X-ray Correlation Spectroscopy: the VIPIC 3D-IC Project

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X-ray Correlation Spectroscopy: the VIPIC 3D-IC Project D. Peter Siddons, NSLS-II Brookhaven National Laboratory, Upton, NY 11973, USA Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 1 1

Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 Co-authors Fermilab: G. Deptuch, F. Fahim AGH Krakow: P. Grybos, P. Maj, Piotr Kmon, R. Szcziegiel BNL: A. K. Rumaiz, A. N. Kuczewski, J. Mead ANL: R. Bradford, J. Weizorick SLAC: G. A. Carini Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 2

Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 XCS requires timestamping of each detected photon to high resolution Intensities are rather low Full-frame readout is wasteful, since most of pixels contain no hits. Sparsified readout essential. Replace with VIPIC ROIC and sensor Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 3 3

3D integration: What and Why? 3D integration refers to the stacking of CMOS circuits in the third dimension as a way to increase device complexity without heroic measures with device feature size. Now in production for memory applications, but VIPIC is the first successful mixed-mode design for photon science applications. True separation of digital and low-noise analog circuits Allows choice of technology node which is optimal for each function Provides screening of sensitive, low-noise circuits from digital noise Allows easy power distribution to large-area ASICs. Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 4 4

Via-middle process flow Conventional CMOS process flow Two extra steps between front-end and back-end processes: Etch vias into silicon of wafer Passivate via walls Fill vias with conductor Then process all interconnect layers as usual Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 5

Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 Flip second layer and oxide-bond to first, aligning contacts. Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 6

Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 Grind off bottom wafer to expose TSVs Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 7

Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 Deposit oxide layer and make contacts Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 8

Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 Oxide-bond detector to 2-layer ASIC Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 9

Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 Grind off top layer to expose TSVs Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 10

Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 Attach bumps for Flip-Chip mounting to PCB Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 11

3D opens the door to truly gap-free large-area detectors The availability of Through-Silicon Vias (TSVs) allows direct contact to the circuitry from any point on the device Allows dense interconnection to sensor Allows dense interconnection to outside world No need to leave edge-space for wire-bonding and its resulting gap in active area of detector. Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 12 12

VIPIC1 (1st 3D MPW run by HEP) Vertically Integrated Photon Imaging Chip Small prototype: 64×64 pixels, 80 mm pitch, Si 500+ mm thick sensor 2009 measure time-of-arrival (ToA) for 2D autocorrelation @ <10 ms develop practices and techniques applicable later in devices for HEP and Photon Science APS beam tests July and October 2014 Samples of nanoparticle colloids and standard XCS analysis (multi-tau correlator) allowed observation of dynamics with sub- millisecond relaxation times 2014 13 Topical Workshop on Novel Radiation Detectors, 6 Feb 2017

VIPIC1 Noise Performance 3D integrated pixels merge good features of monolithic (noise) and hybrids (functionality rad hardness, sensor optimization) competitive to monolithic pixels! Bigger & faster signals ENC on fusion bonded device is close to that measured for floating inputs! ENC=36.2 e- symmetrical noise distribution with <3.4 % of pixels outside of ±3 s 14 Topical Workshop on Novel Radiation Detectors, 6 Feb 2017

Tests performed at 8ID-I beamline at the APS in July and October 2014 VIPIC1 XCS results Tests performed at 8ID-I beamline at the APS in July and October 2014 Microsecond-scale relaxation times, which are inaccessible by conventional frame oriented detectors, were measured using VIPIC1. Given sufficient intensity, it is now possible to collect data continuously from the microsecond time scale up to minutes, which opens up the XCS field to a much wider range of scientifically interesting experiments. Time-integrated image of scattering pattern recorded by VIPIC 15 Topical Workshop on Novel Radiation Detectors, 6 Feb 2017

Temperature changes of Latex spheres in Glycerol This data shows the autocorrelation function of a sample of latex spheres suspended in a glycerol solution. The different curves show the result for several temperatures. The samples were sealed in a glass capillary to prevent evaporation at high temperature. The data is continuous from a few microseconds to a few minutes, and represents several times 10^8 time intervals. Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 16

Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 Bunches Data was collected with a frame time of 153 ns, synchronized to the APS ring round-trip time. The graph shows this data plotted over the accelerator bunch current The close correspondence between our data and the independent measurement by the storage ring diagnostic system shows that the detector functions correctly down below 1 microsecond. Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 17

Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 VIPIC-L ASIC Building a full-scale (1 Mpixel) version Smaller pixel (65 microns) Large ASIC; >100M transistos 192 x 192 pixels each 65um^2 12.85 mm x 12.85 mm 36 LVDS data lines per chip 400 Mbs serial rate -> 14.4 Gb/s Sparsified readout or full-frame readout @ 50k frames/sec. Analog tier Digital tier Topical Workshop on Novel Radiation Detectors, 6 Feb 2017

Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 Sensors P-in-N diodes on 6” wafers. Each wafer carries three 2x6 blocks plus 8 single-ASIC blocks for initial testing. (a) shows the wafer level, (b) shows pixel details.. Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 19

VIPIC: >1MPixel 3D Camera Ultimate GOAL: To build a single module 3D camera with minimal gap Contains three 2x6 arrays of large ASICs each with ~37000 pixels (1.3Mpixel camera module) LTCC hosts FPGA based processing units Approximately 1 FPGA per chip. No dead space between ASICs within 2 x 6 array. 20 Topical Workshop on Novel Radiation Detectors, 6 Feb 2017

Front-end motherboard Three modules, each 2 x 6 ASICs Monolithic sensor per module, no gaps Water-cooling. Zynq processor to handle slow controls and data flow via FPGA fabric.

Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 Summary We have built the first fully-functional mixed-mode 3D integrated circuit for photon science The technology opens the door for more functionality per pixel with optimized processes for each tier It allows much better power distribution to a large-area ASIC It provides a lower-noise sensor interconnect than bump-bonding It shows the way towards zero-gap tiling of detectors since there is no need for an exposed ASIC edge for wire-bonds We have tested a prototype detector at beamline 8-ID at APS using samples with a range of dynamic behaviour, showing that it performs as expected down to at least 10 microsecond intervals, and even into the 100 nanosecond regime. Topical Workshop on Novel Radiation Detectors, 6 Feb 2017 22

Acknowledgments We thank David Kline and Tim Madden from the APS Detector Group, Scott Holm, Albert Dyer and Alpana Shenai from the Fermilab ASIC Group, and Tareque Aziz from BNL. Fermilab is funded by DOE-HEP under contract number DE-AC02-07CH11359. APS is funded by DOE BES under Contract No.DE-AC02-06CH11357. BNL is funded by DOE-BES under DOE contract DE-SC0012704. IFDPS, Mount Fuji, 2016 23