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From: Frank Zimmermann <Frank.Zimmermann@cern.ch>
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To: sl clic studies <daniel.schulte@cern.ch>, francesco.ruggiero@cern.ch,
   frank.zimmermann@cern.ch, Grahame Blair <g.blair@rhbnc.ac.uk>,
   helmut.burkhardt@cern.ch, jacques.gareyte@cern.ch, john.jowett@cern.ch,
   juliette.thomashausen@cern.ch, maxim.korostelev@cern.ch,
   ralph.assmann@cern.ch, stefano.redaelli@cern.ch, thys.risselada@cern.ch
Subject: Summary of FAT/CLIC meeting 15 March
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Minutes of the FAT CLIC meeting on 15.03.2002

Present: R.A., H.B., M.K., S.R., T.R., D.S., F.Z. 


(1) CLIC Damping Ring Study (Maxim Korostelev)

Maxim solved the three coupled differential equations 
describing the time evolution of the emittance under
the influence of synchrotron radiation and intrabeam
scattering (Piwinski theory), using mathematica and
assuming a smooth approximation for the arcs made
from TME cells and for the wiggler sections.
He made a grid scan of the final equilibrium emittances as 
a function of both the horizontal emittance without intrabeam 
scattering and of the horizontal damping time, and from 
this he derived the optimum parameters for arcs and wigglers.

The low-current normalized emittance for this optimum 
case would be 465 nm, the horizontal damping time 4.2 ms;
the beam energy is 2.424 GeV, the ring circumference
268.8 m. Assuming an emittance coupling ratio of 3.8% 
he obtained a final horizontal normalized emittance 
of about 830 nm, and a rather large vertical emittance. 
The longitudinal emittance value meets the CLIC 
specification. Maxim showed the time evolution of 
emittances and IBS growth times during the store, 
for the same parameters. The final horizontal 
IBS growth time is about 8 ms.

He now plans to create a MAD model corresponding
to this parameter set, and then to compute IBS growth
rates with MAD. A study of the dynamic aperture 
and its optimization is also foreseen.

(2) Pantaleo's Damping Ring (Maxim Korostelev and
                             Frank Zimmermann) 

The parameters of Pantaleo's lattice are beam energy =
2.42 GeV, U0=0.57 MeV, Vrf=1 MV, C=180.15 m (this can 
fit 4-5 trains). The SR damping times are tau_x = 2.3 ms,
tau_y = 5.1 ms, tau_z=6.5 ms. The store time would be
much longer, about 50 ms.
The equilibrium emittances w/o IBS are 0.83 micron (x),
0.008 micron (y, 1% coupling), and sigma_z0=1.8 mm, 
sigma_delta0 = 1.2e-3. The longitudinal norm. emittance
is about 5000 eVm, exactly the CLIC requirement.

The IBS (emittance) growth times computed by MAD
are tau_x = 0.96 ms, tau_y=200 ms, tau_z=11.5 ms,
indicating that the horizontal blow up due to IBS 
will be quite substantial.

(3) 500-GeV Collimation System (Thys Risselada) 

Thys reported that an attempt to scale the 3-TeV
lattice to 500 GeV, increasing the bending angles 
by a factor of 4 and keeping all lengths constant,
was not successful. The chromatic properties of the
beam line degraded substantially (in particular the
energy dependence of the beta function), exactly the 
opposite effect of what was expected. On the positive side, 
it appeared that the unscaled 3-TeV collimation system 
might still work satisfactorily even at 500 GeV.

(4) Muon Studies and Visit of H.-J. Schreiber (Helmut Burkhardt)

Heinz-Juergen Schreiber (DESY/Zeuthen) visited CERN for two days 
at the beginning of the week. He fully supports the GEANT4 
programming effort of Helmut and collaborators. Heinz-Juergen
and Helmut discussed the EPAC paper on the CLIC muon studies. 
Concerning GEANT4, the new cross sections derived by the Russian 
collaborators and implemented by Helmut in the code are still 
confidential, until the collaborators have published their results.
Grahame Blair's program development should also be kept
in mind and integrated with the muon simulations. Grahame's
programme has the great advantage that it can read 
optics files produced by MAD. Heinz-Juergen is interested 
in the energy calibration for linear colliders, and he might
attend the Nanobeam 2002 workshop.

(4) Comparison of Simulation Codes (Stefano Redaelli, 
                                    Daniel Schulte)

Stefano showed a table comparing the simulation results
for a CLIC final focus, as obtained by DIMAD, MAD and Merlin.
He considered two different vertical emittances, beams with
and without nonzero energy spread, and with synchrotron 
radiation switched on or off. He used the same initial particle 
distribution for all tracking programmes. The agreement 
between the three codes is impressive. Discrepancies are 
mainly seen if synchrotron radiation is on, and here, 
the fluctuation for DIMAD seems to be higher than in the 
other two codes. For off-energy particles (no SR), 
MAD appears to be more different from DIMAD and Merlin. 

Stefano is presently trying to also get a result from PTC, 
with the help of Frank Schmidt. Without SR, PTC gives the 
same result as the other codes, but there is still a problem 
running the latest version of PTC including radiation. 

Ralph pointed out that Grahame's simulations should also 
be included in the code comparison.

Daniel presented results from an independent simulation
with PLACET (to which he has recently added bending magnets 
etc.). His results were in excellent agreement with the
other three codes, and extremely close to those of Merlin.
He pointed out that the generator of the synchrotron radiation 
energy spectrum is the same in both Merlin and PLACET. 
It is a generator written by Helmut Burkhardt.  

Daniel also mentioned that most of the blow up from
the Oide effect arises in the second-to-last quadrupole.

(5) AOB 

A discussion started on our strategy for integrated
simulations, the tools to be used, and the interfaces. 
There was no final conclusion, and this question 
will be a topic of the next meeting.
The Oide effect on the luminosity will be studied 
by Stefano with help from Ralph.

The next chairman will be Ralph Assmann.



************************************************************
Email: Frank.Zimmermann@cern.ch
Address: CERN, SL Division, AP Group 
CH-1211 Geneva 23, Switzerland
Telephone: +41 (22) 767 9054
TeleFax:   +41 (22) 783 0552




