Status of RTML design in TDR configuration A.Vivoli, N. Solyak, V. Kapin Fermilab.

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Presentation transcript:

Status of RTML design in TDR configuration A.Vivoli, N. Solyak, V. Kapin Fermilab

KILC Apr.24,2012 OUTLINE: Latest changes in central region (ERTL/PRTL) Return Line Dog-Legs design (ELTL/PLTL) ML Treaty point definition and matching Earth curvature in Return Lines (ELTL/PLTL) Latest changes in 2 stage Bunch Compressor Magnet count and Heat Load/Cost estimation Summary A. Vivoli, N.Solyak, V.Kapin, “Status of RTML design” 2

KILC Apr.24,2012 RTML Beamlines Courtesy of B. List (updated by V. Kapin & N. Solyak) 3 A. Vivoli, N.Solyak, V.Kapin, “Status of RTML design”

KILC Apr.24,2012 Latest changes in central region (ERTL/PRTL) 4 Beam lines geometry in global coordinate defined in document EDMS D* A. Vivoli, N.Solyak, V.Kapin, “Status of RTML design”

KILC Apr.24,2012 Latest changes in central region (ERTL/PRTL ) 5 Twiss parameters defined in document EDMS D* A. Vivoli, N.Solyak, V.Kapin, “Status of RTML design” Parameterx-value (target)y-value (target)z-value (height) Positron Extraction Lines:Ring1 / Ring2 Treaty point position108.42m a m4.72m a 5.59m-1.3m / +1.3m Treaty point angle(p ) rad0.0mrad0.0mrad / 0.0mrad Ext septum position*75.59m0.0m-1.3m / +1.3m h and h’ a b45.0m29.96m--- Electron Extraction Line:Ring1 Treaty point position m5.59m0.0m Treaty point angle(p ) rad0.0mrad Ext septum position*-75.59m0.0m h and h’ a b45.0m29.96m---

KILC Apr.24,2012 ERTL/PRTL (Electron-Ring-to-Linac) lines DRs are is separated vertically by 1.3m: electron ring has the same elevation as RTML in ML tunnel Sources need cryomodules and SC solenoids, heavy objects sitting at floor (w orking agreement between sources, DR, RTML, CFS) Positron Merger/Splitter e-e- e+ Courtesy of N. Solyak 6 A. Vivoli, N.Solyak, V.Kapin, “Status of RTML design”

KILC Apr.24,2012 Latest changes in central region (ERTL/PRTL) Geometrical configuration of central region Beam lines Courtesy of V. Kapin 7 A. Vivoli, N.Solyak, V.Kapin, “Status of RTML design”

KILC Apr.24,2012 Latest changes in central region (ERTL/PRTL) Matching results with MAD8: Courtesy of V. Kapin PRTL – positron line in central area ERTL – electron line in central area 8 A. Vivoli, N.Solyak, V.Kapin, “Status of RTML design”

KILC Apr.24,2012 Geometry of the dog-leg defined in document EDMS: D* Return Line Doglegs design A. Vivoli, N.Solyak, V.Kapin, “Status of RTML design” 9 (ELTL/PLTL)

KILC Apr.24,2012 Matching results with MAD8 for the ELTL/PLTL Dog-Legs: Courtesy of V. Kapin Return Line Doglegs design (2) A. Vivoli, N.Solyak, V.Kapin, “Status of RTML design” 10 (ELTL/PLTL)

KILC Apr.24,2012 Main Linacs/RTML treaty points defined in document: D* Geometrical matching of the 2 RTML beam lines is made by tuning the cell length of the Return Lines FODO system and the bending angles in the horizontal and vertical doglegs upstream the Turn Around ELTL FODO system PLTL FODO system Hor. & Ver. Doglegs e- Main Linac e+ Main Linac ML Treaty points definition and matching A. Vivoli, N.Solyak, V.Kapin, “Status of RTML design” 11

KILC Apr.24,2012 For Cryogenic requirements main linacs need to follow the curvature of the Earth. Return lines are located in the same tunnel with ML’s, then they need to be curved too. Geometric curvature of the beam lines are realized in MAD8 with combinations of VKICKERS and thin vertical BENDS. The beam orbit is curved by introducing vertical dipole correctors at each quadrupole of the FODO lattice, which create a small vertical dispersion. This is then matched to the straight lines by means of 4 vertical dipole correctors upstream and downstream the curved section. Vertical correctors Earth curvature in Return Lines (ELTL/PLTL) A. Vivoli, N.Solyak, V.Kapin, “Status of RTML design”12

KILC Apr.24,2012 MAD8_51 results for curved PLTL beam line: Vertical correctors for dispersion matching Straight line Earth curvature in Return Lines (ELTL/PLTL) A. Vivoli, N.Solyak, V.Kapin, “Status of RTML design” 13

KILC Apr.24,2012 A. Vivoli, N.Solyak, V.Kapin, “Status of RTML design” 14 Latest changes in 2 stage Bunch Compressor New RF in BC is defined in document D* :

KILC Apr.24,2012 A. Vivoli, N.Solyak, V.Kapin, “Status of RTML design” 15 Latest changes in 2 stage Bunch Compressor MAD8 results for 2 stage BC optics:

KILC Apr.24,2012 A. Vivoli, N.Solyak, V.Kapin, “Status of RTML design” 16 Initial beamBC1 parameters Beam after BC1BC2 parameters Final beam dp/p, % MeV) σ z, mm E, MeV A/-φ, MeV/ deg R 56, mm dp/p, % σ z, mm E, Me V A/-φ, MeV/ deg R 56, mm dp/p, % MeV) σ z, mm E, MeV / e3/ / e3/ / e3/ Simulations of 2 stage Bunch Compressor Simulation results by S. Seletskiy:

KILC Apr.24,2012 Lucretia Simulations of ILC 2-stage BC Parameters: Initial Energy: 5 GeV Initial Norm. Emittance (H/V): 8e-6/20e-9 m rad Acc. Gradient (BC1/BC2): 18.7/27.1 MV/m Total Voltage (BC1/BC2): 465/11700 MV RF phase (BC1/BC2): -115/-30 deg R 56 (BC1/BC2): /-55.2 mm Norm. Emittance Growth (H/V): <0.75/<2.0 % Final Energy: GeV A. Vivoli, N.Solyak, V.Kapin, “Status of RTML design” 17

KILC Apr.24,2012 BC Performance for different initial energy spread and bunch length Initial Bunch Length: 6.0 mm Initial Energy Spread: % Final Bunch Length: mm Final Energy Spread: % Initial Bunch Length: 5.0 – 7.0 mm Initial Energy Spread: 0.15 % Final Bunch Length: mm Final Energy Spread: % A. Vivoli, N.Solyak, V.Kapin, “Status of RTML design” 18

KILC Apr.24,2012 Magnet count and Heat Load/Cost estimation A. Vivoli, N.Solyak, V.Kapin, “Status of RTML design” 19 Magnet count and Heat & Power Load for RTML estimated with RDR parameters.

KILC Apr.24,2012 A. Vivoli, N.Solyak, V.Kapin, “Status of RTML design” 20 Magnet count and Heat Load/Cost estimation Cost for RTML magnets & PS estimated using RDR data.

KILC Apr.24,2012 Summary and outlook A. Vivoli, N.Solyak, V.Kapin, “Status of RTML design” 21 Central region, return lines and Bunch Compressor have been designed according to specifications. Earth curvature in return lines have been designed. Geometrical matching of DR/ML Treaty points have been performed, optics matching almost done. Simulations of BC have been performed with good results. Magnet count and Heat Load/Cost estimations almost completed.

Thanks for your attention.

BACK UP SLIDES

KILC Apr.24,2012 Layout A. Vivoli, N.Solyak, V.Kapin, “Status of RTML design” 24 RTML LAYOUT Lines EC_DL and BC1_DL have same lattice design.