PPT-Recent measurements of linear & nonlinear optics at the ESRF storage ring

Andrea Franchi ESRF Grenoble on behalf of the Beam Dynamics amp Diagnostics groups TWDULER 2018 DIAMOND 19 th 20 th April 2018 Andrea Franchi Optics Measurements ESRF 2 Outlines. Di64256erentiating 8706S 8706f Setting the partial derivatives to 0 produces estimating equations for the regression coe64259cients Because these equations are in general nonlinear they require solution by numerical optimization As in a linear model Framework in . Py. . A. . Da. . Ronch. University of. L. iverpool. , . UK. Liverpool, . 16. March 2012. Target. . Nonlinear models . for flexible aircraft (hierarchy). Nonlinear . model reduction. Identifying functions . on tables, graphs, and equations.. Irma Crespo 2010. Warm Up. Graph y = 2x + 1. Rewrite the linear equation 3y + x = 9 to its slope-intercept form or the “y = ” form.. What is the linear equation for this graph?. 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.. Optics Measurements, Corrections & Modeling for High-Performance Storage Rings, . June 20-22, 2011. J. Safranek. Linear . Optics . from . Closed Orbits . (LOCO). Given linear optics (quad. gradients), can calculate response matrix.. 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. Bishwajyoti Dey. Department of Physics,. University of Pune, Pune. With Galal Alakhaly. GA, BD Phys. Rev. E 84, 036607 (1-9) 2011. Nonlinear localised excitations – solitons, breathers, compactons.. August 17, 2017. Garnet Ring Measurements. Garnet Ring Test Stand. Measurements have been made on . Ring 1 (wrong size). Ring 2 (chipped). Empty cavity. . First Result . First measurements on the rings showed a significant difference in Q between the rings and from the predicted curve.. 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. 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 8-pole magnet. M. . Aiba. , M. . Böge. , Á. . Saá. Hernández, . D. . Mayilyan. and A. . Streun. Paul . Scherrer. . Institut. Contents. SLS. “Local” LOCO. Emittance monitor status. Energy spread measurement using TBT data. Reports can now be submitted independently of new proposals Adam Johnson¹, Paul Bremner. 3. Matt Griebel¹, Brent Erickson¹, Joel Sills. 2. 1. Quartus Engineering Incorporated. 2. NASA Engineering and Safety Center. 3. AeroHydroPLUS. Background. Vibration testing of the Orion Multi-Purpose Crew Vehicle (MPCV) Configuration 4 (C4) Structural Test Article (STA) was performed in the reverberant acoustic chamber at Lockheed Martin. 20. th. ESLS RF Meeting. - PSI. Villigen. , 16. . – . 17 November . 2016. Status of RF operation and RF upgrade . for the future . E. xtremely . B. rilliant . S. ource (EBS) at the ESRF. OUTLOOK.