CPAD 2019 in Madison Wisconsin

Session

Solid State Tracking Detectors

Dec 9, 2019, 1:30 PM

Monona Terrace Convention Center

Conveners

Solid State Tracking Detectors

• Sally Seidel (University of New Mexico)

Solid State Tracking Detectors: Solid State Tracking Detectors

• Sally Seidel (University of New Mexico)

Solid State Tracking Detectors: Solid State Tracking Detectors

• Sally Seidel (University of New Mexico)

60. R&D on LGAD Radiation Tolerance: the HL-LHC and Beyond

12/9/19, 1:30 PM

55. From LGADs to AC-coupled LGADs for fast timing applications

Gabriele Giacomini (Brookhaven National Lab)

12/9/19, 1:50 PM

57. Performance of LGADs and AC-LGADs towards 4D tracking

Gabriele D'Amen

12/9/19, 2:10 PM

59. Low Gain Avalanche Detectors: Towards Higher Granularity and Repetition Rate

Prof. Bruce Schumm (UC Santa Cruz)

12/9/19, 2:30 PM

65. Development of a 3D detector on a hydrogenous amorphous silicon substrate

Dr Mauro Menichelli (INFN)

12/9/19, 2:55 PM

34. Feasibility Study of Charge Multiplication by Design in Thin Silicon 3D Sensors

Sally Seidel (University of New Mexico)

12/9/19, 3:20 PM

Solid State Tracking Detectors

Talk

We report on a novel 3D sensor design, featuring very small inter-electrode distance, aimed at controlled charge multiplication at voltages of the order of 100 V, both before and after irradiation. Moderate gain values of a few units are achieved, which are however sufficient to compensate the loss of charge signal due to the use of thin substrates and to counteract charge trapping effects...

116. New proton irradiation facility at Fermilab

Petra Merkel (Fermilab)

12/9/19, 3:40 PM

102. Chronopixel CMOS Sensor Development for the ILC

James Brau (University of Oregon)

12/10/19, 9:00 AM

Solid State Tracking Detectors

Talk

James Brau, Nikolai Sinev, David Strom University of Oregon, Eugene, Oregon Oliver Baker, Charles Baltay, Christian Weber Yale University, New Haven, Connecticut A monolithic CMOS pixel detector with time-stamping capability (Chronopixel) has been developed based on design goals of the International Linear Collider (ILC). Each hit is accompanied by a time tag with sufficient precision...

81. RD53 Status

Cesar Gonzalez Renteria (Lawrence Berkeley National Laboratory)

12/10/19, 9:25 AM

Solid State Tracking Detectors

Talk

The readout circuit (RD53B) for the pixel detector is a joint effort by both the ALTAS and CMS experiments by the RD53 collaboration. In this talk I will give the status of the RD53 collaboration work on the design and verification of RD53B. Using 65nm technology and spanning a 384x400 pixel matrix expecting a maximum hit-rate of 3 GHz/cm2, this chip is the most complex ASIC designed for...

83. Modelling radiation damage to pixel sensors in the ATLAS detector

Aidan Grummer (University of New Mexico)

12/10/19, 9:50 AM

Solid State Tracking Detectors

Talk

Silicon pixel detectors are at the core of the current and planned upgrade of the ATLAS experiment at the LHC. Given their close proximity to the interaction point, these detectors will be exposed to an unprecedented amount of radiation over their lifetime. The current pixel detector will receive damage from non-ionizing radiation in excess of ${10}^{15}$ $1$ MeV neq cm${}^2$, while the pixel...

27. Tracking and Timing with Induced Current Detectors

Dr Ronald Ronald Lipton (Fermilab)

12/10/19, 10:10 AM

Solid State Tracking Detectors

Talk

Technologies such as 3D electronics/sensor integration and CMOS-based pixel sensors, combined with continued scaling of CMOS electronics has enabled detectors with small pixels with low power and very low load capacitance. This low capacitance and associated fast response allows us to use information from transient current signals rather than the normal fully integrated charge. In a detector...

44. Status and Plans of the CMS High Granularity Calorimeter Upgrade Project

Zoltan Gecse (Fermilab)

12/10/19, 11:00 AM

Solid State Tracking Detectors

Talk

The High Luminosity extension of the LHC program (HL-LHC) will impose in an order of magnitude larger radiation levels and pile-up conditions in CMS. To cope with the challenges, the endcap calorimeter of CMS will be replaced with a highly granular imaging calorimeter (HGCal). It will use about 6 million silicon diode based channels of 0.5-1 cm${}^2$ size and about four hundred thousand...

56. Large-area Si(Li) detectors for X-ray spectrometry and particle tracking for the GAPS experiment

Field Rogers (MIT)

12/10/19, 11:20 AM

Solid State Tracking Detectors

Talk

Novel large-area lithium-drifted silicon (Si(Li)) detectors have been developed for the General Antiparticle Spectrometer (GAPS) Antarctic balloon mission. GAPS will search for antinuclei signatures of dark matter using a novel detection technique based on exotic atom capture and decay. As the GAPS instrument will require ~10 square-meters of instrumented silicon in order to achieve...

76. Scintillation detector based on InAs quantum dots in a GaAs semiconductor matrix for charged particle tracking: first measurements of the response to alpha-particles

Pavel Murat (Fermi National Accelerator Laboratory)

12/10/19, 11:40 AM

Solid State Tracking Detectors

Talk

We measured response to 5.5 MeV alpha particles of a 20 um thick integrated scintillating detector based on InAs quantum dots (QDs) embedded into GaAs matrix. The operational principle of the tested detector is as follows: photons emitted by InAs QDs have energy lower than the GaAs bandgap, which makes the GaAs bulk transparent to the QD emission. The QD emission is detected by a 1 um...