Minutes for 07-Feb-2006 Telephone meeting
Present:
Anne-Marie Magnon Paul Dauncey, Hakan Yilmaz,
Fabrizio Salvatore, Michele Faucci-Gianelli, Mike Green,
Chris Targett-Adams,
George Mavromanolakis, David Ward, Wenbiao Yan,
Yoshi Mikami, Nigel Watson
Minutes: Nigel
- Notes from 24-Jan meeting
- Updates
- Monitor application test code -
George
Described his monitoring server/client framework, which
several people had volunteered to test for him. Chris had already
tried this, found easy to install, and the simple GUI and
production of histograms worked OK. Event display part of the
application can be configured to have different update
frequency from histograms, and may be useful to do this. Some
confusion about which process was client and which server,
different convention than some people had been familiar with.
Input is in form of binary files from DAQ, output is root file
from client. If a web server is running locally (or there is
writable area accessible from a central web server), can save .gif
to web pages for reference. Could also be run after end of run on
binary files for reference. George would also like to have
e.g. leakage current data available to histogram, and asked for
any feedback/bugs/requests for additional features from people who
tested it. (Since 7-Feb, Anne-Marie and Yoshi have also both
installed and tried out George's package.)
Discussion over how the package would deal with partially
completed runs, and distinguish between end of run and one in
progress - at some level, would rely on sensible manual intervention
from shift crew.
- Position
resolution in test beam data - earlier study by Mark
Stockton
Discussion about simulation of drift chamber and scintillator hits and the
information needed to study position resolution in ECAL. Scintillator uses
simtracker hits, drift chamber not certain. Would lose position
resolution if dch hits stored as SimCalorimeterHit (FS
clarified afterwards that dch stores its data as
SimTrackerHit). Note a significant difference in the information
defined by SimTrackerHits and SimCalorimeterHits is that the latter
should contain the momentum vector of the particle which initiated
the shower of which the current hit is a part, while tracker hits
contain momentum of the particle which created the individual hit
itself.
- Michele - ZHH studies
Had found that the missing energy in some events noted at a
previous meeting had been due to an overflow in the number of
hits in certain reconstructed tracks. This caused the
MarlinReco processor to lose information about the charged
particle momentum reconstructed in the tracking chambers.
Therefore, events with high energy muons were more affected than
those having electrons, as the electron energies were still
reconstructed by the calorimeters. This is a problem in
reconstruction rather than simulation, and Michele will for the
moment exclude these events (knowing that there may be some
small bias resulting from this).
- Mike G. - single electron resolution study
Used D09Scint model in mokka with 4T B field, had found DeltaE/E proportional to
1/sqrt(E) for intermediate energies of a few GeV, but differs
from this at both lower and higher energies. Had recently
carried out simulations without B field, and found (e.g.) mean
reconstructed energy of single 5 GeV electrons to be 4.8 GeV,
and noted that the response varied with the B field. With 4T
field, found r.m.s. DeltaE/E = 0.298 GeV, compared with 0.262
GeV for B=0.
Next, to try LDC01 model. David W. had found similar behaviour
with electrons ~1 GeV; also for muons, but due to the electron
component of the energy.
- Discussion of evolving task list
- volunteers
Long discussion of what we understood (or did not) about the
different items on this list. Revised list made public and sent
to CALICE mailing list, with intention of discussion at the
6-Mar meeting at UCL, and
assignment of names to tasks (to actually carry out the studies).
Integration with activity in HCAL in many areas would be natural but
we do not have this information at present.
- Plans for LCWS / ILC s/w meeting at Cambridge
- Test beam data analysis
- WW/ZZ separation plot - 0.3/sqrt(E)?
- Detector optimisation: variation of length, B field, radius,
granularity (longitudinal and transverse)
- Presentation of MAPS (concept, backed up by some performance
indicators, h/w and s/w aspects)?? Less likely
- Next steps