PPT-Introduction to Silicon Detectors

EGVillani STFC Rutherford Appleton Laboratory Particle Physics Department 1 Outlook Part I Introduction to physics of Si and detection Part II Examples of detectors Conclusions 2 Introduction. . Will it contribute to energy independence. ?. . Mustafa KOCAMAN, Taha ÖNGEL. May 08, 2013. Solar . cells are devices which convert solar light energy directly into electricity and function by the photovoltaic effect.  Photo- means light and -voltaic means electrical current or electricity  (light-electricity).  A solar cell provides direct current (DC) electricity that can be used to power DC motors and light bulbs among other things.  Solar cells can even be used to charge rechargeable batteries so that electricity can be stored for later use when the sun is not available. The fully charged batteries are portable energy that can be used whenever and wherever they are needed. After procuring raw sand and separating the silicon, the excess material is disposed of and the silicon is purified in multiple steps to finally reach semiconductor manufacturing quality which is called electronic grade silicon. The resulting purity is so great that electronic grade silicon may only have one alien atom for every one billion silicon atoms. After the purification process, the silicon enters the melting phase. In this picture you can see how one big crystal is grown from the purified silicon melt. The resulting mono-crystal is called an ingot.. Detectors for Astronomy 2009 W Detectors for Astronomy 2009 W Detectors for Astronomy 2009 W Detectors for Astronomy 2009 Workshop 14 October AM5Maximilian Fabricius K. Hara. University of Tsukuba. Faculty of Pure and Applied Sciences. EDIT2013 March 12-22,2013. Applications of Si detectors. vertexing. tracking. whole tracking. VLSI. UA2. F. Hartmann (2009). First t. Hrvoje Štefančić. . Theoretical Physics Division . Ruđer Bošković Institute . (based on joint work with . Hrvoje Abraham . and . Predrag Lazić. ). Electric field strength in a segment of a Si microstrip detector. Studen. , . Karol . Brzezinski. , . Enrico. . Chesi. , Vladimir . Cindro. , . Neal. H. . Clinthorne. , Milan . Grkovski. , Borut . Grošičar. , Klaus . Honscheid. ,. . S. S. . Huh. , Harris . IRAD 2731. What is a semiconductor?. Types of semiconductors. Why is it different than . scintillators. Agenda. Semiconductor – has electrical conductivity between metals and insulators. Pure- pure Si or . Overview. David Christian. Fermilab. June 9, 2011. Outline. History: Why semiconductor detectors?. (Concentrating on silicon). Energy Resolution. Position Resolution (leverage of IC technology). Transition to the present. Ruqayyah Askar. PHYS 689 . April 27, 2018. Outline. Introduction. General principles. Historical overview. Types of IR . detectors. Current IR . technologies. Parameters of IR Detectors. Emerging . Technologies. R. . . A. . . Akbarov. a,b,c. , . S. . . M. . . Nuruyev. a,b. , . G. . . S. . . Ahmadov. a,b,c. , Z. . . Y. . . Sadiqov. a,c. , . F. . . Ahmadov. b,c. , . S. . Tyutyunnikov. a. , . A. . Sadigov. b,c. 12 minutes. . budgets, list of projects, and new graduate students who are entering (. Bruce: please send me numbers and names). . SBIR's and SLAC proposal  and US Japan . Bruce please send me information on your SBIRs and anything similar. M. Bruzzi. 1. , R. Mori. 1. , M. Scaringella. 1. , Z. Li. 2. 1. INFN and University of Florence, Florence (Italy). 2. BNL, Upton New York (US). M. . Bruzzi. , R. Mori, M. . Scaringella. , Z. Li . Shallow levels analysis in n-type MCZ Si detectors after mixed irradiation, . EDIT 2018. Michelle Stancari | Noble Element Detectors | EDIT 2018. 2. Abundant ionization and scintillation light. No electronegativity, free electrons travel large distances (if no impurities). Dobromir. . Pressyanov. Sofia University “St. . Kliment. . Ohridski. ”. , Bulgaria. The focused challenge: How to evaluate by short-term (e.g. one week) integrated measurements at normal living conditions the radon reduction achieved after the mitigation work is completed? .