ATF and ATF2 news · sdfsd Folding the halo from 5 to 2.5 is possible, but... PLACET. ATF2:...

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ATF and ATF2 news From a visit to KEK during December 2006 Rogelio Tomas      9 th -March-2007

Transcript of ATF and ATF2 news · sdfsd Folding the halo from 5 to 2.5 is possible, but... PLACET. ATF2:...

Page 1: ATF and ATF2 news · sdfsd Folding the halo from 5 to 2.5 is possible, but... PLACET. ATF2: Emittance blow up due to octupoles Octupole tail folding in ATF2 needs either larger collimator

ATF and ATF2 newsFrom a visit to KEK during December 2006

Rogelio Tomas               9th­March­2007

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Contents

● ATF project:– complex– achievements– goals– problems

● ATF2 project:– schedule– complex– goals– problems

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ATF complex

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Achievements: Emittance

PRLVol 92Num. 52004 

Minimum normalized vertical emittance = 0.01m

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Achievements: Instrumentation 

Demonstration of operational 50nm resolution BPMs

Q­BPM, S. Boogert  et al

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Achievements: Instrumentation II

● ATF ‘in the ring’ laserwire is a high resolution  beam size monitor   1% resolution @ 5um

● Fast (3ns)  kicker (0.6mrad) for ILC Damping ring

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ATF Goals

Demonstrate 2nm resolutionIP­BPM

Fast Feedback system: 23ns latency

Beam dynamics: Fast ion instability, impedance measurement, microwave instability, etc.

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ATF problems I

Extraction line emittance larger than ring emittance !!                  Coupling?   Non­linear aberrations? 

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ATF problems II

­Are resonances a problem in the Damping ring?

­Experiments to measure resonance driving terms  have been performed by: R. Tomas, K. Kubo,   S. Kuroda, T. Naito, T. Okugi, J. Urakawa and  F. Zimmermann.

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ATF problems II

First measurement of the resonance (3,0) at two BPMs in ATFDR.Reasonable agreement with model but lack of long. information.

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ATF problems II

Attempt to measure resonance (1,2) failed because of not enough kick strength in both planes (simultaneously).Vertical plane remains not probed.

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ATF problems III: Energy oscillations

e

Everlasting energy oscillations after injection

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ATF ­ ATF2 schedule

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ATF2 layout

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ATF2 Goals

● Experimental demonstration of the Final Focus System

● Achievement of 37nm vertical IP spot size● Experimental demonstration or test of other 

aspects of Linear Colliders:– Collimation and wakefields– Correction of aberrations (2nd order dispersion, etc.)– Instrumentation

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ATF2 problems: Achieving 37nm

G. White

Alignment and tunning do not guarantee y < 100nm

Shintake monitor only measures below 100nm (now 300nm)

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ATF2 problems: Beam size monitorsShintake monitor:2nm resolution,y < 300nm

New monitor based on a pattern target:10% resolution, y~350­1000nm

New tuning simulations required to prove performance 

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ATF2: Octupole Tail Folding?Permanent octupole magnetshave been proposed to testoctupole tail folding.

Y. Iwashita

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Principle of octupole tail folding

Requirements for efficient halo folding:­Low halo divergence (large beta)­Octupole doublet placed after collimators­Octupole doublet placed in front of a quadrupole

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ATF2 Final Focus optics

No good location for vertical Octupole Doublet 

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ATF2: Horizontal tail folding simulations

sdfsd

Folding the halo from 5 to 2.5 , ... is possible but

PLACET

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ATF2: Emittance blow up due to octupoles

Octupole tail folding in ATF2 needs either larger collimatorgaps or different collimator location (for the vertical case).

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ATF2: Magnetic field stability?

The observed temperature coefficient of the iron coreelectromagnet is about +14 ppm/degree. It is positive andcannot be explained by the standard Bloch theory.

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CLIC Table

Benoit Bolzon

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ATF2: Coupling & Dispersion problemInflector area

Problem: Skew quadrupolar errors in this area cause verticaldispersion

DR FFS

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ATF2: Coupling & Dispersion problem

● With orbit correctors:  Large orbit bumps are required, which at the sextupoles produce large betatron coupling (T. Okugi ). 

● With skew quadrupoles: These certainly produce large betatron coupling (M. Woodley).

This vertical dispersion can be corrected in two ways:

No matter what large coupling needs to be corrected

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Coupling & dispersion problem: T. Okugi

In Okugi's approach existing skew quadrupoles are too weak.                    Solution:  new stronger skew quads?

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Coupling & dispersion problem: Woodley

Two extra skew quadrupoles in the inflector area are enoughto cancel vertical dispersion originated in this area. Couplingcorrection is easier than in Okugi's approach.However: Residual vert. dispersion cannot be handled.

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Coupling & dispersion problem: me

4 new dispersion + 4 betatron skew quads cancel any couplingand any dispersion.  However: Difficult correction procedureand we still need 4 new skew quads...

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Coupling & dispersion: conclusion

● If residual dispersion is below 5mm,                   M. Woodley's approach is the best.

● If residual dispersion is above 5mm,                         there is no easy solution.

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Summary & Outlook

● ATF and ATF2 are the largest facilities built exclusively to test Linear Collider's concepts. 

● Very open international collaboration:– Call for new R&D proposals at ATF (until May)

● Very interesting open problems

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Links

ATF2 third project meeting:http://ilcagenda.linearcollider.org/conferenceDisplay.py?confId=1295

ATF collaboration web page:                        http://atf.kek.jp/collab