ECAL Alignment with e and π data D. BOUMEDIENE LPC Clermont-Ferrand CALICE meeting – Argonne 19/03/2008.

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Presentation transcript:

ECAL Alignment with e and π data D. BOUMEDIENE LPC Clermont-Ferrand CALICE meeting – Argonne 19/03/2008

19/03/2008D. BOUMEDIENE | CALICE meeting, ANL2 Outlook Introduction Alignment with e data (y dimension) Method Results Alignment with π data (x and y dim.) Method Results and comparisons Conclusion

19/03/2008D. BOUMEDIENE | CALICE meeting, ANL3 Alignment with e - data Aim : To measure the position of the layers w. r. t. the first layer Used data: all 2006 e runs Event selection + Fiducial volume (  no lateral leakage and energy flat beam ) Method : Measurement of the relative position of the guard rings relatively to the first layer. Guard ring positions extracted from the energy profile. Energy profile : Energy in a layer = f ct ( track position on first layer ) Electron position on the first layer given by the tracking.

19/03/2008D. BOUMEDIENE | CALICE meeting, ANL4 Fit of the guard rings positions Usual Gaussian model The typical precision on the gap centre is 0.1mm / sample Exemple: layer #12, 20GeV

19/03/2008D. BOUMEDIENE | CALICE meeting, ANL5 Exemple : the 20 GeV sample of aug. 26 th 2006 Two remarks : The direction can be recontructed from the first 10 layers There is a systematic shift between the two layers of a given slab (mm, in the first layer CS) z layer

19/03/2008D. BOUMEDIENE | CALICE meeting, ANL6 Exemple : the 20 GeV sample of aug. 26 th 2006 After subtraction of the direction : layers alignment Systematic shift in a slabThe 9 th slab : singularity

19/03/2008D. BOUMEDIENE | CALICE meeting, ANL7 Mean positions over all 2006 data Remarks : Not large misalignment. Systematic shift between two layers of the same slab (with the exception of the 9 th slab) confirmed Can be refined by splitting the measurement over different periods (alignment per run / per day) The most misaligned slab +0.1mm (in first 2 stacks)

19/03/2008D. BOUMEDIENE | CALICE meeting, ANL8 On each slab Slab 0 Slab 1 Slab 2 Slab 3 Slab 4 Slab 5 Slab 6 Slab 7 Slab 8

19/03/2008D. BOUMEDIENE | CALICE meeting, ANL9 Layer positions per day (ly # 1 to 8) Day 1 Day 2 Day 3 Day 4 Day 5 Day 6 Layer 0Layer 1

19/03/2008D. BOUMEDIENE | CALICE meeting, ANL10 Alignment per day (ly # 9 to 17) Layer 9

19/03/2008D. BOUMEDIENE | CALICE meeting, ANL11 Example : alignment per run. Ly #9 to 17

19/03/2008D. BOUMEDIENE | CALICE meeting, ANL12 Mean positions over all 2006 data Detailed numbers and figures are given in CALICE Int. Note CIN-003 Precision better than 30 µm in first stack 100 µm in second stack 550 µm in third stack

19/03/2008D. BOUMEDIENE | CALICE meeting, ANL13 Alignment with π data Aim : measurement of the x and y position of the layers w. r. t. the first layer Used data: 2006 π runs (6, 17, 30, 40 and 50 GeV) Event selection : Cut on a “MIP χ ²“ (event / event basis) Consider layers with NHits layer < 5 (layer / layer basis) Method : Measurement of the relative position of the guard rings relatively to the first layer. Guard ring positions extracted from the profile of the number of hits in the layer vs. the track position on first layer ( cf. David WARD talk Ph. Meeting 31/10/07 ) Electron position on the first layer given by the tracking.

19/03/2008D. BOUMEDIENE | CALICE meeting, ANL14 Nb hits vs. track position Y tr0 X tr0

19/03/2008D. BOUMEDIENE | CALICE meeting, ANL15 Mean y positions from 2006 π data Précision better than 30 µm in first stack 50 µm in second stack 80 µm in third stack

19/03/2008D. BOUMEDIENE | CALICE meeting, ANL16 Mean y positions from 2006 π data But … Comparison with e - based alignment : Same precision in the first stack 2 times better in the second stack 6 times better in the third stack Position of layers 27 to 29 accessible

19/03/2008D. BOUMEDIENE | CALICE meeting, ANL17 Mean y positions over different 2006 π data ly4 ly10 e - data π data ly4 & 10 : to be understood Need to be refined : position per day

19/03/2008D. BOUMEDIENE | CALICE meeting, ANL18 On each slab (π samples) Shift = 30GeV 40GeV 50GeV The same effect is observed using independent π samples Compatible with the shift observed using e - samples 30 GeV 40 GeV

19/03/2008D. BOUMEDIENE | CALICE meeting, ANL19 Mean x positions over 40 GeV π data The nominal shifts of 2.5mm/slab and 1.3mm layer/layer were subtracted

19/03/2008D. BOUMEDIENE | CALICE meeting, ANL20 Mean value of x positions from 2006 π data Comparison with y alignment : same precision shifts in first stack <0.2 mm global shift of the 3rd stack ~1mm 6, 30 and 40GeV π

19/03/2008D. BOUMEDIENE | CALICE meeting, ANL21 Conclusion Method : The alignment can be performed using the guard ring positions in the x and y axis In y the precision varies from 30µm to 0.6mm with e- and 20µm to 70µm with π. For x the precision varies from 30µm to 130µm with π. Misalignment : The observed misalignment in the y axis is < 1.3 mm (electrons), <0.5mm (pions) The misalignment in x is < 0.3mm in the first stack, <0.5mm in the second stack. The third stack has a global shift of ~1mm Layers of the third stack are the most misaligned both in y and x Remarks : The alignment does not have any impact on the resolution/linearity A misalignment may bias (increase) the Molière radius, but the measured values in the x & y axis indicate a negligible effect ( < 1 mm). Taking into account the misalignment for the MC simulation should improve the agreement MC/data (interwafer gap description). There is a systematic shift in y axis between the guard rings on two layers of the same slab, except the 9th slab. The shift is 0.13±0.01mm.