PPT-Nonlinear Optics as a Path to High-Intensity Circular Machines

S Nagaitsev A Valishev Fermilab and V Danilov ORNL Draft talk for HB2010 Sep 23 2010 2 Report at HEAC 1971 CBX layout 1962 1965 Priceton Stanford CBX First mention of an 8pole magnet. CMSC 435/634. Light. Electromagnetic wave. E & M perpendicular to each other & direction. Photon wavelength . l. , frequency f = c/. l. Visbile. . l. ≈ 380 nm (blue) to 720 nm (red). Photon energy q = h f = h c/. Circular motion. We will be looking at a special case of kinematics and dynamics of objects in uniform circular motion (constant speed). Cars on a circular track (or on a curved road). Roller coasters in loop. by Mike Plum. Ring Area Manager. Spallation Neutron Source. Workshop on Optics . Measurements, Corrections, and Modeling at High Performance Storage . Rings, CERN, . June 20-22, 2011 . High . i. ntensity challenges. Honors senior undergraduate and graduate level course.. Approximately 24-26 lecture hours + 3 seminars.. Lectures 2-4:15 Saturday, Sunday, Tuesday and Wednesday. Designed to provide a . working. knowledge of Nonlinear Optics.. Indus Synchrotrons Utilization Division. RRCAT, Indore. Advances in Science, Engineering and Technology Colloquium . TIFR, August 20, 2010. lodha@rrcat.gov.in. Focused X-Ray . Beams :. Generation . and Applications. 5.1 . Uniform Circular Motion. DEFINITION OF UNIFORM CIRCULAR MOTION. Uniform circular motion is the motion of an object . traveling at a constant speed on a circular path.. 5.1 . Uniform Circular Motion. nouveaux guides d’ondes, nouvelles non linéarités, . nouvelles directions … . John Dudley. CNRS Institut FEMTO-ST. Université de Franche-Comté . Besançon, France. Mardi 2 décembre 2014. Workshop INSIS - Optique électromagnétique. Dylan R. Card and Ross A. . Lazear. Department of Atmospheric & Environmental Sciences, State University of New York, Albany New York. Motivation. :. T. he . rear flanking . downdraft . (RFD) and secondary rear flanking downdraft (SRFD) . Circular Motion Lab Results. Part 1: Radius’ effect on velocity. Mass, centripetal force kept constant. Part 2: Mass’ effect on velocity. Radius, centripetal force kept constant. Part 3: Force’s effect on velocity. Third order nonlinear optics offers a wide range of interesting phenomena which are very . different. from . what is expected from linear optics. The most important are due to changes in the . properties. Andrea Franchi (ESRF, Grenoble). on behalf of the . Beam Dynamics & Diagnostics groups. TW-DULER 2018, DIAMOND, 19. th. -20. th. April 2018. Andrea Franchi Optics Measurements @ ESRF. 2. Outlines. Synchrotron . Optics. Simulations. : . 3-Codes . T. utorial . 3 - 5. June 2013, ESRF, . France. O. . Chubar. Photon Sciences Directorate, BNL. NSLS-II @ BNL. Outline. Light . Source Developments Driving . UCRL-PRES-226145Alan Conder Terry Alger Jim Chang Warren Massey Jack Nguyen Ben PeraltaSteve Azevedo Steve Glenn Laura Kegelmeyer Judy Liebman Scott LernerNIF Optics Inspection TeamImagine the scale o at PW-class Lasers. and beyond. Stepan Bulanov. BELLA Center, ATAP Division, LBNL . “Extreme High-Intensity Laser Physics” (. ExHILP. ) Conference, . Max Planck Institute for Nuclear Physics (MPIK) in Heidelberg, Germany, 21-24 July 2015.