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Compact Hard X-Ray Synchrotron Radiation Source with Superconducting Bending Magnets (project). E . I . Antokhin , A . A . Gvozdev , G.N. Kulipanov , N.A.Mezentsev, A.V. Philipchenko , K.V. Zolotarev Budker Institute of Nuclear Physics, Novosibirsk. Reasons.
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Compact Hard X-Ray Synchrotron Radiation Source with Superconducting Bending Magnets(project) E.I. Antokhin, A.A. Gvozdev, G.N. Kulipanov, N.A.Mezentsev, A.V. Philipchenko,K.V. Zolotarev Budker Institute of Nuclear Physics, Novosibirsk
Reasons • Absence of specialized SR source in Siberian SR Center (SSRC) • Great experience of BINP in developing and fabrication of superconducting insertion devices for SR centers Budker Institute of Nuclear Physics, Novosibirsk
HistorySuperconducting compact SR sources NIJI-III (ETL) • Compact SR sources for X-ray lithographyAURORA (Sumitomo), NIJI-III (ETL), COSY, SXLS, Helios, Super-ALIS (199X). • BINP projects (1992) • 6 T superconducting bending magnet prototype • Siberia-SM • Siberia-MP • Siberia-HB • 9 T superconducting bending magnet forBESSY-II (BINP, 2004) Siberia-MP ( BINP) Budker Institute of Nuclear Physics, Novosibirsk
Main parameters of magnet Budker Institute of Nuclear Physics, Novosibirsk
Профиль магнитного поля в сверхпроводящем магните для BESSY-II Budker Institute of Nuclear Physics, Novosibirsk
Main parameters of SR source Budker Institute of Nuclear Physics, Novosibirsk
Optical functions (TME lattice) Budker Institute of Nuclear Physics, Novosibirsk
Linear optics design layout П=55.8m Qx/Qz = 4.10/3.67 Cx/Cz = -26.78/-9.64 Jx=1.038 α=4.74 10-3 δE/E=1.33 10-3 εx = 10.2 nm rad ΔE = 180.2 keV/turn τ = 2.38ms Budker Institute of Nuclear Physics, Novosibirsk
Layout Budker Institute of Nuclear Physics, Novosibirsk
Cost estimation Budker Institute of Nuclear Physics, Novosibirsk
Schedule Budker Institute of Nuclear Physics, Novosibirsk