Difference between revisions of "Twin Tubes"
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| − | == What are Twin Tubes? == | + | === What are Twin Tubes? === |
The precision measurements of muons in ATLAS are done by Monitored Drift Tubes (MDT's). The whole muon spectrometer will reach precision smaller than 80 <math>\mu m</math> in the bending direction of the magnetic field. Many corrections need to be done to get the actual drift-time from measured signals. The correction for the delay due to the signal propagation along the tube turns out to be one of the larger corrections. The longer the signal has to travel along the wire the larger the correction, so outer chambers particularly 5m-long BOL's need precise measurement of the hit position along the tube. In the original design of ATLAS the position of the hit along the tube is measured by trigger chambers (RPC's). However the '''twin tube''' concept enables us to measure the propagation correction using MDTs themselves. | The precision measurements of muons in ATLAS are done by Monitored Drift Tubes (MDT's). The whole muon spectrometer will reach precision smaller than 80 <math>\mu m</math> in the bending direction of the magnetic field. Many corrections need to be done to get the actual drift-time from measured signals. The correction for the delay due to the signal propagation along the tube turns out to be one of the larger corrections. The longer the signal has to travel along the wire the larger the correction, so outer chambers particularly 5m-long BOL's need precise measurement of the hit position along the tube. In the original design of ATLAS the position of the hit along the tube is measured by trigger chambers (RPC's). However the '''twin tube''' concept enables us to measure the propagation correction using MDTs themselves. | ||
=== Operating Principle === | === Operating Principle === | ||
Two MDTs are interconnected at the high voltage (HV) end via an impedance matched jumper. Consequently the tubes are read-out at both ends. A muon hitting an MDT not only creates a signal in the hit tube but as well a signal in its twin partner. The time difference between these two signal is used to calculate the propagation correction. | Two MDTs are interconnected at the high voltage (HV) end via an impedance matched jumper. Consequently the tubes are read-out at both ends. A muon hitting an MDT not only creates a signal in the hit tube but as well a signal in its twin partner. The time difference between these two signal is used to calculate the propagation correction. | ||
| − | [[Image:Twin tube pair.jpg|left|thumb| | + | [[Image:Twin tube pair.jpg|left|thumb|200px|Schematic view of the operating principle of a twin pair]] |
| − | For further details on the concept and performance reader is refered [http://www. | + | Twin tubes have been succesfully tested on BOL chambers in Amsterdam, BOS chambers in Munich and recently on an EOL chamber at CERN. For further details on the concept and performance reader is refered to a [http://agenda.cern.ch/askArchive.php?base=agenda&categ=a054212&id=a054212s11t2/moreinfo talk] given at Cetraro ATLAS Muon Workshop and a [http://www.sciencedirect.com/science?_ob=MImg&_imagekey=B6TJM-4J32H1V-2-2X&_cdi=5314&_user=606230&_orig=search&_coverDate=05%2F10%2F2006&_qd=1&_sk=994399997&view=c&wchp=dGLbVlz-zSkWA&md5=ac40d0dffbfb3883fd8885ff1b1ac935&ie=/sdarticle.pdf paper] published in Nuclear Instruments & Methods in Physics Research. |
=== Current Status === | === Current Status === | ||
| + | As was proposed and accepted a few BOL chambers will be equipped with twin tube HV-cards in the region where there is limited coverage by the trigger chambers. One multilayer of '''BOL4A13''' and one of '''BOL4C13''' were fit out with twin tube cards. Subsequently they have succefully passed the BB5 test procedure and are awaiting installation. Both chambers are accessible for replacement of the twin tube cards if need be. | ||
| + | |||
| + | Software used for online DAQ need not be modified for chambers with twin tube cards. NIKHEF will provide software to store, calibrate and analyse the twin information in the muon Event Data Model for offline analysis. | ||
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| + | ''More references:'' | ||
| + | *[http://cdsweb.cern.ch/search.py?recid=620198&ln=en ''Precision of the ATLAS muon spectrometer; Martin's PhD Thesis''] | ||
| + | *[http://www.nikhef.nl/~ajkoutsm/TwinTubes.ps ''Pulse Analysis for ATLAS MDT Twin Tubes; Alex' Master Thesis (.ps-file)''] | ||
Latest revision as of 11:53, 29 September 2006
What are Twin Tubes?
The precision measurements of muons in ATLAS are done by Monitored Drift Tubes (MDT's). The whole muon spectrometer will reach precision smaller than 80 in the bending direction of the magnetic field. Many corrections need to be done to get the actual drift-time from measured signals. The correction for the delay due to the signal propagation along the tube turns out to be one of the larger corrections. The longer the signal has to travel along the wire the larger the correction, so outer chambers particularly 5m-long BOL's need precise measurement of the hit position along the tube. In the original design of ATLAS the position of the hit along the tube is measured by trigger chambers (RPC's). However the twin tube concept enables us to measure the propagation correction using MDTs themselves.
Operating Principle
Two MDTs are interconnected at the high voltage (HV) end via an impedance matched jumper. Consequently the tubes are read-out at both ends. A muon hitting an MDT not only creates a signal in the hit tube but as well a signal in its twin partner. The time difference between these two signal is used to calculate the propagation correction.
Twin tubes have been succesfully tested on BOL chambers in Amsterdam, BOS chambers in Munich and recently on an EOL chamber at CERN. For further details on the concept and performance reader is refered to a talk given at Cetraro ATLAS Muon Workshop and a paper published in Nuclear Instruments & Methods in Physics Research.
Current Status
As was proposed and accepted a few BOL chambers will be equipped with twin tube HV-cards in the region where there is limited coverage by the trigger chambers. One multilayer of BOL4A13 and one of BOL4C13 were fit out with twin tube cards. Subsequently they have succefully passed the BB5 test procedure and are awaiting installation. Both chambers are accessible for replacement of the twin tube cards if need be.
Software used for online DAQ need not be modified for chambers with twin tube cards. NIKHEF will provide software to store, calibrate and analyse the twin information in the muon Event Data Model for offline analysis.
More references: