Spin–spin coupling tensors as determined by experiment and
... NMR spectroscopy of molecules dissolved in liquid crystalline media (liquid crystal NMR, LCNMR) or solid samples either as powders or single crystals. Interpretation of hyperfine data taken from molecular beam experiments is also discussed in this context. Quantum chemical electronic structure calcu ...
... NMR spectroscopy of molecules dissolved in liquid crystalline media (liquid crystal NMR, LCNMR) or solid samples either as powders or single crystals. Interpretation of hyperfine data taken from molecular beam experiments is also discussed in this context. Quantum chemical electronic structure calcu ...
physics at surfaces
... making all that quarter of the pond, perhaps half an acre, as smooth as a looking-glass. (Seeger, 1973.) Remarkably, Franklin did not perform the simple calculation which would have led him to conclude that the film thickness was only about one nanometer! The firm establishment of modern methods of ...
... making all that quarter of the pond, perhaps half an acre, as smooth as a looking-glass. (Seeger, 1973.) Remarkably, Franklin did not perform the simple calculation which would have led him to conclude that the film thickness was only about one nanometer! The firm establishment of modern methods of ...
density
... Special thanks to David Ambrosek for so much help with so many things. Family, friends, without you I am nothing—I silently thank you for your support and understanding! ...
... Special thanks to David Ambrosek for so much help with so many things. Family, friends, without you I am nothing—I silently thank you for your support and understanding! ...
Essay code B3
... usually found on lead pencils. Graphene is a one atom thick single layer sheet of sp2 hybridized carbon atoms. Therefor Graphene is considered to be the thinnest of all materials available. The professors extracted Graphene from Graphite in 2004 by merely using an adhesive scotch tape. The unique me ...
... usually found on lead pencils. Graphene is a one atom thick single layer sheet of sp2 hybridized carbon atoms. Therefor Graphene is considered to be the thinnest of all materials available. The professors extracted Graphene from Graphite in 2004 by merely using an adhesive scotch tape. The unique me ...
Relativistic coupled cluster theory - in molecular properties and in
... In the second part of this thesis we will move into the discussion of molecular properties. In the first chapter of this part we will theoretically analyze the role of spin-orbit coupling in various molecular properties. This analysis helped us to conclude that Spin Orbit Coupling (SOC) has a great ...
... In the second part of this thesis we will move into the discussion of molecular properties. In the first chapter of this part we will theoretically analyze the role of spin-orbit coupling in various molecular properties. This analysis helped us to conclude that Spin Orbit Coupling (SOC) has a great ...
Experiments to Control Atom Number and Phase
... limited in their applicability to a small number of atoms, single-photon cooling is much more general and should in principle be applicable to almost all atoms in the periodic table. The experiment described in this dissertation demonstrates a one-dimensional implementation of the cooling scheme. Co ...
... limited in their applicability to a small number of atoms, single-photon cooling is much more general and should in principle be applicable to almost all atoms in the periodic table. The experiment described in this dissertation demonstrates a one-dimensional implementation of the cooling scheme. Co ...
entropy and superfluid critical parameters of a strongly interacting
... is “A good experimental physicist is always an excellent engineer,” which is one of many John’s quotations I love. John has been a fantastic mentor and a true friend during my years at Duke. I am sure that I will look back on this time in my life with fond memories with such a great mentor. In our ...
... is “A good experimental physicist is always an excellent engineer,” which is one of many John’s quotations I love. John has been a fantastic mentor and a true friend during my years at Duke. I am sure that I will look back on this time in my life with fond memories with such a great mentor. In our ...
Quantum information with Rydberg atoms
... 共Bloch, 2008兲. They share many features in common with trapped ion systems including long-lived encoding of quantum information in atomic hyperfine states and the possibility of manipulating and measuring the qubit state using resonant laser pulses. Neutral atoms distinguish themselves from ions whe ...
... 共Bloch, 2008兲. They share many features in common with trapped ion systems including long-lived encoding of quantum information in atomic hyperfine states and the possibility of manipulating and measuring the qubit state using resonant laser pulses. Neutral atoms distinguish themselves from ions whe ...
Luminescence studies of strontium sulphide based
... studies of strontium sulphide based phosphors for display applications " is based on the original research work done by me under the supervision and guidance of Dr. M.K. Jayaraj, Reader, Department of Physics, Cochin University of Science and Technology, Cochin-682022 and has not been included in an ...
... studies of strontium sulphide based phosphors for display applications " is based on the original research work done by me under the supervision and guidance of Dr. M.K. Jayaraj, Reader, Department of Physics, Cochin University of Science and Technology, Cochin-682022 and has not been included in an ...
TGD AND EEG
... 3.4 Models for ionic superconductivity and topological condensation at the magnetic flux quanta of endogenous magnetic field . . . . . . . . . . . . . . . . . . . . . . . . . . . . 198 3.4.1 Model for ionic superconductivity based on Cooper pairs . . . . . . . . . . . . 198 3.4.2 Super conductors of ...
... 3.4 Models for ionic superconductivity and topological condensation at the magnetic flux quanta of endogenous magnetic field . . . . . . . . . . . . . . . . . . . . . . . . . . . . 198 3.4.1 Model for ionic superconductivity based on Cooper pairs . . . . . . . . . . . . 198 3.4.2 Super conductors of ...
The effect of boron on the amount and type of carbides in
... as wear resistant materials under conditions of strong loading, whereas in other cases the behaviour of these materials depends on the type, fraction, size and morphology of the carbide phase.1,2 Carbide, or cementite, is an extremely hard, brittle compound of carbon with either iron or strong carbi ...
... as wear resistant materials under conditions of strong loading, whereas in other cases the behaviour of these materials depends on the type, fraction, size and morphology of the carbide phase.1,2 Carbide, or cementite, is an extremely hard, brittle compound of carbon with either iron or strong carbi ...
An introduction to magnetic reconnection
... Characteristics of magnetic reconnection: a) it generates an electric field which accelerates particles parallel to B b) it dissipates magnetic energy (direct heating) c) it accelerates plasma, i.e. converts magnetic energy into kinetic energy d) it changes the magnetic topology (further relaxation ...
... Characteristics of magnetic reconnection: a) it generates an electric field which accelerates particles parallel to B b) it dissipates magnetic energy (direct heating) c) it accelerates plasma, i.e. converts magnetic energy into kinetic energy d) it changes the magnetic topology (further relaxation ...
Emittance growth induced by electron cloud in proton storage rings
... quasi–continuous interaction with the electrons, whose distribution can be chosen independently at each location. Preliminary results of these simulations are presented, in the weak–strong approximation, as a first important step toward the modelization of realistic accelerator components. ...
... quasi–continuous interaction with the electrons, whose distribution can be chosen independently at each location. Preliminary results of these simulations are presented, in the weak–strong approximation, as a first important step toward the modelization of realistic accelerator components. ...
AP Phys B FRQ - Blue Valley Schools
... through a pair of parallel plates, as shown above. The plates are separated by a distance d = 6.0 x I o- m, and a constant potential difference V is maintained between them. A uniform magnetic field of magnitude B 0.20 T directed into the page exists both between the plates and in a region to the ri ...
... through a pair of parallel plates, as shown above. The plates are separated by a distance d = 6.0 x I o- m, and a constant potential difference V is maintained between them. A uniform magnetic field of magnitude B 0.20 T directed into the page exists both between the plates and in a region to the ri ...
Experimental Characterization of Nonclassical
... and characterized to serve as the foundation of experiments generating polarization squeezing and entanglement. These nonclassical polarization states have been generated not only in fiber systems but also by Optical Parametric Oscillators (OPO) [19, 20] and cold atomic samples [21, 22]. Additionall ...
... and characterized to serve as the foundation of experiments generating polarization squeezing and entanglement. These nonclassical polarization states have been generated not only in fiber systems but also by Optical Parametric Oscillators (OPO) [19, 20] and cold atomic samples [21, 22]. Additionall ...
Phase change memory technology
... A critical property of phase change materials is the so-called threshold switching[45–48]. Without this effect PCM would simply not be a feasible technology, because in the high resistance state extremely high voltages would be required to deliver enough power to the cell to heat it above the crysta ...
... A critical property of phase change materials is the so-called threshold switching[45–48]. Without this effect PCM would simply not be a feasible technology, because in the high resistance state extremely high voltages would be required to deliver enough power to the cell to heat it above the crysta ...
FABRICATION AND STUDY OF ITO THIN FILMS
... spectrum shown in Figure 5-2, calculated with the standard and the modified model......................................................................................... 56 ...
... spectrum shown in Figure 5-2, calculated with the standard and the modified model......................................................................................... 56 ...
Condensed matter physics
Condensed matter physics is a branch of physics that deals with the physical properties of condensed phases of matter. Condensed matter physicists seek to understand the behavior of these phases by using physical laws. In particular, these include the laws of quantum mechanics, electromagnetism and statistical mechanics.The most familiar condensed phases are solids and liquids, while more exotic condensed phases include the superconducting phase exhibited by certain materials at low temperature, the ferromagnetic and antiferromagnetic phases of spins on atomic lattices, and the Bose–Einstein condensate found in cold atomic systems. The study of condensed matter physics involves measuring various material properties via experimental probes along with using techniques of theoretical physics to develop mathematical models that help in understanding physical behavior.The diversity of systems and phenomena available for study makes condensed matter physics the most active field of contemporary physics: one third of all American physicists identify themselves as condensed matter physicists, and the Division of Condensed Matter Physics is the largest division at the American Physical Society. The field overlaps with chemistry, materials science, and nanotechnology, and relates closely to atomic physics and biophysics. Theoretical condensed matter physics shares important concepts and techniques with theoretical particle and nuclear physics.A variety of topics in physics such as crystallography, metallurgy, elasticity, magnetism, etc., were treated as distinct areas, until the 1940s when they were grouped together as solid state physics. Around the 1960s, the study of physical properties of liquids was added to this list, forming the basis for the new, related specialty of condensed matter physics. According to physicist Phil Anderson, the term was coined by him and Volker Heine when they changed the name of their group at the Cavendish Laboratories, Cambridge from ""Solid state theory"" to ""Theory of Condensed Matter"" in 1967, as they felt it did not exclude their interests in the study of liquids, nuclear matter and so on. Although Anderson and Heine helped popularize the name ""condensed matter"", it had been present in Europe for some years, most prominently in the form of a journal published in English, French, and German by Springer-Verlag titled Physics of Condensed Matter, which was launched in 1963. The funding environment and Cold War politics of the 1960s and 1970s were also factors that lead some physicists to prefer the name ""condensed matter physics"", which emphasized the commonality of scientific problems encountered by physicists working on solids, liquids, plasmas, and other complex matter, over ""solid state physics"", which was often associated with the industrial applications of metals and semiconductors. The Bell Telephone Laboratories was one of the first institutes to conduct a research program in condensed matter physics.References to ""condensed"" state can be traced to earlier sources. For example, in the introduction to his 1947 ""Kinetic theory of liquids"" book, Yakov Frenkel proposed that ""The kinetic theory of liquids must accordingly be developed as a generalization and extension of the kinetic theory of solid bodies"". As a matter of fact, it would be more correct to unify them under the title of ""condensed bodies"".