Linear Collider Detector
R&D Issues
The planning for the linear collider
detector research and development program will first
require a careful analysis of the most important and relevant
R&D goals. In order to present an initial point for discussion,
we offer the following comments on some of the issues.
Your comments and criticism are welcome.
-- Jim Brau
General Goals
Our goal is to be prepared to submit a detailed technical proposal for an experiment in a few years (when the accelerator proposal is ready).
We must evaluate subsystem by subsystem what needs to be developed or
demonstrated. Of course the overall detector function is the most
important issue, and subsystem choices constrain other subsystems.
So integration into a full detector, respecting the overall constraints,
on the one hand, while optimizing the performance, can be a challenging
effort.
In previous studies of the Linear Collider
physics, the most important constraints on the detector have come from the
following considerations:
- Hermeticity (good forward coverage)
- Charged track momentum resolution
- Charged track impact parameter resolution (heavy flavor tagging with the highest possible level of efficiency and purity)
- Electromagnetic & hadronic calorimeter energy resolution
- Granularity (calorimeter segmentation, 2-track separation)
- Electron / muon identification
In addition, special needs for the Linear Collider Detector include:
- Shielding from beam-induced e+e- pairs
- Accurate differential luminosity measurement
- Subdetectors that correctly handle 90 bunches / train at 2.8 ns separation (see TESLA parameters below)
Special constraint:
Final focus quads (2 meters from I.P.) that must be anchored to bedrock
Reminder of the LC Beam Parameters (see below for TESLA parameters ):
- Ecm = 0.5 Tev (L ~ 5 x 1033)
- Ecm = 1 - 1.5 TeV (L > 1034)
- 90 bunches per train (bunch spacing 2.8 nsec)
- 120 - 180 trains/second
- P(e-) ~ 80%
- Backgrounds:
- muons - < 1 mu / train
- synchrotron rad. - collimation controlled
- e+e- pairs - potential problem -> large B field
- mini-jets (gamma-gamma -> hadrons) few jets per train @ 1 TeV
-> timing to 1 nsec useful
- Beam spot size:
- tiny
- sigma(X) ~ 0.3 microns
- sigma(Y) ~ 0.006 microns)
- know to
- sigma(XY) ~ 4 microns
- sigma(Z) ~ 10 microns)
- Beamstrahlung:
- ave(del E) ~ 3% @ 0.5 TeV
- ave(del E) ~ 12% @ 1.0 TeV
- TESLA
- Different parameters, such as 4500 bunches/train at 189 nsec spacing @ 800 GeV
- TESLA parameters are available on the web
A central issue is the overall size of the detector.
While many different options for the geometry could be considered, many considerations
drive the design to one of two limits:
- A large detector, which optimizes the tracking and calorimeter segmentation, with a relatively low magnetic field. This choice will result in beam backgrounds that limit the vertex detector.
- A compact detector with a high magnetic field, allowing very close pacement of the vertex detector, but with small size constraining the tracking and calorimetry.
It is important to understand the strengths and weakness of each of these strategies, as well as alternative strategies which might be proposed.
CCD Vertex Detector Development
The physics of LC demands the best possible vertex detector performance, enabling
clean separation of b, c, and udsg jets, and tau's
Vertexing provides:
- background suppression
- combinatorial reduction within events
- measurement of key branching rations
- H -> bb
- H -> cc
- H -> light quarks and gluons
The route to optimized flavor tagging follows from:
- track resolution
* determined by technology:
CCDs, active pixels, others ??
- outer radius
* constrained by outer detector
compact, conventional, ??
- inner radius
* limited by LC parameters and detector field
( beam backgrounds
( B-field to constrain
- radiation immunity
* improve CCDs, or pixels
The current state-of-the-art on CCDs for linear collider vertex detectors is:
- SLD vertex detector operating with 307,000,000 pixels
- 10 MHz readout of CCDs developed (5 MHz operational)
- 5 micron point resolution
- exceptional efficiency and purity
Linear Collider physics requirements justify further improvements,
which can be divided in the following areas of R&D:
- Development of Technology (or Technologies):
CCDs (and APS active pixel sensors? or other concepts?)
- Demonstration of technical suitability and selection
- Minimization of the beampipe radius (with a 1 cm goal).
The Linear Collider
Vertex Detector design goals are:
- Maximum Precision ( < 5 microns)
- Minimal Layer Thickness
( -> 0.12% X0)
- Minimal Layer 1 Radius (-> 12 mm)
- Polar Angle Coverage (cos theta ~ 0.9)
- Standalone Track Finding (perfect linking)
- Layer 1 Readout Between Bunch Trains (4.6 msec)
- Deadtimeless Readout (high trigger rate)
Directed R&D efforts will be aimed at
- increasing the readout speed to 50 MHz
- developing a thinner ladder (0.12% X0)
- improving the radiation hardness (with supplementary channels)
Simulation studies are a very important element of the R&D program.
Some of the initial simulation studies will concentrate on the following
issues:
- Apply heavy quark tag performance to physics channels
- Investigate stand-alone track finding: 1.) background tolerance,
and 2.) layer 1 issues
- Develop detailed CCD signal simulation: how can the point resolution be improved even further?
- Create detailed GEANT model of vertex detector and investigate impact of material on overall LC detector performance
- Continue studies of the issues impacting systems outside the vertex detector (machine backgrounds, solenoidal field, etc.)
Tracking Issues
Some of the issues that must be understood:
- What is the tracking volume? (this will be constrained by
the overall detector design)
- What resolution is needed? This issue is coupled to
the jet reconstruction issues of the calorimeter subsystem.
The smaller tracking volume of a compact detector may be
ameliorated with higher magnetic fields and better point precision
(for example with silicon) but at lower momenta (and not so low)
the multiple scattering will degrade resolution.
- Is outer tracking one technology or more?
- What technology is it?
- straw tubes (inner?)
- scin fibers (inner?)
- silicon strips (Snowmass)
- TPC (ECFA)
- Drift (JLC)
- GEM
- MSGC
- Occupancy
- Forward Tracking
Particle ID?
- Is there any?
- what are the physics requirements?
- If so, what?
- Presampler?
Calorimetry
The goals for the calorimetry are precise electron and gamma measurements,
jet reconstruction and measurements, and missing energy measurements.
For the electromagnetic calorimeter, one important benchmark process
is the measurement of the Higgs decay to two photons. Naively, this
process calls for the best possible electromagnetic resolution.
However, the precise impact of lessened EM resolution (as a trade-off
for improved jet resolution) needs to be more fully undersood.
The traditional jet measurement strategy is to
measure the jet energy through total absorption in a calorimeter.
It is thought that at the Linear Collider a different strategy will
be more effective. This involves reconstructing the jet energy by
measuring the deposition in the tracker and the calorimeter detectors,
and then reconstructing the jet. The procedure, sometimes referred to
as an "energy flow analysis," appears in at least two manifestations:
- In one, the tracker and electromagnetic energies are combined
directly, and the hadronic calorimeter response is applied as a correction.
This approach has been promoted at ALEPH.
- Alternatively, the calorimeter energy can be summed and a tracking
correction applied. This approach is closer to the traditional
approach.
In each of these approaches, and particularly in the first, the
granularity of the electromagnetic calorimeter is critical in separating
the electromagnetic energy deposition from incoming charged particles.
Very detailed longitudinal granularity could help here.
The calorimeter subsystem will focus on the key issues of
- energy resolution
- granularity
- longitudinal segmentation
- tolerance to high magnetic field
The calorimeter group must work through
many options with different advantages and
determine the relative importance of the feature each brings to the
application.
The calorimeter working group must also ensure that the masking design to control the fluence of synchrotron radiation, and pairs, does not unacceptably impact the calorimeter performance (see Backgrounds below).
Muon Detection
The muon system must reside outside of the rest of the detector
volume, and therefore is highly constrained and driven by inner detector choices. The physics requirements need to be more precisely defined.
Presumably, the precision of the inner tracker is adequate for momentum
measurements. This would require the muon system to tag and trigger on muons.
What performance is needed to achieve these goals?
Trigger and DAQ
A system with flexibilty to adjust for the backgrounds must be developed.
The strategy for triggering on each of the physics signatures needs to
be enunciated.
Luminosity Measurement
The colliding electron and positron bunches disrupt one another and induce
radiation, and the actual luminosity and energy spectrum of e+e- annihilation reactions depends on these effects. Therefore, it is important to measure the differential luminosity spectrum directly. This requires an acollinearity angular
measurement for the small-amgle Bhabha scattering to better than 1 mrad at
theta ~ 200-500 mrad. An electromagnetic calorimeter with such precision must
reside within the synchrotron radiation mask.
Polarization Measurement
It will be necessary to measure the polarization of the beam (or beams)
at the Linear Collider. Presumably this will be accomplished with the
Compton scattering technique which has been so successfully exploited at
the SLC. However, thinking and plans need to begin.
- Where will the detector be located?
- What backgrounds will need to be dealt with?
- Will the detector need to provide some background immunity.
- What will the chromatic effects be?
Backgrounds
Experience with SLC and simulations of the Linear Collider have led to the
following estimates of the expected backgrounds. Here we see tolerable
levels, but it will be wise to prepare for the unexpected.
- muons - < 1 mu / train - limited by toroidal muon spoilers
- synchrotron rad. - masking and collimation critical in controlling this very large background.
- e+e- pairs - potential problem (105 pairs per bunch crossing) -> large detector B field required
- mini-jets (gamma-gamma -> hadrons) few jets per train @ 1 TeV
(timing to 1 nsec useful)
The shielding of the detector to backgrounds requires masking at small angles, as mentioned above. The design of this masking system must be studied in conjunction with the performance of the subsystems (i.e. calorimetry) to ensure acceptable impact on the hermiticity of the detector.
Simulation
see
Plans for the US/Canada Linear Collider Detector
Simulation Study
Comment
An important general issue for all subsystems is timing.
Does an individual subdetector try to
keep track of signal times well enough
to make its own bunch assignment or
does it rely on global pattern recognition
to sort things out later?
Conclusion
There are many issues that need to be resolved in order confidently propose an experiment for the next Linear Collider.
Now is the time to get on with planning and executing the detector R&D.
Next we need to develop detailed plans covering all subsystems and issues.
References:
- Zeroeth-order Design Report for the NLC, SLAC Report 474
- Physics and Technology of the NLC, SLAC Report 485
- Snowmass 96, New Directions for HEP, DPF/DPB of APS
- JLC Physics (www-jlc.kek.jp)
- DESY 1997-048, Concept. Design Report for a 500 GEV e+e- LC.....
- 2nd Joint ECFA/DESY Study, Orsay (April, 1998), www.desy.de