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The FCC study covered an energy-frontier hadron collider (FCC-hh), a highest-luminosity high-energy lepton collider (FCC-ee), the corresponding 100 km tunnel infrastructure, as well as the physics opportunities of these two colliders, and a high-energy LHC, based on FCC-hh technology

FCC-hh: Longitudinal beam dynamics and RF requirements. Ivan Karpov and Elena Shaposhnikova Acknowledgements: S. Arsenyev, P. Baudrenghien, R. Calaga, D. Schulte, D. Teytelman. Update since 2018. •RF and beam parameters in CDR are mainly defined by single-bunch stability in longitudinal plane (loss of Landau damping) Since last FCC meeting, we. Figure 1: FCC-hh layout and key parameters of the main and low-luminosity Experimental Interaction Regions. The FCC-hh, housed in a 97.75 km perimeter racetrack tunnel [5] lled with 16 T SC magnets, includes four EIRs two for nominal/high luminosity and two for low-luminosity experiments. Each of the EIR straight sections is 1400 A short animation showing the assembly of a detector for FCC-hh. This is based on the first design concept layout and a final layout will be presented by the..

FCC-hh: The Hadron Collider - Home - Springe

FCC-hh: The Hadron Collider: Future Circular Collider

  1. The FCC-hh concept comprises in the baseline scenario a power-saving, low-temperature superconducting magnet system based on an evolution of the Nb3Sn technology pioneered at the HL-LHC, an energy-efficient cryogenic refrigeration infrastructure based on a neon-helium (Nelium) light gas mixture, a high-reliability and low loss cryogen distribution infrastructure based on Invar, high-power distributed beam transfer using superconducting elements and local magnet energy recovery and re-use.
  2. osity high-energy lepton collider (FCC-ee), the corresponding 100km tunnel infrastructure, as well as the physics opportunities of these two colliders, and a high-energy LHC, based on FCC-hh technology. This document constitutes the third volume of the FCC Conceptual.
  3. reference [6] for an introduction to the FCC-hh tracker design. A schematic of the inner and outer tracker for the FCC-hh reference detector is shown in figure3, with the triplet replacing the innermost layer of the outer tracker barrel. Note that the forward tracker (which extends up-to 16m in z) has been removed from the schematic for clarity
  4. The FCC-hh concept comprises in the baseline scenario a power-saving, low-temperature superconducting magnet system based on an evolution of the Nb3Sn technology pioneered at the HL-LHC, an energy-efficient cryogenic refrigeration infrastructure based on a neon-helium (Nelium) light gas mixture, a high-reliability and low loss cryogen distribution infrastructure based on Invar, high-power.
  5. Abstract: Part of the Future Circular Collider (FCC-hh) study is dedicated to the development of the 16 Tesla Nb 3 Sn superconducting dipole magnets. The design of the magnets was enabled by a cooperative effort of national research institutes, universities, and CERN
  6. Given that the FCC-hh (Future Circular Collider) and the SPPC (Super proton-proton Collider), proposed projects of hadron-hadron colliders at the center-of-mass energy of 100 TeV, have long been under consideration and extensively studied, the discovery potential for new physics beyond the SM would be increased largely with its high collision energy

Home / Archives / Vol. 3 (2017): Physics at the FCC-hh, a 100 TeV pp collider Vol. 3 (2017): Physics at the FCC-hh, a 100 TeV pp collide This study covers a highest-luminosity high-energy lepton collider (FCC-ee) and an energy-frontier hadron collider (FCC-hh), which could, successively, be installed in the same 100 km tunnel. The scientific capabilities of the integrated FCC programme would serve the worldwide community throughout the 21st century The FCC-hh energy goal is reached by combining higher-field, 16 T magnets, based on Nb3Sn superconductor, and a new 100 km tunnel connected to the LHC complex. In addition to the FCC-hh proper, the FCC study is also exploring the possibility of a High-Energy LHC (HE-LHC), with a centre-of-mass energy of 25-27 TeV, as could be achieved in the existing 27 km LHC tunnel using the FCC-hh magnet. The FCC-hh is an international design study aiming at establishing the feasibility and cost of a 50+50 TeV hadron collider, to be built eventually in the Geneva area. The FCC-hh adopts the same concept as the LHC, twin-bore superconducting (SC) magnets, and can host two large general-purpose detectors (á-la ATLAS/CMS) Future Circular Collider (18. Dec 2018) The Hadron Collider (FCC-hh) Page 3 of 20 2 Objectives The objective is to develop, build and operate a 100 TeV hadron collider, with an integrated luminosity at least a factor of 5 larger than the HL-LHC, to extend the current energy frontier by almost an order of magnitude

Most recently, the FCC-hh detector magnet working group provided an entertaining overview of the evolution of the design towards a smaller, simpler and especially more cost-effective solution (the story also features in the cover of this issue!) Introduction. With the goal of colliding proton beams at an energy of 50 TeV, the total stored energy per beam at the FCC-hh will be of about 8 GJ, more than one order of magnitude larger than at the LHC N1 - 13 pages, chapter 5 in Physics at the FCC-hh, a 100 TeV pp collider. PY - 2017/6/22. Y1 - 2017/6/22. N2 - In this chapter we explore a few examples of physics opportunities using the existing chain of accelerators at CERN, including potential upgrades The lecture will present FCC-hh, the hadron collider of the Future Circular Collider. The conceptual design and basic parameters will be discussed. Key beam dynamic FCC-hh Higgs studies Michelangelo L. Mangano michelangelo.mangano@cern.ch Theoretical Physics Department CERN Snowmass 2021 — Energy Frontier WG-01 meeting: Higgs distributions and CPV 24 June 2020 For an overview of Higgs studies and links to existing documents, see C.Helsens, M.Mangano, M.Selvaggi

FCC-hh - Overview of the detector design - YouTub

heavy resonances at FCC-hh the results are summarised in figure 1 right for different integrated luminosity scenarios. References [1]T. Sjöstrand et al., An Introduction to PYTHIA 8.2, Comput. Phys. Commun. 191 (2015) 159 [2]J. Alwall et al., The automated computation of tree-level and next-to-leading order differential cros These electron cloud effects are considered as a serious issue for the FCC-hh as they cause coherent instabilities. The stability of the beam depends crucially on the secondary electron emission yield (SEY) of the surface. High-temperature superconductors show a bad SEY value up to δ m a x = 2. 54 FCC-hh Detector Studies . Albert De Roeck , CERN . On behalf of the FCC-hh Detector Study Group . IAS Meeting Hong Kong. 18-21 January 2016 Based on material from W. Riegler. W. Riegler, CERN 2 International FCC collaboration (CERN as host lab) to study

International audienceThe Future Circular Collider (FCC-hh) is being designed as a 100 km ring that should collide 50 TeV proton beams. At 8.3 GJ, its stored beam energy will be a factor 28 higher than what has been achieved in the Large Hadron Collider, which has the highest stored beam energy among the colliders built so far Talk given at the Higgs and Effective Field Theory workshop (HEFT) 2021.14/04/2021 Evening Session (5) Full Title: Precision from Diboson Processes at FCC-hh.. It summarizes the FCC-hh physics discovery opportunities, presents the FCC-hh accelerator design, performance reach, and staged operation plan, discusses the underlying technologies, the civil engineering and technical infrastructure, and also sketches a possible implementation LLCP at FCC-hh (√s = 100 TeV) Sho IWAMOTO Based on Jonathan. L. Feng, S.I., Yael Shadmi, Shlomit Tarem [1505.02996] (collected in FCC report [1606.00947]) 18 Jan. 2017 1st FCC Physics Workshop @ CERN UC Irvine Technion ATLAS. Technion Israel Institute of Technolog

Fcc Cd

The design of a muon detector and first-level muon trigger system for the FCC-hh baseline experiment is presented. The baseline FCC-hh detector configuration with a solenoid magnet system providing a field integral of 18 Tm over a wide pseudorapidity interval and a muon system around the solenoid and the calorimeter system is assumed FCC-hh is a proposedfuture energy-frontierhadroncol-lider, based on dipole magnets with a field around 16 T installedina newtunnelwith acircumferenceofabout100 km, which would provide proton collisions at a centre-of-mass energy of 100 TeV, as well as heavy-ion collisions a One of the FCC options, the FCC-hh, is designed to provide proton-proton collisions at the proposed 100 TeV centre-of-mass energy with peak luminosity 5 × 10 34 cm −2 s −1 [31, 32]. In this study, we investigate the potential of the process pp → γγγ at FCC-hh in the existence of anomalous Higgs boson couplings at Hγγ and HZγ. The FCC-hh CDR foresees using the LHC at 3.3 TeV as injector for the FCC-hh. An attractive alternative, which could be further explored, is the injection from a new fast-ramping superconducting SPS, at an energy of, e.g. around 1.3 TeV. The longest straight section of the FCC-hh, with a length of 2.8 km, is allocated for betatron collimation

Website For First Christian Church Huber Heights. The story of Christmas begins long before a manger in Bethlehem. Before the creation of the world, the Father's plan for rescuing his children was to send Jesus to earth In addition, the FCC-hh provides the unique opportunity to precisely measure the Higgs self-coupling in the di-photon and b-jets channel. Excellent photon and jet energy resolution at low energies as well as excellent angular resolution for pion background rejection are required in this challenging environment Our estimated bounds are one order of magnitude better than projections at HL-LHC and is better than global fits at future lepton colliders. The sensitivity to $\mathcal{O}_{\varphi q}^{(3)}$ is competitive with other channels that could probe the same operator at FCC-hh This wiki describes fast and full simulations of a FCC-hh detector for multi-TeV energy range. People: A.Kotwal (Fermilab/Duke), L.Gray (Fermilab), S.Chekanov (ANL), J.Strube (PNNL), N.Tran (Fermilab), S-S. Yu (NCU), S.Sen (Duke), J.Repond (ANL) The current goal of the studies is to understand physics requirements and design options using the FCC-performance detector, called SiFCC

FCC Week 2019 (24-28 June 2019): FCC-hh accelerator

CONTACT US. Address 6114 Fishburg Rd. Huber Heights, OH 45424 Phone: 937-236-8029 Fax: 937-236-6779 e-mail: info@fcchh.org Sunday Services 9:30 and 11:00 A Hadron Colliders Parameters parameter FCC-hh HE-LHC HL-LHC LHC collision energy cms [TeV] 100 27 14 14 dipole field [T] 16 16 8.33 8.33 circumference [km] 97.75 26.7 26.7 26.7 beam current [A] 0.5 1.1 1.1 0.58 bunch intensity [1011] 1 1 2.2 2.2 1.15 bunch spacing [ns] 25 25 25 25 25 synchr. rad. power / ring [kW] 2400 101 7.3 3.6 SR power / length [W/m/ap.] 28.4 4.6 0.33 0.1 FCC-hh physics analysis meeting. 05.04.2018. see all events. MCnet. MCnet Vietnam School on Monte Carlo Event Generators for the LHC. 14.09.2019. see all events. Search. Search. Search. Contact Us. CERN. Directorate Office for Research and Computing. Esplanade des Particules 1. 1211 Geneva Switzerland

The FCC-hh will collide protons at a centre of mass en-ergy of 100 TeV, and like the Large Hadron Collider (LHC), there is also the possibility to collide heavy ions. Due to its nature as a discovery machine, the desired parameter set is expected to exceed the current LHC in every aspect. In order to maximise the physics discovery potential. FCC-hh Nb 3Sn wire development: superconducting and magnetic properties of prototype samples M. Ortino,1 A. Moros,2 M. Alekseev,3 A. Tsapleva,3 P. Lukyanov,3 M. First Steps Preschool is a new Christian preschool in Huber Heights, OH, in the Dayton area with a focus on faith and academics serving children ages 2.5 to 5 The future circular hadron-hadron collider (FCC-hh), however, considers a novel utilization of superconductors reliant on the high frequency response of HTS at extremely challenging conditions 6 Abstract: The Future Circular Collider (FCC-hh) project is a conceptual study whose goal is to design the successor of the Large Hadron Collider, increasing the collision energy from 14 to 100 TeV. The energy stored in the 16-T superconducting dipole magnets and the length of the sectors composing the 100-km FCC tunnel are considerably larger than those in present accelerators

In the context of design studies for future pp colliders, we present a set of predictions for average soft-QCD event properties for pp collisions at E CM = 14 , 27, and 100 TeV. The current default Monash 2013 tune of the Pythia 8.2 event generator is used as the baseline for the extrapolations, with uncertainties evaluated via variations of cross-section parametrisations, PDFs, MPI energy. FCC-hh Detector Studies Albert De Roeck January 15 (Material from W. Riegler) 2 Baseline Parameters The present working hypothesis is : - peak luminosity baseline: 5E34 - peak luminosity ultimate: <= 30E34 - integrated luminosity baseline ~250 fb -1 (average per year) - integrated luminosity. The FCC-hh would use the LHC and its pre-injector accelerators to feed the collider that could reach a top energy of 100 TeV - seven times greater than the LHC. CERN will now carry out a more detailed costing of the FCC as well as continue research and development into the magnet technology that will be required for such a machine at higher energies

FCC-hh Nb 3 Sn Wire Development: Exploring the Microstructure of Prototype Samples Acknowledgements This work is part of the Marie Skłodowska-Curie Action EASITrain, funded by the European Union'sH2020 Framework Programme under grant agreement no. 764879 A possible first stage for the FCC-hh at CERN would be the FCC-ee, an electron-positron collider. The FCC-ee would collide electrons and positrons in a 100-kilometer (62-mile) circular tunnel passing under Lac Leman at the border of France and Switzerland. The FCC-ee tunnel would provide a ready-made home for the FCC-hh FCC-hh will also provide huge statistics of HH events (40 times more than LHC) to determine the self-coupling and the top quark Yukawa coupling to %-level depending on the systematic assumptions. A quantitative analysis of the physics potential of some of these future facilities has been performed in the context of the European Strategy study group as shown in Figure 2 [ 1905.03764 ] In particular, starting from the centre-of-mass energy of 3 TeV a muon collider is the most-energy efficient type of collider, while at 10 TeV it would have a physics reach comparable to that of the proposed 100 TeV hadron collider, FCC-hh, while fitting in a ring of the size of the LHC (27 km), without the need for a much more expensive 100-km.

GitHub - HEP-FCC/FCCSW: FCC software, common to FCC-hh

  1. high-energy particle collisions with CERN's LHC and the ATLAS detector, and ideas for future accelerators such as the FCC hh-ee-he; experiments with neutrinos (T2K, Hyper-Kamiokande) astroparticle physics experiments on the ground (IceCube, CTA) and in space (AMS, POLAR, DAMPE
  2. osity lepton collider (FCC-ee) as a first step, followed by an energy-frontier proton collider (FCC-hh) will offer unprecedented precision in studying nature at its most fundamental scales through a diverse physics programme spanning 70 years
  3. o FCC-hh will be filled with groups of proton bunches that are pre-accelerated by the 26 km long LHC which will be recycled to become a fast cycling injector for FCC-hh. The injection energy into the LHC is 450 GeV, the maximum number of proton bunches in the LHC is 2800

FCC-hh: The Hadron Collider - CERN Document Serve

FCC hh h. Nb3Sn conductor program Nb3Sn is one of the major cost & performance factors for FCC-hh and must be given highest attention c ERN 3000 2000 Hi 1000 FCC LHC 1500 Lumi osity 1000 Field (T) m Main development goals until 2020: Jc increase (16T, 4.2K) > 1500 Almm2 i.e. 50% increase wrt HL-LHC wire Reference wire diameter 1 m FCC-hh. is a 100 TeV proton-proton collider -> Defines infrastructure needs. Alignment precision requirement : ~ 150 . μ. m. FCC-ee is a high-luminosity, high-precision electron-positron collider -> Potential intermediate step. Alignment precision requirement: ~ 17 . μ. m FCC-eh combines the intense hadron (proton and ion) beams of the LHC. • pp-collider (FCC-hh) defining infrastructure requirements • e+e-collider (FCC-ee) as potential intermediate step • p-e (FCC-he) option •80-100 km infrastructure in Geneva area ~16 T 100 TeV pp in 100 km ~20 T 100 TeV pp in 80 k The FCC-hh would have a total integrated luminosity of around 15-20 ab-1 - a factor of 5-10 more than that produced at the HL-LHC - and corresponding to 10 10 Higgs bosons being produced. It would also be used to search for new particles at higher masses than possible at the LHC as well as discover or rule-out the existence of thermal dark-matter particles known as WIMPs

FCC-hh: The Hadron Collider - INSPIR

Support is provided through our launchpad site (), where questions will be answered ().. The current versions are 2.8.5 (Sep 16th 2020) and 3.0.0β (August 30th 2020) The WHIZARD project is a part of the Strategic Helmholtz Alliance Physics at the Terascale.We are furthermore supported or have been supported in earlier stages of this work by the German Bundesministerium für Bildung und. The LHC Physics Centre at CERN organised a number of activities centred on the physics programme of the LHC and its upgrades, including 7 workshops and 32 working group meetings. It also organised 2 workshops and 14 WG meetings for the physics study of the FCC-hh project. The two following references give some of the history of CERN-TH Postdoc on Physics studies at FCC-hh (20 February 2020) Staff position in the area Data science in experimental particle physics (20 February 2020) Koordination des Mentoring-Programms dynaMENT (5 February 2020) PhD position on Extreme Timing for Collider Detectors (31 January 2020) Postdoc on Extreme Timing for Collider Detectors (31. Left: Luminosity evolution for FCC-hh phase 2 from Table 2 for three different values of the transverse emittance damping time (nominal value: 1 hour). Right: Integrated luminosity per year for FCC-hh phases 1 and 2 from Table 2 as a function of turnaround time. Reuse & Permission

After 10 years of physics at the Large Hadron Collider (LHC), the particle physics landscape has greatly evolved. Today, a staged Future Circular Collider (FCC), consisting of a luminosity-frontier highest-energy electron-positron collider (FCC-ee) followed by an energy-frontier hadron collider (FCC-hh), promises the most far-reaching physics program for the post-LHC era. FCC-ee will be a. FCC-hh: The Hadron Collider: Future circular collider conceptual design report volume 3: THE EUROPEAN PHYSICAL JOURNAL. SPECIAL TOPICS: 2019: HE-LHC: The High-Energy large hadron collider future circular collider conceptual design report volume 4: THE EUROPEAN PHYSICAL JOURNAL. SPECIAL TOPICS: 201

FCC-hh: The Hadron Collider - INSPIRE-HE

  1. First Christian Church of Huber Heights was live. Good morning. Thanks. thanks for joining us online and in person my name is cherry
  2. Average event properties from LHC to FCC-hh. Helen Brooks * and Peter Skands. School of Physics and Astronomy, Monash University, Clayton, VIC, 3800, Australia * e-mail: Helen.Brooks@monash.edu. Received: 31 August 2018 Accepted: 14.
  3. This Chapter summarises the physics opportunities for the study of Higgs bosons and the dynamics of electroweak symmetry breaking at the 100 TeV pp collider
  4. g information of 10 ps or less will be necessary to reject the large background of particles from spurious collisions
  5. For future circular colliders, the target dipole field has been set at 16 T for FCC-hh, allowing proton-proton collisions at an energy of 100 TeV, while China's proposed pp collider (SppC) aims at a 12 T dipole field, to be followed by a 20 T dipole
  6. -Drove the design efforts for the FCC-hh magnets in partnership with European national lab magnet & beam dynamics experts; co-led the EuroCirCol project and was the responsible CERN scientist for several collaborations with national labs & universities with 50+ experts engaged; developed cost model and finalized successfully a conceptual design report for the magnet system of FCC-hh

An asymmetric layout near the interaction region reduces the critical energy of SR photons on the incoming side of the IP to values below 100 keV, while matching the geometry to the beam line of the FCC proton collider (FCC-hh) [A. Chancé et al., Proceedings of IPAC'16, 9-13 May 2016, Busan, Korea, TUPMW020 (2016).] as closely as possible Dear colleagues, We would like to thank you for submitting a Letter of Interest (LOI). These letters have been tremendously helpful for the frontier and topical-group conveners as they plan the sessions in the Community Planning Meeting which will take place in ~5 weeks We study the sensitivity of anomalous neutral triple gauge couplings (aNTGC) via production in the 4 channel at 100 TeV center of mass energy of future circular hadron collider, FCC-hh. The analysis including the realistic detector effects is performed in the mode where both Z bosons decay into same-flavor, oppositely charged lepton pairs Conceptual design of the FCC-hh dipole circuits with integrated CLIQ protection system M Prioli, B Auchmann, L Bortot, M Maciejewski, T Salmi, A Verweij IEEE Transactions on Applied Superconductivity 29 (8), 1-9 , 201

The CLIQ Quench Protection System Applied to the 16 T FCC

  1. osity-frontier high-energy electron-positron collider (FCC-ee) as first stage, followed by an energy-frontier hadron collider (FCC-hh) as second stage, and promises the most.
  2. The particle physics community in Europe is in the midst of updating the European Strategy for Particle Physics. The latest input is a newly published 250-page physics briefing book, the result of an intense year-long effort to capture the status and prospects for experiment, theory, accelerators and computing for high-energy physics
  3. expanding to FCC-hh (pp at 100 TeV) SiD Build a FCC-like detector for studies of CAL transverse and longitudinal granularity, depth, material, magnetic fields, pixel sizes etc. Use the SLIC setup for ~ tens TeV-scale particles/jets 6 m ~10 m FCC-hh Designing a Geant4 simulation for high-granular calorimeter for ~20 TeV jets (particles

Probing single stop production at the FCC-hh/SPPC

  1. spired by successful LEP - LHC programs at CERN. Comprehensive cost-effective program maximizing physics opportunities: Stage 1: FCC-ee (Z, W, H, tt) as Higgs factory, electroweak & and top factory at highest lu
  2. HepSim is a public repository with Monte Carlo simulated events for particle-collision experiments. The HepSim repository was started at ANL during the US long-term planning study of the American Physical Society's Division of Particles and Fields (Snowmass 2013). It contains predictions from leading-order (LO) parton shower models, next-to-leading order (NLO) and NLO with matched parton.
  3. al FWHM pulse duration of 30 fs, and ~2 mJ in the soft x-ray undulator for a no
  4. Depending on the model, the lighter regions of the spectra could be accessible at CLIC, while the FCC‐hh will be able to test large parts of the predicted spectrum of each model. The lightest supersymmetric particle, a neutralino, is considered as a cold dark matter candidate and put to test using the latest MicrOMEGAs code

FCC-hh: The Hadron Collider: Future Circular Collider Conceptual Design Report Volume 3 A Apyan, H Denizli, KY Oyulmaz, A Senol, P Barjhoux, JM Bernhardt, The European Physical Journal Contact Information. Phone: 937-965-7929. Fax: 937-660-3066 . firststepsofficestaff@gmail.com. 6114 Fishburg Road Huber Heights, Ohio 4542 FCC-hh: The Hadron Collider: Future Circular Collider Conceptual Design Report Volume 3 A Abada, M Abbrescia, SS AbdusSalam, I Abdyukhanov, J Abelleira Fernandez, A Abramov, M Aburaia, AO Acar, PR Adzic, P Agrawal, JA Aguilar-Saavedra, JJ Aguilera-Verdugo, M Aiba, I Aichinger, G Aielli, A Akay, A Akhundov, H Aksakal, JL Albacete, S Albergo, et al

GitHub - FCC-hh-framework/EventProducer: Produce Events

David Curtin Assistant Professor Canada Research Chair in Theoretical Particle Physics pronouns: he/him High Energy Theory Group Department of Physics, MP1113. dcurtin@physics.utoronto.ca office: +1 416-978-4784. Research. I am a high energy phenomenologist, interested in finding and analyzing theories of particle physics beyond the Standard Model FCC-hh: The Hadron Collider: Future Circular Collider Conceptual Design Report Volume 3 the FCC Collaboration, 1 Jul 2019, In: European Physical Journal Special Topics. 228, 4, p. 755-1107 353 p. HE-LHC: The High-Energy Large Hadron Collider: Future Circular Collider Conceptual Design Report Volume CLDR Kids Tornadoes.pdf - Google Drive Sign i PhD in Particle Physics You can submit an on-line application here Applications for funded 2021 PhD entry are welcome at all times. Applications submitted before Christmas 2020 will be processed in time for the first round of interviews in early 2021

ICMAB - A year in review: ICMAB most cited articles of 2019Simulating Proton Synchrotron Radiation in the Arcs of theCOLLOQUIUM - Mercoledì 9 Gennaio 2019 Ore 16:30 - ProfHeavy resonances at energy-frontier hadron collidersResearch | PARTICLES AND COSMOLOGY - ANTUSCH GROUPAAPPS BulletinOut-of-plane displacements at SOF (back view), MOF (sideHepSim
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