002266048 001__ 2266048
002266048 005__ 20230314203235.0
002266048 0248_ $$aoai:cds.cern.ch:2266048$$pcerncds:CERN$$pcerncds:CERN:FULLTEXT$$pcerncds:REPORT$$pcerncds:FULLTEXT
002266048 0247_ $$2DOI$$9bibmatch$$a10.1088/1361-6471/aaa171
002266048 037__ $$9arXiv$$aarXiv:1705.08783$$cphysics.acc-ph
002266048 035__ $$9arXiv$$aoai:arXiv.org:1705.08783
002266048 035__ $$9Inspire$$aoai:inspirehep.net:1601165$$d2023-03-06T19:24:31Z$$h2023-03-14T15:05:42Z$$mmarcxml$$ttrue$$uhttps://inspirehep.net/api/oai2d
002266048 035__ $$9Inspire$$a1601165
002266048 041__ $$aeng
002266048 100__ $$aAngal-Kalinin, D.$$uDaresbury$$vASTeC, STFC, Daresbury, United Kingdom
002266048 245__ $$9arXiv$$aPERLE: Powerful Energy Recovery Linac for Experiments - Conceptual Design Report
002266048 246__ $$9arXiv$$aPERLE: Powerful Energy Recovery Linac for Experiments - Conceptual Design Report
002266048 269__ $$c2017-05-24
002266048 260__ $$c2018-05-02
002266048 300__ $$a71 p
002266048 500__ $$9arXiv$$a112 pages, 63 figures
002266048 520__ $$9IOP$$aA conceptual design is presented of a novel energy-recovering linac (ERL) facility for the development and application of the energy recovery technique to linear electron accelerators in the multi-turn, large current and large energy regime. The main characteristics of the powerful energy recovery linac experiment facility (PERLE) are derived from the design of the Large Hadron electron Collider, an electron beam upgrade under study for the LHC, for which it would be the key demonstrator. PERLE is thus projected as a facility to investigate efficient, high current (HC) (>10 mA) ERL operation with three re-circulation passages through newly designed SCRF cavities, at 801.58 MHz frequency, and following deceleration over another three re-circulations. In its fully equipped configuration, PERLE provides an electron beam of approximately 1 GeV energy. A physics programme possibly associated with PERLE is sketched, consisting of high precision elastic electron–proton scattering experiments, as well as photo-nuclear reactions of unprecedented intensities with up to 30 MeV photon beam energy as may be obtained using Fabry–Perot cavities. The facility has further applications as a general technology test bed that can investigate and validate novel superconducting magnets (beam induced quench tests) and superconducting RF structures (structure tests with HC beams, beam loading and transients). Besides a chapter on operation aspects, the report contains detailed considerations on the choices for the SCRF structure, optics and lattice design, solutions for arc magnets, source and injector and on further essential components. A suitable configuration derived from the here presented design concept may next be moved forward to a technical design and possibly be built by an international collaboration which is being established.
002266048 520__ $$9arXiv$$aA conceptual design is presented of a novel ERL facility for the development and application of the energy recovery technique to linear electron accelerators in the multi-turn, large current and large energy regime. The main characteristics of the powerful energy recovery linac experiment facility (PERLE) are derived from the design of the Large Hadron electron Collider, an electron beam upgrade under study for the LHC, for which it would be the key demonstrator. PERLE is thus projected as a facility to investigate efficient, high current (> 10 mA) ERL operation with three re-circulation passages through newly designed SCRF cavities, at 801.58 MHz frequency, and following deceleration over another three re-circulations. In its fully equipped configuration, PERLE provides an electron beam of approximately 1 GeV energy. A physics programme possibly associated with PERLE is sketched, consisting of high precision elastic electron-proton scattering experiments, as well as photo-nuclear reactions of unprecedented intensities with up to 30 MeV photon beam energy as may be obtained using Fabry-Perot cavities. The facility has further applications as a general technology test bed that can investigate and validate novel superconducting magnets (beam induced quench tests) and superconducting RF structures (structure tests with high current beams, beam loading and transients). Besides a chapter on operation aspects, the report contains detailed considerations on the choices for the SCRF structure, optics and lattice design, solutions for arc magnets, source and injector and on further essential components. A suitable configuration derived from the here presented design concept may next be moved forward to a technical design and possibly be built by an international collaboration which is being established.
002266048 540__ $$aarXiv nonexclusive-distrib. 1.0$$barXiv$$uhttp://arxiv.org/licenses/nonexclusive-distrib/1.0/
002266048 540__ $$3publication$$9IOP$$aCC-BY-3.0$$uhttp://creativecommons.org/licenses/by/3.0/
002266048 65017 $$2arXiv$$aphysics.acc-ph
002266048 65017 $$2SzGeCERN$$aAccelerators and Storage Rings
002266048 690C_ $$aCERN
002266048 690C_ $$aREPORT
002266048 695__ $$2INSPIRE$$9bibclassify$$aelectron: beam
002266048 695__ $$2INSPIRE$$9bibclassify$$acurrent: high
002266048 695__ $$2INSPIRE$$9bibclassify$$alinear accelerator: energy recovery
002266048 695__ $$2INSPIRE$$9bibclassify$$abeam: current
002266048 695__ $$2INSPIRE$$9bibclassify$$abeam: energy
002266048 695__ $$2INSPIRE$$9bibclassify$$aphoton: beam
002266048 695__ $$2INSPIRE$$9bibclassify$$amagnet: superconductivity
002266048 695__ $$2INSPIRE$$9bibclassify$$aelectron: accelerator
002266048 695__ $$2INSPIRE$$9bibclassify$$aRF system: superconductivity
002266048 695__ $$2INSPIRE$$9bibclassify$$aelectron p: scattering
002266048 695__ $$2INSPIRE$$9bibclassify$$astructure
002266048 695__ $$2INSPIRE$$9bibclassify$$acavity
002266048 695__ $$2INSPIRE$$9bibclassify$$aCERN LHC Coll
002266048 695__ $$2INSPIRE$$9bibclassify$$abeam loading
002266048 695__ $$2INSPIRE$$9bibclassify$$adeceleration
002266048 695__ $$2INSPIRE$$9bibclassify$$aquenching
002266048 695__ $$2INSPIRE$$9bibclassify$$aupgrade
002266048 695__ $$2INSPIRE$$9bibclassify$$alattice
002266048 695__ $$2INSPIRE$$9bibclassify$$ahadron
002266048 695__ $$2INSPIRE$$9bibclassify$$aoptics
002266048 700__ $$aArduini, G.$$uCERN$$vCERN,Geneva,Switzerland
002266048 700__ $$aAuchmann, B.$$uCERN$$vCERN,Geneva,Switzerland
002266048 700__ $$aBernauer, J.$$uMIT$$vMassachusetts Institute of Technology,Cambridge,MA,USA
002266048 700__ $$aBogacz, A.$$uJefferson Lab$$vJefferson Lab,Newport News,VA,USA
002266048 700__ $$aBordry, F.$$uCERN$$vCERN,Geneva,Switzerland
002266048 700__ $$aBousson, S.$$uOrsay, IPN$$vInstitute de Physique Nucleaire Orsay,France
002266048 700__ $$aBracco, C.$$uCERN$$vCERN,Geneva,Switzerland
002266048 700__ $$aBrüning, O.$$uCERN$$vCERN,Geneva,Switzerland
002266048 700__ $$aCalaga, R.$$uCERN$$vCERN,Geneva,Switzerland
002266048 700__ $$aCassou, K.$$uOrsay, LAL$$vLAL,CNRS-IN2P3,Université Paris-Sud,Centre Scientifique d'Orsay,France
002266048 700__ $$aChetvertkova, V.$$uCERN$$vCERN,Geneva,Switzerland
002266048 700__ $$aCormier, E.$$uCELIA, Bordeaux$$vCELIA,University of Bordeaux 1,CNRS UMR 5107,Talence,France
002266048 700__ $$aDaly, E.$$uJefferson Lab$$vJefferson Lab,Newport News,VA,USA
002266048 700__ $$aDouglas, D.$$uJefferson Lab$$vJefferson Lab,Newport News,VA,USA
002266048 700__ $$aDupraz, K.$$jORCID:0000-0001-5848-232X$$uOrsay, LAL$$vLAL,CNRS-IN2P3,Université Paris-Sud,Centre Scientifique d'Orsay,France
002266048 700__ $$aGoddard, B.$$uCERN$$vCERN,Geneva,Switzerland
002266048 700__ $$aHenry, J.$$uJefferson Lab$$vJefferson Lab,Newport News,VA,USA
002266048 700__ $$aHutton, A.$$uJefferson Lab$$vJefferson Lab,Newport News,VA,USA
002266048 700__ $$aJensen, E.$$uCERN$$vCERN,Geneva,Switzerland
002266048 700__ $$aKaabi, W.$$uOrsay, LAL$$vLAL,CNRS-IN2P3,Université Paris-Sud,Centre Scientifique d'Orsay,France
002266048 700__ $$aKlein, M.$$jORCID:0000-0002-8527-964X$$uU. Liverpool (main)$$vUniversity of Liverpool,UK
002266048 700__ $$aKostka, P.$$uU. Liverpool (main)$$vUniversity of Liverpool,UK
002266048 700__ $$aLasheras, N.$$uCERN$$vCERN, Geneva, Switzerland
002266048 700__ $$aLevichev, E.$$uNovosibirsk, IYF$$vBINP, Novosibirsk, Russia
002266048 700__ $$aMarhauser, F.$$uJefferson Lab$$vJefferson Lab,Newport News,VA,USA
002266048 700__ $$aMartens, A.$$uOrsay, LAL$$vLAL,CNRS-IN2P3,Université Paris-Sud,Centre Scientifique d'Orsay,France
002266048 700__ $$aMilanese, A.$$uCERN$$vCERN,Geneva,Switzerland
002266048 700__ $$aMilitsyn, B.$$uDaresbury$$vASTeC,STFC,Daresbury,UK
002266048 700__ $$aPeinaud, Y.$$uOrsay, LAL$$vLAL,CNRS-IN2P3,Université Paris-Sud,Centre Scientifique d'Orsay,France
002266048 700__ $$aPellegrini, D.$$uCERN$$vCERN,Geneva,Switzerland
002266048 700__ $$aPietralla, N.$$uDarmstadt, Tech. Hochsch.$$vInstitut für Kernphysik Technische Universität Darmstadt
002266048 700__ $$aPupkov, Y.A.$$uNovosibirsk, IYF$$vBINP,Novosibirsk
002266048 700__ $$aRimmer, R.A.$$uJefferson Lab$$vJefferson Lab,Newport News,VA,USA
002266048 700__ $$aSchirm, K.$$uCERN$$vCERN,Geneva,Switzerland
002266048 700__ $$aSchulte, D.$$uCERN$$vCERN,Geneva,Switzerland
002266048 700__ $$aSmith, S.$$uDaresbury$$vASTeC,STFC,Daresbury,UK
002266048 700__ $$aStocchi, A.$$uOrsay, LAL$$vLAL,CNRS-IN2P3,Université Paris-Sud,Centre Scientifique d'Orsay,France
002266048 700__ $$aValloni, A.$$uCERN$$vCERN,Geneva,Switzerland
002266048 700__ $$aWelsch, C.$$uU. Liverpool (main)$$vUniversity of Liverpool,UK
002266048 700__ $$aWillering, G.$$uCERN$$vCERN,Geneva,Switzerland
002266048 700__ $$aWollmann, D.$$uCERN$$vCERN,Geneva,Switzerland
002266048 700__ $$aZimmermann, F.$$uCERN$$vCERN,Geneva,Switzerland
002266048 700__ $$aZomer, F.$$uOrsay, LAL$$vLAL,CNRS-IN2P3,Université Paris-Sud,Centre Scientifique d'Orsay,France
002266048 773__ $$c065003$$n6$$pJ. Phys. G$$v45$$y2018
002266048 8564_ $$81316111$$s7326963$$uhttp://cds.cern.ch/record/2266048/files/arXiv:1705.08783.pdf
002266048 8564_ $$81402825$$s8476415$$uhttp://cds.cern.ch/record/2266048/files/pdf.pdf$$yFulltext
002266048 960__ $$a13
002266048 980__ $$aREPORT
002266048 980__ $$aARTICLE