CERNSeptember/October 2020 cerncourier.com COURIERReporting on international high-energy physics WLCOMEE CERN Courier – digital edition Welcome to the digital edition of the September/October 2020 issue of CERN Courier. NUCLEAR PHYSICS This issue’s cover feature (p36) describes recent results from CERN’s ISOLDE facility, where researchers are probing the extremities of the nuclear landscape to complete AT THE our understanding of the nuclear interaction. Advanced laser and trapping techniques developed over many years at ISOLDE are also bringing new ways to test physics EDGE beyond the Standard Model.
This autumn CERN launches its quantum technology initiative (p47) – part of a fast-growing interdisciplinary effort taking place worldwide to develop quantum computing, communication, sensing and other devices that promise to underpin a “second quantum revolution” (p49).
Sticking with CERN science, we report on new tetraquark discoveries by LHCb (p25), NA62’s evidence for an ultra-rare kaon decay (p9), the first signs of Higgs– muon coupling (p7), and how the Higgs boson has so far delivered three fundamental discoveries (p41). Also, don’t miss our special feature on careers from the CERN Alumni Network (p56).
Elsewhere in this issue: the European Spallation Source nears completion (p29); neutrinos prove rare solar-fusion process (p11); how particles attract Nobel prizes (p70); reports from ICHEP and Neutrino 2020 (p19); news in brief (p13); reviews (p53), and more.
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EDITOR: MATTHEW CHALMERS, CERN DIGITAL EDITION CREATED BY IOP PUBLISHING High-energy careers One Higgs, three discoveries CERN and quantum technologies
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Tetraquarks Recent LHCb observations On target The European Spallation Source Quantum future Alberto Di Meglio on reignite the meson-diquark debate. 25 nears completion. 29 CERN’s quantum technology initiative. 47
NeWS people
ANALYSIS ENERGY FRONTIERS FIELD NOTES CAREERS OBITUARIES Higgs-muon coupling The LHC as a photon ICHEP a virtual success Growing the high- Ulrich Becker 1938–2020 The x740 is a CAEN Waveform Digitizers family able to perform basic waveform • XENON1T excess colldier • The exotic • Neutrino 2020 zooms energy network • Claude Détraz 1938– • Signs of ultra-rare nature of X(3872) into virtual reality CERN alumni 2020 • John Flanagan recording and run real-time advanced Digital Pulse Processing (DPP) kaon decay • CERN’s • J/ψ polarisation in • Terascale summer demonstrate the value 1964–2020 • Henri impact on the UK lead collisions school goes global. 19 placed by employers on Laporte 1928–2020 • Estonia joins CERN • LHCb’s search for the skills acquired in high- • George Trilling CHECK THIS OUT! • CNO process detected. 7 dark photon. 15 energy physics. 56 1930–2020. 65 V/VX2740 - 64 Channel 16 bit 125 MS/s Digitizer 1GbE or 10GbE • 64 channel, 125 MS/s, 16 bit waveform digitizer FeAtureS • Four 40 pin, 2 mm header connectors CMS-PHO-EVENTS-2019-002-7 • Adapters to 1.27 mm flat cables or coax MULTI-QUARK STATES NEUTRON SCIENCE EXOTIC NUCLIDES HIGGS BOSON • Differential or SE inputs Tetraquarks back ESS under Exploring nuclei One Higgs, in the spotlight construction at the limits three discoveries 1 DAC output (signal • 1GbE or 10GbE or CONET2 (optional) The debate over whether The European Spallation Recent studies of exotic ATLAS and CMS have inspection or trigger sum) • USB 3.0 type C tetraquarks are loosely Source will provide nuclides at ISOLDE made three distinct • Common Trigger (waveforms) or Individual Self-trigger modes bound pairs of mesons new research into offer new ways to look discoveries regarding • DPP options: PHA, QDC, PSD, CFD or tightly bound pairs of material properties and for physics beyond the the Higgs, argues • Advanced Waveform Readout modes: ZLE, DAW diquarks. 25 fundamental physics. 29 Standard Model. 36 Yosef Nir. 41 Open • Open FPGA FPGA • 4 LEMOs + 16 LVDS programmable I/Os • 1 DAC output (1ch 125MS/s 14bit) opINIoN DepArtmeNtS • Independent 5MS/ch of max. Record Length • Available in desktop form factor VIEWPOINT INTERVIEW REVIEWS FROM THE EDITOR 5 CERN and quantum Lessons in An intuitive NEWS DIGEST 13
Four 40pin, 2mm FIRMWARE SOFTWARE technologies leadership approach to teaching APPOINTMENTS 60 header connectors CERN’s new quantum The best leaders are New textbook by Common Trigger (waveforms) or & AWARDS technology initiative those who don’t want to Larkoski • Accelerator G Audi/W Huang/AMDC-NUCLEUS Individual Self-trigger modes & WAVE RECRUITMENT 61 DUMP can enrich its research be leaders per se, says radiation protection. 53 On the cover: The nuclear CAEN programme, says experimentalist landscape, showing mass BACKGROUND 70 Alberto Di Meglio. 47 Ian Shipsey. 49 excess (vertical) versus Z, N C and LabVIEW™libraries available for custom developments. and decay mode (colour). 36
CERN COURIER SEPTEMBER/OCTOBER 2020 3 Small details… Great differences
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ISOLDE: shaping the nuclear landscape AMDC-NUCLEUS (G Audi, W Huang, D Lunney) (G W Huang, Audi, AMDC-NUCLEUS fter 100 years of expanding and exploring the chart of the nuclides (cover image) physicists are still without A a complete understanding of nuclear interactions. An early picture of the nucleus was of an incompressible liquid drop. Systematic surveys of the nuclear chart later revealed that protons and neutrons arrange themselves in quantum orbits or shells, with certain “magic” numbers of nucleons Matthew resulting in greater stability. Reconciling the drop and shell Chalmers models has been a longstanding quest, but a lack of predictive Editor power has required further exploration of the nuclear chart to reveal clues. By continuing to innovate in the production and purification of the most exotic species, CERN’s ISOLDE facility leads the charge in probing the extremities of the nuclear landscape (see p36). Understanding nuclear structure relies on measurements of the mass and radii of nuclei, made possible by precision Onwards and outwards Nuclear mass excess versus proton and laser and trapping techniques developed at ISOLDE over many neutron number. Colours show decay mode (stable nuclides in black). years, which have been adopted by facilities worldwide. The farther experimenters venture from the valley of stability, Quantum future the more surprises they find – the most dramatic being the This autumn, CERN launches its quantum technology initiative erosion of the stabilising magic of closed nuclear shells, which (p47). New quantum computing, communication and sensing gives way to nuclei in contorted dis-equilibrium. devices that harness properties such as entanglement promise ISOLDE’s ability to produce the most exotic nuclides is also to underpin a “second quantum revolution”, following the stimulating developments in theory, in particular ab-initio information and communication technology that resulted techniques, derived using chiral effective field theory that from the birth of quantum mechanics in the 20th century. respects the symmetries of QCD. Recently, precision laser and Several major national programmes are already under way, mass spectroscopy have brought radioactive molecules within with the US recently announcing more than $500M for five its grasp – offering a new way to detect possible electric dipole quantum-science institutes at its national laboratories (p13). moments that would point to new physics. In its sixth decade, Though relatively new to the game, CERN has significant expe- ISOLDE continues to innovate and evolve. rience in many of the relevant domains and provides valuable CERN’s science is a strong theme of this issue, with recent use-cases, particularly in quantum computing. results from LHCb reinvigorating the tetraquark debate (p25), As our interview (p49) explores, it is too early to tell how NA62 establishing evidence for an ultra-rare kaon decay (p9), quantum technologies will impact society – just as nobody and the LHC experiments reporting the first indications of in the 1950s could have predicted that billions of transistors CERN’s couplings of the Higgs boson to a second-generation fermion would be packed into our pockets today. But it is clear that science is a (p7 and p41). Our special feature on the CERN Alumni Network high-energy physics stands to benefit from new computing, strong theme (p56), meanwhile, highlights the high value placed by employ- sensing and other quantum-technology applications, and of this issue ers on skills gained from training in high-energy physics. that labs like CERN have the potential to make a real impact.
Reporting on international high-energy physics
CERN Courier is distributed Editor Laboratory correspondents INFN Antonella Varaschin UK STFC Jane Binks Technical illustrator General distribution to governments, institutes Matthew Chalmers Argonne National Jefferson Laboratory SLAC National Accelerator Alison Tovey Courrier Adressage, CERN, and laboratories affiliated Associate editor Laboratory Tom LeCompte Kandice Carter Laboratory Melinda Baker Advertising sales 1211 Geneva 23, Switzerland; with CERN, and to Mark Rayner Brookhaven National JINR Dubna B Starchenko SNOLAB Samantha Kuula Tom Houlden e-mail courrier- individual subscribers. Archive contributor Laboratory Achim Franz KEK National Laboratory TRIUMF Laboratory Recruitment sales adressage@cern.ch It is published six times Peggie Rimmer Cornell University Hajime Hikino Marcello Pavan Chris Thomas per year. The views Astrowatch contributor D G Cassel Lawrence Berkeley Advertisement Published by CERN, 1211 expressed are not Merlin Kole DESY Laboratory Laboratory Spencer Klein Produced for CERN by production Katie Graham Geneva 23, Switzerland necessarily those of the E-mail Till Mundzeck Los Alamos National Lab IOP Publishing Ltd Marketing and Tel +41 (0) 22 767 61 11 CERN management. [email protected] Enrico Fermi Centre Rajan Gupta Temple Circus, Temple circulation Laura Gillham Guido Piragino NCSL Ken Kingery Way, Bristol BS1 6HG, UK Printed by Warners Advisory board Fermilab Kurt Nikhef Robert Fleischer Tel +44 (0)117 929 7481 Advertising (Midlands) plc, Bourne, Peter Jenni Riesselmann Novosibirsk Institute Tel +44 (0)117 930 1026 Lincolnshire, UK Christine Sutton Forschungszentrum S Eidelman Head of Media Jo Allen (for UK/Europe display Claude Amsler Jülich Markus Buescher Orsay Laboratory Head of Media advertising) or © 2020 CERN Philippe Bloch GSI Darmstadt I Peter Anne-Marie Lutz Business Development +44 (0)117 930 1164 (for ISSN 0304-288X Roger Forty IHEP, Beijing Lijun Guo PSI Laboratory P-R Kettle Ed Jost recruitment advertising); Mike Lamont IHEP, Serpukhov Saclay Laboratory Content and production e-mail sales@ Joachim Kopp Yu Ryabov Elisabeth Locci manager Ruth Leopold cerncourier.com
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Your partner in Non Destructive NEWS Diagnostic Solutions ANALYSIS for Low Current Measurements
Higgs boson Turning the screw on H → μμ CMS-PHO-EVENTS-2020-017-1 CMS-PHO-EVENTS-2020-017-1 The first evidence for the coupling of the Higgs boson to a second-generation fermion, the muon, has been reported at the LHC. At the 40th International Conference on High Energy Physics, Turbo-ICT & BCM-RF held from 28 July to 6 August (see p19), CMS reported a 3σ excess of H → μμ decay candidates compared to the expected sample under the hypothesis Very low charge measurement of no coupling between the Higgs boson of ultra-short bunches and the muon. A similar analysis by the ATLAS collaboration yielded a 2σ excess for the coupling. The latest measurements of the Resolution down to 10 fC Higgs boson by ATLAS and CMS follow 5σ observations of its coupling to the tau lepton in 2015 and to the top and bottom quarks in 2018, all of which are third-generation fermions. Its couplings to W and Z bosons have also been estab- lished at 5σ confidence. Within present experimental accuracy, all couplings between the Higgs boson and other Standard Model particles correspond to the strength of interaction that would give the particles their observed masses, New topology ons observed at the LHC; vector-boson are compatible with the Standard Model,” CWCT & BCM-CW according to the Brout–Englert–Higgs A CMS candidate fusion; the production of a Higgs boson says ATLAS physics coordinator Klaus mechanism. In this model, the parti- for Higgs-boson in association with a weak vector boson; Mönig. “Assuming the H → μμ coupling cles acquire mass through spontane- production via and its production in association with predicted by the Standard Model, and ous symmetry breaking; the W and Z vector-boson a top quark–antiquark pair. Uniquely, extrapolating the current results, the Precise average current measurement of as a result of a local gauge symmetry fusion and its decay CMS simulated the background to the combined sensitivity could get near the and the fermions, such as the muon, into two muons vector-boson-fusion signal rather than observation threshold of 5σ at the end Continuous Wave beams or macropulses as a result of Yukawa couplings to the (red lines). fitting it from data – a procedure that of Run 3, from 2022 to 2024.” Higgs field – a novel type of interaction would have incurred additional statistical If there is only a single Higgs field, among fundamental particles that is not uncertainty – resulting in the topology it should provide the masses for all the Resolution down to 0.5 µA derived from a symmetry principle (see contributing roughly equal statistical Standard-Model particles, but there may p41). Any deviation from the expected power compared to gluon fusion. be additional Higgs fields that could make couplings would imply that the Higgs contributions to their masses. The new sector is more complicated than this Machine learning results therefore reduce the scope avail- minimal scenario. “The fi rst e v idence i n C M S w a s reac he d able to such multi-Higgs models, and Couplings to lighter particles are thanks to the excellent performance of sharpen the question of why there is a expected to be proportionately smaller our muon and tracking systems, and an hierarchy of particle masses, says John a n d m or e d i ffic u lt t o o b s e r v e. T h e d e cay improved signal/background discrim- Ellis of King’s College London. “Why is to two muons, H → μμ, is expected to ination with machine-learning tech- the Higgs coupling to the muon so dif- Visit www.bergoz.com occur with a branching fraction of just niques,” says Andrea Rizzi, CMS physics ferent from its coupling to the tau lepton, one in 5000 Higgs-boson decays, and is The new co-coordinator. whereas the couplings of the W boson to overwhelmed by backgrounds from the results The signature for the decay is a small tau leptons and muons are equal to within Drell–Yan process. sharpen the excess of events near a muon-pair a couple of percent? The more we learn The new ATLAS and CMS analyses, question of invariant mass of 125 GeV – the mass of about the Higgs, the more mysterious DISTRIBUTORS MANUFACTURER which deploy the entire 13 TeV Run-2 a Higgs boson. CMS reports an overall it seems!” why there is data set, include events where the Higgs signal strength of 1.2 ± 0.4, while ATLAS U.S.A.: GMW Associates India: GEEBEE International BERGOZ Instrumentation boson was produced according to four a hierarchy finds a signal strength of 1.2 ± 0.6, with Further reading www.gmw.com www.geebeeinternational.com www.bergoz.com topologies: gluon fusion, which accounts of particle the uncertainties dominated by their sta- ATLAS Collab. 2020 arXiv.org:2007.07830. [email protected] [email protected] 156 rue du Mont Rond for the creation of 87% of the Higgs bos- masses tistical component. “Both measurements CMS Collab. 2020 CMS-PAS-HIG-19-006. Espace Allondon Ouest Japan: Hayashi-Repic China: Beijing Conveyi Limited 01630 Saint Genis Pouilly, France www.h-repic.co.jp www.conveyi.com CERN COURIER SEPTEMBER/OCTOBER 2020 7 [email protected] [email protected] [email protected]
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Dark m atter R aRe decays Researchers grapple with XENON1T excess Double digits for ultra-rare kaon decay NA62 collaboration NA62 collaboration CERN’s NA62 collaboration has pre- run, and plans to improve its sensitivity 10–4 An intriguing low-energy excess w i l l fi n d it w it h i n t h e fi r s t h o u r s ofrun- sented its latest progress in the search for Camerini experimental upper limit @ 90% CL to less than 0.1 per billion by increasing of background events recorded by 120 ning,” says Garcia Irastorza. K+ → π +νν– – a “golden decay” with excep- the beam intensity and upgrading the 10–5 experimental measurement the XENON1T detector at Gran Sasso A second new-physics explanation tional sensitivity to physics beyond the theoretical prediction KOTO detectors. Klems National Laboratory in Italy has sparked 100 cited for XENON1T’s low-energy excess Standard Model (SM). The new analysis 10–6 As experimental uncertainties are XENON collaboration Cable a series of preprints speculating on its is an enhanced rate of solar neutrinos provides the strongest evidence yet for _ expected to approach the theoretical νν ) Asano underlying cause, ranging from unex- interacting in the detector. In the Stand- the existence of this ultra-rare process, + 10–7 precision in coming years, explains 80
→ π → E787 pected background sources to phenom- ard Model, neutrinos have a negligi- at 3.5σ sig n i fica nce. “A f ter se ver a l yea rs theo rist Andrzej Buras of the Institute + 10–8
ena beyond the Standard Model. On 17 keV) bly small magnetic moment, however, of a very challenging analysis, battling 10 for Advanced Study in Garching, Germany, .
BR(K E787 + + 0 60 –9 – and K – decays can probe June the XENON collaboration, which should they be Majorana rather than orders of magnitude of background over 10 + E949 K → π νν L → π νν
year NA62
searches for excess nuclear recoils in a . Dirac fermions, and identical to their the signal, we are proud to have achieved scales as high as a few hundred TeV – –10 one-tonne liquid-xenon time-projection 40 antiparticles, their magnetic moment the first statistically significant evidence 10 beyond the reach of most B-meson decays. chamber (TPC), reported an unexpected should be larger, and proportional to for a process that has great sensitivity to “K+ → π +νν– is most sensitive to hypothet- 10–11 excess of events at energies of a few keV. 20 background model their mass, though still not detectable. new physics,” says lead analyst Giuseppe 1960 1970 1980 1990 2000 2010 2020 ical Z′ gauge bosons, vector-like quark Though acknowledging that the excess New physics could, however, enhance the Ruggiero of Lancaster University, who models, supersymmetry and some lep- events/(tonne science run 1 data year of publication could be due to a difficult-to-constrain 0 magnetic moment further, leading to a presented the result on 5 August during toquark models,” he says. “LHCb studies + – tritium background, the collaboration 2 larger interaction cross section at low the International Conference on High- of KS → μ μ and Belle II studies of B → K(K*) says that solar axions and solar neu- σ energies and an excess of low-energy Energy Physics (see p19). Convergence eight orders of magnitude using parti- νν– will also have a part to play, allow- –2 trinos with a Majorana nature, both of elec t ron recoi ls. X ENON1T fit s i nd icate A flavour-changing, neutral-current Theoretical cle-identification techniques. ing a global analysis to test not only the which would signal physics beyond the that solar Majorana neutrinos with an process, K+ → π +νν– is highly suppressed predictions and The collaboration’s new result, which concept of minimal flavour violation, but 0 5 10 15 20 25 30 Standard Model, are credible explana- enhanced magnetic moment are also in the SM, with contributions from Z- experimental includes the full dataset collected until also probe new CP-violating phases and tions for the approximately 3σ effect. energy [keV] favoured over the background-only penguin and box diagrams with W, top measurements of 2018, adds a further 17 events to its previous right-handed currents.” hypothesis at the level of 3σ. quark and charm exchanges. It is also the K+ → π +νν– analysis, wherein three events observed Theorists expect to reach an accuracy World-leading limits Threshold events X ENON1T data from scientific run 1, very “clean” theoretically, since the branching fraction. in 2016 and 2017 yielded an estimated of 5% on the predicted K+ → π +ν branching +72 The XENON collaboration has been in from Februar y 2017 to Februar y 2018, show an excess of Flurry of activity low-energy hadronic matrix elements are branching fraction of 47 –47 decays per ratio towards the end of the decade. In the pursuit of WIMPs, a leading cold-dark- low-energy electronic recoils above the background model. The community has quickly chimed in just those of the quark currents between trillion. The measured branching fraction same period, the NA62 team is seeking +40 matter candidate, since 2005 with a with additional ideas, with more than the hadronic states. of 110 –35 per trillion is in agreement with to hone its resolution from the current programme of 10 kg, 100 kg and now If the XENON1T signal is 100 papers citing XENON1T’s findings NA62 observes the 6% of positively the SM prediction of 84 ± 10 per trillion. 30% down to 10%. The collaboration will 1 tonne liquid-xenon TPCs. Particles appearing on the arXiv preprint server charged kaons that are produced when The NA62 result is expected to soon resume data taking in 2021, following scattering in the liquid xenon create indeed an axion, IAXO will since the result was released. One pos- 450 GeV protons from the Super Proton be complemented by a measurement of upgrades to both beam and detector tak- 0 – both scintillation light and ionisation sibility is a heavy dark-matter particle Synchrotron strike a beryllium target. The the related CP-violating KL → π νν decay ing place during the ongoing second long electrons; the latter drift upwards in an find it w it hin t he first hours that annihilates or decays to a second, analysis is challenging because of the tiny by the KOTO collaboration at the J-PARC shutdown of CERN’s accelerator complex. electric field towards a gaseous phase much lighter, “boosted dark-matter” branching fraction and the presence of a research facility in Tokai, Japan. This “The horizon of a new-physics programme where electroluminescence amplifies of running particle that could scatter on electrons neutrino pair in the final state. Pioneering even rarer process has a predicted SM with a sensitivity to decay rates well below the charge signal into a light signal. via some new interaction, notes CERN the technique of observing kaon decays branching fraction of just 34 ± 6 per tril- the 10–11 level is now in sight,” says NA62 XENON1T derives its world-leading consistent with the XENON1T excess. theorist Joachim Kopp. Another class i n fl i g ht, t he c ol l a b or at ion me a s u re s t he lion. KOTO’s 2015 data yielded no event spokesperson Cristina Lazzeroni of the limit on WIMPs – the strictest 90% According to this hypothesis, the axions of dark-matter model that has been kinematics of both the initial kaon and the candidates and a 90% confidence upper University of Birmingham, UK. confidence limit being a cross-section would be detected via the “axioelec- proposed, he says, is “inelastic dark final-state pion to isolate the kinematic limit on the branching fraction of 3.0 of 4.1 × 10–47 cm2 for WIMPs with a mass tric” effect, an axion analogue of the matter”, where dark-matter parti- signature of K+ → π +νν–, before then sup- per billion, but the collaboration is now Further reading of 30 GeV – from the very low rate of photoelectric effect. Though a good fit cles down-scatter in the detector into pressing other decay modes by a further fi n a l i si n g it s re s u lt s f rom t he 2016–2018 NA62 Collab. 2020 arXiv:2007.08218. nuclear recoils observed by XENON1T phenomenologically, and like tritium another dark-matter state just a few keV from February 2017 to February 2018. favoured over the background-only below the original one, with the liber- Policy HV Wooding A surprise was in store, however, in hypothesis at approximately 3σ, the ated energy then seen in the detector. the same data set, which also revealed solar-axion explanation is disfavoured “An explanation I like a lot is in terms UK report shows 285 electronic recoils at the lower end of by astrophysical constraints. For exam- of dark photons,” he says. XENON1T’s energy acceptance, from 1 to ple, it would lead to a significant extra The XENON collaboration is soon to impact of CERN 7 keV, over the expected background of energy loss in stars. start taking data with a new detector, 232 ± 15. The sole background-modelling Axion helioscopes such as the CERN XENONnT. With three times the fidu- membership explanation for the excess that the col- Axion Solar Telescope (CAST) experi- cial volume of XENON1T and a factor laboration has not been able to rule out ment will help in testing the hypoth- six reduction in backgrounds, explains T h e b e n e fit s o f C E R N m e m b e r s h i p g o wel is a minute concentration of tritium in esis. “It is not impossible to have an XENON spokesperson Elena Aprile b e y o n d s c i e n c e a n d t e c h n ol o g y, c o n fi r m s the liquid xenon. Though cryogenic dis- axion model that shows up in XENON of Columbia University in New York, a study commissioned by the UK’s Science tillation plus running the liquid xenon but not in CAST, but CAST already con- XENONnT should be able to verify or and Technology Facilities Council (STFC). through a getter is expected to remove strains part of the axion interpretation refute the signal within a few months of The report “Evaluation of the benefits any tritium below the level that would be of the XENON signal,” says CAST deputy data taking. “I am especially intrigued that the UK has derived from CERN”, pub- relevant, there is not yet any instrument spokesperson Igor Garcia Irastorza of the by the possibility to detect axions pro- l i s h e d o n 6 A u g u s t, fi n d s t h a t a r o u n d 500 sensitive enough to directly detect such University of Zaragoza. Its successor, the duced in the Sun,” she says. “Who needs U K fi r m s h a v e b e n e fit t e d f r o m s u p pl ying a trace amount, says the collaboration. International Axion Observatory (IAXO), the WIMP if we can have the axion?” goods and services to CERN during the One explanation proposed by the team which is set to begin data taking in 2024, past decade, bringing in £183.3M in rev- is solar axions, which, should they exist, will have improved sensitivity. “If the Further reading enue. An additional £33.4M was awarded Profit An electroplating plant at UK engineering firm HV Wooding, which is one of 500 UK companies to have s would be produced by the Sun at energies XENON1T signal is indeed an axion, IAXO E Aprile et al. 2020 arXiv.org:2006.09721. to UK firms for CERN experiments benefitted from supplying goods and services to CERN during the past decade.
8 CERN COURIER SEPTEMBER/OCTOBER 2020 CERN COURIER SEPTEMBER/OCTOBER 2020 9
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and from the CERN pension fund, while eight UK universities revealed that 95% B ei ng pa r t valued at more than £495M, before even AstrowAtch a further £1B in turnover and £110M in were attracted to study science because of one of considering the impact of the advances profit is estimated to have resulted from of activities in particle physics, with more the biggest that this research may underpin. Bibli- k n o c k- o n e ffe c t s for U K c o m p a n i e s a f ter than 50% saying they were inspired by ometric analyses also show that CERN Neutrinos confirm rare solar-fusion process working with CERN. the discovery of the Higgs boson. international research underpins many of the UK’s Over the same 10-year period, 1000 In terms of science diplomacy, the scientific most influent ial physics papers. Despite being our closest star, much collaboration Borexino or so individuals who have participated report acknowledges that CERN pro- collaborations The new report supports previous remains to be learned about the exact in CERN’s various employment schemes vides a platform for the UK to engage on the planet s t u d ie s i nt o t h e b e n e fit s o f C E R N me- nature of the Sun and how it produces have received training estimated to be more widely in global initiatives and places the UK bership. In particular, a recent study its energy. Two different fusion pro- worth more than £4.9M. The knowledge international networks, spilling over at t he f r ont ier of the impact of the High Luminosity cesses are thought to be at play in the and skills gained via working at CERN to favourable perceptions of its mem- LHC conducted by economists at the majority of stars: the direct fusion of are deployed across sectors including IT bers and greater engagement in science, of discovery University of Milan concluded that the hydrogen into helium, which is thought and software, engineering, manufactur- technology and beyond. “Fundamental science quantifiable return to society is well in to be responsible for approximately 99% ing, financial services and health, the research requires long-term engage- excess to the project’s costs (CERN Courier of the Sun’s energy; and the fusion of report notes, with young UK researchers ment; international collaboration makes September 2018 p51). hydrogen into helium via the six-stage who have engaged with CERN estimated t h i s e s s e nt i a l p o ol i n g o f e ffor t s p o s s i bl e, The UK is one of CERN’s founding carbon–nitrogen–oxygen (CNO) process to earn 12% more across their careers and the report provides a promising tes- members, and currently contributes (see CNO cycle diagram). Although theo- (corresponding to an extra £489M in timony for the future of CERN member- £144M per year to the CERN budget rised in the 1930s, direct proof of this additional wages in the past 10 years). ship,” said Charlotte Warakaulle, CERN (representing 16% of Member State sub- fusion process was missing. Now, the Each year an average of 12,000 school director of international relations. scriptions) via the STFC. “Being part of international Borexino collaboration students and other members of the pub- Carried out by consulting firm Tech- one of the biggest international scientific directly detected neutrinos produced in lic visit CERN in person; 220,000 visit nopolis, the study also quantified the collaborations on the planet places the UK the CNO cycle, providing the first direct CERN’s website; and 40,000 interact with scientific benefits of CERN membership. at the frontier of discovery science, which proof of this important fusion process. its social media. More than 1000 teachers Over the past decade, more than 20,000 in turn helps to inspire the next gener- The Borexino detector uses 278 tonnes have attended CERN’s national teacher scientific papers with a UK author have ation to study physics and other STEM of liquid scintillator held in a nylon programme in the past decade, who go on cited one of the 40,000 papers based subjects,” says STFC executive chair Mark balloon deep under the mountains at to teach an estimated 175,000 school stu- directly on CERN research published in Thomson. “This is of huge value to the Gran Sasso National Laboratory in Italy Solar focus Borexino’s 2200 photomultipliers detect scintillation light generated by electron/positron recoils dents within three months of their visit. the past 20 years. The report estimates UK – and for the first time this report to detect extremely rare interactions induced by sub-MeV neutrinos. A survey of 673 physics undergraduates in that the production of knowledge can be goes some way to quantify this.” between the scintillator and solar neu- trinos. In 2012 the experiment detected Commons/Borb Creative The spectral measurements performed CERN S Hertzog/CERN 4H neutrinos from the main solar fusion 1H of the CNO cycle exclude a non-detection process. Now, one year before the end of 1H with a statistical significance of more Estonia joins its scheduled operations, the Borexino γ than five sigma. The solar-neutrino +3.0 team has fully probed the solar energy interaction rate (7.2 –1.7 counts per day per CERN production. 100 t o n n e s o f t a r g e t, a t 68% c o n fid e n c e) 12 Despite minimising backgrounds from C furthermore agrees with models which 15 On 19 June the prime minister of Estonia, cosmic rays, trace amounts of radioactive N 13N predict that 1% of the energy produced Jüri Ratas, and CERN Director-General, nuclei that leak into the active volume in the Sun comes from the CNO process. Fabiola Gianotti, signed an agreement of Borexino produce a background of the ν e+ Additionally, the results shine light on admitting Estonia as an associate same magnitude as the sought-after the density of elements other than + member state in the pre-stage to mem- signal. The most important background e ν hydrogen and helium – the metallicity bership of CERN. The agreement will for the CNO analysis was 210Bi, a prod- – of the Sun’s core, which in recent years 15 13C enter into force once CERN has been uct of 210Pb of which trace amounts can O has been debated to potentially differ 14 informed by the Estonian authorities that diffuse into the scintillator from the N from that on the solar surface. The all the necessary approval processes have nylon balloon surface. Since the energy Borexino results indicate that the density been finalised. spectrum of the beta-decay of 210Bi is likely similar, although more precise γ γ “With Estonia becoming an associate resembles that induced by neutrinos 1H measurements with future detectors are member, Estonia and CERN will have the produced in the CNO process, the key to 1H required to confir m t his. opportunity to expand their collabora- detecting CNO neutrinos was to directly The groundbreaking Borexino study, tion in, and increase their mutual ben- Online firstEstonia’s prime minister Jüri Ratas and CERN Director-General Fabiola Gianotti at the signing measure the 210Bi-induced background. CNO cycle A proton is absorbed by a carbon nucleus, followed which required not only some of the efit from, scientific and technological ceremony which, due to the COVID-19 pandemic, took place via a live feed between Tallinn and Geneva – This was made possible by delving by a nuclear decay, then a second and third absorption of a proton, most precise techniques used in particle development as well as education and a first in CERN’s 66-year history. into the fluid dynamics of the liquid followed by another decay, the absorption of a fourth proton and physics but also complex fluid-dynam- training activities,” said CERN Direc- scintillator. finally a decay into a carbon nucleus, a helium nucleus and the ics simulations, provides a first probe tor-General Fabiola Gianotti. “We are the Compact Linear Collider project, “As an associate member, many The 210Bi in Borexino’s scintillator release of around 25 MeV of energy. into the processes at the cores of stars. looking forward to strengthening our a CMS team involved in data analysis important opportunities open up for produces 210Po, which undergoes alpha Although it has now been proved that t ies f ur t her.” and the Worldwide LHC Computing Estonian entrepreneurs, scientists and decay with a half-life of 134 days. As the the scintillator material by stabilising the CNO process is responsible for only After joining the CMS experiment in Grid, and another team taking part in researchers to work together on innova- alpha decay is relatively easy to identify, the temperature, both through insula- a fraction of the Sun’s energy, for heav- 1997, Estonia became an active member the TOTEM experiment. tion and R&D, which will greatly benefit the team used 210Po decays to deduce the tion and direct temperature regulation. ier and therefore hotter stars it is pre- of the CERN community. Between 2004 CERN’s associate member states are Estonia’s business sector and the econ- number of 210Bi decays in the detector. After the 210Po decay distribution inside dicted to be the dominant fusion process, and 2016 new collaboration frameworks entitled to participate in meetings of omy as a whole,” said Jüri Ratas, Estonia’s Ho w e v e r, a s t h e d i ffe r e nt i s o t o p e s m o ve the detector was found to be stable over making future high-precision studies gradually boosted scientific and tech- the CERN Council, Finance Committee prime minister, at the signing ceremony. around in the liquid it cannot be guar- times exceeding its half-life, an area important to understand the evolution nical co-operation. Today, Estonia is and Scientific Policy Committee. Their “Becoming an associate member is the anteed that the 210Bi distribution is equal with low 210Po activity was identified of the universe in general. represented by 25 scientists at CERN, nationals are eligible for staff positions next big step for Estonia to deepen its to 210Po unless the flow in the detector is and used to measure the CNO neutrinos comprising an active group of theo- and fellowships, and their industries are co-operation with CERN before becoming well understood. To overcome this, the with a well-understood and relatively Further reading rists, researchers involved in R&D for entitled to bid for CERN contracts. a full member.” collaboration had to reduce the flow of low background. Borexino Collab. 2020 arXiv:2006.15115.
10 CERN COURIER SEPTEMBER/OCTOBER 2020 CERN COURIER SEPTEMBER/OCTOBER 2020 11
CCSepOct20_NewsAnalysis_v4.indd 10 09/09/2020 11:05 CCSepOct20_NewsAnalysis_v4.indd 11 09/09/2020 11:06 CERNCOURIER www. V o l u m e 6 0 N u m b e r 5 S e p t e m b e r / O c t o b e r 2 0 2 0 CERNCOURIER.COM NEWS Books in High Energy Physics DIGEST Find your next read from over 800 high quality textbooks & research references Brilliant synchrotron begins and achieve an unprecedented Simplifying sums
www.tinyurl.com/wsparticlephys R Hahn Following a 20-month shutdown, precision of 21 ppt. The proton’s A team led by Pierpaolo Mastrolia the European Synchrotron mass discrepancy is the latest (Padova) and Sebastian Mizera Lectures on Quantum Field Lectures on Accelerator Physics Radiation Facility (ESRF), in in a series of oddities observed (Princeton) has published a new Theory (2nd Edition) By Alexander Wu Chao (SLAC National Accelerator Lab., USA) Grenoble, France, is back in in recent years, including the exposition of their 2017 idea for By Ashok Das (Univ. of Rochester, USA) Accelerators have been driving research and industrial advances action with users now able to converging proton-radius puzzle using techniques in algebraic for decades. This textbook illustrates the physical principles behind carry out experiments using a and the long-standing proton geometry to circumvent some Reviews of the First Edition: these incredible machines, often with intuitive pictures and simple Alex Romanenko (Fermilab) with a brand new fourth-generation spin crisis (CERN Courier May/June of the challenges relevant to “Ashok Das has written an excellent, mathematical models. The style is informal and accessible to qubit based on RF-cavity technology. high-energy synchrotron light 2019 p38). computing multi-loop Feynman comprehensive introduction to modern graduate-level students without prior knowledge in accelerators. source, the Extremely Brilliant amplitudes. The approach quantum field theory, covering both its US invests in quantum technology Source (EBS). The new machine Muon-collider study initiated uses “twisted cohomology”, theoretical underpinnings and basic com- 700pp Oct 2020 putational methods. It will be very useful to 978-981-122-796-7(pbk) US$88 / £75 Following a competitive will provide users across a wide A new international design a mathematical theory students, teachers, and researchers as a 978-981-122-673-1 US$188 / £165 peer-review process, the US range of disciplines with an study for a future muon collider previously only applied to string course text, and as a volume for self-study Department of Energy has funded X-ray brilliance and coherence began in July, following the theory, to tame the algebraic and reference.” Reviews of Accelerator Science and Technology new quantum-technology 100 times greater than ESRF’s recommendations of the 2020 complexity inherent to multi- Stephen L Adler, IAS, Princeton Volume 10: The Future of Accelerators centres at five national previous storage ring. It is update of the European strategy loop computations. Their new laboratories: Argonne, Berkeley, based on the hybrid multi-bend for particle physics (CERN Courier paper provides further evidence Edited by: Alexander W Chao (SLAC National Accelerator Lab., “This book is a comprehensive introduction to modern quan- Brookhaven, Fermilab and Oak achromat – with seven, July/August 2020 p7). Initiated by that the technique could be USA) & Weiren Chou (Fermi National Accelerator Lab., USA) tum field theory. The topics under consideration would be of Ridge. Each lab will receive a as opposed to two, bending the Large European Laboratory used in the future to perform great interest for every physicist and mathematician who are Beginning with a short article by Chen Ning Yang, this book contains $115 million investment over magnets per cell, reducing the Directors Group, which exists calculations for the LHC that are interested in methods of the quantum physics.” the more personal views, perspectives, and advices from frontier five years plus contributions horizontal emittance (CERN to maximise co-operation in out of the reach of conventional Zentralblatt MATH researchers on the future possibilities of accelerator research and from industrial partners. The Courier December 2018 p17). the planning, preparation and techniques (arXiv:2008.04823). development. 940pp Jul 2020 successful proposals include bids execution of future projects, the 978-981-122-216-0(pbk) US$98 / £85 352pp Sep 2019 to use accelerator technology in study will initially be hosted Laplace vindicated
978-981-122-086-9 US$198 / £175 978-981-120-959-8 US$158 / £140 quantum computing, by using KoelemeijJ at CERN, and carried out in Two centuries ago, Pierre-Simon New Books superconducting radio-frequency collaboration with international Laplace modelled t he effect of cavities to make niobium qubits. partners. Institutes can join t he Moon’s g rav it y on a t hin fluid Earlier this year, such Fermilab by expressing their intent to coating a smooth sphere, and cavities broke the world record collaborate via a Memorandum deduced that continent-sized for qubit coherence, achieving of Understanding. The goal of the pressure waves would periodically stability over a period of seconds study is to evaluate the feasibility sweep across the planet at (Phys. Rev. Applied 13 034032). of both the accelerator and its hundreds of kilometres per hour.
The five labs will also develop physics experiments (CERN Courier T Sakazaki quantum-sensor technology for May/June 2020 p41). CERN’s use in applications including The ion trap used to measure the Daniel Schulte has been appointed dark-matter searches. In June, proton-electron mass ratio. as interim project leader. CERN also launched a quantum- technology initiative (see p47). Proton slimmed down KEK reclaims luminosity record A new precision laser A new record for the highest by Albert Schwarz by Michel Rausch de Traubenberg edited by Swapan Chattopadhyay by S Y Lee edited by Carlos Pérez High-performance collaboration spectroscopy measurement of luminosity at a particle collider (University of California (Strasbourg Univ., CNRS Inst. (Northern Illinois Univ., USA), Gérard (Indiana University, de los Heros (Uppsala On 22 July, CERN and the Square the proton-electron mass ratio has been set by SuperKEKB at Resonant modes can be randomly at Davis, USA) Pluridisciplinaire Hubert Curien, Mourou (École Polytechnique, France), USA) University, Sweden) Kilometer Array (SKA) signed using trapped HD+ ions supports Japan’s KEK laboratory. On 15 June, excited in the atmosphere. France) & Mauricio Valenzuela Vladimir D Shiltsev (Fermi National an agreement to co-operate other recent indications that electron–positron collisions at (Centro de Estudios Científicos Accelerator Lab., USA) & Toshiki Tajima (CECs), Chile) (Univ. of California, Irvine, USA) with European networking the proton is less massive than the 3 km-circumference machine Takatoshi Sakazaki (Kyoto) and data-management previously thought (10.1126/ reached an instantaneous and Kevin Hamilton (Hawaii) AD LY 08 20 04 E International Journal of Modern Physics A (IJMPA) organisations GÉANT and PRACE science.aba0453). In the last few luminosity of 2.22 × 1034 cm–2 s–1 have now analysed 38 years of on the development of high- years, traditional Penning-trap — surpassing the LHC’s record atmospheric data to prove him Modern Physics Letters A (MPLA) performance computing in high- measurements (e.g. Phys. Rev. of 2.14 × 1034 cm–2 s–1 set with correct (J. Atmos. Sci. 2020 77 2519). Particles and Fields ∙ Gravitation ∙ Cosmology ∙ Astrophysics ∙ Nuclear Physics energy physics and astronomy. Lett. 119 033001) have weighed proton–proton collisions in Sakazaki and Hamilton observed Accelerator physics ∙ Quantum Information Analysing the data sets generated in at around 300 parts per 2018. SuperKEKB is an upgrade the ringing of randomly excited by the High-Luminosity LHC trillion (ppt) and three standard of the KEKB B-factory, which global-scale resonant modes • 35 years of publishing since 1986 at CERN and the SKA radio- deviations lighter than the held the luminosity record in precise accord with those telescopes planned for Australia previously accepted mass. The of 2.11 × 1034 cm−2 s−1 for almost hypothesised by Laplace. With • Approximately 600 papers published each year and South Africa will depend new measurement, obtained by 10 years until the LHC edged past periods as short as two hours, • Frequent special issues focusing on latest research upon “exascale” supercomputers, researchers in the Netherlands it. SuperKEKB’s new record was the new excitations complete developments capable of 1018 operations per and France, deployed a pair achieved thanks to a novel “nano- t he e x perimental pict ure first • Feature contributions (Review papers and Brief Reviews) second, which are expected to of narrowly detuned counter- beam” scheme that squeezes the hinted at by the observation of the by world’s leading physicists including Nobel Laureates emerge in the next few years propagating lasers to eliminate vertical height of the beams at the fundamental two-hemisphere (CERN Courier April 2018 p39). error due to the Doppler effect collision point to about 220 nm. mode in the 1980s. Visit our website to enjoy FREE access to selected papers: https://worldscientific.com/worldscinet/ijmpa https://worldscientific.com/worldscinet/mpla CERN COURIER SEPTEMBER/OCTOBER 2020 13
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Reports from the Large Hadron Collider experiments ATLAS The LHC as a photon collider
1200 data ATLAS preliminary γγ → WW –1 ATLAS preliminary data 2017 γγ → ττ √s = 13 TeV, 139 fb 1000 –1 qq → WW peμ > 30 GeV 60 √s = 13 TeV, 14.6 fb uncertainty other qq initiated T 800 non-prompt pp → p(γγ → μμ)p Drell–Yan total uncertainty mll ∉ [70, 105] GeV pp → p(γγ → ee)p 600 ee + μμ , 0.02 < ξ < 0.12 events 40 postfit pp → p(γγ → μμ)p* 400 pp → p(γγ → ee)p* combinatorial bkg. 200
events/0.0025 20
When Compromise is Not an Option. 1.4 1.2 1.0 0 High-Performance Digitizers for 0.8 –0.02 0 0.02 0.04 –0.02 0 0.02 0.04
data/pred. 0.6 A A C C ξAFP – ξll ξAFP – ξll 0 1 234 number of reconstructed tracks, n Big Physics Applications trk Fig. 2. A sample of γ γ → ℓℓ events can be isolated by observing a scattered proton in Fig. 1. To isolate a sample of γγ → WW interactions, events with the AFP spectrometer. Here, the proton energy loss measured in the AFP installed either Digitizers from Teledyne SP Devices utilize patented no additional reconstructed charged-particle tracks in the side (A and C) of the collision point (ξAFP, dimensionless) is shown to agree with that vicinity of the electron–muon pair (n = 0) are selected. predicted from measurements of the lepton pair in the main detector (ξ ). calibration technology, the latest data converters, and trk ℓℓ state-of-the-art FPGAs in order to achieve an unrivaled Protons accelerated by the LHC generate p a i r s – a r e t h e o n l y p a r t i c l e s d e t e c t e d i n side of the collision point, the AFP can a large flux of quasi-real high-energy the vicinity. However, if charged par- detec t protons t hat have been scat tered combination of high resolution and sampling rate. Their photons that can interact to produce ticles arise from nearby proton–proton in photon–photon collisions but which versatility makes them ideal for applications such as particles at the electroweak scale. Using collisions, the clean γγ → W W s i g n a l c a n have nevertheless been focused by the the LHC as a photon collider, the ATLAS be missed. The main background is W LHC’s magnets. Its pioneering results beam position monitoring, Thomson scattering plasma collaboration recently announced a set b o s o n p a i r s pr o d u c e d i n h e a d- o n pr o t o n– so far analyse a standard-candle pro- diagnostics, and more. o f l a n d m a r k r e s u l t s, a m o n g w h i c h i s t h e pr o t o n c ol l i s i o n s w h e r e p a r t i c l e s f r o m t h e c e s s w he re a prot on i s s c at t e re d i n p ho- first observation the photo-production breakup of the protons are not detected ton collisions that produce electron or of W-boson pairs. due to imperfect detector coverage or muon pa i rs (γγ → ℓℓ). For these signals, Supported features include: A s it pr o c e e d s v i a t r i l i n e a r a n d q u a r t i c reconstruction (figure 1). A total of 127 the measured proton energy loss is equal gauge-boson vertices involving two W background events are predicted com- to that predicted from the lepton pairs • Up to 10 GSPS sampling rate with 14 bits resolution b o s o n s a n d e it h e r o n e or t w o p h o t o n s, t h e pared to 307 events observed in data. This measured in the main ATLAS detector pr o d u c t i o n o f a p a i r o f W b o s o n s f r o m t w o signal excess corresponds to a statistical (fi g u r e 2). AT L A S r e p or t e d 180 e v e nt s w ith • Open FPGA for custom real-time signal processing photons (γγ → W W ) t e s t s a l o n g-s t a n d i n g significance of 8.4 standard deviations. a proton having matched kinematics to prediction of the Standard Model (SM). This establishes the existence of light the lepton pair with an expected back- • Multiple form factors including MTCA.4, PXIe, and PCIe This process is extremely rare but pre- t r a n s for m i n g i nt o p a r t i c l e s w it h w e a k- ground of about 20 events. This corre- dicted precisely by electroweak theory, s c a le m a ss e s – a re m a rk a ble a nd pre v i- sponds to a significance exceeding nine • Multi-channel synchronization capabilities such that any observed deviation would ously unobserved phenomenon. s t a n d a r d d e v i a t i o n s for b o t h l e p t o n fl a- • White Rabbit synchronization (MTCA.4 only) suggest that new physics is at play. The Precisely testing SM predictions of vours, establishing the presence of the mea surement re l ies on t he l a rge 139 fb–1 photon collisions requires accurate signal and the successful operation of • Peer-to-peer streaming to GPU (PCIe only) dataset of proton–proton collisions knowledge of the rate protons remain t h e A F P s p e c t r o m e t e r i n h i g h-lu m i n o s it y recorded by ATL AS in LHC Run 2. i nt a c t r e l a t i v e t o t h o s e t h a t br e a k a p a r t. Observing data. The detectors were sufficiently well • Application-specific firmware shortens design time Protons usually remain intact or are This is challenging to predict theoret- γγ → WW and u n d e r s t o o d t o m e a s u r e t h e c r o s s s e c t io n s excited into a higher energy state in ically and probing these rates unam- scattered of these processes. photon collisions, with the products of biguously requires directly detecting protons Observing γγ → WW and scattered any subsequent decay not reaching the the intact protons. The ATLAS Forward in γγ → ℓ ℓ protons in γγ → ℓℓ interactions are innermost components of the ATLAS Proton (AFP) spectrometer is becoming interactions long-awaited milestones in an emerg- detector. In these cases, the electron increasingly indispensable for this task. ing experimental programme studying and muon decaying from the W bosons A m o n g t h e n e w e s t a d d it i o n s t o t h e AT L A S are long- photon collisions. These complement – a n e vent top olog y c hosen to avoid t he e x p e r i m e nt, a n d l o c a t e d a fe w m i l l i m e- awaited recent heavy-ion results where ATLAS s h i g h b a c k g r o u n d for s a m e-fl a v o u r l e p t o n tres from the beam 210 metres either milestones measured muon pairs from photon Learn more on our website www.spdevices.com CERN COURIER SEPTEMBER/OCTOBER 2020 15
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collisions and t he k inemat ic proper t ies γγ → WW and γγ → ℓℓ interactions lay interesting with the increased dataset ψ(2S) and χC, and modifying their feed- maximum positive deviation for λθ (cor- o f l i g ht-b y-l i g ht s c a t t e r i n g – a v e r y r a r e t h e g r o u n d w or k for f ut u r e, m or e d e t a i l e d of Run 3 and t he High-Luminosit y LHC. down fractions into the ground state, J/ψ → μ+μ–, helicity responding to a transverse polarisation) 0.8 process predicted by quantum electro- t e s t s o f t h e S M . F u r t h e r r e s u l t s u s i n g t h e J/ψ. T h i s e ffe c t m a y l e a d t o a v a r i a t i onf of 2σ for 2 < pT < 4 GeV in the helicity ref- dynamics. Interestingly, the latter was A F P s p e c t r o m e t e r c a n i m pr o v e t h e or e t i c a l Further reading the overall polarisation values since dif- erence frame. Interestingly, the corre- also used to search for the axion-like understanding of photon collisions that ATLAS Collab. 2020 ATLAS-CONF-2020-038. ferent charmonium states are expected 0.4 sponding LHCb pp result for prompt J/ψ
p a r t i c l e s pr e d i c t e d b y c e r t a i n e x t e n s i o n s will also benefit future measurements ATLAS Collab. 2020 ATLAS-CONF-2020-041. to be produced with different polarisa- at √(sNN) = 7 TeV instead shows a small
of the SM. of γγ → W W pr o d u c t io n. T h e s e l a n d m a r k ATLAS Collab. 2020 CERN-EP-2020-135. tions. In addition, the recombination of θ but significant longitudinal polarisation.
λ 0 The techniques developed to study e x p e r i m e nt a l fe a t s w i l l o n l y b e c o m e m or e ATLAS Collab. 2020 CERN-EP-2020-138. uncorrelated heavy-quark pairs inside T h e o b s e r v a t i o n o f a s i g n i fic a nt d i ffe r- the QGP gives rise to an extra source of ence between J/ψ polarisation results in CMS J/ψ, which can further modify the overall –0.4 pp and Pb–Pb collisions motivates fur-
polarisation with respect to pp collisions. ALICE, Pb–Pb √s NN = 5.02 TeV, 2.5 < y < 4 ther experimental and theoretical stud- CMS reaffirms exotic nature of the X(3872) The ALICE experiment has recently –0.8 LHCb, pp √s = 7 TeV, 3 < y < 3.5 ies, with the main goal of connecting made t he first measurements of t he J/ψ this observable with the known suppres- Exotic charmonium-like states are a very a similar ratio for the decays involving and ϒ(1S) polarisation in Pb–Pb colli- sion and regeneration mechanisms in CMS 140 fb–1 (13 TeV) 02468 10 12 active field of study at the LHC. These ψ(2 S) i s c o n s i s t e nt w it h u n it y. T h i s i s n o t sions. The data correspond to a centre- p [GeV] heavy-ion collisions. For the rarer ϒ(1S), data T states have atypical properties such as expected from naive “spectator-quark” o f-m a s s e n e r g y √(s ) = 5.02 TeV, and the a bound state of a bottom and an anti- 180 fit NN non-zero electric charges and strong con sider at ion s, ba se d on a si mple t re e- rapidity range 2.5 < y < 4. The measure- Fig. 1. Inclusive J/ψ polarisation parameters as a function of bottom quark, the inclusive polarisation (X(3872), φ) decays that violate isospin symmetry. 140 (X(3872), bkg) level diagram, and assuming X(3872) is ments were carried out in the dimuon trans verse momentum for Pb–Pb collisions at √(s NN) = 5.02 TeV. parameters were found to be compatible The exotic X(3872) charmonium state (bkg, φ) a p u r e c h a r m o n iu m s t a t e. T h e m e a s u r e d decay channel, and results were obtained The results are compared to proton–proton collisions observed by with zero within sizeable uncertainties. discovered by the Belle collaboration 100 (bkg, bkg) ratio also happens to be consistent with i n t w o d i ffe r e nt r e fe r e n c e f r a m e s, h e l ic ity LHCb for prompt J/ψ at √s = 7 TeV (Eur. Phys. J. C 2013 73 2631). A higher precision and momentum-dif- in 2003 displays such isospin-violating the analogous ratio for the B0 → X(3872) and Collins–Soper, each of them with its ferential measurement will be enabled strong decays and has a natural width 60 K0 to B + → X(3872)K+ decays, t houg h t he o w n d e fi n it i o n o f t h e q u a nt i s a t i o n a xis. boosted in the quarkonium rest frame by the ten-fold larger Pb–Pb luminosity candidates/5 MeV of about 1 MeV, which is unexpectedly latter ratio has not yet been measured In the helicity frame, the quarkonium is used in the Collins–Soper frame. The expected in Run 3 of the LHC. 20 narrow for a state with mass very close with high accuracy. The results suggest momentum direction in the labora- J/ψ polarisation parameters, evaluated in – to the D*0 D0 t hreshold. that spectator quarks behave differently tory is chosen, while the bisector of the three p bins covering the range between Further reading 3.80 3.85 3.90 3.95 T Several theoretical interpretations in the B + and B 0 two-body decays into angle formed by the two colliding beams 2 and 10 GeV, are close to zero, but with a ALICE Collab. 2020 arXiv:2005.11128. m(J/ψπ+π–) [GeV] (s) of the internal structure of these char- X(3872) and a light meson. In a recent m on iu m-l i k e s t at e s h a v e b e e n pro p o s e d theoretical paper, former CERN Direc- LHCb 1 to explain their peculiar properties. To of the corresponding rates for decays to Fig. 1. The t or-G e n e r a l L u c i a n o M a i a n i a n d c ol l a b - c h o o s e t h e m o s t a d e q u a t e m o d e l for e a c h X(3872) s h o w d i ffe r e n c e s, h o w e v e r, w h i c h reconstructed orators pointed out that the new CMS LHCb explores 4 state, we must continue studying their may provide a clue to the nature of this invariant mass m e a s u r e m e nt c a n n a t u r a l l y b e e x pl a i n e d –1 properties and improving the determi- exotic charmonium-like state. distribution of by a tetraquark model of X(3872), which dark-sector 10 + – 2 nation of their parameters. As for the Recently the CMS collaboration X(3872) → J/ψπ π d e s c r i b e s t h i s e x o t ic p a r t ic l e a s a b o u n d 0 0
confinement [c τ (X)/mm] X(3872), although it is inconsistent with o b s e r v e d t h e d e c a y B s → X(3872)φ for t h e for Bs → X(3872)φ state of a diquark (charm and up quarks)
10 10–2 the predicted conventional charmonium fi r s t t i m e, w it h a s i g n i fic a n c e e x c e eding candidates. and its anti-diquark. 0 s t a t e s a n d d o e s n o t h a v e a d e fi n it e i s o s pi n, five st a nda rd de v iat ions. The X(3872) is Further studies of X(3872) are now The possibility that dark-matter parti- log + – its production partially resembles that of reconstructed via its decay to J/ψπ π , important in order to gain a deeper cles may interact via an unknown force, LHCb ordinary charmonium states such as ψ(2S) followed by a decay of the J/ψ meson into understanding of its exotic properties felt only feebly by Standard Model (SM) –2 10–3
or χc1(1 P). O n e o f t he w a y s t o e v a lu at e t he a pair of muons, and of the φ meson to a and uncover its mysterious nature. The particles, has motivated substantial 0.3 0.5 1 3 d e g r e e o f s i m i l a r it y b e t w e e n X(3872) a n d pair of c harged kaons (fig ure 1). results may have interesting conse- efforts to search for dark forces. The m(X) [GeV] ψ(2 S) i s t o c o m p a r e t h e i r pr o d u c t io n r a t e s At a simple Feynman-diagram level, q u e n c e s for o u r u n d e r s t a n d i n g o f q u a n- force-carrying particle for such hypoth- i n e x c lu s i v e b -h a d r o n d e c a y s. I n t h e c a s e this decay is a close analogue to the tum chromodynamics. esised interactions is often referred to of ψ(2S), which is a conventional char- B+ → X(3872)K+ a n d B 0 → X(3872)K0 d e c a y s as a dark photon, in analogy with the Fig. 1. 90% ios that exhibit confinement in the dark the searches found evidence for a signal m o n iu m s t a t e, t h e br a n c h i n g f r a c t i o n s o f t h a t h a v e pr e v io u s l y b e e n o b s e r v e d. T h e Further reading ordinary photon that mediates the elec- confidence upper sector, similar to how the strong nuclear and exclusion limits were placed on the 0 + + + – t h e d e c a y s B s → ψ (2S)φ, B → ψ (2S)K , a n d ratio of the branching fractions of this CMS Collab. 2020 arXiv:2005.04764. tromagnetic interaction. limits on the kinetic force confines SM quarks, would pro- X → μ μ cross sections, each with min- 0 0 0 + B → ψ (2S)K , are approximately equal to n e w B s d e c a y t o t h a t o f t h e B d e c a y i s s i g- L Maiani, A D Polosa and V Riquer 2020 In the minimal dark-photon scenario, mixing strength duce a high multiplicity of light hidden imal model dependence. each other. Recent CMS measurements n i fic a nt l y b e l o w u n it y a t 0.48 ± 0.10, w h i l e arXiv:2005.08764. the dark photon does not couple directly between photons hadrons from showering processes in a For many types of dark-sector mod- to SM particles; however, quantum- and composite similar way to jet production in the SM. els, these limits are the most stringent ALICE mechanical mixing between the photon hidden-valley These hidden hadrons would typically to date. This is especially true for the J/ψ polarisation Polarisation however, and measurements at the LHC I n p p c ol l i s i o n s, p ol a r i s a t i o n h a s b e e n and dark-photon fields can generate a bosons, X (colour decay displaced from the proton–pro- H V s c e n a r io (s e e fi g u r e), for w h ic h L HC b studies pose significant further challenges. mainly used to investigate the J/ψ pro- small interaction, providing a portal scale), for a scenario ton collision, thus failing the criteria has placed the first such constraints on differs in lead represent ALICE measures quarkonia spin ori- duction mechanism. Reproducing the through which dark photons may be that exhibits employed in previous dark-photon physically relevant HV mixing strengths entations with respect to a chosen axis small values of polarisation parameter produced and through which they might confinement, as a searches to suppress backgrounds due in this mass range. a valuable via a measurement of the anisotropy in o b s e r ve d at t he LHC i s a c h a l le nge for decay into v isible final states. function of mass and to heavy-flavour quarks. Therefore, it These results demonstrate the unique collisions λθ tool for the the angular distribution of the decay m a n y t h e or e t i c a l m o d e l s. Unt i l r e c e nt l y, While the minimal dark-photon model proper decay length. is desirable to perform experimental sensitivity of the LHCb experiment to Q u a r k o n i a, t h e b o u n d s t a t e s o f c h a r m a n d study of the products. The angular distribution is n o c or r e s p o n d i n g r e s u l t s w e r e a v a i l a bl e is both compelling and simple, it is not The grey box was searches for dark sectors that are less dark sectors. Looking forward to Run 3, anti-charm or bottom and anti-bottom properties of parametrised in terms of the polarisa- for nucleus–nucleus collisions, and in the only viable dark-sector scenario. vetoed due to a large model dependent, by not focusing solely the trigger will be upgraded, greatly q u a r k s, a r e a n i m p or t a nt t o ol t o t e s t o u r tion parameters, , and , where this domain polarisation studies rep- quark–gluon λθ λφ λθφ θ Many other well-motivated dark-sector doubly misidentified on the minimal dark-photon scenario. increasing the efficiency to low-mass k n o w l e d g e o f q u a nt u m c h r o m o d y n a m i c s and φ a r e t h e p ol a r a n d a z i m ut h a l e m i s- resent a valuable tool for the study of background. plasma models exist, and some of these would KS Using its Run-2 data sample, LHCb dark sectors, and the luminosity will be (QCD). At t he LHC, t he study of quarko- sion angles. If all of them are null, no the properties of quark–gluon plasma have avoided detection in all previous recently performed searches for both higher. Taken together, these improve-
nia polarisations offers a valuable new polarisation is present, whereas (λθ = 1, (Q GP). T h e for m a t io n o f t h i s d e c o n fi n e d, experimental searches. Fully exploring short-lived and long-lived exotic bos- ments will further expand LHCb’s
window onto how heavy quarks bind λφ = 0, λθφ = 0) a nd (λθ = –1, λφ = 0, λθφ = 0) strongly interacting medium impacts the space of dark sectors is vital given ons that decay into the dimuon final world-leading dark-sector programme. together in such states. Understanding indicate a polarisation of the spin in the differently on the various quarkonium the lack of signals observed thus far in state. These searches explored the quarkonium polarisation has already transverse and longitudinal directions, resonances, inducing a larger suppres- the simplest scenarios. For example, invariant mass range from near the Further reading s proven to be difficult at lower energies, respectively. sion on the less bound excited states so-called hidden-valley (HV) scenar- dimuon threshold up to 60 GeV. None of LHCb Collab. 2020 arXiv:2007.03923.
16 CERN COURIER SEPTEMBER/OCTOBER 2020 CERN COURIER SEPTEMBER/OCTOBER 2020 17
CCSepOct20_EnergyFrontiers_v3.indd 16 09/09/2020 10:46 CCSepOct20_EnergyFrontiers_v3.indd 17 09/09/2020 10:47 CERNCOURIER www. V o l u m e 6 0 N u m b e r 5 S e p t e m b e r / O c t o b e r 2 0 2 0 CERNCOURIER.COM CERNCOURIER.COM ADVERTISING FEATURE FIELD EPICS integration of the ESS NOTES accelerator cryoplant Reports from events, conferences and meetings InternatIonal ConferenCe of HIgH energy PHysICs
The European Spallation Source (ESS) will be the world’s most powerful pulsed neutron source to provide a means for ICHEP’s online success multidisciplinary research in areas such
as materials science, life sciences, energy, ICHEP 2020 Originally set to take place in Prague, the environmental technology, cultural heritage and fundamental physics. ESS plans the first International Conference of High Energy experiments for 2023 with the commencement Physics (ICHEP) took place virtually from 28 July to 6 August. Running a major of the user programme. Ivana Mustać Kostevc describes how it was possible to adapt an biennial meeting virtually was always industrial solution for a cryogenic plant going to be extremely difficult, but the (cryoplant) to the custom requirements of the local organisers rose to the challenge by ESS EPICS environment. embracing technologies such as Zoom and YouTube. To allow global partici- The proton linear accelerator of ESS will pation, the conference was spread over contain three cryogenic refrigeration/ eight days rather than the usual six, with liquefaction plants and an extensive cryogenic presentations compressed into five-hour distribution system. The accelerator cryoplant slots that were streamed twice: first as (ACCP), which is currently in the phase of a live “premiere” and later as recorded commissioning, is the largest of the ESS “r e pl a y” s e s s io n s, for t h e b e n e fit o f p ar- cryoplants. Its primary purpose is to cool the t icipants in different t ime zones. Building bridges A photo-collage of ICHEP delegates mapped to the Charles Bridge – a Prague landmark superconducting RF cavities to a temperature Example of a cryoplant, courtesy of Linde Kryotechnik AG. This was the first ICHEP meeting that has facilitated trade between eastern and western Europe since the 15th century. of 2 K via saturated He-II baths through since the publication of the update of the several cryomodules. Apart from that, a technical safety requirements and For the screen design we used templates, European strategy for particle physics, top quark), indicating the universality of by ATLAS and CMS were truly impressive forced flow of 4.5 K helium is supplied in a deterministic sequence programmes, is wherever possible. which presented an ambitious vision for the Standard-Model Higgs boson as the and we should not forget that it is still second circuit to cool the RF power couplers, carried out by a Siemens Step 7- 400 PLC. the future of CERN. Though VIP-guest mechanism through which all Standard relatively early in the LHC programme. and a third circuit provides helium at around All relevant control points are collected and A large and complex system like a cryoplant Peter Gabriel – rock star and human- Model particles acquire mass. These are In parallel, direct searches for new phe- 40 K to cool the thermal radiation shields. processed by the PLC and distributed and is always customised by an experienced rights advocate – may not have been highly non-trivial statements. nomena, such as supersymmetry and the The ACCP provides cooling for all three of exposed to the operator via a dedicated IOC supplier. However, when considering an aware of this when delivering his open- ATLAS also presented a combined “unexpected”, continues apace. Results these circuits. running EPICS. The interface between the PLC extensive facility such as ESS, all systems ing remarks, his urging that delegates measurement of the Higgs signal from direct searches at the energy fron- and the IOC is implemented through the s7plc must be integrated into the central control speak up for science and engage with strength, which describes a common tier were covered in numerous parallel The two main ACCP subsystems are the warm EPICS driver, which is based on the Siemens system similarly – employing the same politicians resonated with the physicists scaling of the expected Higgs-boson session presentations. The current status compressor station and the coldbox. The send/receive protocol. technologies that are used for other virtually present. yields in all processes, of 1.06 ± 0.07. In was summarised succinctly by Paris Sph- warm compressor station consists of three subsystems. The latter is vital for operators M a n y s c i e nt i fic h i g h l i g ht s w e r e c o v erd this measurement, the experimental and icas (Athens) in his conference summary oil-lubricated compressor skids with a bulk oil The EPICS database covers the input and and becomes a necessity when considering at ICHEP and it is only possible to scratch theoretical uncertainties are now roughly talk: “Looked for a lot of possible new removal system and oil and gas filters, a final output of all relevant control points and maintenance throughout the system’s the surface here. The results from all four equal, emphasising the ever-increasing things. Nothing has turned up yet. Still oil removal system and a gas management additional functionalities such as the lifecycle. In ESS’s case, Cosylab put particular major LHC experiments were particularly importance of theoretical developments looking intensively.” panel consisting of valves and pipe terminals communication logic with the PLC, recovery emphasis on managing device configuration impressive and the collective progress in in keeping up with the experimental pro- for the process control. There is a single of set-points after a system shut down and in the cryoplant as the latter changes during understanding the properties of neutrinos gress; a feature that will ultimately deter- Flavour physics coldbox with a number of heat exchangers, locking access to a single workstation. development and testing. The final product shows no sign of slowing down. mine the precision that will be reached Over the last few years, a number of expansion turbines, a cold compressor Data from the PLC to the IOC is stored and was the functioning “missing link” between system, adsorbers, filters, electrical heaters recovered by the PLC while IOC setpoints the industrial solution of the cryoplant by the LHC and high-luminosity LHC deviations from theoretical predictions and other equipment. are stored on the IOC. The EPICS database manufacturer and the custom requirements Higgs physics (HL-LHC) Higgs physics programmes. have been observed in B-meson decays to provides the option to either initialize all data of ESS’s control system – the EPICS AT L A S a nd C M S pre s e nte d t he fi r s t e v i- More generally, the precision we are final states with leptons. Discrepancies Many manual and remote valves will be to their last values on the IOC, or to copy their environment. dence for the decay of the Higgs boson seeing from the ATLAS and CMS Run 2 have been observed in ratios of decays installed for different purposes, for example respective readbacks from the PLC. into a pair of muons (two and three proton–proton data is truly impressive, to different lepton species, and in the ABOUT THE AUTHOR to isolate specific loops, to protect the system standard deviations, respectively, see p7). and an exciting indication of what is to angular distributions of decay products Ivana Mustać Kostevc started working Combined, the results provide strong evi- come as the integrated luminosity accu- (CERN Courier May/June 2020 p10). Taken against loss of oil or helium and safety valves Since the ACCP is a large and complicated at Cosylab in 2015. She holds a PhD to protect the system against overpressure. system, we structured its graphical user in physics with a topic in elementary dence for the coupling of the Higgs boson mulated by the experiments ramps up, alone, each of these discrepancies are not Measuring points necessary for operation interface hierarchically. At the top level, particle physics. She is a senior to the muon, with the strength of the and then ramps up again in the HL-LHC p a r t ic u l a rl y s i g n i fic a nt, b ut c ol l e c t i v e l y team leader in the Scientific Services The collective and protection of the equipment include a process diagram of the whole system department and an expert in designing coupling consistent with that predicted era. One interesting new example was they may be telling us something new points for helium mass flow and water flow, provides a quick overview of the cryoplant’s EPICS-based control systems. Kostevc in the Standard Model. Prior to these the first observation of WW production progress in about nature. At ICHEP 2020, the LHCb was the technical lead on the EPICS position of all control valves, limit switches most critical measuring points. Due to the integration project for the ESS ACCP. new results, the Higgs had only been from photon–photon collisions, where understanding experiment presented their recently for manual valves, oil-level, oil and helium, complexity of the ACCP control system, we Her hobbies are dancing and cycling. observed to couple to the much heavier the photons are radiated from the incom- the properties published results on the angular analy- e-mail [email protected] 0 *0 + – impurity, helium, water, and oil temperatures. automated as much as possible. Appropriate third-generation fermions and the W and ing proton beams (see p15). This is a neat of neutrinos sis in B → K μ μ . The overall picture These measurements, and control over the Python scripts parse the PLC variables and Z gauge bosons. The measurements also measurement that demonstrates the remains unchanged. The full analysis devices mentioned above, are exposed to the all relevant information to create the EPICS provide further evidence for the linear- breadth of physics accessible at the LHC. shows no of the LHCb Run-2 data set, including operators by the ESS control system. database and configuration files for services ity of the Higgs coupling, now over four Overall, the range and Standard Model sign of updated measurements of the relative s such as the alarm handler and archiving Cosylab, Control System Laboratory orders of magnitude (from the muon to measurements presented at ICHEP 2020 slowing down rates of the muon and electron decay Supervision of all functions of the ACCP service. The latter ensures that all services Tel +386 1 477 66 76 control system, including substantial are up to date with the EPICS database. Email [email protected] | Web www.cosylab.com CERN COURIER SEPTEMBER/OCTOBER 2020 19
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FIELD NOTES
modes (RK and RK*), is eagerly awaited. The search Updates were presented by the NOvA Virtual success The search for rare kaon decays con- for rare experiment in the USA and the T2K A vast range of high-qualify scientific tinues to attract interest. One of the most kaon decays experiment in Japan. Both experiments research was covered in the 800 parallel impressive results presented at ICHEP favour the normal-ordering hypothe- session presentations and summarised was the recent observation by NA62 of continues sis, although not definitively, and there in the 44 plenary talks at ICHEP 2020. the extremely rare kaon decay, K+ → π+ νν–. to attract is currently a slight tension between The quality of the presentations was Occurring only once in every 10 billion interest the CP violation results from the two high, and speakers coped well with the SDD decays, this is an incredibly challenging experiments. It is worth noting that challenge of pre-recording talks. The measurement and the new NA62 result is the combined interpretation of the two “replay” sessions worked extremely Silicon Drift Detectors the first statistically significant obser- experiments is quite complex. The NOvA well too – an innovation that is likely to vation of this decay, based on just 17 and T2K collaborations are working on a persist in the post-COVID world. About events (see p9). Whilst the observed rate combined analysis to clarify the situation. 3000 people registered for the meeting, for Science at the Speed of Light is consistent with the Standard Model There were also a number of pres- which is more than double the previous expectation, its observation opens up entations on the next generation of two events. It was particularly pleasing Technologically Advanced Silicon Drift Detectors a new future avenue for exploring the long-baseline neutrino oscillation to learn that almost 2500 connected to possible effects of new physics. experiments, DUNE in the US and the parallel sessions. Hyper-Kamiokande in Japan, which Despite the many successes, we all Exceptional Rise Time — Rise times <25 ns Neutrino physics aim to make the definitive discovery missed the opportunity to meet col- Neutrino physics continues to be one of of CP violation in the neutrino sector. leagues in person; it is often the informal Outstanding Throughput — Output count rates >5 Mcps the most active areas of research in par- In the context of DUNE, the progress d i s c u s s i o n s o v e r c o ffe e or i n r e s t a u r a nt s ticle physics (CERN Courier July/August with liquid-argon time-projec- and bars that generate new ideas and, Superior Energy Resolution — Energy resolution <230 eV at 3 Mcps (OCR) 2020 p32), so it was not surprising that tion-chamber (LArTPC) detector tech- importantly, lead to new collaborations. the neutrino parallel sessions were the nology is impressive. It was particularly Whilst virtual conferences are likely Unique Sensor Thickness — Thickness available 0.5 mm, 1.0 mm and 2.0 mm best attended of the conference. This pleasing to see a number of physics to remain a feature in the post- is a particularly interesting time, with results from MicroBooNE at Fermilab, COVID world, they will not replace long-baseline neutrino oscillation and the single-phase DUNE detector in-person events. experiments becoming sensitive to the prototype at CERN, that are based on The VORTEX® range Silicon Drift Detectors, available with a selection of configurations including neutrino mass ordering, and beginning the automatic reconstruction of LArTPC Mark Thomson STFC and the University Sensor Thickness — 0.5, 1.0 and 2.0 mm to provide constraints on CP violation. images – a longstanding challenge. of Cambridge. Active Areas — 50, 65 and 100 mm2 NeutriNo 2020 Probe Lengths — From 60 to over 600 mm Neutrino 2020 zooms into virtual reality
Sensor Arrays and Designs — Single, Multiple, Planar, Focused Tutto/Fermilab M Del More than 4000 people from every conti- Environments — Air, vacuum, UHV and He nent, including Antarctica, participated from 22 June to 2 July in the XXIX Inter- Number of Sensors — Single VORTEX® EX and EM SDD national Conference on Neutrino Phys- ics and Astrophysics, which was hosted — Three VORTEX® ME-3 SDD online by Fermilab and the University of Minnesota. Originally planned as a — Four VORTEX® ME-4 SDD five-day in-person June meeting at a large hotel in Chicago city centre, the — Seven VORTEX® ME-7 SDD organisers quickly pivoted in March, due to COVID-19, to an online programme Customization — Contact [email protected] with eight half days over two weeks, four poster sessions with both web-based and virtual-reality displays, and the use of the Slack platform for speaker questions and ongoing discussions. A highlight of the conference was the first observation of solar CNO neutri- nos by the Borexino collaboration, which operates a 280 tonne liquid-scintillator of CNO and 210Bi neutrinos. “The quest Neutrino 2020 was the report from the Gerda collab- detector in Italy’s Gran Sasso Laboratory. for CNO is turned into the quest for 210Bi avatars oration on the search for neutrino-less Dominant in stars more than 1.3 times the through 210Po,” he emphasised. “With The conference’s double beta decay. If observed, this pro- mass of the Sun, the CNO cycle accounts this outcome, Borexino has completely poster session took cess would confirm the long-suspected for about 1% of the Sun’s energy and unravelled the two processes power- place in virtual Majorana rather than Dirac-fermion generates a difficult-to-detect neutrino ing the Sun – the pp chain and the CNO reality. nature of neutrinos – a beyond the flux similar to backgrounds due to decays cycle.” The final data analysis yielded Standard Model feature with intriguing in the detector of 210Bi and its daughter a 5.1σ statistic against a hypothesis of implications for why the neutrino mass nucleus 210Po. Gioacchino Ranucci (INFN, no CNO neutrinos, and a CNO flux at the is so small. Since Neutrino 2018, Gerda +2.9 8 –2 –1 M i l a n o) e x pl a i n e d t h a t t h e s p e c t r a l fit t o Earth of 7.0–1.9 × 10 cm s (see p11). has nearly doubled its Phase 2 exposure s Hitachi High-Tech Science America, Inc. www.hitachi-hightech.com/hhs-us/ the observed data returns only the sum Another highlight from Gran Sasso and added a liquid-argon veto and a 21770 Nordhoff St., Chatsworth, CA 91311 Email: [email protected] Tel: +1-818-280-0745 CERN COURIER SEPTEMBER/OCTOBER 2020 21
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FIELD NOTES HIGH PRECISION POWER SUPPLIES
E ACTLY. new detector string. The now complete A highlight of muon disappearance determined by the in-person conference, the virtual real- HIGH VOLTAGE. Phase 2 result is a 90% confidence level the conference now completed long-baseline MINOS/ ity (VR) poster presentation was novel 26 half-life of > 1.8 × 10 years according w a s t he fi r st MINOS+ collaboration. These limits are and unique. Marco Del Tutto (Fermilab) to a frequentist analysis, or > 1.4 × 1026 in tension with the appearance data from created multiple virtual “rooms” for observation years, according to a Bayesian analysis both LSND and MiniBooNE when ana- five posters each, along with additional with additional prior assumptions. Talks of solar CNO lysed as ev idence for sterile neut rinos. rooms for topical discussions, sightsee- describing a half-dozen other double-be- neutrinos Two talks described the world’s i n g i n C h i c a g o a n d v i s it i n g Fe r m i l a b. T h e ta-decay experiments displayed the high 200 km-scale neutrino-oscillation most enabling feature of the VR was that OUT NOW level of interest in t his field. e x p e r i m e nt s, NO vA a n d T 2 K . T h e d e g e n- the software facilitated dialogue between eracy of mass difference, mixing angle, participants whose avatars could move Sterile neutrinos hierarchy and possible CP violation around the space and speak with one Searches for additional “sterile” neu- make interpretation of these experi- another. For example, if a group of ava- WITH ONBOARD trinos with no Standard Model gauge ments’ results quite complex. Inter- tars clustered around a poster, the par- interactions were also featured. Taka- estingly, there is mild tension, albeit ticipants could discuss the poster as a sumi Maruyama (KEK) described the only at the 1σ level, between the NOvA group. The VR feature attracted 3409 par- 2 PYTHON SCRIPTING liquid-scintillator JSNS experiment as and T2K results regarding leptonic CP ticipants. The VR was also supplemented a direct test of the controversial LSND conservation and the neutrino mass by two-minute videos from presenters, experiment result, first reported about hierarchy. The two collaborations are w h ic h e n a ble d 5800 Yo uT ub e v ie w s a n d 25 years ago. JSNS2 c ol l e c t e d it s fi r s t d a t a now working together on a combined 60,600 web displays. during the three weeks before Neutrino analysis. Several talks discussed future 2020. Adrien Hourlier (MIT) reported on initiatives. Lia Merminga (Fermilab) Exciting physics the now complete analysis of data from r e p or t e d o n L BN F a n d PI P-II, w h i c h w i l l In the closing remarks, the organis- MiniBooNE that was collected during result in a new neutrino beam from Fer- ers acknowledged the challenges of an the past 17 years. Combining neutrino milab to the Sanford Laboratory in South online conference, but also emphasised and anti-neutrino modes, MiniBooNE D a k o t a for t h e DU N E e x p e r i m e nt. C o m- the strengths of this novel approach. reports a 4.8σ excess. Hourlier presented bined, these two projects will result in a The exciting physics of Neutrino 2020 soon-to-be published detailed distribu- beam power of 2.4 MW, more than three w as made av a i lable to a n e x tensive a nd tions that the collaboration hopes “will times the intensity of the current NuMI diverse audience, including many sci- guide theorists to explain our data”. beam. Michael Mooney (Colorado State) entists who would not have been able to Minerba Betancourt (Fermilab) then reported on the enormous progress of the attend an in-person conference because described the Fermilab Short-Baseline DUNE project with two successful pro- of funding, visas, family concerns or Neutrino (SBN) programme, which will totype detectors operating at CERN and other issues. About 60% of participants use three detectors to obtain a defini- pre-excavation work progressing at San- were students or post-docs and the tive result on neutrino oscillations for ford Laboratory. Complementary to the conference reached participants from an LSND and MiniBooNE-like ratio l iq u id-a r gon t e c h nolo g y o f DU N E i s t he 67 countries. The Slack discussions and of oscillation distance to energy of recently approved Hyper-Kamiokande posts on social media indicated wide- ~1 m/MeV. The beam neutrino energy water-Cherenkov detector, which was spread praise that the online format peaks at 700 MeV. A new liquid-argon described by Masaki Ishitsuka (Tokyo worked as well as it did. Some aspects NEW n e a r d e t e c t or (SBN D) w i l l b e pl a c e d 1 10 m Un i v e r s it y o f S c i e n c e). Hy p e r-K w i l l h a v e of Neutrino 2020 may well affect the from the target. The existing MicroBooNE a total mass of 260 kilotonne and 8.4 planning and organisation of future i s l o c a t e d a t 470 m a n d t h e IC A RUS D e t e c- times the fiducial volume of the current in-person and online conferences. EDIT your python script directly on browser or locally with t or, m o v e d f r o m G r a n S a s s o, i s i n s t a l l e d Super-Kamiokande detector. access to all hardware parameters at 600 m. Thomas Carroll (Wisconsin) While much of Neutrino 2020 was Steve Brice and Sam Zeller Fermilab, and reported on sterile-neutrino limits by modelled after the usual features of an Marvin Marshak University of Minnesota. UPLOAD and start the script directly on iCS capable device Ter ascale summer school International per day. Active moderation was key, with appeal students typing questions in the chat CREATE your own visualisation easily in HTML / Javascript / CSS Terascale summer Forced online by box, and the moderator interrupting school goes global the pandemic, the the lecturer when appropriate to give summer school the participants a chance to speak up. THOUSANDS OF APPLICATIONS POSSIBLE drew particularly This format conferred upon less brash Data logging, event driven voltage channel control, testing, external control of voltage (by temperature changes), block rampup. In a new venture by physicists at DESY, high participation participants a more comfortable way to Start easily with the iseg datalogger example, which stores measured values directly on USB flash drive. the first Terascale Summer School took from Cuba, Egypt, ask questions, several students noted. place online from 23 July to 12 August, India, Malaysia and When one brave pioneer had broken the Download the latest version from: www.iseg-hv.com/ics providing more than 160 undergradu- Russia. ice, queries flowed every few minutes – a ate students from more than 30 coun- r e s o n a n c e e ffe c t c h a r a c t e r i s e d b y a l i v e ly, runs on: MMS / Mpod multichannel Low and High Voltage tries with an engaging introduction to stimulating and relaxed atmosphere that supplies with CC24 Controller card SHR labratory High Voltage the world of particle and astroparticle boosted concentration levels. iCSmini2 Source-Measure-Unit physics. Following a wide-ranging three With its global reach and breathing controller box weeks of teaching, an impromptu fort- space for students to explore concepts night-long online tutorial, which only independently, Terascale 2020’s compact concluded yesterday, focused on strong As the school had been forced online online format may merit consideration interactions and Monte Carlo techniques, due to the ongoing pandemic, the organ- during less extraordinary times too. allowing students to deepen their knowl- isers settled upon a reduced programme edge through practical exercises. with just one or two 45 minutes lectures Olaf Behnke DESY Hamburg.
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FEATURE MULTI-QUARK STATES Got radiation? TETRAQUARKS BACK See what you’ve been missing IN THE SPOTLIGHT
A hidden-double-charm tetraquark D Dominguez/CERN observed recently by the LHCb collaboration has reinvigorated the debate over whether tetraquarks are loosely bound pairs of mesons or tightly bound pairs of diquarks.
he existence of particles with fractional charges and fractional baryon numbers was a hard sell in 1964 Twhen Gell-Mann and Zweig independently proposed the quark model. Physicists remained sceptical until the discovery of the J/ψ meson 10 years later. Heavier than any- Photo courtesy of EUROfusion. Website: www.euro-fusion.org thing previously seen and extremely narrow, with a width of just 0.1 MeV and a mass of 3097 MeV, the J/ψ pointed to the existence of a new quark with its own quantum num- Imaging in radiation environments just got easier b e r. T h i s c o n fi r m e d G l a s h o w, I l io p o u lo s a n d M a i a n i’s 1970 hypothesis, which they cooked up to explain peculiarities in rare kaon decays. Any doubt as to the existence of a With superior capabilities for operating in radiation environments, the MegaRAD cameras provide charm–anticharm system was eliminated by observing narrow excitations of the J/ψ, which lined up as expected excellent image quality well beyond dose limitations of conventional cameras, and are well suited in non-relativistic quantum mechanics. The spectrum of for radiation hardened imaging applications charmonium mesons soon became populated by states with widths up to hundreds of MeV as their masses surpassed the threshold for decaying to a pair of “open-charm” mesons with a single charm quark each. Diquark dilemma An artist’s impression of a hidden-double-charm tetraquark. Hadron spectroscopy continues to be a rich area of fun- In the pictured model, a pair of colour-charged diquarks are bound together by damental exploration today, with results from collider the exchange of gluons. experiments over the past two decades revealing the exist- ence of multi-quark states more exotic than the familiar (qqqqq–) and hexaquarks (qqqq––qq–– or qqqqqq) were all sug- mesons and baryons (CERN Courier April 2017 p31). The LHCb gested. In the early 1970s, a deepening understanding of experiment at CERN is at the forefront of this work. Now, the dynamics of strong interactions brought about by QCD a structure in the J/ψ-pair mass spectrum consistent with only furthered the motivation for seeking new multi-quark MegaRAD3 produce color MegaRAD10 produce color KiloRAD PTZ radiation a tetraquark state made up of two charm quarks and two states. QCD not only predicted attractive forces between or monochrome video up to or monochrome video up to resistant camera with charm antiquarks has been observed by the collabora- a quark and an antiquark, and between three quarks, but 6 7 3 x 10 rads total dose 1 x 10 rads total dose Pan/Tilt/Zoom tion. With doubly hidden charm, the new cccc— state is the also between two quarks. most significant evidence so far for the existence of tightly The attraction between two quarks can easily be proven In the United States: International: bound tetraquarks composed of a pair of colour-charged when they are close together and the strong coupling con- THE AUTHORS For customer service, call 1-800-888-8761 For customer service, call [01] 315-451-9410 “d iq u a r k s”, a n d s h e d s l i g ht o n a d i ffic u lt-t o-m o d e l r e g i me stant is small enough to allow perturbative calculations. Marco Pappagallo To fax an order, use 1-315-451-9421 To fax an order, use [01] 315-451-9421 of quantum chromodynamics (QCD). Similar interactions also likely occur in the non-pertur- bative regime. Such systems, known as diquarks, have INFN and University Email: [email protected] Email: [email protected] of Bari, Liupan An Multi-quark states the colour charge of an antiquark. (For example, red and INFN Sezione di Gell-Mann and Zweig both acknowledged that the sym- blue combine to make an anti-green diquark.) As coloured Firenze and metries which led to the quark hypothesis allowed for objects, they can be confined in hadrons by partnering Tomasz Find out more at thermofisher.com/cidtec m or e c o m pl ic at e d q u a r k c o n fi g u r at io n s t h a n ju s t m e s ons with other coloured constituents. A diquark can attract a Skwarnicki (qq–) and baryons (qqq). Tetraquarks (qq–q–q), pentaquarks quark to create a simple baryon. Alternatively, a diquark Syracuse University.
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FEATURE MULTI-QUARK STATES FEATURE MULTI-QUARK STATES LHCb Collaboration Four muons LHCb Collaboration Bucking the trend A J/ψ-pair Yukawa-style bindings cannot, however, explain a large LHCb data candidate event in number of broader tetraquark-like structures with hidden 200 total fit the LHCb detector, charm, with widths of hundreds of MeV, which are not resonance in which both near any hadron–hadron threshold. Such states include threshold BW1 160 threshold BW2 mesons decayed the charged Z (4430) observed by Belle in 2008 and later c DPS into a pair of confirmed by LHCb in 2014, and a family of states that NRSPS muons (green decay to a J/ψ φ fi n a l s t at e, i n c lud i n g X(4 1 40) a n d X(4 274), 120 DPS+NRSPS lines). LHCb w h ic h w e r e o b s e r v e d b y t h e C DF c ol l a b or at io n at Fe r m i l a b observed a i n 2009 a nd l ater by C M S a nd LHCb at CER N. These st ates 80 resonance in the could be either manifestations of diquark interactions or invariant mass of k i n e m at ic e ffe c t s n e a r t h e f a l l-a p a r t t h r e s h old. No s ingle such events, which simple model can account for all of them. 40 weighted candidates / (28 MeV) is indicative of a Reaching states with hidden double charm (cccc—) now hidden-double- promises new insights into multi-quark dynamics, as 0 charm tetraquark. all the quarks are non-relativistic. Furthermore, there 7000 8000 9000 is no known mechanism for two charmonium mesons to Mdi-J/ψ [MeV] be loosely bound, according to a molecular model, as no l i g ht v a le n c e q u a r k s a r e a v a i l a ble t o b e e x c h a n g e d. C o m- pact diquark-type tetraquarks have been predicted for tures also appear in the invariant mass spectra of other Di-J/ψ bump The such quark combinations, but it is not clear whether they charmonium or doubly charmed baryon pairs. X(6900) structure and an antidiquark can attract each other to create a Experiments to the fore might lead to experimentally detectable signatures – the The first LHCb upgrade is currently in progress and data (solid red curve) tetraquark. As a result of their direct colour couplings, Molecular tetraquark proposals were fuelled in 2003 by tetraquarks could be too broad or their production rate too taking will recommence at the beginning of LHC Run 3 observed in the such compact tetraquarks can have binding energies of the unexpected discovery by the Belle collaboration, at small. While collisions at the LHC provide enough energy to in 2022, with a second upgrade phase planned to collect a J/ψ-pair mass several hundreds of MeV. the KEKB electron–positron collider in Tsukuba, Japan, of simultaneously produce pairs of charm–anticharm quark muc h l a r g e r d at a s e t b y 2030. T h e AT L A S a n d C M S e x p e r- spectrum. Compact two-diquark tetraquarks stand in stark con- a new narrow state, right at the sum of the masses of a combinations, getting them close enough together to form iments have highly performing muon detectors too, and trast to the alternative “molecular” model for tetraquarks, charmed-meson pair. Unlike other charmonium states near diquarks is a tall order. Additionally, while observations c o u ld a l s o m a k e s i g n i fic a nt c o nt r i b ut io n s t o t h e s t ud y o fthe
which was named by loose analogy with the exchange of its mass, the state is surprisingly narrow, with a width of of beauty-charm mesons such as Bc and doubly charmed n e w X(6900) s t r uc t u r e, w it h b o t h e x i s t i n g a n d f ut u r e d at a.
electrons between atoms in molecules. In this picture, t he order of just 1 MeV. Or ig i na l ly na med X(3872), it is now baryons such as Ξcc showed that LHCb has reached the A key contribution may also be made by Belle’s successor,
the tetraquark is arranged as a pair of mesons that attract conventionally referred to as χ c1(3872), r e fle c t i n g it s n at u re sensitivity to detect the interactions of two heavy quarks, Belle II, currently in its start-up phase, which observes each other by exchanging colour-neutral objects, such as as a possible triplet P-wave state with hidden charm and it was unclear until recently if the interactions of diquark- electron–positron collisions at the SuperKEKB collider at light mesons and glueballs – an idea first proposed in 1935 one unit of total angular momentum. Despite subsequent model tetraquarks could be detected. The observation, energies above the observed J/ψ-pair mass structure. It is by Hideki Yukawa, in the context of interactions between results from collider experiments around the world, there is repor ted i n July, by LHCb, of a h ig h ly sig n i fica nt J/ψ-pair unclear, however, if the collision energy, luminosity and nucleons. Such exchanges only provide a binding energy no consensus about its exact nature, as it variously exhibits mass structure is therefore an exciting moment for the electromagnetic production cross sections will be high of a few MeV per nucleon. features of simple charmonium or a loosely bound molecule. study of multi-quark dynamics. enough to achieve the required sensitivity. Molecular tetraquarks are therefore expected to be only Stronger evidence for the loose meson–meson binding of Re s e a rc h i s a l r e a d y m o v i n g for w a rd q u ic k l y, w it h f u r t h e r loosely bound, with masses near the sum of the masses of mu lt i-q u a r k s t at e s w a s pr o v id e d b y o b s e r v at io n s i n 2013 o f Introducing the X(6900) evidence for diquark tetraquarks coming from an even
their constituent mesons, however they could have rather a hidden-charm tetraquark candidate Zc(3900) by the BES Exploiting the full data set collected from 2011 to 2018, LHCb more recent discovery by LHCb of two “X(2900)” states narrow widths if their mass lies below the “fall-apart” III collaboration at the BEPC II electron–positron collider investigated the J/ψ-pair invariant mass spectrum, where with widths between 57 and 110 MeV. As they decay to a threshold. As such states are most likely to be created in Beijing, China, and by Belle, and of the Z (4020), also by J/ψ meson candidates are reconstructed from the dimuon D+K– fi n a l s t at e, t h e y a r e b o t h o p e n l y c h a r m i n g a n d openly c –– without angular momentum between the mesons, the BES III. Since they have electrically charged forms, they decay mode. A narrow peaking structure at 6900 MeV and s t r a n g e. T h e i r m o s t l i k e l y c o m p o s it io n i s t h at o f a (c s)(ud) spin-parity combinations available to them are highly cannot be counted as charmonium states. They are both a broader structure at approximately twice the J/ψ mass d iq u a r k t e t r a q u a r k. W h i le t h e X(2900) s t at e s d e c a y s t r o n g l y, –– restricted. In contrast, a rich spectrum of radial and relatively narrow states near meson–meson thresholds for t h re s hold w a s o b s e r ve d. The s t r uc t u re of X(6900) i s c on- similar heavy-light diquark systems, such as (cc)(ud), (bc) –– –– angular momentum excitations between the coloured open charm, with widths of the order of tens of MeV. They sistent with the signature of a resonance (see figure), sug- (ud) and (bb)(ud), have been studied theoretically, resulting constituents is predicted for diquark tetraquarks. The are definitely tetraquarks, though it is still a moot point gesting a four-charm-quark state. in varying degrees of confidence that some may be stable
widths of these states could be large, as they can easily if they are genuinely bound states or merely manifesta- While the peaking X(6900) structure is close to the χc0 χ c1 with respect to strong interactions, and instead decay fall apart into lighter hadrons, with their binding energy tions of non-binding hadron–hadron forces that manifest meson-pair threshold, its width, of the order of a hundred w e a k l y, w it h m e a s u r a ble l i fe t i m e s. Hu nt i n g for s uc h s t at e s transformed into a light quark–antiquark pair. in complicated forms. The molecular interpretation had M eV, s e e m s t o o l a r g e t o fit i nt o t h e lo o s e-bi n d i n g s c h eme, i s a n e x c it i n g pr o s p e c t for t h e up g r a d e d L HC b e x p e r i m e nt. Unfortunately, it is difficult to rigorously apply QCD in also been reinforced in 2012 by Belle’s observations of the wherein decay modes other than the “fall-apart” topology LHCb’s new tetraquark observations have once again
t h e c o n fi n i n g r e g i m e o f mu lt i-q u a r k s t at e s. It i s t h e r e fore hidden-beauty Zb(10610) and Z b(10650) tetraquarks. These are expected to be strongly suppressed, and in any case, thrown open the debate on the nature of multi-quark up to experiments to discover which multi-quark states states also have relatively narrow widths of the order of tens there is no known loose binding mechanism between two states. With the theory still mired in non-perturbative This actually exist in nature. There have been some hints of of MeV and masses near the threshold for falling apart, in charmonium states. Charmonium-pair re-scattering calculations, experimental observations will be decisive observation tetraquark states built out of light quarks, though without this case to “open-beauty” mesons. effects are also disfavoured due to the requirements of i n le a d i n g t h e d e v e lo p m e nt o f t h i s s u bj e c t. T h e c o m mu n it y It is up to is the most definite proof. This is largely because additional light quark Pentaquark observations have also weighed in on the such interactions. This observation is therefore the most i s w a it i n g e a g e rl y t o s e e i f o t h e r e x p e r i m e nt s c o n fi r m t h e intriguing experiments pairs can easily be created in the decay process of simple debate. Last year’s observation of three narrow hid- intriguing experimental indication so far for hadrons made LHCb obser v at ion, and shed light on its nature. to discover mesons and baryons, and the highly relativistic nature of den-charm pentaquarks by the LHCb collaboration, with out of diquarks. experimental which multi- such states makes model predictions for their excitations widths below tens of MeV and masses close to the charm It is less clear if the observed structure is made of one Further reading indication so quark states unreliable. Hidden charm states have proved helpful again, meson-baryon threshold (CERN Courier M a y/ Ju n e 2019 p15), state, or several that may or may not interfere with each LHCb Collaboration 2020 arXiv:2006.16957. far for hadrons actually exist however, as the charmonium spectrum and the properties also points to loose hadron–hadron binding, in this case other. There is no information on the spin-parity of the LHCb Collaboration 2020 arXiv:2009.00025. made out of in nature of such states are well predicted. between a meson and a baryon. o b s e r v e d s t r uc t u r e. Ne it h e r d o w e y e t k n o w i f m a s s s t r uc- LHCb Collaboration 2020 arXiv:2009.00026. diquarks
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ADVERTISING FEATURE FEATURE NEUTRON SCIENCE
ZAO® based non-evaporable Getter pumps in optics vacuum chambers
Vacuum engineers and scientists have long known that even if a sample material is initially clean and handled with ultrahigh- vacuum (UHV) standards, a carbon contamination layer will deposit and grow on the material’s surface after placing it in a high vacuum (HV) or UHV chamber. This condition is also true for the optics vacuum chambers found in particle accelerators and synchrotron beamlines. For the optics vacuum chambers, this situation is worsened by X-ray irradiation, which can result in a one to two orders of magnitude pressure increase and high yield of carbon contaminants. The effects of carbon contamination on the X-ray optics can significantly reduce the X-ray transmission downstream to the experimental stations, carbon K edge, around 285 eV, as well as at conditions. Carbon contamination is not only and as next-generation synchrotrons usher higher energies around 1000 eV. As early as experimentally detected; it is also visually in X-ray brightness increases of two to three the 1980s, this carbon contamination layer evident after a few months to a year of orders of magnitude, it is critical to minimize was shown to cause intensity modulations beamline operation. It will usually appear as a these losses from carbon contamination. in X-ray absorption spectra that closely black line where the X-rays strike the optics. resembled those above the carbon K edge Read the full paper online. Multiple studies have shown that carbon in bulk crystalline graphite. These results contamination develops on X-ray optics and suggested the formation of graphitic SAES Group S.p.A reduces the transmission of photons near the carbon contamination even under UHV Web www.saesgroup.com
On track An aerial view of the European Spallation Source (ESS) construction site in Lund, Sweden, on 28 May 2020. (Credit: P Nordeng/ESS) ESS UNDER CONSTRUCTION
The European Spallation Source (ESS) will provide neutron beams 100 times brighter than those from reactor sources, enabling new research into material properties and fundamental physics.
ust a few years after the discovery of the neutron by James about atomic and molecular structure and dynamics. Neu- Chadwick in 1932, investigations into the properties of trons also carry a magnetic moment. This property, com- Jneutrons by Fermi and others revealed the strong energy bined with their absence of electric charge, make neutrons dependence of the neutron’s interactions with matter. This u n iq ue l y s e n s it i v e t o m a g n e t i s m at a n at o m ic le v e l. O n t h e knowledge enabled the development of sustainable neutron downside, the absence of electric charge means that neu- production by fission, opening the era of atomic energy. The tron-scattering cross sections are much weaker than they fi r s t nuc le a r-fi s s io n r e a c t or s i n t h e 1940 s w e r e a l s o e q u i ped are for X-rays and electrons, making neutron flux a limiting with the capacity for materials irradiation, and some provided factor in t he power of t his met hod for scient ific researc h. low-energy (thermal) neutron beams of sufficient intensity Throughout the 1950s and 1960s, incremental advances in for studies of atomic and molecular structure. Despite the t h e p o w e r o f nuc le a r-r e s e a rc h r e a c t or s a n d i m pr o v e m e nt s high cost of investment in nuclear-research reactors, neutron in moderator design provided increasing fluxes of thermal THE AUTHORS science flourished to become a mainstay among large-scale neutrons. In Europe these developments culminated in the Håkan Danared, facilities for materials research around the world. construction of the 57 MW high-flux reactor (HFR) at the Shane Kennedy and The electrical neutrality of neutrons allows them to probe Institut Laue-Langevin (ILL) in Grenoble, France, with a Mats Lindroos d e e p i nt o m at t e r i n a n o n-d e s t r uc t i v e m a n n e r, w h e r e t h e y compact core containing 9 kg of highly enriched uranium European Spallation scatter off atomic nuclei to reveal important information enabling neutron beams with energies from around 50 μeV Source, Sweden. www.goodfellow.com | [email protected] | 0800 731 4653
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FEATURE NEUTRON SCIENCE FEATURE NEUTRON SCIENCE ESS U Hammarlund/ESS ESS ESS
Monolith The 6000-tonne target station monolith, consisting of concrete and steel shielding, will surround the target wheel, moderator, cooling systems and beam extraction system. Cool view A section of the cryogenic system for the 600 m-long linear accelerator.
ESS from above Left: the ESS site layout, showing accelerator buildings (dark blue), target (violet), instrument halls (light blue), offices and labs for macromolecular crystallography, two small-angle scat- bi-spectral neutron moderator, which allows a high degree (green) and auxiliary buildings (red and yellow). Right: the positions of the first 15 neutron instruments: diffractometers for hard-matter structure tering instruments for the study of large-scale structures, of flexibility in the choice of neutron energy. determination (DREAM, HEIMDAL and MAGIC), macromolecular crystallography (NMX) and engineering studies (BEER); small-angle scattering t w o r e fle c t o m e t e r s for t h e s t ud y o f s u r f a c e s a n d i nt e r f a c es, instruments for the study of large-scale structures (LOKI and SKADI); reflectometers for the study of surfaces and interfaces (ESTIA and FREIA); five spectrometers for the study of atomic and molecular Accelerator and target spectrometers for the study of atomic and molecular dynamics (BIFROST, C-SPEC, MIRACLES, T-REX and VESPA); and a neutron imaging station (ODIN). dynamics over an energy range from a few μeV to several Most of the existing spallation neutron sources use a linear hundred meV, a diffractometer for engineering studies accelerator to accelerate protons to high energies. The to 500 meV. When the HFR came into operation in 1972, by more than two orders of magnitude. and a neutron imaging station (see “ESS layout” figure). particles are stored in an accumulator ring and are then however, it was clear that nuclear-fission reactors were The idea for the ESS was advanced in the early 1990s. Given that the ESS target system has the capacity for two extracted in a short pulse (typically a few microseconds in already approaching their limit in terms of steady-state The decision in 2009 to locate it in Lund, Sweden, led to neutron moderators and that the beam extraction system le n g t h) t o a h e a v y-m e t a l s p a l l at io n t a r g e t s uc h a s t u n g s t e n neutron flux (roughly 1.5 × 1015 neutrons per cm2 per second). the establishment of an organisation to build and operate a l lo w s v ie w i n g o f e a c h m o d e r at or b y up t o 4 2 b e a m p or t s, or mercury, which have a high neutron yield. A notable In an effort to maintain pace with advances in other the facility (ESS AB) in 2010. Ground-breaking took place there is the potential for many more neutron instruments exception is SINQ at PSI, which uses a cyclotron that pro- methods for materials research, such as synchrotron X-ray i n 201 4, a n d t o d a y c o n s t r uc t io n i s i n f u l l s w i n g, w it h fi r s t w it h o ut m aj or i n v e s t m e nt i n t h e b a s ic i n f r a s t r uc t u r e. T h e duces a continuous beam. facilities and electron microscopy, accelerator-based neu- science e x pected in 2023 and f ull user operat ion in 2026. ESS source also has a unique time structure, with far longer ESS has a linear accelerator but no accumulator ring, tron sources were established in the 1980s in the US (IPNS The ESS is organised as a European Research Infrastructure pulses than existing pulsed sources, and an innovative and it will thus have far longer proton pulses of 2.86 ms. and LANSCE), Japan (KENS) and the UK (ISIS). Spallation Consortium (ERIC) and at present has 13 member states: has long been hailed as the method with the potential to Czech Republic, Denmark, Estonia, France, Germany, Hun- Fundamental physics at the ESS push through to far greater neutron fluxes, and hence to gary, Italy, Norway, Poland, Spain, Sweden, Switzerland provide a basis for continued growth of neutron science. a nd t he U K. S we de n a nd D e n m a rk a re t he hos t c ou nt r ie s, The ESS will offer a multitude of from 1 to 100 TeV, far beyond observed baryon asymmetry of open up for other kinds of However, after nearly 50 years of operation, and with 10 providing nearly half of the budget for the construction opportunities for fundamental the threshold of direct particle the universe. fundamental physics as well as more modern medium- to high-flux neutron sources phase. Around 70% of the funding from the non-host coun- physics with neutrons, neutrinos production at accelerators, A design study, financed for new perspectives in neutron and potentially other secondary (including five spallation sources) in operation around tries is in the form of in-kind contributions, meaning and resolve the tiny effects of through the European scattering, and muon storage rings. particles from additional the world, the HFR is still the benchmark source for neu- that the countries are delivering components, personnel hadronic weak interactions, Commission’s Horizon 2020 Finally, a proposal has been target stations. While neutron tron-beam research. Of the spallation sources, the most or other support services to the facility rather than cash. enabling quantitative tests of programme, is also under way submitted to ESS concerning brightness and pulse time the non-perturbative limit of for the ESS Neutrino Super coherent neutrino–nucleus powerful (SNS at Oak Ridge National Laboratory in the The unprecedented brightness of ESS neutrons will enable structure are key parameters for US and J-PARC in Japan) have now been in operation for s m a l le r s a m ple s, f a s t e r m e a s u r e m e nt s a n d m or e c o m ple x neutron scattering (the main quantum chromodynamics. Beam (ESSνSB) project. This scattering (CEνNS). The high more than a decade. SNS has reached its design power experiments than what is possible at existing neutron focus of ESS experiments), the Another collaboration ambitious project would see an proton beam power together of 1.4 MW, and J-PARC is planning for tests at 1 MW. At sources. This will inevitably lead to discoveries across total intensity is more important is proposing a two-stage accumulator ring and a separate with the 2 GeV proton energy these power levels the sources are competitive with ILL a wide range of scientific disciplines, from condensed- for many fundamental-physics experiment at the ESS to search neutrino target added to the will provide a 10 times higher for leading-edge research. It has long been known that matter physics, solid-state chemistry and materials experiments. for baryon-number violation. The ESS facility, with the aim of neutrino flux from the spallation the establishment of a new high-flux spallation neutron sciences, to life sciences, medicine and cultural heritage. A cold neutron-beam facility first stage, HIBEAM, will look for sending neutrinos to a large target than previously obtained facility is needed if European science is to avoid a severe A wide range of industrial applications in polymer science for particle physics called ANNI evidence for sterile neutrinos. As underground detector in mid- for CEνNS. Measured for the shortage in access to neutron science in the coming years and engineering are also anticipated, while new avenues is proposed to allow precision a second stage, NNBAR could be Sweden, 400–500 km from the first time by the COHERENT (CERN Courier May/June 2020 p49). i n f u n d a m e nt a l p h y s ic s w i l l b e o p e n e d (s e e “F u n d a m e nt a l measurements of the beta decay, installed at the large beam port, ESS. Here, the neutrinos would collaboration in 2017 at ORNL’s physics at the ESS” panel). hadronic weak interactions and with the purpose to search for be detected at their second Spallation Neutron Source, Spallation Unprecedented performance From the start, the ESS has been driven by the neu- electromagnetic properties of oscillations between neutrons oscillation maximum, giving CEνNS offers a new way to has long been The European Spallation Source (ESS), with a budget of tron-scattering community, with strong involvement from the neutron. ANNI will improve and anti-neutrons. Observing the highest sensitivity for probe the properties of the hailed as the €1.8 billion (2013 figures), is a next-generation high-flux all the leading neutron-science facilities around Europe. the accuracy of measurements of such a transition would show that discovery and/or measurement neutrino including searches method with neutron source that is currently entering its final con- To ma x imise its scient ific potent ial, a reference set of 22 neutron beta decay by an order the baryon number is violated of the leptonic CP-violating for sterile neutrinos and a the potential to struction phase. Fed by a 5 MW proton linac, and fitted instrument concepts was developed from which 15 instru- of magnitude. Experiments will by two units and that matter phase. An accumulator ring neutrino magnetic moment, and push through with the most compact neutron moderator and matched ments covering a wide range of applications were selected probe a broad range of new- containing neutrons is unstable, and the resulting short proton could help reduce the mass of to far greater neutron transport systems, at full power the brightness for c o n s t r uc t io n. T h e s u it e i n c lud e s t h r e e d i ff r a c t o m e t e r s physics models at mass scales potentially shedding light on the pulses needed by ESSνSB would neutrino detectors. neutron fluxes of the ESS neutron beams is predicted to exceed the HFR for h a rd-m at t e r s t r uc t u r e d e t e r m i n at io n, a d i ff r a c t o m e t e r
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FEATURE NEUTRON SCIENCE FEATURE NEUTRON SCIENCE
and construction of the neutron instruments and the struction phase ends in late 2025, ESS is expected to be sample-environment e uipment. SS has developed its operating at 2 MW, and all 15 neutron instruments will be own detector and chopper technologies for the neutron in operation or ready for hot-commissioning.