002156862 001__ 2156862
002156862 003__ SzGeCERN
002156862 005__ 20230505040714.0
002156862 0247_ $$2DOI$$a10.1007/s10948-016-3660-6
002156862 0248_ $$aoai:cds.cern.ch:2156862$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
002156862 035__ $$9arXiv$$aoai:arXiv.org:1605.08777
002156862 035__ $$9Inspire$$a1466350
002156862 037__ $$9arXiv$$aarXiv:1605.08777$$cphysics.ins-det
002156862 041__ $$aeng
002156862 100__ $$aKlyukhin, V.I.$$uSINP, Moscow
002156862 245__ $$aSuperconducting Magnet with the Minimum Steel Yoke for the Hadron Future Circular Collider Detector
002156862 269__ $$c27 May 2016
002156862 260__ $$c2016
002156862 300__ $$a8 p
002156862 500__ $$9arXiv$$a8 pages, 6 figures, presented at ICSM2016 - 5th International Conference on Superconductivity and Magnetism on April 26, 2016 at Fethiye, Turkey
002156862 520__ $$aThe conceptual design study of a hadron Future Circular Collider (FCC-hh) with a center-of-mass energy of the order of 100 TeV in a new tunnel of 80-100 km circumference assumes the determination of the basic requirements for its detectors. A superconducting solenoid magnet of 12 m diameter inner bore with the central magnetic flux density of 6 T in combination with two superconducting dipole and two conventional toroid magnets is proposed for a FCC-hh experimental setup. The coil of 23.468 m long has seven 3.35 m long modules included into one cryostat. The steel yoke with a mass of 22.6 kt consists of two barrel layers of 0.5 m radial thickness, and the 0.7 m thick nose disk and four 0.6 m thick end-cap disks each side. The maximum outer diameter of the yoke is 17.7 m; the length is 62.6 m. The air gaps between the end-cap disks provide the installation of the muon chambers up to the pseudorapidity about \pm 2.7. The superconducting dipole magnets allow measuring the charged particle momenta in the pseudorapidity region greater than \pm 3. The conventional forward muon spectrometers provide the muon identification in the pseudorapidity region from \pm 2.7 to \pm 5. The magnet modeled with Cobham's program TOSCA. The total current in the superconducting solenoid coil is 123 MA-turns; the stored energy is 41.8 GJ. The axial force onto each end-cap is 450 MN. The stray field at the radius of 50 m off the coil axis is 13.7 mT and 5.2 mT at the radius of 100 m. All other parameters presented and discussed.
002156862 520__ $$9arXiv$$aThe conceptual design study of a Future Circular hadron-hadron Collider (FCC-hh) with a center-of-mass energy of the order of 100 TeV, assumed to be constructed in a new tunnel of 80-100 km circumference, includes the determination of the basic requirements for its detectors. A superconducting solenoid magnet of 12-m-diameter inner bore with the central magnetic flux density of 6 T, in combination with two superconducting dipole magnets and two conventional toroid magnets is proposed for an FCC-hh experimental setup. The coil of 23.468 m length has seven 3.35-m-long modules included into one cryostat. The steel yoke with a mass of 22.6 kt consists of two barrel layers of 0.5 m radial thickness and a 0.7-m-thick nose disk and four 0.6-m-thick end-cap disks each side. The outer diameter of the yoke is 17.7 m. The full length of the magnetic system is 62.6 m. The air gaps between the end-cap disks provide for the installation of the muon chambers up to an absolute pseudorapidity about 2.7. The superconducting dipole magnets provide measurement of charged particle momenta in the absolute pseudorapidity region greater than 3. The conventional forward muon spectrometer allows muon identification in the absolute pseudorapidity region from 2.7 to 5. The magnet is modeled with the program TOSCA from Cobham CTS Limited. The total current in the superconducting solenoid coil is 123 MA-turns; the stored energy is 41.8 GJ. The axial force acting on each end-cap is 450 MN. The stray field is 13.7 mT at a radius of 50 m from the coil axis, and 5.2 mT at a radius of 100 m. Many other parameters are presented and discussed.
002156862 540__ $$aarXiv nonexclusive-distrib. 1.0$$barXiv$$uhttp://arxiv.org/licenses/nonexclusive-distrib/1.0/
002156862 540__ $$3publication$$aCC-BY-4.0
002156862 542__ $$3publication$$dThe Author(s)$$g2016
002156862 595__ $$aLANL EDS
002156862 65017 $$2arXiv$$aDetectors and Experimental Techniques
002156862 690C_ $$aARTICLE
002156862 690C_ $$aCERN
002156862 695__ $$9LANL EDS$$aphysics.ins-det
002156862 700__ $$aHervé, A.$$uU. Wisconsin, Madison (main)
002156862 700__ $$aBall, A.$$uCERN
002156862 700__ $$aCuré, B.$$uCERN
002156862 700__ $$aDudarev, A.$$uCERN
002156862 700__ $$aGaddi, A.$$uCERN
002156862 700__ $$aGerwig, H.$$uCERN
002156862 700__ $$aMentink, M.$$uCERN
002156862 700__ $$aDa Silva, H. Pais$$uCERN
002156862 700__ $$aRolando, G.$$uCERN
002156862 700__ $$aten Kate, H. H. J.$$uCERN
002156862 700__ $$aBerriaud, C.P.$$uIRFU, Saclay
002156862 773__ $$c3660$$oJournal of Superconductivity and Novel Magnetism, Article 3660 (2016)$$pJ. Supercond. Novel Magn.$$v29$$y2016
002156862 8564_ $$uhttp://arxiv.org/pdf/1605.08777.pdf$$yPreprint
002156862 8564_ $$81240818$$s1317009$$uhttp://cds.cern.ch/record/2156862/files/art-3660.pdf$$ySpringer Open Access article
002156862 8564_ $$81240818$$s1925287$$uhttp://cds.cern.ch/record/2156862/files/art-3660.pdf?subformat=pdfa$$xpdfa$$ySpringer Open Access article
002156862 8564_ $$82451879$$s274235$$uhttp://cds.cern.ch/record/2156862/files/arXiv:1605.08777.pdf
002156862 916__ $$sn$$w201622
002156862 960__ $$a13
002156862 962__ $$b2201654$$k3660$$nfethiye20160424
002156862 980__ $$aARTICLE
002156862 980__ $$aConferencePaper