PPT-Thermomechanicle examinations for the design of the radiation cooled positron target

Sabine Riemann DESY Andriy Ushakov UHH Alexandre Ignatenko DESY Kahled Alharbi DESY Felix Dietrich DESY THWildau Peter Sievers CERN Laboratoire lAccélératuer. Chemistry. ________________ involve changes with electrons. . ________________ involve changes in atomic nuclei. . Spontaneously-changing nuclei emit ________ and. are said to be _________. . Chemical reactions. . LCWS . 2014, Belgrade, October 6. th. -10. th. , . 2014. Steffen Döbert, BE-RF. No changes to the electron injector. Some work started on optimizing the. positron source with a student started recently . Wei Gai for the ILC e- and e+ collaboration . PAC review, 2012. KEK, Japan. ILC site layout and location of e- and e+ sources. Page . 3. The Baseline ILC Electron Source . Electron source provides polarized electron beam and consists of all systems from source laser to 5 GeV injection to damping rings. ( 325 MHz SHB). Global Design Effort. 1. ALCPG11 – Eugene. Positron Source. N. Collomb. J. Clarke, D. Angal-Kalinin,. 20/03/2011. Global Design Effort. 2. Positron Source UK summary. Presentation covers the following:. Yongjoong. Lee. ESS, Materials. , Target Division. 5. th. High Power . Targetry. Workshop. May 20, 2014. Spallation Target at ESS. 5 MW spallation source. 5 MW (2.0 GeV/2.5 mA) proton beam . 2.86 ms long beam pulse with 14 Hz repetition rate. Global Design Effort. 1. Positron Source meeting. J. Clarke, D. Angal-Kalinin, N. Collomb. 10/02/2011. Global Design Effort. 2. Positron Source close out. Positron Source is broken down into the following parts. Lessons Learned from Our Past. Collider-Accelerator Department. 5-28-2013. Take 5 for Safety. Event at J-PARK. In the Hadron Experimental . Facility, . experiments were conducted with the elementary particles that had been generated by irradiating gold target with proton . Configuration Design of the Fusion . Power Core . for. the ACT. (Draft). X.R. Wang. M.S. Tillack. S. Malang. Sept. 29, 2011. One sector (22.5 degree). ARIES-ACT 1B(Aggressive Physics), Posted at ARIES Web: June 8, 2011. Yongjoong. Lee. ESS, Materials. , Target Division. 5. th. High Power . Targetry. Workshop. May 20, 2014. Spallation Target at ESS. 5 MW spallation source. 5 MW (2.0 GeV/2.5 mA) proton beam . 2.86 ms long beam pulse with 14 Hz repetition rate. Radiation Backgrounds for Future High Energy Electron Positron Colliders Hongbo Zhu (IHEP, Beijing) On behalf of the CEPC Study Group Workshop on the Circular Electron Positron Collider – EU edition, 24 – 26 May, Rome Fermilab. 11. th. November 2015. 1. Chris Densham. STFC Rutherford Appleton Laboratory. On behalf of the T2K beam collaboration. 2. 2015 Breakthrough Prize in Fundamental Physics awarded to Professor . A person working with radioisotopes wears protective clothing and gloves and stands behind a shield.. 2. Radioactive Isotopes. A . radioactive isotope . has an unstable nucleus. emits radiation to become more stable. Dr Sarah Bohndiek. Learning outcomes. After . this lecture, you should be able to. :. Describe how . ionising. radiation is generated for medical imaging. Explain the differences between an X-ray tube and a linear accelerator. . LCWS 2014, Belgrade, Serbia. 7. th. October 2014. Sabine Riemann, DESY, Peter . Sievers. , . CERN/ESS,. Andriy. . Ushakov. , Hamburg U. ILC positron target. Ti. . alloy wheel . diameter . = . 1m.