Y. Unno , E. Bach , J. Dandoy , V. Fadeyev , C. Fleta , C. Jessiman , J. Keller , C.T. Klein , T. Koffas , E. Staats , M. Ullan
{"title":"Analysis of MOS capacitor with p layer with TCAD simulation","authors":"Y. Unno , E. Bach , J. Dandoy , V. Fadeyev , C. Fleta , C. Jessiman , J. Keller , C.T. Klein , T. Koffas , E. Staats , M. Ullan","doi":"10.1016/j.nima.2024.170045","DOIUrl":null,"url":null,"abstract":"<div><div>The ATLAS18 strip sensors of the ATLAS inner tracker upgrade (ITk) are in production since 2021. Along with the large-format n<span><math><msup><mrow></mrow><mrow><mo>+</mo></mrow></msup></math></span>-in-p strip sensor in the center of 6-inch wafer, test structures including Metal–Oxide–Silicon (MOS) capacitors are laid out in the open space for monitoring the performance of the strip sensor and its fabrication process. One of the MOS capacitors is with a p-implantation in the surface of silicon to access the p-stop doping for isolating the n<span><math><msup><mrow></mrow><mrow><mo>+</mo></mrow></msup></math></span> strips, the MOS-p capacitor. The capacitance measurement of the standard MOS capacitor as a function of gate voltage (C–V) shows characteristic behavior in the accumulation, depletion, and inversion regimes, from which one can deduce the amount of the interface charge. The MOS-p capacitor shows the C–V characteristics 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 three incidents, we have observed anomalous behaviors which implied lower density of p-layer. To study the cause, we have simulated the MOS-p capacitor with a TCAD device simulator. The normal characteristic curve is reproduced successfully with p-density and interface charge within the expected ranges, including a feature caused by a geometrical offset. The anomalous C–V characteristics cannot be explained simply by low p-density, but instead explained with the p-layer density near the specification which goes to zero at the surface. The loss of density could have been introduced with an n-type surface contamination or some other effect such as “dopant segregation”. These simulations have helped to take final acceptance decisions for the batches in production.</div></div>","PeriodicalId":19359,"journal":{"name":"Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment","volume":"1071 ","pages":"Article 170045"},"PeriodicalIF":1.5000,"publicationDate":"2024-11-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0168900224009719","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"INSTRUMENTS & INSTRUMENTATION","Score":null,"Total":0}
引用次数: 0
Abstract
The ATLAS18 strip sensors of the ATLAS inner tracker upgrade (ITk) are in production since 2021. Along with the large-format n-in-p strip sensor in the center of 6-inch wafer, test structures including Metal–Oxide–Silicon (MOS) capacitors are laid out in the open space for monitoring the performance of the strip sensor and its fabrication process. One of the MOS capacitors is with a p-implantation in the surface of silicon to access the p-stop doping for isolating the n strips, the MOS-p capacitor. The capacitance measurement of the standard MOS capacitor as a function of gate voltage (C–V) shows characteristic behavior in the accumulation, depletion, and inversion regimes, from which one can deduce the amount of the interface charge. The MOS-p capacitor shows the C–V characteristics 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 three incidents, we have observed anomalous behaviors which implied lower density of p-layer. To study the cause, we have simulated the MOS-p capacitor with a TCAD device simulator. The normal characteristic curve is reproduced successfully with p-density and interface charge within the expected ranges, including a feature caused by a geometrical offset. The anomalous C–V characteristics cannot be explained simply by low p-density, but instead explained with the p-layer density near the specification which goes to zero at the surface. The loss of density could have been introduced with an n-type surface contamination or some other effect such as “dopant segregation”. These simulations have helped to take final acceptance decisions for the batches in production.
期刊介绍:
Section A of Nuclear Instruments and Methods in Physics Research publishes papers on design, manufacturing and performance of scientific instruments with an emphasis on large scale facilities. This includes the development of particle accelerators, ion sources, beam transport systems and target arrangements as well as the use of secondary phenomena such as synchrotron radiation and free electron lasers. It also includes all types of instrumentation for the detection and spectrometry of radiations from high energy processes and nuclear decays, as well as instrumentation for experiments at nuclear reactors. Specialized electronics for nuclear and other types of spectrometry as well as computerization of measurements and control systems in this area also find their place in the A section.
Theoretical as well as experimental papers are accepted.