1 US Testing Status-Anthony AffolderModule Testing Meeting, Dec. 11, 2003 Update of US Testing Status Anthony Affolder On behalf of the US testing group.

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Presentation transcript:

1 US Testing Status-Anthony AffolderModule Testing Meeting, Dec. 11, 2003 Update of US Testing Status Anthony Affolder On behalf of the US testing group

2 US Testing Status-Anthony AffolderModule Testing Meeting, Dec. 11, 2003 Fine Tuning of Fault Finding Cuts Combined measurements of all modules produced with old hybrids (100  resistor to inverter) Fit Gaussian to central core of each distribution  Found 5  region  All cuts now used (but 1) outside of this region  Low noise requirement too tight 2.8  Deconvolution Mode 3.2  Peak Mode Led to 33 false one sensor open flags Re-applied fault finding with 5  requirements N i > 1.55 (Deconvolution) N i > 1.2 (Peak) Old Hybrids Removes false flagging while not missing any new real faults This tuning should be done for each module type Root combination software available from UCSB Channels Affected By Change in Cut

3 US Testing Status-Anthony AffolderModule Testing Meeting, Dec. 11, 2003 Comparison of Modules With Old Vs. Final Hybrids Resistor to inverter stage changed from 100  to 50  Good News  A small number of each type of TOB modules made  All types have similar distributions of cut variables Gives hope to idea that only two sets of cuts needed (1 sensor modules and 2 sensor modules) Bad News  The noise (or gain maybe) appears to be 5-10% lower  May have to re-tune again  Hopefully, gain changed due to resistor switch Final Hybrids Old Hybrids

4 US Testing Status-Anthony AffolderModule Testing Meeting, Dec. 11, 2003 Newest CMN Problem Module (1051) Last SS6 module built using one sensor with 1.2  A extra current (450 nA vs 1700 nA) in UCSB re- probing at 450 V.  Well within old selection criteria  No large addition increase in current during module assembly  Old sensors CMN seen in chip 46 with extremely high noise in channels  Sensor flaw seen between two channels Not clear if flaw cause of problem  Begins at 400 V where database and measured bias current diverge ~0.5  A difference

5 US Testing Status-Anthony AffolderModule Testing Meeting, Dec. 11, 2003 New CMN Problem Module (1051) Module tested at slightly elevated voltage to measure effect as function of current  Bias current 3.7  A, < 2  A more than expected from database For first half of chip, CM subtracted noise a factor of ~1.75 higher than typical noise.  A very little amount of micro- discharge can cause the CM subtraction algorithm not to work properly CM subtraction algorithm used is same as LT, and test beam software

6 US Testing Status-Anthony AffolderModule Testing Meeting, Dec. 11, 2003 IV Test Results (UCSB) Environmental conditions tightly controlled  Temperature C  RH < 30% at all times An increase greater than 5  A can cause CMN Much better results with newer OB2 sensors (2002) None of the 20 newest (2003) OB2 sensor show any increase in bias current!!! Sensors> 2  A > 5  A >10  A >20  A >100  A < -2  A <-5  A <-10  A OB2 (’00-01)15%9%8%5%1%8%3%1% OB1 (’00-01)6%3% 0% OB2 (’02)3% 0% 2% 0% OB2 (’03)0% Probed UCSB (400 V) – QTC Measurement (400 V)

7 US Testing Status-Anthony AffolderModule Testing Meeting, Dec. 11, 2003 IV re-probing (FNAL) FNAL has begun extensive re- probing program  See R. Demaria’s talk in sensor meeting  Plan on re-probing all sensors received so far 328 sensors already re-probed  24% are Grade B (>1.5  A)  >15% have >1.5  A increase in bias current relative to QTC measurements Earlier indications are that the agreement between QTC and re-probing improved in 2003 sensors 81 sensors from 2003 re- probed so far

8 US Testing Status-Anthony AffolderModule Testing Meeting, Dec. 11, 2003 CMN vs Batch Sensors which cause CMN are fairly evenly distributed throughout production years Early indications are that 2003 may be better  Extremely low statistics  Only low bias current sensors used

9 US Testing Status-Anthony AffolderModule Testing Meeting, Dec. 11, 2003 Study of Common Mode The common mode point is calculated event-by-event for groupings of 32 channels  The spectra of the common mode is fit for groupings within a chip with CMN problems Excluding the grouping with high noise channel Spectra is fit with two Gaussians  Central core plus tail  Fit parameters are: Fraction of events in tail Width of central core Width of tail Study how parameters vary with current

10 US Testing Status-Anthony AffolderModule Testing Meeting, Dec. 11, 2003 Fit Result of Common Mode Point Fraction of events is flat with bias current (~strip current) Width of central core increases with bias current (~strip current) Width of tail increases with bias current (~strip current) and may flattens out at some current

11 US Testing Status-Anthony AffolderModule Testing Meeting, Dec. 11, 2003 Studies with “Final” Sensors 10 modules produced with 20 “final” production sensors  OB2 produced in weeks of 2003  Extremely high quality Bias currents between 1-2  A Only 2 pinholes not indicated in sensor database No high noise channels Effects of thermal cycling/strain studied  Modules fixed to cold box plates at thermal contacts by screws Modules thermal cycled for about a week  1 mm shims added under 1 or 2 contact points in order to stress silicon ~3  more than offset in rod attachment points

12 US Testing Status-Anthony AffolderModule Testing Meeting, Dec. 11, 2003 Effects of Strain on Modules Modules attached to cold plate with 4 screws through thermal contacts To test the effects of twisting modules, 1 mm shims added under thermal contacts  Bias current measured with 1 or 2 shims for all 10 modules No change in current seen 1 mm shim 1 2

13 US Testing Status-Anthony AffolderModule Testing Meeting, Dec. 11, 2003 Modules Thermal Cycles Modules thermal cycled on modified cold plates with/without shims  168 module-hours with a total of 36 thermal cycles without shims  ~1000 module-hours with a total of ~200 thermal cycles with 2 shims No change in bias currents or noise seen

14 US Testing Status-Anthony AffolderModule Testing Meeting, Dec. 11, 2003 Single Rod Test Stand at UCSB Complete set of electronic ready to test single rods  Test box provides dry, dark, and electrical isolated environment  Connects to Rod burn-in chiller for cooling First production rod tested in stand (J. Lamb & P. Gartung)

15 US Testing Status-Anthony AffolderModule Testing Meeting, Dec. 11, 2003 Rod Testing Results Faults clearly seen in rod using new LT  Only opens on rod so far Laser gain differences add complication to data analysis  Fixed noise cuts will NOT work due to 50% variation in laser gain  Hopefully laser gain can be measured by header height Similar work on optimization of calculation of pulse height & peak time variable needed as in module LT  See P. Gartung’s talk More statistics needed in order to know how best to test rod ARCS Rod LT