The STAR PXL detector cooling system LBNL: Eric Anderssen, Giacomo Contin, Leo Greiner, Joe Silber, Thorsten Stezelberger, Xiangming Sun, Michal Szelezniak,

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Presentation transcript:

The STAR PXL detector cooling system LBNL: Eric Anderssen, Giacomo Contin, Leo Greiner, Joe Silber, Thorsten Stezelberger, Xiangming Sun, Michal Szelezniak, Chinh Vu, Howard Wieman UT at Austin: Jo Schambach PICSEL group, IPHC, Strasbourg: Marc Winter et al.

Outline  The MAPS-based PXL detector for STAR  PXL cooling system  HFT status and performance  Conclusions 2 STAR PXL Cooling

SSD r = 22 IST r = 14 PXL r 2 = 8 r 1 = 2.8 STAR HFT Physics Motivation Extend the measurement capabilities in the heavy flavor domain, good probe to QGP: Direct topological reconstruction of charm hadrons (e.g. D 0  K , c  m  The STAR detector RHIC GeV Au-Au RHIC  dN ch /d  ~ 700 in central events TPC – Time Projection Chamber (main tracking detector in STAR) HFT – Heavy Flavor Tracker  SSD – Silicon Strip Detector  IST – Intermediate Silicon Tracker  PXL – Pixel Detector  = ~1 mm  = ~300  m  = ~250  m  = <30  m Tracking inwards with gradually improved resolution: R (cm) Need to resolve displaced vertices in high multiplicity environment STAR PXL Cooling

HFT Subsystems: PiXeL detector (PXL) STAR PXL Cooling 4 First vertex detector at a collider experiment based on Monolithic Active Pixel Sensor technology

PXL Detector Design Parameters STAR PXL Cooling 5 DCA Pointing resolution (10  24 GeV/p  c)  m LayersLayer 1 at 2.8 cm radius Layer 2 at 8 cm radius Pixel size 20.7  m X 20.7  m Hit resolution 3.7  m (6  m geometric) Position stability 5  m rms (20  m envelope) Material budget first layerX/X 0 = 0.39% (Al conductor cable) Number of pixels356 M Integration time (affects pileup)  s Radiation environment20 to 90 kRad / year 2*10 11 to MeV n eq/cm 2 Rapid detector replacement< 1 day 356 M pixels on ~0.16 m 2 of Silicon

PXL System Overview 10 sectors total 5 sectors / half 4 ladders / sector 10 sensors / ladder Mechanical support with kinematic mounts (insertion side) Cantilevered support Ladder with 10 MAPS sensors (~ 2×2 cm each) carbon fiber sector tubes (~ 200 µm thick) Highly parallel system STAR PXL Cooling 6

PXL sensor 4 sub-arrays to help with process variation  Digital section  End-of-column discriminators  Integrated zero suppression (up to 9 hits/row)  Ping-pong memory for frame readout (~1500 w)  2 LVDS data 160 MHz  Ultimate-2: third generation sensor developed for PXL by the PICSEL group of IPHC, Strasbourg  Monolithic Active Pixel Sensor technology  Pixel matrix  928 rows * 960 columns = ~1M pixel  In-pixel amplifier  In- pixel Correlated Double Sampling (CDS) STAR PXL Cooling 7  High resistivity p-epi layer  Reduced charge collection time  Improved radiation hardness  S/N ~ 30  MIP Signal ~ 1000 e-  Rolling-shutter readout  A row is selected  For each column, a pixel is connected to discriminator  Discriminator detects possible hit  Move to next row   s integration time  ~170 mW/cm² power dissipation

PXL Material Budget STAR PXL Cooling 8  Thinned Sensor  50  m  0.068% X 0  Flex Cable  Aluminum-Kapton  two 32  m-thick Al layers  0.128% X 0  Copper version  0.232% X 0  Carbon fiber supports  125  m stiffener  250  m sector tube  0.193% X 0  Cooling  Air cooling: negligible contribution  Total material budget on inner layer: 0.388% X 0 (0.492% X 0 for the Cu conductor version)  Curved sensor  40-60% yield after thinning, dicing and probe testing  Fully characterized before installation  Power and signal lines  Wire bond encapsulant largest contribution  Acrylic adhesive to deal with different CTE HFT DCA pointing resolution: ( 10  24/p)  m

PXL Assembly and Installation STAR PXL Cooling 9  Precision vacuum chuck fixtures to position sensors by hand  Sensors are positioned with butted edges. Acrylic adhesive prevents CTE difference based damage Cable reference holes for assembly Hybrid cable with carbon fiber stiffener plate on back in position to glue on sensors. Sensor positioning Kinematic mounts Novel insertion approach  Inserted along rails and locked into a kinematic mount inside the support structure

Air cooling of silicon detectors - CFD analysis air flow path – flows along both inside and outside surface of the sector Silicon power: 100 raised to 170 mW/cm 2 (~ power of sunlight) 350 W total Si + drivers 10

Air cooling – CFD analysis air flow velocity 9-10 m/s maximum temperature rise above ambient: 12 deg C sector beam surface – important component to cooling dynamic pressure force 1.7 times gravity stream lines with velocity silicon surface temperature velocity contours 11

12 Full scale mockup to verify cooling capability Platinum on thinned silicon to simulate detector chip heat load Additional heaters to reproduce driver heat sources Input and output thermocouple monitoring of air temperature Thermistors distributed on mockup pixel ladders IR camera to measure surface temperatures Air blower with static head of 9 inches of water air velocities measured with a hot wire velocity sensor Thermal image of sector-1 at 290 W dissipated in the detector and at the air flow speed of 12.2 m/s. The image was stitched from 8 individual images of small subsections. Ambient air temperature 31  C Result:  T = 11  C with 10.4 m/s air velocity, verifying CFD estimate In these tests we failed to get good total mass flow measurements which complicated specifying the final cooling blower system. STAR PXL Cooling

13 test of operating PXL system with full power and cooling flow Air Innovations Cooling air supply.14 m 3 /s at 2200 Pascal temperature regulated to 23±1  C Ladders viewed through IR window installed in the Pixel Support Tube PXL detector assembly hottest point on the chip, middle of the digital section. center of the middle chip (active region) center of the digital section of the middle chip 12  C MAX deviation from ambient STAR PXL Cooling

STAR HFT Cooling unit and Safety Interlocks (immediate power shut down)  ECU – Cooling Unit  Low Air Flow  Low/High Air Temperature  STAR interlock  Any condition potentially harmful for STAR Air Flow sensors at detector inlet ECU Cooling Unit 14

Running PXL temperature monitoring Typical ladder temperature trend from online monitoring Temperature diode reading from the last ladder sensor Relative measurement Plots: Sector 3 Ladder 2 Not calibrated ~ 6h RHIC fill ~ 2w cosmic run 15

16 Static displacement and vibration induced by cooling air flow Sector vibration modes were examined with FEA Prototype sector vibrations measured with airflow tests. This was determined to be less time consuming than setting up transient CFD calculations. Measurement of completed detector

vibration modes with reinforced end cap The message –Lots of complicated modes close in frequency –End cap raises frequencies a bit 259 Hz 397 Hz 276 Hz 441 Hz 497 Hz 17

air velocity probe two positions shown capacitance vibration probe two positions shown carbon fiber sector beam wind tunnel setup to test vibration and displacement adjustable wall for air turn around air in air out C:\Documents and Settings\Howard Wieman\My Documents\aps project\mechanical\PXL phase 1 sept 2008\sector ph1 wind tunnel.SLDASM 18 STAR PXL Cooling

-167 µm 6 µm 17 µm -179 µm -248 µm measured static deformation from 9 m/s air flow -156 µm -163 µm -113 µm 9 µm 11 µm 1 µm open end reinforced end 19 STAR PXL Cooling

measured vibration (RMS) induced by 9 m/s air flow 13 µm 14 µm 4 µm 6 µm 8 µm 3 µm 2 µm 11 µm 4 µm open end reinforced end 20 STAR PXL Cooling

Radial sector motion measured with capacitive probe inserted through hole in PST North half sectors populated with operating ladders. South half populated with empty sector tubes. System operated with full cooling air 21 capacitive probe measurement of completed PXL detector

Typical screen shot at full air flow Probe signal FFT, see next page for more detail Stdev = 5  m Probe conversion = 1  m/0.04 V 22 capacitive probe measurement of completed PXL detector

Fourier transform of sector vibration 40 Hz 70 Hz 230 Hz Main resonance of the carbon sector tube 23 capacitive probe measurement of completed PXL detector close to 260 Hz from original FEA simulation

Measured sector radial vibration as a function cooling air flow for edge ladder The measured vibration with no air flowing: 35 nm RMS 24 capacitive probe measurement of completed PXL detector

cooling air induced vibration and static displacement Sector vibration in the radial direction scales as:flow 2 Sector vibration at full flow:5 µm RMS Sector DC displacement scales as:flow 2 Sector moves in radially (static) at full flow:25 µm - 30 µm 25 capacitive probe measurement of completed PXL detector

PXL Position Control  Position stability  Vibration at air cooling full flow: ~5  m RMS  Stable displacement at full air flow: ~30  m  Stable displacement at power on: ~5  m  Global hit position resolution: ~ 6.2  m Vibration test through capacitive probe Sector in the metrology setup  Metrology survey  3D pixel positions on sector are measured with touch probe and related to tooling balls  Sector tooling ball positions related to kinematic mounts  Detector-half is fully mapped HFT DCA pointing resolution: ( 10  24/p)  m 26 STAR PXL Cooling

27 Performance: Hit Residuals and Track DCA PXL hit residuals (for cosmics) after sector alignment < 25 μ m 200 GeV Au+Au event Residuals for detector- half pointing to the inner layer of the other half (from cosmic data) Preliminary STAR PXL Cooling

Conclusions  The STAR HFT has been successfully taking data in 2014, 2015 and 2016  State-of-the-art MAPS technology proved to be suitable for vertex detector application  The air cooling allowed for stable operations, with limited induced vibration and static displacement  The HFT enabled STAR to perform a direct topological reconstruction of the charmed hadrons Thank you for your attention! 28 STAR PXL Cooling

Thank you for your attention! 29 STAR PXL Cooling

Backup slides 30 STAR PXL Cooling

 DCA pointing resolution  Design requirement exceeded: 46 µm for 750 MeV/c Kaons for the 2 sectors equipped with aluminum cables on inner layer  ~ 30 µm for p > 1 GeV/c  From 2015: all sectors equipped with aluminum cables on the inner layer  Physics of D-meson productions  High significance signal  Nuclear modification factor R AA  Collective flow v 2 HFT Performance from 2014 data D 0  K  production in √s NN = 200GeV Au+Au collisions (partial event sample) 46 µm 31 STAR PXL Cooling

HFT status and operations  Collected minimum bias events in HFT acceptance:  2014 Run1.2 Billion √s NN = 200GeV  2015 √s NN = 200GeV  2016 √s NN = 200GeV  Typical trigger rate of ~0.8kHz with dead time <5%  PXL status in 2016 Run  Latch-up induced damage:  1 full ladder off  5 sensors dead ~ 1 Billion p+p ~ 0.6 Billion p+Au ~ 1.5 Billion p+p ~ 0.3 Billion d+Au 32 STAR PXL Cooling

Si 50um (0.0529%) acrylic 50um (0.0148%) Encapsulant + bond wires (0.070%) Capacitors + solder (0.0035%) Coverlay (0.0075%) Al 30um – both sides (0.0248%) kapton 50um (0.0148%) acrylic 50um (0.0148%) Carbon composite 125um (0.0293%) % 0.128% % from older estimate Carbon composite 250um (0.1017%) Si adhesive 100 um (0.0469%) % Total = 0.388% NOTE: Does not include sector tube side walls Radiation length in low mass area 33 STAR PXL Cooling

2 m (42 AWG TP) 11 m (24 AWG TP) 100 m (fiber optic) Highly parallel system  4 ladders per sector  1 Mass Termination Board (MTB) per sector  1 sector per RDO board  10 RDO boards in the PXL system RDO motherboard w/ Xilinx Virtex-6 FPGA DAQ PC with fiber link to RDO board Mass Termination Board (signal buffering) + latch-up protected power PXL Detector Powering and Readout Chain Clk, config, data, power Clk, config, data PXL built events Trigger, Slow control, Configuration, etc. Existing STAR infrastructure PXL Sector 34 STAR PXL Cooling

PXL insertion mechanics Interaction point view of the PXL insertion rails and kinematic mount points Carbon fiber rails Kinematic mounts 35 STAR PXL Cooling