
Subnanometre resolution in three-dimensional magnetic resonance
... the dark-spin PSF there is no reliance on magnetic-field modelling or iterative deconvolution schemes that must be simultaneously solved for both an unknown signal and an unknown PSF. The spatial resolution of NV-MRI is given by 1/(t.g|∇Btip|), where g and t are the target spin’s gyromagnetic ratio a ...
... the dark-spin PSF there is no reliance on magnetic-field modelling or iterative deconvolution schemes that must be simultaneously solved for both an unknown signal and an unknown PSF. The spatial resolution of NV-MRI is given by 1/(t.g|∇Btip|), where g and t are the target spin’s gyromagnetic ratio a ...
The Puzzling Story of the Neutral Kaon System or what we can learn
... Discrete 2010, Beatrix C. Hiesmayr ...
... Discrete 2010, Beatrix C. Hiesmayr ...
pdf - VUB
... Note that these theories have di culty accounting for why items that are dissimilar or even opposite might nevertheless belong together; for example, why white might be more likely to be categorized with black than with ¯at, or why dwarf might be more likely to be categorized with giant than with s ...
... Note that these theories have di culty accounting for why items that are dissimilar or even opposite might nevertheless belong together; for example, why white might be more likely to be categorized with black than with ¯at, or why dwarf might be more likely to be categorized with giant than with s ...
Full Text - J
... By means of Laplace transform, in [4] a complete system of Stokes multipliers for (1) is computed in terms of connection coe‰cients, connecting selected vector solutions of (3) (called associated functions) at di¤erent Fuchsian singularities. The definition of associated functions, connection coe‰cie ...
... By means of Laplace transform, in [4] a complete system of Stokes multipliers for (1) is computed in terms of connection coe‰cients, connecting selected vector solutions of (3) (called associated functions) at di¤erent Fuchsian singularities. The definition of associated functions, connection coe‰cie ...
Document
... Illustration #1 -- two atoms are excited and entangled but not communicating with each other. Result #1 -- both atoms decay, diag e-2gt and offdiag e-gt , just as expected; but entanglement of the atoms behaves qualitatively differently. Illustration #2 -- two atoms fly apart in molecular ...
... Illustration #1 -- two atoms are excited and entangled but not communicating with each other. Result #1 -- both atoms decay, diag e-2gt and offdiag e-gt , just as expected; but entanglement of the atoms behaves qualitatively differently. Illustration #2 -- two atoms fly apart in molecular ...
1 Path Integrals and Their Application to Dissipative Quantum Systems
... The most often used and taught approach to nonrelativistic quantum mechanics is based on the Schrödinger equation which possesses strong ties with the the Hamiltonian formulation of classical mechanics. The nonvanishing Poisson brackets between position and momentum in classical mechanics lead us t ...
... The most often used and taught approach to nonrelativistic quantum mechanics is based on the Schrödinger equation which possesses strong ties with the the Hamiltonian formulation of classical mechanics. The nonvanishing Poisson brackets between position and momentum in classical mechanics lead us t ...
Nicolas Gisin - Quantum Nonlocality
... Edited by Bernard Cohen, assisted by Robert E. Schofield Harvard University Press, Cambridge, Massachusetts, 1958 ...
... Edited by Bernard Cohen, assisted by Robert E. Schofield Harvard University Press, Cambridge, Massachusetts, 1958 ...
Localized - Current research interest: photon position
... In standard quantum mechanics a measurement is associated with an operator and collapse to one of its eigenvectors. For the position observable this requires a position operator and collapse to a localized state. The generalized theory of observables only requires a partition of the identity operato ...
... In standard quantum mechanics a measurement is associated with an operator and collapse to one of its eigenvectors. For the position observable this requires a position operator and collapse to a localized state. The generalized theory of observables only requires a partition of the identity operato ...