36 research outputs found

    Rad-hard vertical JFET switch for the HV-MUX system of the ATLAS upgrade Inner Tracker

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    This work presents a new silicon vertical JFET (V-JFET) device, based on the trenched 3D-detector technology developed at IMB-CNM, to be used as switches for the High-Voltage powering scheme of the ATLAS upgrade Inner Tracker. The optimization of the device characteristics is performed by 2D and 3D TCAD simulations. Special attention has been paid to the on-resistance and the switch-off and breakdown voltages to meet the specific requirements of the system. In addition, a set of parameter values has been extracted from the simulated curves to implement a SPICE model of the proposed V-JFET transistor. As these devices are expected to operate under very high radiation conditions during the whole experiment life-time, a study of the radiation damage effects and the expected degradation on the device performance is also presented at the end of the paper.Comment: KEYWORDS: Radiation-hard electronics; Voltage distributions; Large detector systems for particle and astroparticle physics. 9 Pages, 7 Figure

    Thermal and hydrodynamic studies for micro-channel cooling for large area silicon sensors in high energy physics experiments

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    Micro-channel cooling initially aiming at small-sized high-power integrated circuits is being transferred to the field of high energy physics. Today`s prospects of micro-fabricating silicon opens a door to a more direct cooling of detector modules. The challenge in high energy physics is to save material in the detector construction and to cool large areas. In this paper, we are investigating micro-channel cooling as a candidate for a future cooling system for silicon detectors in a generic research and development approach. The work presented in this paper includes the production and the hydrodynamic and thermal testing of a micro-channel equipped prototype optimized to achieve a homogeneous flow distribution. Furthermore, the device was simulated using finite element methods.Comment: 10 pages, submitted to NIMA (accepted

    Lithium ion-induced damage in silicon detectors

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    Silicon diodes processed by CNM on standard and oxygenated silicon substrates have been irradiated by 58 MeV lithium ions. The radiation-induced effects are very similar to the one observed after proton irradiation: substrate space charge sign inversion (SCSI), lower increase of the effective substrate doping concentration after SCSI for the oxygenated devices. The experimental radiation hardness factor has been determined to be 45.01, within 8.2% with the expected value. These results suggest that 58 MeV Li ions are a suitable radiation source for radiation hardness studies by ions heavier than protons for the future very high luminosity hadron colliders

    New evidence of dominant processing effects in standard and oxygenated silicon diodes after neutron irradiation

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    Abstract Silicon diodes processed on standard and oxygenated silicon substrates by three different manufacturers have been irradiated by neutrons in a nuclear reactor. The leakage current density ( J D ) increase is linear with the neutron fluence. J D and its annealing curve at 80°C do not present any sizeable dependence on substrate oxygenation and/or manufacturing process. The acceptor introduction rate ( β ) of the effective substrate doping concentration ( N eff ) is independent from the oxygen concentration when standard and oxygenated devices from the same manufacturer are considered. On the contrary, β significantly varies from one manufacturer to another showing that the β dependence on the particular process can be important, overtaking the small substrate oxygenation effect. Finally, the average saturation value of the N eff reverse annealing is slightly lower for the oxygenated samples, pointing out a positive effect of the substrate oxygenation even for devices irradiated by neutrons

    Desarrollo y optimizacion de tecnologias bipolares avanzadas y BICMOS

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    Centro de Informacion y Documentacion Cientifica (CINDOC). C/Joaquin Costa, 22. 28002 Madrid. SPAIN / CINDOC - Centro de Informaciòn y Documentaciòn CientìficaSIGLEESSpai

    TCAD simulation of the electrical performance of the ATLAS18 strip sensor for the HL-LHC

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    To cope with the increased occupancy and radiation dose expected at the High-Luminosity LHC, the ATLAS experiment will replace its current Inner Detector with the Inner Tracker (ITk), consisting of silicon-based pixel and strip sub-detectors. The strip detector will consist of n+n^+-in-pp sensors fabricated by Hamamatsu Photonics, with 300 μ\mum signal-generation thickness and approximately 75 μ\mum strip pitch. To guide the operation of these sensors in the ITk, it is desirable to understand the basic mechanisms underlying their performance, including the effects of the radiation fluence (up to 1.6×10151.6 \times 10^{15} 1-MeV neq_\text{eq}/cm2^2) expected during operation. To this end, we have used Sentaurus TCAD to develop a 2D simulation of the ITk large-format strip sensor, based on detailed optical and electrical measurements of the sensors and of test devices fabricated on the same wafers. Current-voltage and capacitance-voltage behaviour is reproduced in the simulation by implementing charge trapping due to defects in the silicon, and the dependence of sensor behaviour on the location of these defects is investigated. Trapping parameters are informed by existing frameworks, such as the Perugia model of surface and bulk radiation damage, and by deep-level transient spectroscopy of test devices on the sensor wafers

    Thermal and hydrodynamic studies for micro-channel cooling for large area silicon sensors in high energy physics experiments

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    Micro-channel cooling initially aiming at small-sized high-power integrated circuits is being transferred to the field of high energy physics. Today`s prospects of micro-fabricating silicon opens a door to a more direct cooling of detector modules. The challenge in high energy physics is to save material in the detector construction and to cool large areas. In this paper, we are investigating micro-channel cooling as a candidate for a future cooling system for silicon detectors in a generic research and development approach. The work presented in this paper includes the production and the hydrodynamic and thermal testing of a micro-channel equipped prototype optimized to achieve a homogeneous flow distribution. Furthermore, the device was simulated using finite element methods

    Analysis of MOS capacitor with p-layer with TCAD simulation

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    The ATLAS18 strip sensors of the ATLAS inner tracker upgrade (ITk) are under production since 2021. Along with the large-format n^+-in-p strip sensor in the center of the wafer, test structures are laid out in the open space for monitoring the performance of the strip sensor and its fabrication process. One of the structures is a 1.2×1.0 mm^2 test chip that includes representative structures of the strips, and Metal-Oxide-Silicon (MOS) capacitors. In addition to the standard MOS capacitor, a MOS capacitor with a p-layer in the surface of silicon, the MOS-p capacitor, is designed with a p-density representative of the p-stop doping for isolating the n+ strips. The C-V curve of the MOS capacitor shows characteristic behavior in the accumulation, depletion, and inversion regions as a function of bias voltage, from which one can estimate the amount of the interface charge. The MOS-p capacitor shows the C-V curve modulated by the properties of the p-layer. With over 50% of the full production complement delivered, we have observed consistent characteristics in the MOS-p capacitors. Rarely and currently only in 3 batches, we have observed abnormalities. To further study them, we have simulated the MOS-p capacitor with TCAD software, which successfully reproduces the normal behavior, including a feature caused by a geometrical setback of the p-layer to the metal area, with the p-density and the interface charge within the expected range. By contrast, the overall shapes of the abnormal cases are only reproduced with 1/10 of the p-density to the specification and possible charge traps in the p-layer area. A smaller but distinctive feature in the behavior may require a non-uniform distribution of the p-density and the interface charge or something else. These simulations help to take final decisions for the batches in production
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