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First Look at EMEC Weights using the FFT Algorithm Combined Test Beam Meeting 19 November 2002 Naoko Kanaya & Rob McPherson University of Victoria.

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Presentation on theme: "First Look at EMEC Weights using the FFT Algorithm Combined Test Beam Meeting 19 November 2002 Naoko Kanaya & Rob McPherson University of Victoria."— Presentation transcript:

1 First Look at EMEC Weights using the FFT Algorithm Combined Test Beam Meeting 19 November 2002 Naoko Kanaya & Rob McPherson University of Victoria

2 2002-11-19Rob McPherson2 Overview  Want to predict physics pulse shape from calibration pulse shape Use this for determining “optimal” filtering weights  At least two methods “on the market” Time domain convolution “NR” method Kurchaninov/Strizenec used in previous HEC analyses Fourier transform “FFT” method Neukermans, Perrodo, Zitoun, used in EM community  Here we look at the FFT method for the EMEC in the 2002 combined run

3 2002-11-19Rob McPherson3 FFT Method I  See: ATL-LARG-2001-008 Idea is to simplify the complicated picture:

4 2002-11-19Rob McPherson4 FFT Method II  Very simplified picture:  Calibration current:   Exponential  Ical(t)  Y (t) (  + (1-  )exp(-t/  c ))  Physics current:  Triangle  Iphy(t)  Y (t) Y(-t)(1-t/  d )) MeasureMeasure Uphy(t)Uphy(t) Ucal(t)Ucal(t)

5 2002-11-19Rob McPherson5 FFT Method III  Use FT “transfer function” property: Time Domain Convolution  Frequency Domain Multiplication  Ingredients Measured physics pulse shape Uphy(t) (take 128 samples in 1nsec bins) Calculate (discrete) FFT[Uphy(t)] = DFT[Uphy](  ) Assume: FT[Uphy](  ) = FT[Iphy](  ) x H det  ) x H ro  ) Measured calibration pulse shape from delay runs Ucal(t) (also 128 x 1 nsec) Calculate (discrete) FFT[Uphy(t)] = DFT[Ucal](  ) Assume: FT[Ucal](  ) = FT[Ical](  ) x H cal  ) x H ro  )

6 2002-11-19Rob McPherson6 FFT Method IV  Finally: FT[Uphy](  ) = FT[Ucal](  ) x G (    In simple model: G ana (   FT[Iphy](  ) /FT[Ical](  ) x  0 2 / (  0 2 -  2 ) With  0 2 = 1 / LC  Algorithm: 1) Measure Ucal(t) with delay run 2) Calculate DFT[Ucal](  3) Predict FT[Uphy](   2 free parameters: LC and t 0 (Iphy – Ical) 4) Calculate predicted Uphy(t  5) Minimize predicted-measured Uphy(t   Using uncorrelated  2 with unit error for now

7 2002-11-19Rob McPherson7 Data and Tools  Physics and calibration data athena  root file  In root: use “fftw” ( http://www.fftw.org ) http://www.fftw.org  Physics run: 13153 in middle gain 120 GeV e, 20000 events channel : 897 (  = 8  =17 layer=2(middle)) E cubic >0.4*Etot TDC: wac=720, guard_region=20)  Calibration run: 12836(middle gain) DAC4000 - DAC10

8 2002-11-19Rob McPherson8 First attempt at fit  See oscillations in best predicted pulse:  Best parameters, fixed = 450 nsec, =370 nsec: (note: not yet fitted, just scanned and minimum found)  Best parameters, fixed  d = 450 nsec,  c =370 nsec: (note: not yet fitted, just scanned and minimum found) LC = 19.5 nHxnF t 0 = 6.1 nsec  0.075 Maximum residual: 7.1%

9 2002-11-19Rob McPherson9 Look in frequency domain  PHYSICS  1 / f ??? CALIB

10 2002-11-19Rob McPherson10 Transfer function G(f)  Data  1 / f 2 ??? Analytic

11 2002-11-19Rob McPherson11 Flaw in the model or method?  Many theories: Discrete FT windowing  leakage Reduce pole height Affect high/low frequency But not an offset  Side note: the authors of this talk disagree on this point … Or … maybe simple model not powerful enough? ????

12 2002-11-19Rob McPherson12 Modified simple model  Allow a high frequency physics tail with extra resistor: r

13 2002-11-19Rob McPherson13 New G(  ) I With  0 2 = 1 / LC 1/rC New time constant 1/rC 02020202 (  0 2 -  2 )   0 2 + j  /(rC) (  0 2 -  2 ) + j  /(rC) LC = 29.5 nHnF rC = 0.02 nsec t 0 = 0.5 nsec Maximum residual: 1.8% (t < 120 nsec) Best parameters (fixed = 450 nsec, =370 nsec): Best parameters (fixed  d = 450 nsec,  c =370 nsec):

14 2002-11-19Rob McPherson14 New G(  ) II  New fit: No visible oscillation Fitted LC corresponds well with peak in FFT[Uphy] / FFT[Ucal LC = 29.6 nHnF  f 0 = 0.0293 Hz = 3.74/128 Hz

15 2002-11-19Rob McPherson15 Measure LC ? I  In principle: instead of fit, can measure LC from: FFT[Uphy] / FFT[Ucal]  But the peak isn’t obvious: Can we do better?

16 2002-11-19Rob McPherson16 Measure LC ? II  Know from Fourier Transform theory Time shift  Frequency oscillation And we don’t know t 0 very well  Average over range of min time bins used in FFTs to smooth out oscillation (frequency pole is independent) Recall: “best” LC was 3.7/128 … seems promising

17 2002-11-19Rob McPherson17 Conclusions  Implemented FFT calibration for EMEC in combined run  “out of the book” FFT method seems to have (known) problems  EM community has some fixes that (I think) use more model parameters / complication  Have instead made small change to the simple model (extra resistor in parallel with L)  Seems to be a promising way of directly measuring LC with no fit at all!  Next: will pursue as far as filtering weight calculation

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