letters to nature Em, the simulation suggests that this matrix becomes much closer to is the realization of a cavity with both high quality factor, Q, and the ideal one(keeping almost ideal outputs for 110) and 111)input small modal volume, V. The ratio Q/V determines the strength of states)if we slightly decrease the rise/fall

INTERNATIONAL UNION OF PURE AND APPLIED CHEMISTRY INORGANIC CHEMISTRY DIVISIOI COMMISSION ON ATOMIC WEIGHTS AND ISOTOPIC ABUNDANCES* SUBCOMMITTEE FOR ISOTOPIC ABUNDANCE MEASUREMENTS *N ISOTOPIC COMPOSITIONS OF THE ELEMENTS 1997 by KJR ROSMAN AND PDP TAYLOR2 Department of Applied Physics, Curtin University of Technology, GPO Box U1987, Perth 6001

From: physics. nist. gov/constants Fundamental Physical Constants- Complete Listing Relative std UNIVERSAL speed of light in vacuum c,co299792458

Graphlte works as a lubrlcant because the planes,held together by strong chemlcal (covalent) bonds between the carbon atoms, can sllde across each other wlth only J.M.H.L.S. weak Van der Waals bonds between the planes belng broken

Ultra-cold Fermi Gases From Molecular Bose-Einstein Condensation to BCS Pairing cks CENTRE NATIONAL DE LA RECHERCHE SCIENTIHIQL Bose-Einstein condensate

physicsweb Physics news, jobs and resources Fermionic first for condensates Physics in Action: March 2004 The creation of the first fermionic condensate will herald a new generation of research into the properties of superfluids and superconductors

When an electric charge is supported at rest in a static gravitational field, its electric field is not supported with the charge, and it falls freely in the gravitationa field. Drawing the electric field lines continuously in time, we find that they always emerge from the charge, but the electric field is curved and there is a stress force between the freely falling (curved)field and the static charge. The charge radiates

Radiation from a Uniformly Accelerated Charge and the Equivalence Principle Stephen Parrott Department of Mathematics University of Massachusetts at Boston

constraint on cano us magnetism in T superconductor has also preprnsa gr-qe/pdi

第一章 绪论 第二章 单轴液晶连续体弹性形变理论 第三章 弹性形变理论的应用 第四章 丝状和螺旋状液晶中的缺陷… 第五章 丝状与螺旋状液晶的流体动力学方程 第六章 丝状和螺旋状液晶电磁流体动力学 第七章 丝状和螺旋状液晶的流动 第八章 丝状和螺旋状液晶中的不稳定性 第九章 丝状液晶分子场理论 第十章 分子场理论的应用 第十一章 丝状液晶和螺旋状液晶的光散射 第十二章 层状液晶和盘形分子液晶