I.Laktineh GranSasso MAY 2003 Stopping / at PSI dE/dX Measurement Bern, Naples,Neuchatel,Lyon Aim:...

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I.Laktineh GranSasso MAY 2003 Stopping / at PSI dE/dX Measurement Bern, Naples,Neuchatel,Lyon m: to identify stopping pions and muons in the bri using the dE/dX information. at is the difference with the Japanese attempt? In Europe we can obtain almost a pure beam of ons (muons) at PSI. no need for a sophisticated setup This will allow more efficient characterization specially with he European scanning system (access to grain information)

Transcript of I.Laktineh GranSasso MAY 2003 Stopping / at PSI dE/dX Measurement Bern, Naples,Neuchatel,Lyon Aim:...

Page 1: I.Laktineh GranSasso MAY 2003 Stopping  /  at PSI dE/dX Measurement Bern, Naples,Neuchatel,Lyon Aim: to identify stopping pions and muons in the bricks.

I.Laktineh GranSasso MAY 2003

Stopping / at PSI dE/dX Measurement

Bern, Naples,Neuchatel,Lyon

Aim: to identify stopping pions and muons in the bricks using the dE/dX information.what is the difference with the Japanese attempt? In Europe we can obtain almost a pure beam of pions (muons) at PSI. no need for a sophisticated setup

This will allow more efficient characterization specially with he European scanning system (access to grain information)

Page 2: I.Laktineh GranSasso MAY 2003 Stopping  /  at PSI dE/dX Measurement Bern, Naples,Neuchatel,Lyon Aim: to identify stopping pions and muons in the bricks.

At PSI we can use two beam linesPions beam PiM1 with strict cuts on the momentum

P = 200 MeV

Muon beam MuE1

P = 120 MeV muons produced from pion decay

collected in a solenoid.

(more information available on the PSI website)

Purity of each beam is about 99 %

Thanks to Urs, things can be done easily but we have to decideNOW

Page 3: I.Laktineh GranSasso MAY 2003 Stopping  /  at PSI dE/dX Measurement Bern, Naples,Neuchatel,Lyon Aim: to identify stopping pions and muons in the bricks.

x(µ)

y(µ)

x(µ)

z(µ)

Muons(without decay products)

Page 4: I.Laktineh GranSasso MAY 2003 Stopping  /  at PSI dE/dX Measurement Bern, Naples,Neuchatel,Lyon Aim: to identify stopping pions and muons in the bricks.

Pions(without decay products)

z(µ)

x(µ)

x(µ)

y(µ)

Page 5: I.Laktineh GranSasso MAY 2003 Stopping  /  at PSI dE/dX Measurement Bern, Naples,Neuchatel,Lyon Aim: to identify stopping pions and muons in the bricks.

The mean distance of the pions in the brick is 5 cmThe mean distance of the muons in the brick is 2.5 cm Rate: from 100-1000 particles/ cm2

Strategy to follow

Take two bricks (or two half-bricks with lead in front)add 2-3 emulsion sheets together in the front (inside ?)( to cut bgk)

Expose each to both beamsone half for the pions, one half for the muons ( to reduce systematic)

Page 6: I.Laktineh GranSasso MAY 2003 Stopping  /  at PSI dE/dX Measurement Bern, Naples,Neuchatel,Lyon Aim: to identify stopping pions and muons in the bricks.

Brick preparation and development at cern (Gianni)Scanning in Lyon, Bern and also in Naples laterInvolved persons: Urs, Jerome, Igor, Samuel, Frederic, Markus, Imad, Perrine, Giovanni, NicolaDevelopment (thickness? More than 44 microns if possible)

When ? July seems to be the best for allScanning:Lyon : (at least 50% of time)Bern : (at least 80% of time)Naples : ?

Page 7: I.Laktineh GranSasso MAY 2003 Stopping  /  at PSI dE/dX Measurement Bern, Naples,Neuchatel,Lyon Aim: to identify stopping pions and muons in the bricks.

Conclusions

• Tough but challenging and necessary study for OPERA

• We are collaborating with our Japanese colleagues in order to get profit of their experience (Toshito)

• The European scanning system advantages can be tested

• This study is necessary for the exotic decay of the Lead proposed by the Bologna group (see Miriam talk)

WE REQUEST TWO BRICKS FOR JOLY (if possible)