- 117 Views
- Uploaded on
- Presentation posted in: General

Manchester and Collimation studies

Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author.While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server.

- - - - - - - - - - - - - - - - - - - - - - - - - - E N D - - - - - - - - - - - - - - - - - - - - - - - - - -

Manchester and Collimation studies

Roger Barlow

Manchester/Cockcroft

New Institute for UK Accelerator Science

Manchester-Liverpool-Lancaster joint project

Located at Daresbury

Working closely together with CCLRC ASTeC group

ILC central (but not only) theme

COLSIM meeting, CERN, Dec 4 2006

NS-FFAG (EMMA) construction

- Roger Barlow
- Adriana Bungau
- Adina Toader

- Rob Appleby
- Dragan Toprek
- Federico Roncarlo
- Anthony Scarfe

- Roger Jones
- Ian Shinton
- Chris Glasman
- Ben Spencer
- Narong Chanlek

- Ian Shinton
- Keith Potter (Hon. Prof.)
- New lecturer being advertised

Collimation and Wakefields for EuroTev and LC-ABD

ILC Beam Dump

2mrad optics

LHC through FP420

Wakefields in RF cavities, HFSS, LIAR, GDFIDL

COLSIM meeting, CERN, Dec 4 2006

COLSIM meeting, CERN, Dec 4 2006

- Damage studies. GEANT4 simulation compared with FLUKA (Adriana)
- Effect of collimation on beam (Adriana)
- SLAC ESA beam tests (Adriana)
- Halo: Production and behaviour. Long talked about but never started. Adina now learning PLACET to do this
- Wakefields: Implementation of short-range (intra-bunch) wakefields in Merlin (and other programs?): rest of talk

COLSIM meeting, CERN, Dec 4 2006

r’

s

s

r

Effect of leading particle on trailing particle, integrated over path through aperture and ignoring transverse motion during passage, is Impulse W(r,r’,s)

Dimensions of Potential

Maxwell’s EquationsW is the derivative of some function which is a solution of the 2D Laplacian

Fourier Expansion in angle gives (= -’) for devices with axial symmetry

wT = m Wm(s) r’m rm-1 [cos(m) r- sin(m)]

COLSIM meeting, CERN, Dec 4 2006

COLSIM meeting, CERN, Dec 4 2006

Less calculation means losing detail

- Impulse on trailing particle of single particle leading by distance s . ‘wake potential’.
- Impulse on trailing particle of slice of particles leading by distance s: Merlin
- Impulse on trailing particle from all leading particles:(s’) W(s’-s) ds’.‘bunch potential’: PLACET
- Average Impulse. (s’) (s) W(s’-s) ds ds’Most literature
But going from 12 gives massive computation gain for almost no loss of detail

COLSIM meeting, CERN, Dec 4 2006

Divide ~100,000 particle bunch into ~100 slices

Transverse wakefield*.

Dipole (m=1)term only

Ignores axial component

y’= Wcomponent(s) Qslice

(Q is slice charge x offset)

W(s) evaluated only ~100 times

Takes ~100,000 x 100 /2 rather than ~100,000 x 100,000/2 calculations

W(s) function cunningly attached to beamline component

* MERLIN also does longitudinal wakefields, but they’re not very important for collimators

COLSIM meeting, CERN, Dec 4 2006

- Include more modes W(m,s)
- Include axial terms. Not just T but x and y
Ignoring axial force. assumes =’

beampipe

bunch

COLSIM meeting, CERN, Dec 4 2006

wT = m Wm(s) r’m rm-1 [cos(m(- ’)) r- sin(m(- ’))]

rand unit vectors resolved into x,y

Leading and trailing particle quantities all mixed up, but…

Putting it all together and applying trig formulae the effect o a particle due to a slice is

WX = m W m (s) rm-1{ C m cos[(m-1) ] + S m sin[(m-1)]}

WY = m W m (s) rm-1 { S m cos[(m-1)] - C m sin[(m-1) ]}

where C m= r’m cos(m’) S m= r’m sin(m’)

Factorisation!!

Simple sum over <trailing particle>x<aperture>x<leading slice> terms and can be calculated almost as easily as standard Merlin

COLSIM meeting, CERN, Dec 4 2006

- Couple of changes needed to Merlin (functions made virtual)
- New SpoilerWakeProcess class that does the summations. Inherits from WakeProcess
- New SpoilerWakePotentials class that provides prototypes for W(m,s) functions. Inherits from WakePotentials. Pure virtual.
- Particular collimator types implemented by providing a class that inherits from SpoilerWakePotentials and provides actual W(m,s)

COLSIM meeting, CERN, Dec 4 2006

Tapered collimator – diffractive regime

Wm (s)= 2(1/a2m- 1/b2m)e-ms/a(s)

TaperedCollimatorWakePotentials:SpoilerWakepotentials{

double a,b;

double* coeff;

public:

TaperedCollimatorWakePotentials(double aa, double bb, int nmax){

a=aa;

b=bb;

nmodes=nmax; // nmodes is a data member of SpoilerWakePotentials

coeff=new double[nmodes];

for (int i=0;i<nmodes;i++) {coeff[i]=2*(pow(a,-2*i)-pow(b,-2*i);}

}

~TaperedCollimatorWakePotentials(){delete[]coeff;}

Wtrans(double s, int m){return s>0? coeff[m]/exp(m*s/a):0);}

}

COLSIM meeting, CERN, Dec 4 2006

- Charge 2 1010
- x=3 m
- y=10 m
- x=36 10-9 mm
- y=1 10-9 mm
- E=1.19 GeV
- Z=0.65 mm
- Collimator Aperture 1.9 mm length 40 cm

COLSIM meeting, CERN, Dec 4 2006

nmodes 1 2 3 4 5

Offset

.5mm

1mm

1.5 mm

COLSIM meeting, CERN, Dec 4 2006

- For small offsets, dipole mode is good enough
- For large offsets, dipole mode is not good enough
- Kick factors (<y’/y>) are not enough. There is a big variation in the kick (which increases ) and it is systematic so shape is non-Gaussian. After the first collimator anyway
- For detailed studies we need to know particle-by-particle wake. Not integrated over Gaussian – the code does that

COLSIM meeting, CERN, Dec 4 2006

Formulae given – CLIC note 671

y’=(2Nre/a2) exp(z2/2z2) y

(diffractive regime)

Clearly has shape folded in – need to unfold

Cannot trace in Stupakov(1995)

Positive exponential is puzzling

Still, can implement as MERLIN class…

COLSIM meeting, CERN, Dec 4 2006

1.0 mm offset

.5 mm offset

Effect increases with offset

Scale is crazy – probably simple units problem

Behaviour at large z incomprehensible

1.5 mm offset

COLSIM meeting, CERN, Dec 4 2006

Roger:

- Talk tomorrow to experts here and understand formulae and how to implement them
- Implement other standard aperture formulae
- Extend to non-axial apertures.. (Chao ‘considerably more complicated’. Yokoya + Stupakov for Gaussian bunch?) Possible at the expense of another summation?
- Implement in other codes? BDSIM unsuitable(?) . PLACET looks possible
Adina

- Retrain as accelerator physicist
- become familiar with using PLACET – use for halo simulations
- Visit CERN for ~2 weeks in New Year to gain experience
- Numerical wakefield simulation and adaptation to MERLIN-style approach
Adriana

– next talk

COLSIM meeting, CERN, Dec 4 2006