Tip-Enhanced Fluorescence Microscopy at 10 Nanometer Resolution
... where Fz=F1 is the detected fluorescence rate normalized to the background rate (F1 ), and is the fieldenhancement factor. The solid curves show least-squares fits to Eq. (1) ( , a free parameters) while the dashed curves are exponential decays. The data are clearly consistent with a power law, ...
... where Fz=F1 is the detected fluorescence rate normalized to the background rate (F1 ), and is the fieldenhancement factor. The solid curves show least-squares fits to Eq. (1) ( , a free parameters) while the dashed curves are exponential decays. The data are clearly consistent with a power law, ...
Semiclassical theory of helium atom
... distinction of singlet states (total spin S = 0) and triplet states (S = 1) often referred to as parahelium and orthohelium, respectively. Figure 4 depicts, as a representative case, the level diagram of parahelium. The helium states and energy levels can be classified as follows: (i) the ground sta ...
... distinction of singlet states (total spin S = 0) and triplet states (S = 1) often referred to as parahelium and orthohelium, respectively. Figure 4 depicts, as a representative case, the level diagram of parahelium. The helium states and energy levels can be classified as follows: (i) the ground sta ...
PDF
... the statistical operator formalism: A quantum mixed state so expressed should not be thought of as an ensemble of pure states, but as a set of probability distributions, each one defined over the eigenvalues of each observable of the system. Thus, Stein concludes, the insolubility proof cannot const ...
... the statistical operator formalism: A quantum mixed state so expressed should not be thought of as an ensemble of pure states, but as a set of probability distributions, each one defined over the eigenvalues of each observable of the system. Thus, Stein concludes, the insolubility proof cannot const ...
Quantum Evolution installation and user manual
... Within the FULL DISPLAY SEQUENCE an a switching sequence of all or a selection of cameras can be set, with individual times allocated to selected cameras. Within the QUAD DISPLAY SEQUENCE a selection of screens displaying 4 cameras at a time can be set-up, the quad displays are fixed e.g. Quad 1 con ...
... Within the FULL DISPLAY SEQUENCE an a switching sequence of all or a selection of cameras can be set, with individual times allocated to selected cameras. Within the QUAD DISPLAY SEQUENCE a selection of screens displaying 4 cameras at a time can be set-up, the quad displays are fixed e.g. Quad 1 con ...
Physlets and Open Source Physics for Quantum Mechanics:
... Figure 6 shows the short-term time evolution of the probability density of a Gaussian wave packet in an infinite well with walls at x = 0 and x = 1. The packet has an initial momentum to the right and the images are shown at equal-time intervals. We are supposed to imagine the motion of the packet ...
... Figure 6 shows the short-term time evolution of the probability density of a Gaussian wave packet in an infinite well with walls at x = 0 and x = 1. The packet has an initial momentum to the right and the images are shown at equal-time intervals. We are supposed to imagine the motion of the packet ...
The Large D Limit of Planar Diagrams arXiv:1701.01171v1 [hep
... different purposes, in the ongoing quest to define d ≥ 3 dimensional quantum gravity from the continuum limit of a sum over discretized higher dimensional geometries (see e.g. [18] and references therein). It is gratifying that the technology developed there can find an entirely different applicatio ...
... different purposes, in the ongoing quest to define d ≥ 3 dimensional quantum gravity from the continuum limit of a sum over discretized higher dimensional geometries (see e.g. [18] and references therein). It is gratifying that the technology developed there can find an entirely different applicatio ...
