002674092 001__ 2674092
002674092 005__ 20220312090333.0
002674092 0247_ $$2DOI$$9arXiv$$a10.18429/JACoW-eeFACT2018-WEXBA02$$qpublication
002674092 0248_ $$aoai:cds.cern.ch:2674092$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
002674092 037__ $$9arXiv$$aarXiv:1905.03528$$cphysics.acc-ph
002674092 037__ $$9arXiv:reportnumber$$aISBN: 978-3-95450-216-5
002674092 035__ $$9arXiv$$aoai:arXiv.org:1905.03528
002674092 035__ $$9Inspire$$aoai:inspirehep.net:1733990$$d2022-03-10T03:25:35Z$$h2022-03-12T03:01:31Z$$mmarcxml$$ttrue$$uhttps://inspirehep.net/api/oai2d
002674092 035__ $$9Inspire$$a1733990
002674092 041__ $$aeng
002674092 100__ $$aBoscolo, M.$$jJACoW-00000787$$mmanuela.boscolo@lnf.infn.it$$uFrascati$$vINFN/LNF, Frascati, Italy
002674092 245__ $$9arXiv$$aMachine detector interface for the $e^+e^-$ future circular collider
002674092 269__ $$c2019-05-09
002674092 260__ $$c2019-04-21
002674092 300__ $$a6 p
002674092 500__ $$9arXiv$$a6 pages, 7 figures, 62th ICFA ABDW on High Luminosity Circular $e^+e^-$ Colliders, eeFACT2018, Hong Kong, China
002674092 520__ $$9JACoW$$aThe international Future Circular Collider (FCC) study~[fccweb] aims at a design of p-p, \rm e⁺e⁻, e-p colliders to be built in a new 100~km tunnel in the Geneva region. The \rm e⁺e⁻ collider (FCC-ee) has a centre of mass energy range between 90 (Z-pole) and 375~GeV (t\bar{t}). To reach such unprecedented energies and luminosities, the design of the interaction region is crucial. The crab-waist collision scheme~[ref:cw] has been chosen for the design and it will be compatible with all beam energies. In this paper we will describe the machine detector interface layout including the solenoid compensation scheme. We will describe how this layout fulfills all the requirements set by the parameters table and by the physical constraints. We will summarize the studies of the impact of the synchrotron radiation, the analysis of trapped modes and of the backgrounds induced by single beam and luminosity effects giving an estimate of the losses in the interaction region and in the detector.
002674092 520__ $$9arXiv$$aThe international Future Circular Collider (FCC) study aims at a design of $pp$, $e^+e^-$, $ep$ colliders to be built in a new 100 km tunnel in the Geneva region. The $e^+e^-$ collider (FCC-ee) has a centre of mass energy range between 90 (Z-pole) and 375 GeV (tt_bar). To reach such unprecedented energies and luminosities, the design of the interaction region is crucial. The crab-waist collision scheme has been chosen for the design and it will be compatible with all beam energies. In this paper we will describe the machine detector interface layout including the solenoid compensation scheme. We will describe how this layout fulfills all the requirements set by the parameters table and by the physical constraints. We will summarize the studies of the impact of the synchrotron radiation, the analysis of trapped modes and of the backgrounds induced by single beam and luminosity effects giving an estimate of the losses in the interaction region and in the detector.
002674092 540__ $$3preprint$$aCC-BY-4.0$$uhttp://creativecommons.org/licenses/by/4.0/
002674092 65017 $$2arXiv$$ahep-ex
002674092 65017 $$2SzGeCERN$$aParticle Physics - Experiment
002674092 65017 $$2arXiv$$aphysics.acc-ph
002674092 65017 $$2SzGeCERN$$aAccelerators and Storage Rings
002674092 690C_ $$aCERN
002674092 690C_ $$aARTICLE
002674092 700__ $$aBlanco-Garcia, O.R.$$jJACoW-00048126$$moscar.blancogarcia@lnf.infn.it$$uFrascati$$vINFN/LNF, Frascati, Italy
002674092 700__ $$aBacchetta, N.$$jJACoW-00095042$$mnicola.bacchetta@cern.ch$$uCERN$$vCERN, Geneva, Switzerland
002674092 700__ $$aBelli, E.$$jJACoW-00076898$$meleonora.belli@roma1.infn.it$$uCERN$$vCERN, Geneva, Switzerland
002674092 700__ $$aBenedikt, M.$$iINSPIRE-00521008$$jJACoW-00001655$$mmichael.benedikt@cern.ch$$uCERN$$vCERN, Geneva, Switzerland
002674092 700__ $$aBurkhardt, H.$$iINSPIRE-00444053$$jJACoW-00001681$$mhelmut.burkhardt@cern.ch$$uCERN$$vCERN, Geneva, Switzerland
002674092 700__ $$aGil Costa, M.$$jJACoW-00051809$$mmiguel.gil.costa@cern.ch$$uCERN$$vCERN, Geneva, Switzerland
002674092 700__ $$aElsener, K.$$iINSPIRE-02702285$$jJACoW-00001607$$mkonrad.elsener@cern.ch$$uCERN$$vCERN, Geneva, Switzerland
002674092 700__ $$aLeogrande, E.$$iINSPIRE-00416444$$jJACoW-00068670$$memilia.leogrande@cern.ch$$uCERN$$vCERN, Geneva, Switzerland
002674092 700__ $$aJanot, P.$$jJACoW-00060560$$mpatrick.janot@cern.ch$$uCERN$$vCERN, Geneva, Switzerland
002674092 700__ $$aTen Kate, H.$$iINSPIRE-00224330$$jJACoW-00001836$$mherman.tenkate@cern.ch$$uCERN$$vCERN, Geneva, Switzerland
002674092 700__ $$aEl Khechen, D.$$jJACoW-00068770$$mdima.el.khechen@cern.ch$$uCERN$$vCERN, Geneva, Switzerland
002674092 700__ $$aKolano, A.$$jJACoW-00051829$$manna.maria.kolano@cern.ch$$uCERN$$vCERN, Geneva, Switzerland
002674092 700__ $$aKersevan, R.$$jJACoW-00057096$$mroberto.kersevan@cern.ch$$uCERN$$vCERN, Geneva, Switzerland
002674092 700__ $$aLueckhof, M.$$uCERN$$vCERN, Geneva, Switzerland
002674092 700__ $$aOide, K.$$jJACoW-00002811$$uCERN$$vCERN, Geneva, Switzerland
002674092 700__ $$aPerez, E.$$jJACoW-00023839$$memmanuel.perez@cern.ch$$uCERN$$vCERN, Geneva, Switzerland
002674092 700__ $$aTeherani, N.A.$$uCERN$$vCERN, Geneva, Switzerland
002674092 700__ $$aViazlo, O.$$jJACoW-00112008$$moleksandr.viazlo@cern.ch$$uCERN$$vCERN, Geneva, Switzerland
002674092 700__ $$aVoutsinas, Y.$$uCERN$$vCERN, Geneva, Switzerland
002674092 700__ $$aZimmermann, F.$$iINSPIRE-00138581$$jJACoW-00001653$$mfrank.zimmermann@cern.ch$$uCERN$$vCERN, Geneva, Switzerland
002674092 700__ $$aDam, M.$$jJACoW-00100208$$mdam@nbi.dk$$uBohr Inst.$$vNiels Bohr Institute, Copenhagen, Denmark
002674092 700__ $$aBlondel, A.$$iINSPIRE-00067542$$jJACoW-00001757$$malain.blondel@cern.ch$$uGeneva U.$$vDPNC/Geneva University, Geneva, Switzerland
002674092 700__ $$aKoratzinos, M.$$iINSPIRE-00443269$$jJACoW-00033390$$mmichael.koratzinos@cern.ch$$uGeneva U.$$vDPNC/Geneva University, Geneva, Switzerland
002674092 700__ $$aNovokhatski, A.$$jJACoW-00002507$$mnovo@slac.stanford.edu$$uSLAC$$vSLAC, Menlo Park, California, USA
002674092 700__ $$aSullivan, M.$$iINSPIRE-00145025$$jJACoW-00002581$$msullivan@slac.stanford.edu$$uSLAC$$vSLAC, Menlo Park, California, USA
002674092 700__ $$aBogomyagkov, A.V.$$iINSPIRE-00355199$$jJACoW-00001217$$ma.v.bogomyagkov@inp.nsk.su$$uNovosibirsk, IYF$$vBINP SB RAS, Novosibirsk, Russia
002674092 700__ $$aLevichev, E.B.$$jJACoW-00001177$$me.b.levichev@inp.nsk.su$$uNovosibirsk, IYF$$vBINP SB RAS, Novosibirsk, Russia
002674092 700__ $$aSinyatkin, S.$$jJACoW-00004573$$ms.v.sinyatkin@inp.nsk.su$$uNovosibirsk, IYF$$vBINP SB RAS, Novosibirsk, Russia
002674092 700__ $$aCollamati, F.$$jJACoW-00090832$$mfrancesco.collamati@roma1.infn.it$$uINFN, Rome$$vINFN-Rome1, Rome, Italy
002674092 773__ $$cWEXBA02$$qeeFACT2018$$wC18-09-24.11$$y2019
002674092 8564_ $$81479960$$s1101907$$uhttps://cds.cern.ch/record/2674092/files/1905.03528.pdf$$yFulltext
002674092 8564_ $$81479961$$s68553$$uhttps://cds.cern.ch/record/2674092/files/fig6.png$$y00003 Hits per bunch crossing in the different CLD subdetectors (see the abscissa) due to SR with (blue line) and without (green line) Tungsten shielding.
002674092 8564_ $$81479962$$s172669$$uhttps://cds.cern.ch/record/2674092/files/fig7.png$$y00002 Loss map in the IR.The loss peaks correspond to the restriction of the vacuum chamber between the last drift and final focus quadrupole QC2.
002674092 8564_ $$81479963$$s256353$$uhttps://cds.cern.ch/record/2674092/files/fig4.png$$y00001 HOM absorbers design.
002674092 8564_ $$81479964$$s248850$$uhttps://cds.cern.ch/record/2674092/files/fig5.png$$y00000 Upper plot: MDISim simulation showing the origin of the photons generated by a beam starting at about -550~m from the IP (see the red arrow); the IP is at z = 0 m. Lower plot: energy distribution from the SR produced by the last bend upstream the IP.
002674092 8564_ $$81479965$$s178943$$uhttps://cds.cern.ch/record/2674092/files/fig2.png$$y00006 IR layout top view (x-z plane); note the expanded scale for the ordinate ($\pm200$mm) with respect to the abscissa ($\pm$3m).
002674092 8564_ $$81479966$$s97925$$uhttps://cds.cern.ch/record/2674092/files/fig3.png$$y00005 3D CAD view of the IR vacuum chamber in the region where two beam pipes are merged together.
002674092 8564_ $$81479967$$s97007$$uhttps://cds.cern.ch/record/2674092/files/fig1.png$$y00004 Schematic layout of the FCC-ee collider rings. The green line indicates the beamline of the FCC-ee booster and hadron collider FCC-hh. The plot in the middle shows the two beams trajectories at the IP.
002674092 8564_ $$81528593$$s1164238$$uhttps://cds.cern.ch/record/2674092/files/fulltext1733990.pdf$$yFulltext
002674092 960__ $$a13
002674092 962__ $$b2674168$$kWEXBA02$$nhongkong20180924
002674092 980__ $$aARTICLE
002674092 980__ $$aConferencePaper