A tunable two-impurity Kondo system in an atomic point contact
... cobalt adatoms on the Au(111) surface (Fig. 2(a)), which can be identified by their characteristic Kondo resonance. In tunnelling spectra, the Kondo resonance is detected as a Fano line shape due to interference between electrons tunnelling into the conduction band of the substrate and into the Kond ...
... cobalt adatoms on the Au(111) surface (Fig. 2(a)), which can be identified by their characteristic Kondo resonance. In tunnelling spectra, the Kondo resonance is detected as a Fano line shape due to interference between electrons tunnelling into the conduction band of the substrate and into the Kond ...
Spatial Light Modulators for the Manipulation of Individual Atoms
... Any tight spatial confinement of atoms in dipoleforce traps relies on small foci of the trapping light. Therefore, an optical system of high numerical aperture is necessary. This can be done with either a sophisticated microscope objective [22] or a single aspheric lens [23]. Typically, these are di ...
... Any tight spatial confinement of atoms in dipoleforce traps relies on small foci of the trapping light. Therefore, an optical system of high numerical aperture is necessary. This can be done with either a sophisticated microscope objective [22] or a single aspheric lens [23]. Typically, these are di ...
A statistical mechanics approach to the factorization problem
... carry operation. Thus, while the distribution of bond strengths in the full factorization problem is exponentially broad, it is not broad enough to allow us to apply a greedy algorithm in which we satisfy the bonds one at a time. ...
... carry operation. Thus, while the distribution of bond strengths in the full factorization problem is exponentially broad, it is not broad enough to allow us to apply a greedy algorithm in which we satisfy the bonds one at a time. ...
α-clustering & universal law for reduced widths III. Coherent
... which is fulfilled by all cluster and particle emission processes 2) CSM is able to decribe energy levels and B(E2)-values in vibrational, transitional and rotational even-even nuclei in terms of the deformation parameter d. 3) CSM describes α-transitions to excited states these nuclei by using an u ...
... which is fulfilled by all cluster and particle emission processes 2) CSM is able to decribe energy levels and B(E2)-values in vibrational, transitional and rotational even-even nuclei in terms of the deformation parameter d. 3) CSM describes α-transitions to excited states these nuclei by using an u ...
FEATURE ARTICLE
... Clearly the total energy is also a functional of the ground state density. There is, however, a subtle point here: the operator Ô in (2.4) now being the Hamiltonian, we should be clear about the potential V(r) to be used in the Hamiltonian. There are two main possibilities. If for each F we take th ...
... Clearly the total energy is also a functional of the ground state density. There is, however, a subtle point here: the operator Ô in (2.4) now being the Hamiltonian, we should be clear about the potential V(r) to be used in the Hamiltonian. There are two main possibilities. If for each F we take th ...
Electronic Structure of Atoms
... come from analysis of the light either emitted or absorbed by substances. To understand electronic structure, therefore, we must first learn more about light. The light that we can see with our eyes, visible light, is an example of electromagnetic radiation. Because electromagnetic radiation carries ...
... come from analysis of the light either emitted or absorbed by substances. To understand electronic structure, therefore, we must first learn more about light. The light that we can see with our eyes, visible light, is an example of electromagnetic radiation. Because electromagnetic radiation carries ...
Appendix-Revised_FINAL
... where J is the angular momentum quantum number. The first order energy spectrum of the three fold degenerate vibration 3 state is complicated by the Coriolis interaction of the total angular momentum and the vibrational angular momentum of the 3 state (l3=1) and results in the splitting of each of ...
... where J is the angular momentum quantum number. The first order energy spectrum of the three fold degenerate vibration 3 state is complicated by the Coriolis interaction of the total angular momentum and the vibrational angular momentum of the 3 state (l3=1) and results in the splitting of each of ...
Driven Dirac-like equation via mirror oscillation: Controlled cold
... DOI: 10.1103/PhysRevA.81.023608 ...
... DOI: 10.1103/PhysRevA.81.023608 ...
Iridates - UCSB Physics
... hole state leading to the destructive interference at the L2 edge, we calculate the scattering amplitudes. The most general wave function for the hole state in the t2g manifold involves six basis states, which can be reduced by block-diagonalizing the spin-orbit Hamiltonian as c1 jxy, þs〉 þ c2 jyz,− ...
... hole state leading to the destructive interference at the L2 edge, we calculate the scattering amplitudes. The most general wave function for the hole state in the t2g manifold involves six basis states, which can be reduced by block-diagonalizing the spin-orbit Hamiltonian as c1 jxy, þs〉 þ c2 jyz,− ...
Observation of oscillatory energy exchange in a coupled-atom
... The choice of normalization for x and y permits a straightforward interpretation. y is the intracavity field in the absence of atoms, and x the intracavity field in the presence of atoms, where jxj2 , jyj2 express an intracavity photon number of units of n0 . Equations (3) are written in a rotating ...
... The choice of normalization for x and y permits a straightforward interpretation. y is the intracavity field in the absence of atoms, and x the intracavity field in the presence of atoms, where jxj2 , jyj2 express an intracavity photon number of units of n0 . Equations (3) are written in a rotating ...
84, 013608 (2011)
... process that generates steady charge currents of electrons through adiabatically and periodically time-varying potentials, is a standard method for charge transport in solid-state circuits [1–5]. In quantized charge transport, the number of particles pumped out during each cycle of the potential mod ...
... process that generates steady charge currents of electrons through adiabatically and periodically time-varying potentials, is a standard method for charge transport in solid-state circuits [1–5]. In quantized charge transport, the number of particles pumped out during each cycle of the potential mod ...
5, 4023 (2014)
... and the system shows an interesting superradiant phase with a macroscopic occupation of photons and non-vanishing spin polarization26–28. Even though this model has been solved and is well understood theoretically, the experimental observation was achieved only recently by coupling a BEC to an optic ...
... and the system shows an interesting superradiant phase with a macroscopic occupation of photons and non-vanishing spin polarization26–28. Even though this model has been solved and is well understood theoretically, the experimental observation was achieved only recently by coupling a BEC to an optic ...
Entropy and the Shelf Model: A Quantum Physical Approach to a
... particles are larger than within liquids or gases, which means that the level spacing is larger and the entropy smaller. Thus the shelf model helps to illustrate that normally the entropy of solid materials is smaller than that of liquids or gases where the particles are not forced to stay in such a ...
... particles are larger than within liquids or gases, which means that the level spacing is larger and the entropy smaller. Thus the shelf model helps to illustrate that normally the entropy of solid materials is smaller than that of liquids or gases where the particles are not forced to stay in such a ...
Electron Deep Orbits of the Hydrogen Atom1
... - 1. Only the relativistic equations can predict EDOs with mean radius of order femto-meter. We can even give a simple mathematical reason for this fact. So, for example, one can see that with a non-relativistic Schrödinger equation, one can obtain “anomalous” solutions, but they are not EDOs. - 2. ...
... - 1. Only the relativistic equations can predict EDOs with mean radius of order femto-meter. We can even give a simple mathematical reason for this fact. So, for example, one can see that with a non-relativistic Schrödinger equation, one can obtain “anomalous” solutions, but they are not EDOs. - 2. ...
Paper
... lations N6q of thermally excited Bogoliubov quasiparticles at wave vectors 6q. However, in our measurements using stimulated scattering from two laser beams, the contribution of the thermal excitations cancels out [14], and thus we extract the zero-temperature structure factor. In contrast, by measu ...
... lations N6q of thermally excited Bogoliubov quasiparticles at wave vectors 6q. However, in our measurements using stimulated scattering from two laser beams, the contribution of the thermal excitations cancels out [14], and thus we extract the zero-temperature structure factor. In contrast, by measu ...
