PPT-Non-intercepting diagnostic for high brightness electron be

A Cianchi 12 M Castellano 3 L Catani 2 E Chiadroni 3 G Gatti 3 K Honkavaara 4 G Kube 4 1 University of Rome Tor Vergata v della Ricerca Scientifica. - . X-ray vision. http://www.bjwinslow.com/albums/medicalcharts/broken_arm_radius_and_ulna_x_ray_10.jpg. http://www.museumboerhaave.nl/AAcollection/AAJPEGS/M22/9955.jpg. http://www.uab.edu/surgonc/cases/GI/case2/ctscanof.htm. People Management Network. 1. Overview of the session. Introduction to the project . An explanation of the Diagnostic. Conclusions – what I have learnt. Developed . from the Strengthening the Performance Framework Project. throughout the radiation belts. Sarah . Glauert. British . Antarctic Survey, Cambridge, UK. SPACECAST . stakeholders . meeting, . BAS, . 7 February 2014. Electron Radiation Belts. High energy electrons (E>500 keV) are trapped by Earth’s magnetic field. nanotube : Small source many fringes:N. Jonge, et al. Nature 420, 393 (2002) Thermal electron source. Few fringeshttp://em-outreach.ucsd.edu/web-course/Sec-I.D/Sec-I.D.html Fresnel Fringes J. Elec. M James . B. Murphy, Director. BES Scientific User Facilities . Division. Status of International Light Sources:. Today and in the Near Future. presented . to the. BESAC . Meeting. 25 July 2013. Light Sources: ERL, . Evan Walsh. Mentors: Ivan . Bazarov. . and David Sagan. August 13, 2010. Accelerating charges emit electromagnetic radiation. For synchrotron radiation, the radiation is usually X-rays. One of the main goals of the new . Evan Walsh. Mentors: Ivan . Bazarov. . and David Sagan. August 13, 2010. Accelerating charges emit electromagnetic radiation. For synchrotron radiation, the radiation is usually X-rays. One of the main goals of the new . Brightness Limiting Phenomena. Simulated bunch profile for 20pC and 80pC bunch charges from a realistic . birefringent. . pulse-stacked laser profile. .. The onset of the . virtual cathode instability (VCI). Chad . Auginash. April 20, 2015. Abstract. High electron mobility transistor(HEMT) is a transistor that operates at higher frequencies, typically in the microwave range. They are used in applications that require high frequency, such as cell phones, RF applications, and some power applications. HEMTs are transistors that utilize the 2-dimensional electron gas(2DEG) created by a junction between two materials with different band gaps called a heterojunction. The two most commonly used materials to create the heterojunction are a highly doped n-type donor material, typically . High Brilliance Beam Diagnostics A. Cianchi University of Rome “ Tor Vergata” and INFN Advanced Accelerator Physics Course 2015 Outline Brightness and Brilliance Fundamental parameters Transverse and longitudinal measurements Alexander Cahill. UCLA Dept. of Physics and Astronomy. For the UCLA/SLAC/INFN collaboration. June 30, 2017. Outline. Motivation. Cryo. RF Experiments. RF Photoinjector Design. Beam Dynamic Studies. Conclusions. Amir . Abdurahim. EE4611. 04/11/2016. Introduction. Is a . FET. Uses Hetero-junction . instead of . PN . junction . Uses . high mobility . m. aterials (. GaAs. /. AlGaAs. , . GaN. /. AlGaN. , III-V). Figure 1:Field emitter gun; the electron source in field emission scanning electron microscope. The only electron source designed for highresolution imaging and suitable for various kinds of materials Kurt . Aulenbacher. . (Uni. Mainz). Erdong Wang. . (BNL). 6/26/17. 1. Talks. . summary:. . Photocathode. 6/26/17. 2. 1. 6. 1. 3. 3. 6. . invitation. . talks+1. . contribution. . talks. 1. 5. 1.