PPT-Quasi-Elastic Scattering on

MINERvA Kevin McFarland University of Rochester NuINT11 Dehradun 8 March 2011 ν Goddess μ To India via Indiana Thank you to the organizers for their efforts to allow me to attend . Miguel A. Gonzalez. Institut. Laue-. Langevin. (Grenoble, France). gonzalezm@ill.eu. Outline. General remarks and reminders. The main equations and their physical meaning. QENS models for translational diffusion and localized motions. . True Experiments. Characteristics. Threats to validity controlled by experiments. Threats not controlled by experiments. Obstacles to true experiments in the field. . Quasi-experiments. The logic of quasi-experiments . Yong Ma. Sparse model space for projected Hessian. Quasi-Newton FWI. Eigenvector (largest . eigenvalue. ). Eigenvector (smallest . eigenvalue. ). CM34 @ RAL. Timothy Carlisle. 1. Intro.. MICE performance predicted using the cooling formula (. CF. ):. G4MICE . ≠. CF. (see . prev. CMs). Simulation disagrees with C.F by up to 20%.. MS calc. typically approx.: . DJ . Strouse. University of Southern California. Andrew M. Childs. University of Waterloo. Why Scatter on Graphs?. NAND Tree problem:. Best classical algorithm:. Randomized. Only needs to evaluate of the leaves. Research Objective. Show direct cause & effect. Study relationships among variables for existing groups. Explain outcomes after the fact. Type of Design. True Experiment. Quasi-Experiment. Cross-Sectional. Lecture 3. Free Particle:. Energy . , In Cartesian and spherical Coordinates.. Wave function: . . (plane waves in Cartesian system) . Green’s Function: . The Green function will be used in Born. approximation of scattering amplitude and therefore. first we try to understand a little about Green function.. The Green’s function of an operator . Ken Herwig. Instrument and Source Division. Neutron Sciences Directorate. Oak Ridge National Laboratory. August 13, 2016. OUTLINE. Background – the incoherent scattering cross section of H. Neutrons and QENS. Neutron Scattering. Ken Herwig. Instrument . and Source Division. Neutron . Sciences . Directorate. Oak Ridge . National Laboratory. June 22, 2015. OUTLINE. Background – the incoherent scattering cross section of H. Neutron Scattering. Ken Herwig. Instrument . and Source Division. Neutron . Sciences . Directorate. Oak Ridge . National Laboratory. June 22, 2015. OUTLINE. Background – the incoherent scattering cross section of H. Ya. -Qi Wei*,. . Jian-Zhong Chen, Lei Lin, Yu-Tong Zhao, Jia Chen. E-mail: yqweii@qq.com.com. Abstract. Diffusion Metasurface Design. Results. Conclusions. A novel optically transparent diffusion metasurface composed of 1-bit coding elements is presented. Two circular quasi-Minkowski closed-loops with different geometric scales are considered as 1-bit coding elements. The quasi-Minkowski closed-loops on the upper layer of the substrate and the back-ground on the lower layer are filled with metallic tangent ring mesh to improve the light transmittance. Low scattering is achieved by redirecting EM energies to all directions through optimization of the arrangement of coding elements. The low back-scattering characteristics with wide-angle and polarization independence below –10 dB of the diffusion metasurface are achieved over a wide frequency band from 9 GHz to 16 GHz. The proposals offer new opportunities for manipulating the microwave scattering with simultaneously high optical transparency in visible frequencies and demonstrate significant scientific value in practical applications.. a+. 208. Pb Elastic Scattering. M . Nure. . Alam. Abdullah. , M Zahid Hasan, . Sinthia. . Binte. . Kholil. and Dipika Rani . Sarker. Department of Physics, Jagannath University, Dhaka-1100 Bangladesh. Based on the ITER-like and Snowflake divertor configuration of CFETR (Phase I, R = 5.7 m), SOLPS simulation is performed to understand the performance of radiative quasi-snowflake . divertor . with argon seeding..