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arXiv:quant-ph/0610027v1 4 Oct 2006
arXiv:quant-ph/0610027v1 4 Oct 2006

... The optimal error probability of discriminating two quantum states ρ0 and ρ1 has been identified a long time ago by Helström [3]. We consider the two hypotheses H0 and H1 that a given quantum system is prepared either in the state ρ0 or in the state ρ1 , respectively. Since the (quantum) Chernoff b ...
Working Group "Young DPG" Arbeitsgruppe junge DPG (AGjDPG
Working Group "Young DPG" Arbeitsgruppe junge DPG (AGjDPG

... are dominated by a continuum of fluctuations. Such states arise in the vicinity of phase transitions, which are accessed by the variation of a non-thermal control parameter at zero temperature, so-called quantum phase transitions. Even though quantum phase transitions are strictly defined to be at z ...
Polarized excitons in nanorings and the optical Aharonov
Polarized excitons in nanorings and the optical Aharonov

Influence of measurements on the statistics of work performed on a
Influence of measurements on the statistics of work performed on a

Quantum Rings with Two Deeply Bound Electrons under a Magnetic
Quantum Rings with Two Deeply Bound Electrons under a Magnetic

Microcanonical distributions for quantum systems
Microcanonical distributions for quantum systems

Quantum approach to Image processing
Quantum approach to Image processing

Energy Levels Of Hydrogen Atom Using Ladder Operators
Energy Levels Of Hydrogen Atom Using Ladder Operators

... Hermite polynomials by solving differential equations. Then, we will use algebraic ladder operator methods in order to find the energy eigenvalues which should result in the same answer. In the second section the aim is to find the the energy levels of the Hydrogen atom[1] using the two methods[2] e ...
Dissipative decoherence in the Grover algorithm
Dissipative decoherence in the Grover algorithm

Lecture notes 6: Strong and weak interactions
Lecture notes 6: Strong and weak interactions

... charged with color and the physics of these exchanges are termed “quantum chromodynamics”. Protons and neutrons combine three quarks with different colors such that both protons and neutrons are color free, or white. This is also true of the mesons discussed below which are composed of a quark and a ...
The True End of Theoretical Physics
The True End of Theoretical Physics

Gaussian resolutions for equilibrium density matrices
Gaussian resolutions for equilibrium density matrices

... the potential U ðxÞ ¼ 4  4x2 þ x4 . Now a grid of 14 points with 3 < qn < 3 was used. The corresponding results using both the unsymmetrized and symmetrized Gaussians are shown in Fig. 2. The agreement between the exact result (fully converged diagonalization of H^ in a large basis) and that compu ...
5. Particles in a Magnetic Field
5. Particles in a Magnetic Field

... there is a transition between di↵erent plateaux. This phenomenon, called the integer Quantum Hall E↵ect, was discovered by Klaus von Klitzing in 1980. For this, he was awarded the Nobel prize in 1985. It turns out that the integer quantum Hall e↵ect is a direct consequence of the existence of discre ...
Inertial mass and the quantum vacuum fields
Inertial mass and the quantum vacuum fields

... known as quantum field theory, is both conceptually rich and quantitatively successful: witness the agreement between theory and experiment of the magnetic moment of the electron to thirteen significant figures. Although the technique that has been used so far to develop the hypothesis connecting in ...
Quantum Chaos
Quantum Chaos

... Let us define the Wigner distribution (for a pure state; extension for a general  density matrix follows straightforwardly): ...
With 0 order Bessel function of the first kind Jo(x) we define
With 0 order Bessel function of the first kind Jo(x) we define

Nobel Lecture: Fractional quantization
Nobel Lecture: Fractional quantization

... simple rules that may be verified experimentally, mediates the attractive interaction responsible for conventional superconductivity, and so forth, and none of these things depends in detail on the underlying equations of motion. They are generic properties of the crystalline state. The phonon cease ...
The strange (hi)story of particles and waves*
The strange (hi)story of particles and waves*

... that was to replace the concept of deterministic trajectories by formal probabilistic rules. Together with Born and Jordan, Heisenberg then constructed an elegant algebraic framework that could be used to “quantize” all mechanical systems. This mathematical abstraction perfectly matched Heisenberg’s ...
Single and Entangled Photon Sources
Single and Entangled Photon Sources

... a paper describing the EPR paradox. This paper described how in quantum mechanics a pair of quantum systems could be illustrated by a single wave function. This notion had the writers believe that there either was some interaction between the particles, or the information on the outcomes of the meas ...
Quantum Probabilistic Dyadic Second-Order Logic⋆
Quantum Probabilistic Dyadic Second-Order Logic⋆

... Institute for Logic, Language and Computation, Universiteit van Amsterdam Science Park 107, 1098XG Amsterdam, The Netherlands. ...
Advances in Effective Field Theories
Advances in Effective Field Theories

The Spin Quantum Number
The Spin Quantum Number

Here
Here

... (bottom) surface; i.e. there exists a domain wall between two adjacent plateaux of IQHE Such a domain wall will trap a chiral Fermi liquid which is responsible for the net Hall effect Note: in general there will also be other non-chiral states on this side surface; they are irrelevant since only one ...
Measuring the quantum mechanical wave function
Measuring the quantum mechanical wave function

Giant gravitons: a collective coordinate approach
Giant gravitons: a collective coordinate approach

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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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