Garfield simulations on Micromegas CERN Summer Student Programme

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Garfield simulations on Micromegas CERN Summer Student Programme 2013 Tomohiro Yamaji SV: Theo Alexopoulos

Garfield simulations on Micromegas CERN Summer Student Programme 2013 Tomohiro Yamaji SV: Theo Alexopoulos

Objectives Garfield-9/++ simulation of Micromegas(MM) ◆Objictive : Making movies which describe how MM works

Objectives Garfield-9/++ simulation of Micromegas(MM) ◆Objictive : Making movies which describe how MM works  ・Simple configuration(2 D, flat cathode)  ・realistic structure(3 D, cathode stripe, not perfect)

How to make movies ①Garfield-9(source code modified)  ・Avalanche simulation(Call microscopic_avalanche)   The default setup of

How to make movies ①Garfield-9(source code modified)  ・Avalanche simulation(Call microscopic_avalanche)   The default setup of garfield-9 cannot write whole electron path to output files.    →source code is modified(Thanks to Mr. Kataoka)      When any drift lines are simulated, electron path are printed. ②Manipulate output files  ・Convert the structure of output files to simple ASCII format  ・For further manipulation, digitize data and do linear interpolations  ・Rearrange data according to time series ③Drawing movies  ・Processing 2, a java-like program which is suitable for drawing pictures/movies    

Movie(Simple configuration) ◆Very simple configuration  ・ 2 D, grounded wire. Flat cathode  ・primary electron

Movie(Simple configuration) ◆Very simple configuration  ・ 2 D, grounded wire. Flat cathode  ・primary electron starts between wires

Some features deduced from movie ◆drift property  ・electron   Electrons in an avalanche can reach

Some features deduced from movie ◆drift property  ・electron   Electrons in an avalanche can reach anode by about 1 nsec  gap between strips and mesh: 128 μm electron drift velocity in amplification region: 120μm/nsec  ・ions   Ions reach mesh by about 100~200 nsec   →Ions are one hundred slower than electrons   Some Ions(<10%) escape to drift region ◆apparent wrong behavior  ・amplification is very small, only about 100   →probably due to defects in integration parameters of microscopic method     By using AVALANCHE function, an amplification factor: ~5× 104     

Movie(more realistic)

Movie(more realistic)

Muon track

Muon track

Backups

Backups

Avalanche amplification in amplification region ◆simulation condition  ・ 2 D Cell grounded mesh →simple

Avalanche amplification in amplification region ◆simulation condition  ・ 2 D Cell grounded mesh →simple wire  ・No B field ・AVALANCHE function used ◆results  ・avalanche multiplication: ~5. 5× 104

Drift velocity/Lorentz angle ◆Drift property when B fields (perpendicular to E field) are induced

Drift velocity/Lorentz angle ◆Drift property when B fields (perpendicular to E field) are induced ・Drift velocity  vd=4. 6919 cm/μsec @E=600 V/cm, B=0 T  vd=4. 6299 cm/μsec @E=600 V/cm, B=0. 3 T ・Lorentz angle  17. 2071 deg @ E=600 V/cm, B=0. 3 T