PDF-Measurement of the ionization rates in diffused silicon junctions

Author : alexa-scheidler | Published Date : 2017-04-10

OF THE IONIZATION RATES IN DIFFUSED SILICON VAN OVERSTRAETEN and H DE Electronic Research Laboratories Section Solid State Electronics Catholic University of Louvain

Presentation Embed Code

Download Presentation

Download Presentation The PPT/PDF document "Measurement of the ionization rates in d..." is the property of its rightful owner. Permission is granted to download and print the materials on this website for personal, non-commercial use only, and to display it on your personal computer provided you do not modify the materials and that you retain all copyright notices contained in the materials. By downloading content from our website, you accept the terms of this agreement.

Measurement of the ionization rates in diffused silicon junctions: Transcript

OF THE IONIZATION RATES IN DIFFUSED SILICON VAN OVERSTRAETEN and H DE Electronic Research Laboratories Section Solid State Electronics Catholic University of Louvain 94 Kardinaal XJercierlaan H. Tran sm ission Lin Mod l RR WL U W L RR 2006 International Conference on Microelectronic Test Structures 1424401674062000 575132006 IEEE 13 brPage 2br RR L W L RR RL R B Cu rren d rectio n in flu en ce Di ffusion Silic de Blocking mask 14 brPage 3br Au+Au. collisions at √. s. NN. = 200 . GeV. in STAR experiment at RHIC. Jaiby Joseph Ajish. 11/9/2011. Outline. Introduction. Why collide nuclei at high energies?. RHIC and STAR. Physics at RHIC. NN. = 200 GeV in STAR experiment at RHIC. Jaiby Joseph . Ajish. 11/2/2011. Outline. Quick summary of my contributions. Introduction. Why . collide nuclei at high energies?. RHIC, STAR. Physics at RHIC. Au+Au. collisions at √. s. NN. = 200 . GeV. in STAR experiment at RHIC. Jaiby Joseph Ajish. 11/9/2011. Outline. Introduction. Why collide nuclei at high energies?. RHIC and STAR. Physics at RHIC. E.G.Villani. 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. NN. = 200 GeV in STAR experiment at RHIC. Jaiby Joseph . Ajish. 11/2/2011. Outline. Quick summary of my contributions. Introduction. Why . collide nuclei at high energies?. RHIC, STAR. Physics at RHIC. Guillermo A. Blanc. Universidad de Chile. OUTLINE. MEASURING ABUNDANCES IN IONIZED GAS. SEL METHOD SYSTEMATICS AND CHALLENGES. IZI: THE BAYESIAN APPROACH. THE ABUNDANCE SCALE DISCREPANCY. CONCLUSIONS. nanocrystals. doped with P, Li, S. N.V. . Derbeneva. , . V.A. . Burdov. Lobachevsky. State University of Nizhniy Novgorod. Published data . by other authors . on . radiative. recombination lifetimes. K. . Sengupta. Indian Association for the Cultivation of Sciences, Kolkata. Overview. Dirac materials: Introduction and basic properties. a) . Graphene. b) Topological Insulators. Alan martin, . sam. . harison. ,. karen. beach and peter . cole. Radiation detection and . measurement . 7.1 GENERAL PRINCIPLES . The . fact that the human body is unable to sense ionizing radiation . C,. 16. O). g. . reaction in . Inverse . Kinematics. Kunihiro. FUJITA. K. . Sagara. , T. . Teranishi. , . M. . Iwasaki, . D. . Kodama, . S. . Liu, . S. . Matsuda, . T. . Mitsuzumi. , . J.Y. . Moon, . Au Au. collisions at √. s. NN. = 200 . GeV. in STAR experiment at RHIC. Jaiby Joseph Ajish. 11/9/2011. Outline. Introduction. Why collide nuclei at high energies?. RHIC and STAR. Physics at RHIC. Swaroop K. Behera. 1. , . Shvetashwa. Suri. 1. Pradeep Rohatgi. 1. , Nathan Salowitz. 2. 1. Department of Material Science and Engineering, UW-Milwaukee . 2. Department of Mechanical Engineering , UW-Milwaukee. presented by. Suman.Thota. M.Pharm . II-Semester. Department. of Industrial Pharmacy. UNIVERSITY COLLEGE OF PHARMACEUTICAL SCIENCES. KAKATIYA UNIVERSITY. WARANGAL. . .

Download Document

Here is the link to download the presentation.
"Measurement of the ionization rates in diffused silicon junctions"The content belongs to its owner. You may download and print it for personal use, without modification, and keep all copyright notices. By downloading, you agree to these terms.