PPT-Nuclear Moments: Recent Tabulations, and Physics of Magnetic Dipole and Electric Quadrupole

and Physics of Magnetic D ipole and Electric Q uadrupole M oments NJStone Oxford and Tennessee IAEA April 2015 Outline 1 Table of Recommended Nuclear Electric Quadrupole Moments. of. the SM (3):. non-. collider. . particle. . physics. FK8022, . Lecture. . 7. Core. text:. Further. . reading. :. C. ollider vs non-. collider. . physics. (1). Can. . see. new . physics. ?. Electric polarisation (. P. ) - . electric. dipole moment per unit vol.. Magnetic ‘polarisation’ (. M. ) - . magnetic. dipole moment per unit vol.. M. . magnetisation . Am. -1 . c.f. . P . polarisation . Magnets. Shashikant . Manikonda. Taylor . Model Methods . VII, . Dec. 14. th. -17. th. , 2011, Key West, Florida. S3 device at SPIRAL2. 2. SHE / VHE - Fusion-evaporation in direct kinematics . SHE / VHE. Multipole. expansion. Prof. Hugo Beauchemin. 1. Introduction . When we studied Gauss’ law, we saw that the field created by a sphere was the same as the one created by a point charge at the center of the sphere. Why?. Determination . of the Scope and Form of Census Data Dissemination. Capacity Building. 2. Scope of Census Data Dissemination. From census data to (standard) information— . Population counts. “Quick” counts. Magnetic fields . Physics 2102. Gabriela Gonz. á. lez. L. Magnetic force on a wire. L. Note: If wire is not straight,. compute force on differential elements and integrate:. Example. By symmetry, F. Solitons. Makoto Kobayashi. KEK. 2011/10/27. Recollections of Nagoya Univ.. Under graduate 1963-1967. Graduate 1967-1972. . Chiral. . s. ymmetry. . Maskawa. , Kondo, Hattori. James Bounds. Organization. Dipole and Quadrupole transitions. Special Laser beam types. Using special laser beams to induce Quadrupole transitions. Experimental Realization. Possible extensions. E-M Fields. … force in . direction. … . sample volume. … magnetic . susceptibility. … magnetic field. … gradient of . the magnetic . field.  . The magnetic susceptibility . characterizes the magnetic properties of materials. eEDM. ) is aligned with the spin and interacts with the giant (~84 GV/cm) effective internal electric field of the . ThO. molecule.. The . statistical sensitivity of the measurement is given . by. STIRAP increases the usable molecule flux by improving the EDM state preparation efficiency.. Allen R. . Majewski. Department of Physics. University of Florida . February 2015. NiCl. 2. - [SC(NH. 2. ). 2. ]. 4. . dichloro. -. tetrakis. -. thiourea. -nickel. Overview. The . value of nuclear quadrupole resonance . RHIC & AGS Annual User Meeting. Brookhaven National Laboratory. June 23, 2011. Timothy J. Hallman. Associate Director for Nuclear Physics. Office of Science, U.S. Department of Energy. 2. To enable U.S. world leadership in discovery science illuminating the properties of nuclear matter in all of its manifestations. Charles Munger, Jr.. As part of the Electron EDM Collaboration:. Ben Feinberg, Harvey Gould, Juris . Kalnins. , Charles Munger, Hiroshi Nishimura, Chris . Tomassi. , and Shawn Zhao (Lawrence Berkeley National Laboratory). :. Bohr magneton. Dr. Mahender Singh. Associate Professor in Physics. PGGC – 11 Chandigarh. Current . loop. Such a current loop would have a magnetic dipole moment m . given by. where I is the current and A is the loop area. m is a vector whose direction is as shown in the diagram..