PPT-1 Self Accelerating Beams of Photons and Electrons

Ady Arie Dept of Physical Electronics TelAviv University TelAviv Israel Heraklion Crete September 20 th 2013 2 Outline The quantummechanical Airy wavefunction and its properties. JIM TURNERLOOK AT ME NOW...WRITTEN BY: CHAS SMITHEXCEPTIONS TO...PHOTOGRAPHED BY: JOHN CAREYWRITTEN BY: JOANNA PRISCOA WOMAN AS...WRITTEN BY: ALICE PFEIFFER 1 1 .functionPoint(x,y){varself={};self.x=x;self.y=y;self.setX=function(d:number){self.x=d;};returnsetTag(point)(self);}ThefunctionPointcreatesanewpoint.Itallocatesanewemptyrecordandstoresitinthelocal Janne Pakarinen. – on behalf of the IS494 collaboration. . – . University of Jyväskylä. ARIS 2014. Tokyo, Japan. Shapes and collectivity in the neutron-deficient . even mass . 188-198. Pb isotopes. 1 1 .functionPoint(x,y){varself={};self.x=x;self.y=y;self.setX=function(d:number){self.x=d;};returnsetTag(point)(self);}ThefunctionPointcreatesanewpoint.Itallocatesanewemptyrecordandstoresitinthelocal LIGHT AMPLIFICATION by STIMULATED ELECTRON RADIATION. Question:. In movies, laser beams are always shown as bright pencils of light streaking through the air or space. If you were to look from the side at a beam from a powerful laser, would you be able to see that laser beam as it travels past you?. at CDF. April 15. th. , 2013. Baylor HEP Seminar. Karen Bland . for the CDF collaboration. Public webpage:. http://www-cdf.fnal.gov/physics/exotic/run2/Zgamgam/index.html. 1. Outline. Introduction. Tevatron. “. Coalescence . of Single Photons Emitted by Disparate Single-Photon Sources: The Example of InAs Quantum Dots and Parametric Down-Conversion . Sources. ,. ” . S.V. . . Polyakov. , A. Muller, E.B. Flagg, A. Ling, N. . Beams:. Comparison with . trusses, plates. . Examples:. 1. simply supported beams. 2. cantilever beams. L, W, t: L >> W and L >> t. L. W. t. Beams - loads and internal loads. Loads: concentrated loads, distributed loads, couples (moments). bandgap. energy illuminates a negative electron affinity (NEA) . GaAs. . photocathode, spin-polarized electrons are emitted [2, 3]. The degree of polarization is defined to be . where . N. ↑. and . Light and Energy. Particles (photons) and waves at the same time! . c = . f. . . The greater. f (frequency), . the smaller. .  (wavelength). The greater. f, . the higher the energy of the EM radiation.. Presented by: Scott McGinnis . Regional Sales Manager . LEED. ®. Associate. Overview. Chilled Beam Systems. Moisture Control. Munters Options Equipment. Whole Goal is to design a system where the Chilled Water temperatures throughout the building are consistent with the needs of the chilled beams and not driven by the OAU.. S.V. Kuzikov. 1. , A.A. Vikharev. 1. , J.L. Hirshfield. 2,3. 1. Institute of Applied Physics RAS, Nizhny Novgorod, Russia. 2. Yale University, New Haven, CT, USA. 3. Omega-P, Inc., New Haven, CT, USA. 0. Accelerators for neutrino physics:. The Beta. . Beam. . . . Elena Wildner, . BE. /. ABP. 0. 2015-11-26. 2015-11-26. Elena Wildner: Beta Beams, ATS Seminar. 1. Outline. General: . Neutrinos. W. Wuensch. 11-12-2009. Accelerating structure assembly. Pulsed ΔT in accelerating structure. Beam-loading compensation. Reacting to breakdown. On/off/ramp mechanism. Dynamic vacuum. Refining design and 10% parameter consistency.