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Sensor Choice The story here is surely damage – See that silicon worked well in the PLT test until we shifted the timing to optimize diamond Reducing BX.

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Presentation on theme: "Sensor Choice The story here is surely damage – See that silicon worked well in the PLT test until we shifted the timing to optimize diamond Reducing BX."— Presentation transcript:

1 Sensor Choice The story here is surely damage – See that silicon worked well in the PLT test until we shifted the timing to optimize diamond Reducing BX “leakage” in diamond increased it for silicon Timing is adjustable for 4 telescopes at a time so we were stuck Assume have same timing issues in a hybrid system – What sort of fluence do we expect for the PLT up to LS2? Cooled sensor/ROC (0C) work well up to 1.5e15 – From irradiation/tests/test beam studies 6/28/20131 W. Johns Pixel Luminosity Telescope ECR

2 Fluence estimate from Simulation Diamond PLT: 1.6 tracks in 8 telescopes/BX @r=4.9 cm, z=175 cm (assume 2835 BX at 1e34/(cm 2 s)) – 6.4e11/fb so Silicon expect 2.6e12/fb from tracks ~500/fb to reach 1.5e15 Try to scale to something we know… (FPiX inner) – Will get a little more due to conversions, use middle radius of FPiX to be conservative in scaling – Scaling estimation from unoffical dose/fluence calculator (charged hadrons) – r = 10 cm, z = 34.5 cm: 1.2e12/(cm 2 fb) FPiX » Lowball inner FPiX radius (~layer 3 of barrel) – r = 4.9 cm, z = 175 cm: 3.1e12 /(cm 2 fb) PLT » Ratio for comparison: PLT sees ~3X damage of the FPiX inner disk – Now we can try to compare to a measurement. 6/28/20132

3 Fluence/aging estimate PLT sees damage at about the same rate as the current Pixel Layer 1 – This lets us compare to the upgrade too FPiX BPiX (Leakage Current / ROC at the end of 2012 from G. Bolla) (Scales adjusted so BPiX is x3 FPiX) 6/28/20133

4 Current Layer 1 Upgrade Layer 1 Upgrade Layer 1 expected to go ~250/fb 6/28/20134

5 – PLT is about the same as the current BPiX layer 1 – Layer 1 damage has been projected using the Hamburg Model (Bias V needed for 99% efficiency) Fluence/aging estimate 6/28/2013 5 (Dec 2012 plot from Seth Zenz) Looks a bit pessimistic PLT starts here PLT Power Supply Limit LS2?

6 – PLT is about the same as the current BPiX layer 1 – Comparing to the Upgrade TDR Layer 1 (x2 Fluence over current Layer 1) suggests PLT lasts a long time – Upgrade TDR used 2 sensor temperatures 0 C and (-4 C) » Replacement of Upgrade layer 1 at 250/fb Upgrade layer 1 sees about 2x fluence of Current Layer 1 » 250/fb: fluence of 1.5e15, current: 47mA (27mA), (600 V max) (PLT x5 less current: 3 sensors not 16 sensors) » Sensor still operates at 3.0e15, but resolution etc. will suffer » Higher temperature will damage faster Seems the critical factor for PLT » PLT HV can go to 500 V, and 10 mA now – Conservative assumption (x2) is PLT can go 250/fb too Fluence/aging estimate 6/28/20136

7 Why 250/fb, 500/fb? Luminosity is coming – By LS3 2e34 y cm-2s-1 (50 ns Bx spacing?) – By LS2, ~250/fb? We actually ended the 2012 running at a higher Luminosity than predicted here (& 50 ns Bx spacing) From European Strategy Preparatory Group Sept 2012 6/28/20137

8 Won’t the PLT suffer at high rate? It’s not just the particle rate, it’s the trigger rate Nucl.Instrum.Meth. A581 (2007) 343-346 0% ~4 kHz ~0.5% The dominant loss mechanism of the PSI46v2 (analog) is the reset of the Double Column The PLT is read out at a much lower rate than the CMS L1A At CASTOR we found a few kHz gave plenty of data -This gives only a small inefficiency in the readout -Less of an effect for the column sum (Fast Or) 6/28/20138 Will be important to do custom studies to monitor inefficiencies.

9 What about the AOH? The innermost AOH sits at about 11 cm from the beam and at about 180 cm in z – Fluence is about x3 less than for the sensor according to the same simulation as shown earlier This is 500/fb 6/28/20139 Hard to compare to BCM AOH since it was uncooled. This plot assumes -10C. The AOH should last a long time for PLT

10 Other chips: SEU troubles? LLD, DOH, delay25, tpll, etc. – Not a lot to compare to since current pixel components are at ~10 times less fluence – But pixels have way more than x10 components than PLT: should be ok TBM – About same fluence as current layer 1 – Same argument, pixels have way more TBMs and bad SEU rate is low in pixels, 1/hr, maybe PLT sees one every few fills ROC – Need to monitor and reset if a DC etc. falls out – We’ve seen this once in CASTOR 6/28/201310

11 Conclusions The PLT sensor should last 250-500/fb The AOH looks like it should last 250-500/fb Other chips SEU rate is small and should be rare in a fill Damage rate for sensors and AOHs is dependent on temperature, we should revisit when we know more about cooling Mitigation strategies: – Damage: PLT components are easy (comparatively) to replace/upgrade if the pixel volume is open – SEU: monitoring and corrective action 6/28/201311


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