Hyperfine Structure of Cs2 Molecules in Electronically Excited States
... one can drive a phase transition from a superfluid (SF) phase to a Mott-insulator (MI) phase. In the SF phase the atoms are delocalized over the lattice. In the MI phase every lattice site is occupied with the same number n (for n =, 1, 2, 3, ...) of atoms. If an external trap is superimposed on the ...
... one can drive a phase transition from a superfluid (SF) phase to a Mott-insulator (MI) phase. In the SF phase the atoms are delocalized over the lattice. In the MI phase every lattice site is occupied with the same number n (for n =, 1, 2, 3, ...) of atoms. If an external trap is superimposed on the ...
I. Course Title Advanced Placement Physics C: Mechanics and
... semester) and electricity and magnetism (second semester), including vector and calculusbased treatment of particle kinematics (motion), Newton’s interaction model, energy, linear momentum, angular momentum, systems of particles, oscillators, and Newtonian gravity in the first semester. Topics cover ...
... semester) and electricity and magnetism (second semester), including vector and calculusbased treatment of particle kinematics (motion), Newton’s interaction model, energy, linear momentum, angular momentum, systems of particles, oscillators, and Newtonian gravity in the first semester. Topics cover ...
GR0177 Solutions
... The Poisson Distribution is intimately related to the raising and lowering operators of the (quantum mechanical) simple harmonic oscillator (SHO). When you hear the phrase “simple harmonic oscillator,” you should immediately recall the number operator√N = a† a, as well as the√characteristic relation ...
... The Poisson Distribution is intimately related to the raising and lowering operators of the (quantum mechanical) simple harmonic oscillator (SHO). When you hear the phrase “simple harmonic oscillator,” you should immediately recall the number operator√N = a† a, as well as the√characteristic relation ...
Abstracts - QCMC 2016 - Centre for Quantum Technologies
... Large-amplitude squeezed optical Schrödinger cat states with minimized non-Gaussian operational cost 12:30 Lunch 14:00 Alex Bocharov, Microsoft Qomputer Science at Microsoft Research 14:30 Julian Kelly, Google Industrializing qubits through automation 15:00 Coffee/Tea Break 15:30 Bill Munro, NTT Qua ...
... Large-amplitude squeezed optical Schrödinger cat states with minimized non-Gaussian operational cost 12:30 Lunch 14:00 Alex Bocharov, Microsoft Qomputer Science at Microsoft Research 14:30 Julian Kelly, Google Industrializing qubits through automation 15:00 Coffee/Tea Break 15:30 Bill Munro, NTT Qua ...
Lecture Notes for Physics 229: Quantum Information and Computation
... The moral we draw is that \information is physical." and it is instructive to consider what physics has to tell us about information. But fundamentally, the universe is quantum mechanical. How does quantum theory shed light on the nature of information? It must have been clear already in the early d ...
... The moral we draw is that \information is physical." and it is instructive to consider what physics has to tell us about information. But fundamentally, the universe is quantum mechanical. How does quantum theory shed light on the nature of information? It must have been clear already in the early d ...
Experiments and theory in cold and ultracold collisions
... the potential difference. The quasimolecule finds itself photoassociated and vibrating within the attractive well. A second field \ v 2 can then further excite or even ionize the photoassociated quasimolecule, or it can relax back to some distribution of the continuum and bound levels of the ground ...
... the potential difference. The quasimolecule finds itself photoassociated and vibrating within the attractive well. A second field \ v 2 can then further excite or even ionize the photoassociated quasimolecule, or it can relax back to some distribution of the continuum and bound levels of the ground ...
Annals of Physics Classical impurities and boundary Majorana zero
... In this paper we aim at identifying clear physical differences associated with the presence or absence of Majorana edges modes in the topologically ordered or non-ordered phases, respectively. We focus on the effects of an impurity that interrupts an otherwise homogeneous 1d chain, or terminates it. ...
... In this paper we aim at identifying clear physical differences associated with the presence or absence of Majorana edges modes in the topologically ordered or non-ordered phases, respectively. We focus on the effects of an impurity that interrupts an otherwise homogeneous 1d chain, or terminates it. ...
Einstein`s quantum theory of the monatomic ideal gas: non
... and the prediction of what came to be known as the Bose-Einstein condensation phenomenon. The third paper, in contrast, has rarely been mentioned, and we have not found any work that would analyze it in some detail. Max Jammer3 , Friedrich Hund4 , Abraham Pais5 , Jagdish Mehra and Hans Rechenberg,6 ...
... and the prediction of what came to be known as the Bose-Einstein condensation phenomenon. The third paper, in contrast, has rarely been mentioned, and we have not found any work that would analyze it in some detail. Max Jammer3 , Friedrich Hund4 , Abraham Pais5 , Jagdish Mehra and Hans Rechenberg,6 ...
Quantum Physics of Atoms, Molecules, Solids, Nuclei, and Particles
... The basic purpose of this book is to present clear and valid treatments of the properties of almost all of the important quantum systems from the point of view of elementary quantum mechanics. Only as much quantum mechanics is developed as is required to accomplish the purpose. Thus we have chosen t ...
... The basic purpose of this book is to present clear and valid treatments of the properties of almost all of the important quantum systems from the point of view of elementary quantum mechanics. Only as much quantum mechanics is developed as is required to accomplish the purpose. Thus we have chosen t ...
IBS for CLIC damping ring/Lattice design for IBS - Indico
... • the diffusion factor B(k, m) of classical and quantum approximations (that account for the scattering) are close to each other in spite of a huge difference between cm and qm (cf, below), k= x’/y’ is the velocity coupling parameter (k=1 for round and k for flat beams) ...
... • the diffusion factor B(k, m) of classical and quantum approximations (that account for the scattering) are close to each other in spite of a huge difference between cm and qm (cf, below), k= x’/y’ is the velocity coupling parameter (k=1 for round and k for flat beams) ...
Topology and geometry in a quantum condensed matter system
... order parameters associated with broken symmetries. Following this analogy, the topological classification of general gapped many-body states of matter may be used to describe the subclass of states that can be described by the band theory of solids. The shape of the band structure and how the energ ...
... order parameters associated with broken symmetries. Following this analogy, the topological classification of general gapped many-body states of matter may be used to describe the subclass of states that can be described by the band theory of solids. The shape of the band structure and how the energ ...
Physik-Department Technische Universität München
... (LMU) in Munich. I soon became a good friend of one of his former students, Dr. Markus J. Storcz, with whom I started discussing about circuit quantum electrodynamics with superconducting flux qubits and developing architectures for the coupling of such qubits with on-chip microwave resonators. It ha ...
... (LMU) in Munich. I soon became a good friend of one of his former students, Dr. Markus J. Storcz, with whom I started discussing about circuit quantum electrodynamics with superconducting flux qubits and developing architectures for the coupling of such qubits with on-chip microwave resonators. It ha ...
Renormalization group
In theoretical physics, the renormalization group (RG) refers to a mathematical apparatus that allows systematic investigation of the changes of a physical system as viewed at different distance scales. In particle physics, it reflects the changes in the underlying force laws (codified in a quantum field theory) as the energy scale at which physical processes occur varies, energy/momentum and resolution distance scales being effectively conjugate under the uncertainty principle (cf. Compton wavelength).A change in scale is called a ""scale transformation"". The renormalization group is intimately related to ""scale invariance"" and ""conformal invariance"", symmetries in which a system appears the same at all scales (so-called self-similarity). (However, note that scale transformations are included in conformal transformations, in general: the latter including additional symmetry generators associated with special conformal transformations.)As the scale varies, it is as if one is changing the magnifying power of a notional microscope viewing the system. In so-called renormalizable theories, the system at one scale will generally be seen to consist of self-similar copies of itself when viewed at a smaller scale, with different parameters describing the components of the system. The components, or fundamental variables, may relate to atoms, elementary particles, atomic spins, etc. The parameters of the theory typically describe the interactions of the components. These may be variable ""couplings"" which measure the strength of various forces, or mass parameters themselves. The components themselves may appear to be composed of more of the self-same components as one goes to shorter distances.For example, in quantum electrodynamics (QED), an electron appears to be composed of electrons, positrons (anti-electrons) and photons, as one views it at higher resolution, at very short distances. The electron at such short distances has a slightly different electric charge than does the ""dressed electron"" seen at large distances, and this change, or ""running,"" in the value of the electric charge is determined by the renormalization group equation.