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Relativistic Effects in Atomic Spectra
Relativistic Effects in Atomic Spectra

... hence compact. In both cases the resolvent map, RA : ρ(A) → B(X), λ 7→ (λ id − A)−1 , is an analytic function on the resolvent set ρ(A). Remark 2.11. The proofs of these statements can be found in standard textbooks. In the literature there are two different ideas to prove the non-emptiness and comp ...
On the equivalence of separability and extendability of quantum states
On the equivalence of separability and extendability of quantum states

Quantum states in phase space • classical vs. quantum statistics
Quantum states in phase space • classical vs. quantum statistics

... correct as it cannot account for number states (in fact, all states that are not of Gaussian form). Here we will derive a proper phase-space picture that allows to associate to each quantum state, pure or mixed, a unique c-number function in phase space that contains all information about the quantu ...
introduction to the many-body problem
introduction to the many-body problem

QFT on curved spacetimes: axiomatic framework and applications
QFT on curved spacetimes: axiomatic framework and applications

Quantization in singular real polarizations: K\" ahler regularization
Quantization in singular real polarizations: K\" ahler regularization

Document
Document

density matrices
density matrices

... Recall that eigenvectors with distinct eigenvalues are orthogonal;  for the subspace of eigenvectors with a common eigenvalue (“degeneracies”), we can select an orthonormal basis ...
Selberg zeta function and trace formula for the BTZ black hole
Selberg zeta function and trace formula for the BTZ black hole

Lie Groups and Quantum Mechanics
Lie Groups and Quantum Mechanics

... Associated with every Lie group is something called its Lie algebra. The Lie algebra is a vector space, but it has additional structure: a binary operation called the Lie bracket. For the rotation group, the elements of the corresponding Lie algebra can be thought of as angular velocities. Indeed, a ...
Compactness and Symmetry in Quantum Logic 1 Introduction
Compactness and Symmetry in Quantum Logic 1 Introduction

... Note that we permit distinct tests to overlap. For later reference, a test space in which distinct tests are disjoint is said to be semiclassical. However, as the examples below illustrate, non-semiclassical test spaces arise quite naturally. Notice also that the probability of an outcome with respe ...
6 Yang-Baxter equation - ENS-phys
6 Yang-Baxter equation - ENS-phys

Quantum Probability - Institut Camille Jordan
Quantum Probability - Institut Camille Jordan

Indirect measurement
Indirect measurement

... form P̂j = Iˆ ⊗ Q̂j where the {Q̂j } are a decomposition of the identity on the ancilla space. In order for them to represent a complete local measurement, they must all be one-dimensional: Q̂j = |φj ihφj |, where {|φj i} is an orthonormal basis on the ancilla space. The probability of outcome j is ...
Superselection Rules - Philsci
Superselection Rules - Philsci

... The notion of superselection rule (henceforth abbreviated SSR) was introduced in 1952 by Wick (1909-1992), Wightman, and Wigner (1902-1995) [13] in connection with the problem of consistently assigning intrinsic parity to elementary particles. They understood an SSR as generally expressing “restrict ...
Lecture Notes for Ph219/CS219: Quantum Information and Computation Chapter 2 John Preskill
Lecture Notes for Ph219/CS219: Quantum Information and Computation Chapter 2 John Preskill

... a two-dimensional Hilbert space, whose state can take any value of the form eq.(2.15). We can perform a measurement that projects the qubit onto the basis {|0i, |1i}. Then we will obtain the outcome |0i with probability |a|2 , and the outcome |1i with probability |b|2 . Furthermore, except in the ca ...
Lecture 14: Quantum information revisited Density matrices
Lecture 14: Quantum information revisited Density matrices

Lecture Notes of my Course on Quantum Computing
Lecture Notes of my Course on Quantum Computing

Continuous Matrix Product States for Quantum Fields
Continuous Matrix Product States for Quantum Fields

... quantum systems can be simulated and understood. The applicability of those approaches has been better understood during the last 5 years by rephrasing those methods in terms of matrix products states (MPS) [3,4]; the success of NRG and DMRG relies on the fact that those MPS give a very accurate des ...
1 Uncertainty principle and position operator in standard theory
1 Uncertainty principle and position operator in standard theory

Exact diagonalization of quantum spin models
Exact diagonalization of quantum spin models

PDF
PDF

2 - arXiv
2 - arXiv

QUANTUM MAPS
QUANTUM MAPS



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Compact operator on Hilbert space

In functional analysis, compact operators on Hilbert spaces are a direct extension of matrices: in the Hilbert spaces, they are precisely the closure of finite-rank operators in the uniform operator topology. As such, results from matrix theory can sometimes be extended to compact operators using similar arguments. In contrast, the study of general operators on infinite-dimensional spaces often requires a genuinely different approach.For example, the spectral theory of compact operators on Banach spaces takes a form that is very similar to the Jordan canonical form of matrices. In the context of Hilbert spaces, a square matrix is unitarily diagonalizable if and only if it is normal. A corresponding result holds for normal compact operators on Hilbert spaces. (More generally, the compactness assumption can be dropped. But, as stated above, the techniques used are less routine.)This article will discuss a few results for compact operators on Hilbert space, starting with general properties before considering subclasses of compact operators.
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