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Advanced Quantum Technologies, 2020
Abstract This review is about single‐particle entanglement. Entanglement occurs when the state of a quantum system with at least two degrees of freedom has a particular non‐separable form. In the case of single‐particle entanglement, this quantum correlation is shared by the same particle being it a photon, a neutron, an ion, or an ...
Azzini, Stefano +4 more
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Abstract This review is about single‐particle entanglement. Entanglement occurs when the state of a quantum system with at least two degrees of freedom has a particular non‐separable form. In the case of single‐particle entanglement, this quantum correlation is shared by the same particle being it a photon, a neutron, an ion, or an ...
Azzini, Stefano +4 more
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Single-Particle Virus Tracking
Cold Spring Harbor Protocols, 2011INTRODUCTIONReal-time, live-cell imaging techniques and single-particle tracking algorithms can be used to follow individual virus particles as they infect cells. This protocol describes the use of one or more fluorescent markers to perform single-particle virus-tracking experiments.
Michael J, Rust +3 more
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2007
Abstract The single-particle approach to solving macromolecular structure (see Frank, 1996, 2006) is based on the premise that the specimen is in the form of many isolated particles that are randomly oriented, collectively presenting a large range of views.
Robert M Glaeser +4 more
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Abstract The single-particle approach to solving macromolecular structure (see Frank, 1996, 2006) is based on the premise that the specimen is in the form of many isolated particles that are randomly oriented, collectively presenting a large range of views.
Robert M Glaeser +4 more
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Single Particle Electron Microscopy
2012Single particle electron microscopy is a versatile technique for the structural analysis of protein complexes in near-native conditions. While tremendous progress has been made during the past few decades in techniques for specimen preparation, imaging, and image analysis, the field is still in development.
Wilson C Y, Lau, John L, Rubinstein
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1995
Abstract In Section 3.3 we have seen that the dynamical processes underlying the velocity autocorrelation function in the liquid range cannot be accounted for by a simplified memory-function analysis. In particular, the assumption that the decay of the memory function is ruled by a single relaxation time must be significantly revised ...
Umberto Balucani, Marco Zoppi
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Abstract In Section 3.3 we have seen that the dynamical processes underlying the velocity autocorrelation function in the liquid range cannot be accounted for by a simplified memory-function analysis. In particular, the assumption that the decay of the memory function is ruled by a single relaxation time must be significantly revised ...
Umberto Balucani, Marco Zoppi
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Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms, 1991
Abstract The high radiation damage of MeV heavy ions does not only destroy targets, it can also be used to produce microstructures in an unusually wide range of materials by a combination of irradiation and chemistry. Unlike any other type of radiation used for microlithography, already a single ion is able to produce a microstructure, usually an ...
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Abstract The high radiation damage of MeV heavy ions does not only destroy targets, it can also be used to produce microstructures in an unusually wide range of materials by a combination of irradiation and chemistry. Unlike any other type of radiation used for microlithography, already a single ion is able to produce a microstructure, usually an ...
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2010
In Chap. 2 we discussed the idea of the guiding center (GC) approximation and the solutions of $$\frac{d{\bf p}}{dt} = q ({\bf E} + {\bf v} \times{\bf B})+{\bf F}_{{non}-EM} $$ (3.1) for homogeneous fields. Here we consider the motion in inhomogeneous fields, starting for simplicity, at the non-relativistic limit \((\gamma =\, 1, \ \mathbf{p}=
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In Chap. 2 we discussed the idea of the guiding center (GC) approximation and the solutions of $$\frac{d{\bf p}}{dt} = q ({\bf E} + {\bf v} \times{\bf B})+{\bf F}_{{non}-EM} $$ (3.1) for homogeneous fields. Here we consider the motion in inhomogeneous fields, starting for simplicity, at the non-relativistic limit \((\gamma =\, 1, \ \mathbf{p}=
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Proceedings, annual meeting, Electron Microscopy Society of America, 1973
All of us are familiar with dust, dirt and smoke particles in the atmosphere. Many of us, in industry, are also familiar with contamination of our products, often by these same atmospheric pollutants. In any program to clean up the atmosphere or to clean up a given industrial product it is helpful, to say the least, to know the chemical composition and
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All of us are familiar with dust, dirt and smoke particles in the atmosphere. Many of us, in industry, are also familiar with contamination of our products, often by these same atmospheric pollutants. In any program to clean up the atmosphere or to clean up a given industrial product it is helpful, to say the least, to know the chemical composition and
openaire +1 more source