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Performance of the LHCb Vertex Locator Thomas Latham (on behalf of the LHCb VELO group) 11/06/20111TIPP 2011 - Chicago.

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Presentation on theme: "Performance of the LHCb Vertex Locator Thomas Latham (on behalf of the LHCb VELO group) 11/06/20111TIPP 2011 - Chicago."— Presentation transcript:

1 Performance of the LHCb Vertex Locator Thomas Latham (on behalf of the LHCb VELO group) 11/06/20111TIPP 2011 - Chicago

2 Introduction to LHCb 11/06/2011TIPP 2011 - Chicago2 LHCb is a dedicated experiment for flavour physics at the LHC, in particular: – Study of CP violation in beauty and charm decays – Search for New Physics in loop processes – Complementary to direct searches at ATLAS and CMS Detector requirements: Efficient trigger for leptonic and hadronic final states Excellent vertex finding ability Extremely good tracking efficiency and particle identification

3 The LHCb detector 11/06/2011TIPP 2011 - Chicago3 Interaction Point in the VELO LHCb σ(pp → H b X) = ( 75 ± 5 ± 13 ) µb Phys. Lett. B 694, 209-216 (2010) Angular acceptance: 15 mrad < θ < 250 mrad

4 The Role of the VELO 11/06/2011TIPP 2011 - Chicago4 b-hadrons have lifetime of O(10 -12 )s Relativistic boost means average flight distance of ~1cm VELO has to precisely locate both primary and secondary vertices Forms essential part of higher level trigger Also a principal tracking device

5 VELO Design 2 retractable detector halves 11/06/2011TIPP 2011 - Chicago5

6 VELO Design 2 retractable detector halves 11/06/2011TIPP 2011 - Chicago6

7 VELO Design 2 retractable detector halves 21 modules (+ 2 pile-up) per half Each module has r and φ sensor Detectors in secondary vacuum 11/06/2011TIPP 2011 - Chicago7

8 VELO Design 2 retractable detector halves 21 modules (+ 2 pile-up) per half Each module has r and φ sensor Detectors in secondary vacuum Separated from LHC vacuum by 300µm foil Foil also guards against RF pickup from beam 11/06/2011TIPP 2011 - Chicago8

9 Sensor Design 11/06/2011TIPP 2011 - Chicago9 2 semi-circular sensor designs – r and φ measuring 300µm n-on-n silicon 2048 strips per sensor 8.2mm inner radius of active silicon Cooled by evaporative CO 2 system – Operating temperature of -30°C

10 VELO Views 11/06/2011TIPP 2011 - Chicago10 Beam-eye view of open VELO Close-up of RF foil VELO modules

11 VELO Performance! 11/06/2011TIPP 2011 - Chicago11

12 Signal and Noise 11/06/2011TIPP 2011 - Chicago12 Overall S/N as per design, > 20 Noise on strips increases with strip length, hence with radius of r strips Noise levels also differ between 3 different types of φ strips: – inner – routed over outer strips – outer – w/ overlaid routing lines – outer – no overlaid routing lines

13 Spatial Alignment 11/06/2011TIPP 2011 - Chicago13 VELO moved for each LHC injection Precise knowledge of alignment critical for lifetime measurements Proceeds in 3 stages: – Sensors within modules – Module to module within half – Inter-half alignment Uses residuals from track fit Module and sensor alignment known to better than 4µm Inter-half stable over time to better than 5µm

14 Hit Resolution 11/06/2011TIPP 2011 - Chicago14 Measure residual of cluster to track made without that cluster Correct for track uncertainty Bin in both strip pitch and projected track angle Best resolution < 4µm !

15 Primary Vertex Resolution 11/06/2011TIPP 2011 - Chicago15 Randomly split tracks into two sets Fit two vertices and measure their separation With 25 tracks per vertex: – x resolution = 13.1µm – y resolution = 12.5µm – z resolution = 71.1µm Approaching design levels

16 Impact Parameter Resolution 11/06/2011TIPP 2011 - Chicago16 IP = distance of closest approach of track to PV Important variable for identifying long lived particles such as B mesons Contributions from PV and hit resolutions plus multiple scattering IP resolution improved with data based alignment Some disagreement with simulation remains – Under investigation Preliminary

17 Material Budget 11/06/2011TIPP 2011 - Chicago17 Use detector model in simulation to estimate material budget Total material budget 0.221X 0 Material before 1 st measurement 0.032X 0

18 Self Imaging 11/06/2011TIPP 2011 - Chicago18 Use vertices of hadronic interactions with material to map VELO Requires precise vertex measurements – Exactly what VELO was designed for! Key features (sensors, RF foil etc.) stand out clearly Preliminary comparisons between data and MC indicate good agreement

19 Velo Radiation Damage Studies LHCb VELO HOT! First Strip only 8mm from LHC beam Outer strip 40mm Maximum Fluence predicted at 14TeV 1.3x10 14 1MeV n eq /cm 2 /2 fb -1 Strongly non-uniform dependence on 1/r 1.9 and station (z) Clear observation of radiation damage IV, CCE, noise versus voltage Annealed at 20 C over shutdown n-on-n sensor Noise vs Voltage Obtained from CCE vs Voltage 11/06/201119TIPP 2011 - Chicago

20 Summary VELO has operated extremely well from day one Operations becoming smoother over time Performance is close to design parameters – Best hit resolution < 4µm – best at LHC! Improvements already made based on 2010 data will reap further benefits for the LHCb physics programme this year Outlook: – Still some room for improvements – work ongoing – Challenges to come from radiation damage First evidence for radiation damage now seen – Replacement VELO under construction 11/06/2011TIPP 2011 - Chicago20

21 BACKUP 11/06/2011TIPP 2011 - Chicago21

22 Time Alignment Nominal LHC bunch spacing 25ns Fine tune timings of front end chips Aim for – Maximum signal/noise – Minimum spillover Sensors individually tuned to account for differences in – Time of flight – Cable length 11/06/2011TIPP 2011 - Chicago22

23 Cluster Finding Efficiency 11/06/2011TIPP 2011 - Chicago23 Only 1 bad chip out of 1344! Efficiency generally extremely good Most inefficiencies understood

24 Velo Radiation Damage Studies Tips of VELO sensors expected to type invert in next months of LHC running LHCb VELO HOT! Middle station Far station TDR Prediction First Strip only 8mm from LHC beam Outer strip 40mm Maximum Fluence predicted at 14TeV 1.3x10 14 1MeV n eq /cm 2 /2 fb -1 Strongly non-uniform dependence on 1/r 1.9 and station (z) 11/06/201124TIPP 2011 - Chicago

25 Velo Radiation Damage Monitoring 1.Current vs applied bias Voltage (IV) -Taken weekly -Current increases with bulk damage, linearly related to fluence -Does not study depletion voltage 2.Noise vs applied bias Voltage -Taken monthly -Sensors decrease capacitance and hence noise when depleted, so sensitive to depletion voltage at least during early running 3.Charge Collection Efficiency vs applied bias voltage -Direct measure of physics relevant parameter -Can study rad. damage as function of position -Requires beam data so only taken a few times per year -April 2010 (~0), April 2011 (40 pb -1 ) Expectation: Depletion voltage of VELO sensors around 40-80V originally. Depletion voltage decreases with fluence till type inversion 11/06/201125TIPP 2011 - Chicago

26 IV Studies Example sensors showing bulk damage Annealed at 20 C over shutdown n-on-n sensor VELO n-on-n, contains one n-on-p module 11/06/201126TIPP 2011 - Chicago

27 Noise vs Voltage Measure voltage required to get noise to reduce by a specified fraction of the total depleted/undepleted change in noise Outermost strips on R sensor less irradiation Ratio ~ 1, i.e. no change in V (noise min) Innermost strips on R sensor most irradiation Ratio < 1, i.e. change in V(noise min) 11/06/201127TIPP 2011 - Chicago

28 Charge Collection Efficiency (CCE) Blue – tracking sensors – at full bias voltage Red – test sensors – bias voltage ramped – 10V steps, 0V-150V – Rotate through patterns, fully automatic scan procedure Tracks fitted through tracking sensors – Charge collected at intercept point on test sensors measured as function of voltage Non-zero suppressed data taken so full charge recorded – Can study regions of sensor 11/06/201128TIPP 2011 - Chicago

29 Charge collection efficiency vs Voltage measured. Voltage at which CCE is 80% extracted 80% chosen as gives best agreement unirradiated with depletion Here, averaged over all sensors, there is dependence of fluence on Z position Region sizes chosen so that fluence varies by factor two in each region Fluence expected to change as 1/r^{1.9} Errors on plot are error on mean from all sensor average Charge Collection Efficiency (CCE) 11/06/201129TIPP 2011 - Chicago

30 Same info. plotted for all regions, all modules Lines are fits to all modules 11/06/201130TIPP 2011 - Chicago

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