Summary FD Support System

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Presentation transcript:

Summary FD Support System Andrea Jeremy: FD Support Tatsuya Kume: Shintake Monitor David Urner: MONALISA

Andrea JEREMIE N.Geffroy, B.Bolzon, G.Gaillard FD support Andrea JEREMIE N.Geffroy, B.Bolzon, G.Gaillard

SUMMARY: Vibrations transmissibility study First eigenfrequency measured: With no masses: 74Hz (Q=12) Masses of 1400Kg: 46Hz (Q=9) First eigenfrequency simulated: With no masses: 56Hz Masses of 1400Kg: 26Hz  Simulations done: gives a good idea of eigenfrequency evolution with masses and boundary conditions Other table transfer function peaks: Due to the fact that supports are not fixed to the table and to the ground

Current QD0 configuration QD0 + mover beam 300mm (from Ghyslain’s drawing) 1200mm Height to compensate! T-plate 260mm 610mm 50mm 30mm Idea for 260mm support is to have a bottom plate clamped to the bloc with some possibility of adjusting the position with big screws

Position adjustment Height adjustment with shims =>so slightly shorter than 260mm 3 to 6 of such devices Adjust position with screw Table: flat surface

FD configuration (T.Okugi’s presentation) Table=2400 IP=> SBPM QC3 FFTB 2.13 S3.00 SF1FF QF1FF 100 450.1 200 180 SD0FF QD0FF 76.2 785 380 2630 Sweeping Honda Shintake S-band BPM slightly outside table on a “light” Sextupole=> how will the S-band BPM be supported? Does this BPM need to be supported?

Mount stabilization for Shintake monitor-6 5th ATF2 Project meeting December 20, 2007 T. Kume, Y. Honda, and T. Tauchi High Energy Accelerator Research Organization (KEK) T. Suehara, H. Yoda, M. Oroku, T. Yamanaka and Y. Kamiya The univ. of Tokyo T. Sanuki Tohoku Univ.

Specifications expected for new table support ~10nm of amplitude for incoherent vibration with floor >Use steal honeycomb core (<Al), thicker (110mm->250mm) >Highly ridged mount on floor without any insulator ±5mm of height adjustable range with accuracy of ±1mm >Shim between table mount and floor ±2.5mm of horizontal position adjustable range perpendicular to beam with accuracy of ±1mm >Slide sheet between vertical table and horizontal table

Shintake monitor mount-side view assuming distance between end face of CLIC table and FF magnet is 20 mm, distance between end face of FF magnet and IP is 1000 mm Downstream ⇔ Upstream

Shintake monitor mount-top view assuming beam goes center of CLIC table

David Urner ATF2 Meeting Dec 19 2007 MONALISA Update David Urner ATF2 Meeting Dec 19 2007

CSM (Compact Straightness Monitor) 10cm 5cm 100cm 6D position transferred from left to right breaking of symmetries is important Preliminary simulation results of CSM Resolution: sy:10nm distance meter resolution: 1nm Positional change of optics components with respect to each other: 1nm That’s the challenge.

Multi-fibre read out (compact launch) FFI: Fixed Frequency Interferometry (OPD 400mm) s=4.5nm Displacement / nm Time (hours) Displacement / mm Fixed frequency laser (FFI) Compact Launch: 25x25x15mm Test shown here with moving mirror First stationary mirror test : resolution 5 nm demonstrated to be improved with vaccuum and laser frequency stabilisation

Frequency stabilisation Frequency standard: 87Rb D2 line at 780 nm Simplified Schematic: Need 20 kHz stability for 1nm over distances of 10m. NPL done ~kHz.

Multi-fibre read out (compact launch) FSI:Frequency Scanning Interferometry (OPD 400mm) s=750nm s=70nm Add box to reduce air turbulence s=750nm Same interferometer can be used for FSI Better resolution by just covering interferometer with box - expect to do even better in vacuum!

Overview of Current Design Plan View End View Elevation