Llea Nasira Samuel Benedict College Charlotte Wood-Harrington

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Presentation transcript:

Drift Time Analysis in ATLAS Muon Spectrometer Under Varying Gas Conditions Llea Nasira Samuel Benedict College Charlotte Wood-Harrington Quarknet Research Program Advisor: Daniel Levin University of Michigan REU 2007 Wednesday 8 August, 2007 Llea Nasira Samuel

Purpose What we are trying to understand if we can distinguish between two different scenarios for an observed change in the maximum drift time: a change in CO2 or perhaps a small diffusion of water vapor into the system. 08/08/2007 Llea Nasira Samuel

Muons and Muon Tracking An elementary particle which can have either a positive or negative electric charge; spin of 1/2. It is the decay product of many particles, one of these being the Higgs: H →Z Z*→ µ-µ+µ-µ+ We can reconstruct events by identifying the muon’s tracks and measuring its momentum 08/08/2007 Llea Nasira Samuel

Muon Spectrometer The muon spectrometer is used in the ATLAS experiment to identify and measure the muon momentum One of its major components: Monitored Drift Tube Chambers Drift Tubes help to provide precise co-ordinate measurements of the muon track 08/08/2007 Llea Nasira Samuel

A 3-D event display of a cosmic muon event, showing the path of a muon traveling through three layers of the barrel muon spectrometer. Three of the eight coils of the barrel toroid magnet can be seen in the top half of the drawing. 08/08/2007 Llea Nasira Samuel

MDT Chambers BARREL DRIFT TUBE CHAMBER 08/08/2007 Llea Nasira Samuel

Schematic view of MDT Aluminum tubes: diameter= 30mm Central tungsten wire: diameter= 50m Tube length:1m-6m ~ 1200 of these chambers in the ATLAS experiment 08/08/2007 Llea Nasira Samuel

MDTs Sense Wire: Aluminum Tube: Gas : Gold-plated Tungsten wire r = 25μm V= 3080 V Stretched by 350g of tension Aluminum Tube: radius inner= 1.46 cm radius outer =1.5 cm Gas : Mixture 93.0% Ar, 7.0% CO2 Pressure: 3 bar Temperature: ~293K Aluminum Tube Gas flow at 1V per day Sense Wire 08/08/2007 Llea Nasira Samuel

Tracking muons Aluminum Tube Electrons drifting toward sense wire Drift Radius Muon Track 08/08/2007 Llea Nasira Samuel

Drift Radius vs Drift Time (RT) Function 08/08/2007 Llea Nasira Samuel

Tracking muons 08/08/2007 Llea Nasira Samuel

Muon Paths Drift Tubes NOT drawn to scale MONTIORED DRIFT TUBE CHAMBER 08/08/2007 Llea Nasira Samuel

Mini MDT Chamber Scintillator 08/08/2007 Llea Nasira Samuel

Monitor on surface station SGX-1 Mini Drift Tube Chamber fresh gas Mixing station Cavern MDT CHAMBERS

Garfield Simulations and Results Garfield: software package created by Rob Veenhof Used to 1) model the MDT tube geometry 2) model the gas mixture 3) model the electric field 4) model the gas properties: temperature and pressure 08/08/2007 Llea Nasira Samuel

DR vs DT: Water 08/08/2007 Llea Nasira Samuel

DR vs DT: CO2 08/08/2007 Llea Nasira Samuel

DR vs DT: Pressure DR vs DT: Temperature 08/08/2007 Llea Nasira Samuel

The graph shows the change in drift time vs drift radius when the mixture is at Ar: 92.4%, CO2: 7.6%. Barely any difference can be seen by the electrons within the first 4 mm from the sense wire. However, after this, there is a steady increase leading to an overall increase of about 0.7 s for the electrons coming -from the electron wall- to make it to the sense wire. 08/08/2007 Llea Nasira Samuel

The graph shows the change in time against the radius when the mixture is at Ar: 92.0%, CO2: 7.0%, H2O: 0.1%. This graph seems to show almost no change in the time taken for electrons to reach the sense wire for the first 0.4 cm. The difference comes after this as a steady rise is seen which makes a maximum time increase of a little less than 0.06 s. 08/08/2007 Llea Nasira Samuel

Drift Time Difference (ns) 08/08/2007 Llea Nasira Samuel

VERY PRELIMINARY Drift Time Difference (ns) 08/08/2007 Llea Nasira Samuel

08/08/2007 Llea Nasira Samuel

Conclusions With a lot more work still to be done, it may be possible to determine, with the use of Garfield, whether variation in DR-DT functions are caused by CO2, or by water contamination. 08/08/2007 Llea Nasira Samuel

Acknowledgements Dr Daniel Levin Prof Jean Krisch Prof Homer Neal Dr. Steven Goldfarb Charlotte Wood-Harrington All members of the MDT group *** National Science Foundation *** ***University of Michigan*** 08/08/2007 Llea Nasira Samuel

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