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example: on the Bloch sphere: this is a rotation around the equator
example: on the Bloch sphere: this is a rotation around the equator

UvA-DARE (Digital Academic Repository) The problem of
UvA-DARE (Digital Academic Repository) The problem of

HW1 solutions - Colorado State University Computer Science
HW1 solutions - Colorado State University Computer Science

What is Probability? - General Guide To Personal and Societies
What is Probability? - General Guide To Personal and Societies

... What is probability? Physicists, mathematicians, and philosophers have been engaged with this question since well before the rise of modern physics. But in quantum mechanics, where probabilities are associated only with measurements, the question strikes to the heart of other foundational problems: ...
Quantum computation of scattering in scalar quantum field theories
Quantum computation of scattering in scalar quantum field theories

... E . However, discretizing a quantum field theory involves special difficulties unfamiliar from the classical context. A discretized system from classical physics converges to a continuum limit when one straightforwardly takes the lattice spacing to zero. In contrast, continuum limits of quantum fiel ...
Unscrambling the Quantum Omelette of Epistemic and Ontic
Unscrambling the Quantum Omelette of Epistemic and Ontic

Physical Chemistry Composite systems Adding angular momenta
Physical Chemistry Composite systems Adding angular momenta

... Orbital terms The orbital wave functions for multielectron systems are simultaneous eigenfunctions of L2 and Lz of the total system Multi-electron states labeled by the total ...
Get PDF - Physics of Information and Quantum Technologies Group
Get PDF - Physics of Information and Quantum Technologies Group

... as the dynamics can in general affect the internal degrees of freedom of the particles. The same is valid for their momentum or other dynamical variables. But their spatial location can actually be used to distinguish them, as shown in figure 1. Let us imagine we have two identical particles, one in A ...
Notas de F´ısica
Notas de F´ısica

Quantum mechanics near closed timelike lines
Quantum mechanics near closed timelike lines

... (i.e. , the existence of negative delays) makes no fundamental difference to the behavior of a network unless there is a closed path for infor mation. Such a path is not necessarily the trajectory of any carrier in the network because bits on different carriers interact and can exchange information ...
qm-cross-sections
qm-cross-sections

... Cross section for potential scattering In a practical scattering situation we have a finite acceptance for a detector with a solid angle W. There is a range of momenta which are allowed by kinematics which can contribute to the cross section. The cross section for scattering into W is then obtain ...
Kondo Screening Cloud Around a Quantum Dot
Kondo Screening Cloud Around a Quantum Dot

Handout 12
Handout 12

PDF
PDF

... of |1i on the initial phase φ (and, therefore, on the final phase φτ ) makes it possible to measure these quantities. As indicated above, these effects can be observed in an experiment where, for example, a stationary collection of atoms are excited repeatedly by a microwave field. However, a more r ...
ap® physics 2 2015 scoring guidelines
ap® physics 2 2015 scoring guidelines

Spin-liquids
Spin-liquids

The Electric Field
The Electric Field

... Analogy The electric field is the space around an electrical charge just like ...
Quantised Singularities in the Electromagnetic Field
Quantised Singularities in the Electromagnetic Field

Revealing novel quantum phases in quantum antiferromagnets on
Revealing novel quantum phases in quantum antiferromagnets on

The pressure increase at 4He l–point explained by means of the
The pressure increase at 4He l–point explained by means of the

... a phenomenon that happens between an ideal gas and its condensed quantum phase. As far as it concerns the liquid He4, the phenomenon is slightly different being, by the fact, a transition between a real gas (in the fluid phase) and its quantum condensed phase so that the transition temperature is sm ...
I-1
I-1

... exist, charges must be of two kinds, positive and negative. Unlike charges attract and like charges repel themselves. • Charges are quantized. They can only be isolated in integer multiples of the elementary charge e = 1.602 10-19 C • In all known processes charges appear or disappear only in pairs ...
Arrows of Time
Arrows of Time

... • There is a close connection between our mental asymmetry and the entropic asymmetry. For starters, in an equilibrated world (entropy already maximized, no entropic time asymmetry) there is no information (that's why Maxwell's demon can't function) so there could be no minds whatever. • The low-ent ...
- Harish-Chandra Research Institute
- Harish-Chandra Research Institute

Uncertainty principle in view of quantum estimation theory
Uncertainty principle in view of quantum estimation theory

... It is proved that SLD CR bound is attainable i hlj jli i is real for any i; j . When SLD-CR bound is attainable, that bound is achieved by a simple measurement, i.e., a projection valued measurement. Especially, when the model has only one parameter, SLD CR bound is always attainable. Is there any ...
3-10 Plates of Charge
3-10 Plates of Charge

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History of quantum field theory

In particle physics, the history of quantum field theory starts with its creation by Paul Dirac, when he attempted to quantize the electromagnetic field in the late 1920s. Major advances in the theory were made in the 1950s, and led to the introduction of quantum electrodynamics (QED). QED was so successful and ""natural"" that efforts were made to use the same basic concepts for the other forces of nature. These efforts were successful in the application of gauge theory to the strong nuclear force and weak nuclear force, producing the modern standard model of particle physics. Efforts to describe gravity using the same techniques have, to date, failed. The study of quantum field theory is alive and flourishing, as are applications of this method to many physical problems. It remains one of the most vital areas of theoretical physics today, providing a common language to many branches of physics.
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