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Lagrangian, functional integrals, effective action
Lagrangian, functional integrals, effective action

Qubits and Quantum Measurement
Qubits and Quantum Measurement

QuVis: The Quantum Mechanics Visualization Project
QuVis: The Quantum Mechanics Visualization Project

... the teaching and learning of quantum mechanics concepts at university level [4,5]. This resource builds on existing education research as well as our teaching experience. The animations are in many ways complementary to other resources: Each animation shows a situation aimed at clarifying a particul ...
Momentum vs. Wavevector
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... • States like |x0〉 and |k0〉 have 〈ψ|ψ〉=∞ • All physical states must have 〈ψ|ψ〉=1 • CONCLUSION 1: states such as |x0〉 and |k0〉 are non-physical, and can therefore only be used as intermediate states in calculations • CONCLUSION 2: Since a measurement of X produces the nonphysical state |x0〉, such a x ...
Chapter 15
Chapter 15

... must satisfy the boundary conditions  (x) =0 at x=0 and x=a. The first and second derivatives of  (x) be well-behaved functions between x=0 must also and x=a. This is the case for  (x) . We conclude that  (x)  x  c sin x / a  d sin 2x / a is an acceptable wave function for the particl ...
Elementary Particles Thornton and Rex, Ch. 13
Elementary Particles Thornton and Rex, Ch. 13

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ppt - ICTS
ppt - ICTS

... bits into N bits with the property that • For any x{0,1}n, i{1,…,n}, and y{0,1}N that differs from f(x) in at most 0.01N locations, we can recover xi by querying only q bits in y For q=2: • The Hadamard code is a LDC with N=2n • This is essentially optimal due to [Kerenidis-deWolf02] ...
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The relation of colour charge to electric charge (E/c) −P2 −Q2 −(mc

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BHs and effective quantum gravity approaches
BHs and effective quantum gravity approaches

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Codeword stabilized quantum codes

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Can Quantum-Mechanical Description of Physical Reality Be

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Heisenberg uncertainty relations for photons
Heisenberg uncertainty relations for photons

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this PDF file - e

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Applications of the Schrodinger Wave Equation The free particle
Applications of the Schrodinger Wave Equation The free particle

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Mathematics of Quantum Mechanics
Mathematics of Quantum Mechanics

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Planetary motion, the hydrogen atom, and superintegrablity

... This is the tip of the iceberg! Superintegrable systems occur in all dimensions n ≥ 2 and for a great variety of conformally flat spaces and potentials on these spaces. They are always associated with noncommuting (non-Lie) algebras of higher order symmetries and the representation theory of the alg ...
Parallel Universes
Parallel Universes

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Fine structure of the hydrogen atom

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While the ramifications of quantum computers

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What determines the structure of quantum physics?

Entropy and Entanglement of Moving Two Atoms in a Squeezed
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Synchronistic Phenomena as Entanglement
Synchronistic Phenomena as Entanglement

... a result of any causal influence of mind on matter or other minds but as ‘meaningful coincidences’, correlations not produced by causal interaction of the kind physicists know and apply successfully but mediated by correspondences of sense and meaning. In fact, it is a common feature of paranormal p ...
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Quantum one-time programs
Quantum one-time programs

... two secret strings (or bits) s0 , s1 ; a receiver can specify a bit c, obtain sc , and then the OTM self-destructs so that sc is lost forever. OTMs are an attractive minimal hardware assumption: their specification is independent of any specific function f , so they could theoretically be mass-produ ...
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Canonical quantization

In physics, canonical quantization is a procedure for quantizing a classical theory, while attempting to preserve the formal structure, such as symmetries, of the classical theory, to the greatest extent possible.Historically, this was not quite Werner Heisenberg's route to obtaining quantum mechanics, but Paul Dirac introduced it in his 1926 doctoral thesis, the ""method of classical analogy"" for quantization, and detailed it in his classic text. The word canonical arises from the Hamiltonian approach to classical mechanics, in which a system's dynamics is generated via canonical Poisson brackets, a structure which is only partially preserved in canonical quantization.This method was further used in the context of quantum field theory by Paul Dirac, in his construction of quantum electrodynamics. In the field theory context, it is also called second quantization, in contrast to the semi-classical first quantization for single particles.
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