest sample of electron-positron collisions at an energy equal to the φ-meson mass, corresponding to about $2.4×10^{10}$ produced φ mesons. In this talk I will review the latest results on neutral kaon physics at KLOE together with the status and prospects of the analyses of KLOE-2 data. I will report about a new measurement of the charge asymmetry in $K_S$ semileptonic decays with 1.7 fb$^{-1}$ of KLOE data, which improves the sensitivity of previous measurements of about a factor two. Furthermore, I will discuss the status of the analysis devoted to directly test T and CPT symmetries in neutral kaons transitions, as well as the search of the pure CP-violating $K_S → 3\pi^0$ decay using part of the recently acquired KLOE-2 dataset.

Speaker: Mr Alessandro Di Cicco (Roma Tre Univeristy)

Slides DiCicco-PHIPSI2019-draft.pdf

15:50 → 18:30 Baryon formfactors

Convener: Prof. Alexander Milstein (Budker Institute of Nuclear Physics)

15:50 Baryon form factors at BESIII

In this talk, I shall present some recent progresses at BESIII for the studies of baryon form factors, including the measuement of Lambda electromagnetic form factors, the proton electromagnetic form factor in e+e-->p pbar in energy region 2.0 - 3.08 GeV. These results will be followed by a short discussion about how does that improve our knowledge of the baryon form factors and the prospects of the BESIII program in this area.

Speaker: Dr Kai Zhu (Institute of High Energy Physics)

Slides phipsi2019_baryon_FFs_ZhuK.pdf

16:10 Coffee break

16:30 The NNbar and multihadron production at the threshold at VEPP2000

A study of hadron production at the nucleon-antinucleon threshold has been performed with the CMD-3 detector at the VEPP-2000 $e^+e^-$ collider. A very fast rise with about 1 MeV width has been observed in the $e^+e^- \to p\bar p$ cross section. A sharp drop in the $e^+e^- \to 3(\pi^+\pi^-)$ cross section has been confirmed and found to have a less than 2 MeV width, in agreement with the observed fast rise of the $e^+e^- \to p\bar p$ cross section. For the first time a similar sharp drop is demonstrated in the $e^+e^- \to K^+K^-\pi^+\pi^-$ cross section. The behavior of the $e^+e^- \to 3(\pi^+\pi^-),~ K^+K^-\pi^+\pi^-$ cross sections cannot be explained by an interference of any resonance amplitude with continuum, therefore this phenomenon cannot be due to a narrow near-threshold resonance. No such structure has been observed in the $e^+e^- \to 2(\pi^+\pi^-)$ cross section.

Speaker: Prof. Evgeny Solodov (BINP)

Slides cmd3_6pi_4pi_2K2p_ppbar2018.pdf

16:50 Baryon Studies at Belle

Although 10 years have passed since the last beam time of Belle, baryon spectroscopy analysis using 980 $\rm fb^{-1}$ data sample collected by the KEKB $e^{+}e^{-}$ collider near $\Upsilon$ resonances is still active. Over the last few years, we have discovered new excited $\Omega$ and $\Xi$ baryons. In the charmed baryon region, we observed a doubly Cabbibo-suppressed decay of $\Lambda_{c}^{+}$ and measured masses and widths of excited $\Xi_{c}$ baryons precisely. In this presentation, there will be a review of the baryon studies in Belle in recent years. The baryon studies expected from Belle $\rm II$ will also be briefly explained.

Speaker: Dr Seongbae Yang (Korea University)

Slides 20190228_phipsi19_yang_ver1_2.pdf

17:10 COMPASS++/AMBER and the Proton Radius Puzzle

CERN provides the large variety of high-energy beams for nuclear and particle physics research. One is the beam line M2 which is optimized to deliver an intense muon beam, but also hadron beams of both polarities. They are brought to an overground hall, which is used since many years almost exclusively by the COMPASS collaboration, with a broad experimental physics program on Quantum Chromodynamics (QCD). The most relevant results and activities of the collaboration, in terms of pion-photon reactions for determination of the chiral anomaly and the related radiative width of the rho meson, will be discussed. Since many questions around QCD remain still open, the follow-up facility COMPASS++/AMBER is envisaged, aiming at up-to-date detector architecture and a large variety of measurements. They range from lowest-Q2 physics as the determination of the proton radius from elastic muon-proton scattering, to average-Q2 reactions for hadron spectroscopy and high-Q2 hadron structure investigations via the Drell-Yan process and deeply-virtual Compton scattering. The recently submitted Letter of Intent for COMPASS++/AMBER will be discussed. Focus will be given to the elastic muon-proton scattering measurement, that may contribute significantly to solve the proton radius puzzle due to the usage of a high-energy muon beam.

Speaker: Dr Jan Friedrich (TU München)

Slides Friedrich-PhiPsi19.pdf

17:30 The proton size radius: experiment vs theory

Brief review of the proton radius problem is given. In the framework of the quasipotential method in quantum electrodynamics we calculate the contribution of light pseudoscalar (PS) and axial-vector (AV) mesons to the interaction operator of a muon and a proton in muonic hydrogen atom. The coupling of mesons with the muon is via two-photon intermediate state. The parametrization of the transition form factor of two photons into PS and AV mesons, based on the experimental data on the transition form factors and QCD asymptotics, is used. Numerical estimates of the contributions to the hyperfine structure of the spectrum of the S and P levels are presented. It is shown that such contribution to the hyperfine splitting in muonic hydrogen is rather important for a comparison with precise experimental data.

Speaker: Prof. Alexander Dorokhov (JINR)

Slides Dorokhov_NSK19_PhiPsi.pdf

17:50 Overview of a baryon-antibaryon pair production from electron-positron annihilation

The well-defined and simple, initial state makes a baryon-antibaryon pair production at an electron-positron collider a perfect system to test discrete symmetries in the baryon sector and to study baryon properties. In particular the production yields are much enhanced at the vector resonances such as J/psi and psi'. The spin orientations of the baryon and antibaryon are correlated and, for spin one-half baryons, the pair is produced either with parallel or antiparallel helicites. The transitions to the respective helicity states can acquire a relative phase, due to the strong interaction in the final state, leading to a time-reversal-odd observable: a transverse spin polarization of the baryons. The polarization could be determined for hyperons using their weak decays. This effect was recently observed at BESIII in the J/psi->Lambda_bar Lambda process. The polarization in baryon-antibaryon exclusive processes allows novel type of experiments such as simultaneous determination of the Lambda and Lambda_bar decay asymmetries. In the talk the method will be described and the prospects for the studies of weak decays of hyperons and for CP tests in baryon sector will be discussed.

Speaker: Prof. Andrzej Kupsc (Uppsala University)

Slides Kupsc190228phipsi.pdf

18:10 The neutron EDM and bounds on rare decays of eta and eta-prime mesons

Here will be present an improved estimate of the CPV coupling constants of the and 0 mesons to two pions using upper limits from data on the neutron electric dipole moment (nEDM). Using a phenomenological Lagrangian approach based on nonderivative couplings of the pseudoscalar mesons with nucleons, we include the full momentum dependence of the eta-pi-pi or eta-prime-pi-pi couplings in a two-loop approach to the nEDM calculation. Furthermore, this approach enables the inclusion of charged pion loops, therefore allowing for the leading electric photon minimal couplings. The upper limits for the rates of the CPV decays eta(eta-prime) into pair of pions that we derive are by orders of magnitude more stringent than those from the existing experiments so far.

Speaker: Dr Alexey Zhevlakov (TSU)

Slides phipsi2019_Zhevlakov_1.pdf

19:00 → 21:30 Conference Dinner

Friday, 1 March

09:00 → 09:40 Mesons of light quarks

Convener: Dr Matteo Fael (University of Siegen)

09:00 The Neutral Pion Radiative Width: The Final Result from PrimEx (Jefferson Lab)

The π 0 →γγ decay amplitude is determined by the chiral anomaly. Recent theoretical calculations have been made within Chiral Perturbation Theory and predict decay width at a percent precision level. Precise measurement of π 0 →γγ decay width gives a possibility to check these predictions. The PrimEx experiment unutilized Primakoff effect to measure π 0 radiative decay width. Primakoff effect is a powerful tool for measuring radiative width of particles. In this talk, the final result of the PrimEx experiment performed in Hall-B at Jefferson Lab will be presented. The PrimEx-I experiment performed in 2004 achieved precision of 2.8%. PrimEx-II has been conducted in 2010 with a collection of five times more statistics and achieved 1.6% precision. η→γγ decay width measurement experiment planned at Jefferson Lab will also be discussed. The project was supported in part by NSF MRI PHY 0079840 and RFBR 18-02-00938.

Speaker: Dr Ilya Larin (University of Massachusetts Amherst)

Slides ilarin_phipsi_2019.pdf

09:20 An amplitude analysis of the e+e−→4π reaction

My talk is about an analysis of the process $e^+e^- \to 4 \pi$ with the CMD-3 detector at the VEPP-2000 Collider in the energy range 0.9--2.007 GeV. In my contribution I will focus on the study of the intermediate dynamics of the reaction, i.e. I will talk about the results in the distinguishing of different intermediate mechanisms. The dominance of the (omega pi0) and (a1 pi) amplitudes will be proved. as well as the contribution of the rho+rho-, rho f0. rho sigma and etc. states will be discussed. Also, I will demonstrate the test of the isospin relation between the processes e+e- \to pi+ pi- 2pi0

Speaker: Mr Evgeny Kozyrev (BINP)

Slides PHIPSI2019_2pi2pi0v9.pdf

09:40 → 13:00 tau-lepton

Conveners: Dr Matteo Fael (University of Siegen) , Dr Pablo Roig (Cinvestav)

09:40 Tau mass measurement at BES-III

We had performed a tau threshold scan with $\int L \approx 130~pb^{-1}$ for a new tau-lepton mass measurement with BES-III detector in 2018. The beam energy is determined by laser backscattering and high-purity germanium detector which is calibrated by $\gamma$-sources. We have done $J/\psi$ and $\psi(2S)$-meson scans to examine beam energy measurement system. In this report we present preliminary result of the tau mass measurement.

Speaker: Dr Ivan Nikolaev (Budker Insitute of Nuclear Physics)

10:00 Semileptonic tau decays: Powerful probes of non-standard charged current weak interactions

Traditionally, nuclear beta decays and radiative pion decays have been thought as the best processes to look for non-standard charged current weak interactions involving light quarks. We put forward recently that semileptonic tau decays are powerful probes in this respect, too. Last advances in this direction will be reviewed and compared to limits from other low-energy processes and LHC bounds.

Speaker: Dr Pablo Roig (Cinvestav)

Slides PhiPsi19Roig.pdf

10:20 Hadronic Decays of the tau Lepton

Several experimental collaborations have recently invested considerable effort in precision studies of hadronic tau decays. With further improvements expected at Belle-II, it is important to discuss the theoretical implications of these experimental advances. In this talk, I will review several such implications. First, we will show that hadronic tau decays represent a clean laboratory for the precise study of Quantum Chromodynamics (QCD) in its non perturbative regime. Second, these decays can be used as a probe of the electroweak interaction. In this respect, we will discuss how tau decays and in particular $\tau \to \ell \pi \pi$ decays can be an interesting probe for lepton flavour violation allowing to unveil new phenomena.

Speaker: Emilie Passemar (Indiana University/JLab)

Slides EPassemar_phipsi2019.pdf

10:40 Coffee break

11:00 Tau physics at Belle II

The Belle II experiment is a detector coupled to the SuperKEKB electron-positron accelerator, located in Tsukuba, Japan. From April to July of 2018, Belle II completed the Phase II of commissioning in which ~500 pb-1 of data was recorded. Phase III will start in 2019 and, by 2025, a dataset of 50 ab-1 is expected. This large dataset will provide a unique opportunity to study tau lepton physics with high precision. In this talk, the tau lepton rediscovery and mass measurement using the Phase II data will be presented, followed by a review of the tau physics program for Phase III.

Speaker: Dr Petar RADOS (Deutsches Elektronen-Synchrotron (DESY))

Slides PhiPsi2019_Tau_Belle2.pdf

11:20 Light mesons from τ decays

The τ is the only lepton massive enough to decay into hadrons. Its semilep- tonic decays provide a privileged scenario to study low-energy effects of the strong interactions under rather clean conditions. Such advantageous framework is used to improve our understanding of the hadronization of QCD currents, to study meson form factors and to extract the physical parameters of the intermediate resonances produced in the decay. In this talk, we will review the status of the hadronic τ decay modes with particular attention to its decays into two hadrons. By exploiting the synergy between dispersion relations and Chiral Perturbation Theory we describe the meson from factors that come up into play. We will also briefly review higher- multiplicity decay modes. These involve a richer dynamical structure but accounting for the strong rescattering effects is not an easy task when three or more hadrons are present. The fantastic possibilities offered by the Belle-II experiment to study τ physics and low multiplicity final states with high precision make these studies of timely interest.

Speaker: Dr Sergi Gonzàlez-Solís (Department of Physics, Indiana University)

Slides PhiPsi19_Sergi.pdf

11:40 Measurement of Michel parameters in tau decays at high luminosity e+ e- factories

Michel parameters (MP) define the Lorentz structure of the Charged Weak Interaction mediated by W boson in the Standard Model (SM). They are in the list of the basic properties of tau lepton. The difference of the measured MP from their SM expectation will exhibit clear signature of the New Physics. We discuss the key points of the analysis of the huge data sample of taus collected at Belle to measure MP in leptonic tau decays. Essential point of the analysis is to consider the spin-spin correlation of taus, which allows us to extract MP related to tau polarization. At the e+ e- factories with unpolarized beams one have to analyze decay products of both taus to be sensitive to the spin-spin correlation. Nonzero average polarization of single tau at the Super Charm-Tau factory with polarized e- beam provides unique possibility to measure all Michel parameters without tagging the opposite tau.

Speaker: Denis Epifanov (BINP)

Slides epifanov_phipsi19.pdf

12:00 Physics with tau leptons at CMS

Tau lepton is an important tool for new physics searches at the LHC. This talk focuses on the measurement of the reconstruction and identification performance of the hadronic tau decays by the CMS detector. The measurements include the performance of the identification, trigger, energy calibration and decay mode classification algorithms for reconstructed tau candidates. Applications of the developed tau reconstruction algorithms to physics measurements with tau leptons at CMS detector are also presented.

Speaker: Dr Vladimir Cherepanov (UF)

Slides phipsi19_cherepanov.pdf

12:20 Leptonic decays of the tau lepton

I will review of theoretical aspects of the tau leptonic decays, including the radiative ($\tau \rightarrow l \gamma \nu \bar \nu $) and the five-body ($\tau \rightarrow l l l \nu \bar \nu$) decay modes, which are among the most powerful tools to study precisely the structure of the weak interaction and to constrain possible contributions beyond the V–A coupling of the Standard Model.

Speaker: Dr Matteo Fael (University of Siegen)

Slides Novosibirsk2019Fael.pdf

12:40 Recent results on tau lepton from Belle

The world's largest statistic of tau is collected with Belle detector. Recently, we measure the branching fraction for tau- -> pi- l+ l- nu, which is predicted by the Standard Model but not yet probed due to its small branching fraction (O(10^-5)). In this presentation, we show the measured result of this mode and briefly report the status of other on-going analyses at Belle, the branching fraction of tau decay into three leptons and two neutrinos, the evaluation of Michel parameters using tau- -> l- nu nu and the branching fraction of tau decay into three hadrons and one neutrino.

Speaker: Yifan Jin (The university of Tokyo)

Slides PhiPsi2019YifanJin.pdf

13:00 → 14:30 Lunch

14:30 → 16:20 Flavour

Convener: Dr Alexey Nefediev (Lebedev Physical Institute)

14:30 Open Charm Physics at BESIII

The BESIII experiment at the BEPCII collider analyses $e^+e^−$ collisions in the charmonium region. The accessible energy range covers several charm related thresholds, such as $D\bar{D}, D_sD_s^*$. BESIII has recorded large samples at those energies and the special topology of quantum-correlated pairs of D decays serves as ideal laboratory for the study of charm decays. In this talk we present recent results from the analysis of $D^0$ , $D^+$ and $D_s$ decays. In particular, the measurement of form-factors and decay constants using leptonic and semi-leptonic final states and results from partial-wave analyses and branching fraction measurements of hadronic final states.

Speaker: Dr Peter Weidenkaff (Institut fuer Kernphysik, Mainz)

Slides Weidenkaff-Bes3Charm-PhiToPsi.pdf Weidenkaff-Bes3Charm-PhiToPsi.pptx

14:50 Open charm studies at Belle

Until recently, parameters of vector charmonia lying above the open-charm threshold were determined from the inclusive cross section of the electron-positron annihilation to hadronic final states. However, the parameters of the resonances obtained this way are model-dependent and they suffer from large uncertainties. On the other hand, measurements of exclusive cross sections of the e^+e^- annihilation to charm hadrons should provide important missing information about strong interaction in this region so that the results of such measurements are of large interest both for developments of experimental methods, and theory. In particular, the aforementioned measurements should shed light on the nature on the charminium states with quantum numbers 1−−, which are not fully understood yet. Determination of the masses and widths of these resonances in a model-independent way and extraction of their coupling constant to elastic open-charm channels will allow to obtain information on the wave functions of the vector charmonia and to verify the phenomenological models for heavy hadrons. New results are obtained for the exclusive cross sections of the e+e− annihilation into charmed hadron pairs with initial state radiation. The analysis is based on the data sample collected with the Belle detector with the integrated luminosity of 951 fb−1. The accuracy of the cross section measurement is increased by a factor of 2 compared with the previous Belle study and, for the first time, the e+e−→D∗D∗ cross section is decomposed into three components corresponding to different helicities of the D∗’s in the final state.

Speaker: Valentina Zhukova (LPI)

Slides phipsi2019_zhukova.pdf

15:10 Charmed mesons and baryons at LHCb

LHCb collected a world-leading sample of charmed baryons during LHC's Run 1 (2010-2012) and Run 2 (2015-2018). With this data set, LHCb is discovering many previously unobserved charmed states and making the most precise determinations of the properties of known states. LHCb's latest results on charmed baryons are presented.

Speaker: Dr Alexey Dzyuba (B.P. Konstantinov Petersburg Nuclear Physics Institute National Research Center "Kurchatov Institute")

Slides A.Dzyuba_PhiPsi_v2.pdf

15:40 A review of present experimental status of the K -> pi nu nubar decays at the NA62

A review of present experimental status of the K -> pi nu nubar decays is given in the talk. The NA62 experiment at CERN SPS is designed to measure the branching ratio of the K+ -> pi+ nu nubar using a novel kaon decay-in-flight technique, while the KOTO experiment at JPARC aims to study the KL -> pi0 nu nubar decay. Both experiments produced new results in 2018. The NA62 experiment observed one candidate event, compatible with the Standard Model prediction. The KOTO experiment improved the existing upper limits on the branching ratio of the neutral kaon decay by an order of magnitude.

Speaker: Dr Artur Shaikhiev (Institute for Nuclear Research RAS)

Slides shaikhiev_phi_psi19.pdf

16:00 Off-shell fermion polarization and t-quark production

Standard calculation of polarization of final electron for pure initial state may be reformulated as a problem of looking for the complete polarization axis of produced state. In this problem the scattering amplitude is used (instead of its square in standard approach) and it gives method for calculation of polarization applicable for both final and intermediate state fermions. For this purpose it is convenient to use fermion propagator (bare or dressed) in form of spectral representation, which is based on eigenvalue problem and gives the system of orthogonal off-shell energy projectors. These two poins together: (i) problem of looking for the complete polarization axis and (ii) spectral representation of fermion propagator allow to give a corrrect definition for polarization of intermediate fermion. Most interesting is the case of fermion resonance (i.e. dressed propagator) in theory with P-parity violation. Corresponding the energy projection operators differ from the standard off-shell projectors and also contain $\gamma^{5}$. Moreover, in such theory the standard spin projectors do not commute with propagator and also should be modified. The obtained projectors are used to give the most accurate parametrization of t-quark resonance curve and simultaneously for its off-shell polarization.

Speaker: Dr Alexander Kaloshin (Irkutsk State University)

Slides Kaloshin.pdf

16:20 → 16:40 Workshop closing