Compact hard x ray synchrotron radiation source with superconducting bending magnets project
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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

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
Reasons Superconducting Bending Magnets

  • 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


History superconducting compact sr sources
History Superconducting Bending MagnetsSuperconducting 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
Main parameters of magnet Superconducting Bending Magnets

Budker Institute of Nuclear Physics, Novosibirsk


Bessy ii
Профиль магнитного поля в сверхпроводящем магните для BESSY-II

Budker Institute of Nuclear Physics, Novosibirsk


Main parameters of sr source
Main parameters of SR source сверхпроводящем магните для

Budker Institute of Nuclear Physics, Novosibirsk


Optical functions tme lattice
Optical functions (TME lattice) сверхпроводящем магните для

Budker Institute of Nuclear Physics, Novosibirsk


Linear optics design layout
Linear optics design layout сверхпроводящем магните для

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


Budker Institute of Nuclear Physics, Novosibirsk сверхпроводящем магните для


Layout
Layout сверхпроводящем магните для

Budker Institute of Nuclear Physics, Novosibirsk


Cost estimation
Cost estimation сверхпроводящем магните для

Budker Institute of Nuclear Physics, Novosibirsk


Schedule
Schedule сверхпроводящем магните для

Budker Institute of Nuclear Physics, Novosibirsk


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