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In mathematics, a linear operator acting on inner product space
{\displaystyle A} . Positive-semidefinite operators are denoted as A ≥ 0 {\displaystyle A\geq 0} . The operator is said to be positive-definite, and written
Positive_operator
Generalized measurement in quantum mechanics
information science, a positive operator-valued measure (POVM) is a measure whose values are positive semi-definite operators on a Hilbert space. POVMs
POVM
Topics referred to by the same term
containing negation Positive number, a number that is greater than 0 Plus sign, the sign "+" used to indicate a positive number Positive operator, a type of linear
Positive
Similar to the basis of a vector space, but not necessarily linearly independent
Benjamin; Moran, Bill; Cochran, Doug (2021). "Positive operator-valued measures and densely defined operator-valued frames". Rocky Mountain Journal of Mathematics
Frame_(linear_algebra)
Mathematical study of linear operators
mathematics, operator theory is the study of linear operators on function spaces, beginning with differential operators and integral operators. The operators may
Operator_theory
Generalization of mass, length, area and volume
charge. Far-reaching generalizations (such as spectral measures and positive operator-valued measures) of measure are widely used in quantum physics and
Measure_(mathematics)
Mathematical operation
the polar decomposition of A. The positive operator P is the unique positive square root of the positive operator A∗A, and U is defined by U = AP−1.
Square_root_of_a_matrix
Group of open reading frames under the same regulation
With positive control, an activator protein stimulates transcription by binding to DNA (usually at a site other than the operator). In positive inducible
Operon
Property of a mathematical matrix
notation comes from functional analysis where positive semidefinite matrices define positive operators. If two matrices A {\displaystyle A} and B {\displaystyle
Definite_matrix
Operation on self-adjoint operators
transform is replaced by self-adjointness for positive operators. Theorem—A symmetric positive operator A {\displaystyle A} is self-adjoint if and only
Extensions of symmetric operators
Extensions_of_symmetric_operators
Concept in functional analysis
In mathematics, more specifically in functional analysis, a positive linear operator from an preordered vector space ( X , ≤ ) {\displaystyle (X,\leq )}
Positive_linear_operator
Mathematical model of quantum mechanics
formalism, effects correspond to positive semidefinite self-adjoint operators which lie below the identity operator in the following partial order: A
Effect_algebra
A = −Δ is a positive operator, whereas Δ is a dissipative operator. Using spectral theory, one can define a square root (1 − Δ)1/2 for the operator (1 − Δ)
Ornstein–Uhlenbeck_operator
Index of articles associated with the same name
Positive-definite kernel Positive-definite matrix Positive-definite operator Positive-definite quadratic form Fasshauer, Gregory E. (2011), "Positive definite kernels:
Positive_definiteness
Mathematical symbols (+ and −)
sign (+) and the minus sign (−) are mathematical symbols used to denote positive and negative functions, respectively. In addition, the symbol + represents
Plus_and_minus_signs
In operator theory, Naimark's dilation theorem is a result that characterizes positive operator valued measures. It is named after Mark Naimark from his
Naimark's_dilation_theorem
Correspondence between quantum channels and quantum states
theory and operator theory, the Choi–Jamiołkowski isomorphism refers to the correspondence between quantum channels (described by completely positive maps)
Choi–Jamiołkowski_isomorphism
Topics referred to by the same term
mathematics, positive semidefinite may refer to: Positive semidefinite function Positive semidefinite matrix Positive semidefinite operator Positive semidefinite
Positive_semidefinite
Measure used in functional analysis
projective measurements.[clarification needed] They are generalized by positive operator valued measures (POVMs) in the same sense that a mixed state or density
Projection-valued_measure
Interpretation of quantum mechanics
Hidden-variable models have been constructed for Werner states even if positive operator-valued measurements (POVM) are allowed, not only von Neumann measurements
Local_hidden-variable_theory
Compact operator for which a finite trace can be defined
orthonormal basis and A : H → H {\displaystyle A:H\to H} a positive bounded linear operator on H {\displaystyle H} . The trace of A {\displaystyle A} is
Trace_class
Theorem in linear algebra
coefficients Metzler matrix (Quasipositive matrix) Positive operator – In mathematics, a linear operator acting on inner product space Krein–Rutman theorem –
Perron–Frobenius_theorem
Image edge detection algorithm
The Sobel operator, sometimes called the Sobel–Feldman operator or Sobel filter, is used in image processing and computer vision, particularly within
Sobel_operator
operators. Positive normal functional are those that are non-negative on positive operators. For every non-zero operator, there is a positive normal functional
Jordan_operator_algebra
Process in quantum mechanical theories
relevant operators O {\displaystyle {\mathcal {O}}} on a Hilbert space H {\displaystyle {\mathcal {H}}} and to construct a positive operator H as a quantum
Canonical_quantization
Generalized normal operator
(T^{*}T)^{p}-(TT^{*})^{p}} is a positive operator.) If p = 1 {\displaystyle p=1} , then T is called a hyponormal operator. If p = 1 / 2 {\displaystyle p=1/2}
Hyponormal_operator
Computational operation
another, the latter being called the modulus of the operation. Given two positive numbers a and n, a modulo n (often abbreviated as a mod n) is the remainder
Modulo
Linear operator equal to its own adjoint
measure on [0, ∞). Compact operator on Hilbert space Unbounded operator Hermitian adjoint Normal operator Positive operator Helffer–Sjöstrand formula The
Self-adjoint_operator
Theorem in relativistic quantum mechanics
it is possible to construct localization observables in terms of positive-operator valued measures that are compatible with the restrictions imposed
Hegerfeldt's_theorem
strong operator topology. 1) If h is a positive operator in (A−)1, then h is in the strong-operator closure of the set of self-adjoint operators in (A+)1
Kaplansky_density_theorem
Property determining comparison and ordering
charge. Far-reaching generalizations (such as spectral measures and positive operator-valued measures) of measure are widely used in quantum physics and
Magnitude_(mathematics)
Mathematical structures that allow quantum mechanics to be explained
density operator; Such quantum state is known as a mixed state. The density operator of a mixed state is a trace class, nonnegative (positive semi-definite)
Mathematical formulation of quantum mechanics
Mathematical_formulation_of_quantum_mechanics
(on a complex Hilbert space) continuous linear operator
{\displaystyle N^{\ast }=N} skew-Hermitian operators: N ∗ = − N {\displaystyle N^{\ast }=-N} positive operators: N = M ∗ M {\displaystyle N=M^{\ast }M} for
Normal_operator
Generalization of a positive-definite matrix
In operator theory, a branch of mathematics, a positive-definite kernel is a generalization of a positive-definite function or a positive-definite matrix
Positive-definite_kernel
Kind of linear transformation
In functional analysis and operator theory, a bounded linear operator is a special kind of linear transformation that is particularly important in infinite
Bounded_operator
Open convex self-dual cones
domains of positivity, are open convex self-dual cones in Euclidean space which have a transitive group of symmetries, i.e. invertible operators that take
Symmetric_cone
Stochastic process
≥ 0 {\textstyle f\geq 0} , i.e., each T t {\textstyle T_{t}} is a positive operator; ‖ T t f ‖ ≤ ‖ f ‖ {\textstyle \|T_{t}f\|\leq \|f\|} for all t ≥ 0
Feller_process
Universal construction of a complex Lie group from a real Lie group
is generated by unitaries, an invertible operator g lies in GC if the unitary operator u and positive operator p in its polar decomposition g = u ⋅ p both
Complexification_(Lie_group)
Type of vector space in math
number λ an operator Eλ, which is the projection onto the nullspace of the operator (T − λ)+, where the positive part of a self-adjoint operator is defined
Hilbert_space
Operator encoding information about iterated map
molecular dynamics. It is often the case that the transfer operator is positive, has discrete positive real-valued eigenvalues, with the largest eigenvalue
Transfer_operator
Calculation rule in quantum mechanics
generalized using positive-operator-valued measures (POVM). A POVM is a measure whose values are positive semi-definite operators on a Hilbert space
Born_rule
a density operator on a Hilbert space). Second, the sharp measurement described by projection operators is supplanted by positive operator valued measures
Quantum_Markov_chain
Generalization of the Perron–Frobenius theorem to Banach spaces
: X → X {\displaystyle T:X\to X} be a non-zero compact operator, and assume that it is positive, meaning that T ( K ) ⊂ K {\displaystyle T(K)\subset K}
Krein–Rutman_theorem
Description of physical properties at the atomic and subatomic scale
specify the state of a subsystem of a larger system, analogously, positive operator-valued measures (POVMs) describe the effect on a subsystem of a measurement
Quantum_mechanics
Linear operator related to topological vector spaces
nuclear operators are an important class of linear operators introduced by Alexander Grothendieck in his doctoral dissertation. Nuclear operators are intimately
Nuclear_operator
Bounded operators with sub-unit norm
be defined. The defect operators of T are the operators DT = (1 − T*T)1⁄2 and DT* = (1 − TT*)1⁄2. The square root is the positive semidefinite one given
Contraction_(operator_theory)
Linear operator defined on a dense linear subspace
functional analysis and operator theory, the notion of unbounded operator provides an abstract framework for dealing with differential operators, unbounded observables
Unbounded_operator
Classification of completely positive maps
theory, the operators {Vi} are called the Kraus operators (after Karl Kraus) of Φ. Notice, given a completely positive Φ, its Kraus operators need not be
Choi's theorem on completely positive maps
Choi's_theorem_on_completely_positive_maps
First-order differential linear operator on spinor bundle, whose square is the Laplacian
{\displaystyle \Delta } is the (positive, or geometric) Laplacian of V {\displaystyle V} , then D {\displaystyle D} is called a Dirac operator. Note that there are
Dirac_operator
a contraction for any positive λ. The utility of this formulation is that if this operator is a contraction for some positive λ then A is dissipative
Dissipative_operator
Theorem
a result from operator theory that represents any completely positive map on a C*-algebra A as a composition of two completely positive maps each of which
Stinespring_dilation_theorem
Term in quantum mechanics
state is a POVM, which is described by a set of Hermitian positive semidefinite operators { F i } {\displaystyle \{F_{i}\}} . When measuring a state
Fidelity_of_quantum_states
Construct in quantum information theory
{\displaystyle H_{A}\otimes H_{B}} . A mixed state ρ is then a trace-class positive operator on the state space which has trace 1. We can view the family of states
Entanglement_witness
Interpretation of quantum mechanics
any single measurement that is a minimal, informationally complete positive operator-valued measure (POVM), this is especially clear: A quantum state is
QBism
Raising and lowering operators in quantum mechanics
or lowering operator (collectively known as ladder operators) is an operator that increases or decreases the eigenvalue of another operator. In quantum
Ladder_operator
Mathematical compact operator
mathematics, a symmetrizable compact operator is a compact operator on a Hilbert space that can be composed with a positive operator with trivial kernel to produce
Symmetrizable compact operator
Symmetrizable_compact_operator
Type of measurement in quantum mechanics
quantum information theory, symmetric, informationally complete, positive operator-valued measures (SIC-POVMs) are a particular type of generalized measurement
SIC-POVM
Linear operator
specify systems of orthonormal polynomials over a finite, positive Borel measure. This operator is named after Carl Gustav Jacob Jacobi. The name derives
Jacobi_operator
In operator theory, a bounded operator T on a Banach space is said to be nilpotent if Tn = 0 for some positive integer n. It is said to be quasinilpotent
Nilpotent_operator
especially operator theory, subnormal operators are bounded operators on a Hilbert space defined by weakening the requirements for normal operators. Some examples
Subnormal_operator
a − 1 {\displaystyle b^{-1}\leq a^{-1}} holds. Nonnegative matrix Positive operator (Hilbert space) Palmer 2001, p. 798. Blackadar 2006, p. 63. Kadison
Positive_element
Matrix with no negative elements
M. A.; Lifshits, Je.A.; Sobolev, A.V. (1990). Positive Linear Systems: The method of positive operators. Sigma Series in Applied Mathematics. Vol. 5.
Nonnegative_matrix
Description of quantum mechanics in which the present depends on both the past and future
measurement Delayed choice experiment Wheeler–Feynman absorber theory Positive operator valued measure Schottky, Walter (1921). "Das Kausalproblem der Quantentheorie
Two-state_vector_formalism
Correspondence in functional analysis
to the identity operator on H {\displaystyle H} . A state on a C ∗ {\displaystyle C^{*}} -algebra A {\displaystyle A} is a positive linear functional
Gelfand–Naimark–Segal construction
Gelfand–Naimark–Segal_construction
In functional analysis, a Hilbert space
a compact, continuous, self-adjoint, and positive operator. The spectral theorem for self-adjoint operators implies that there is an at most countable
Reproducing kernel Hilbert space
Reproducing_kernel_Hilbert_space
= F|D| of D into a self adjoint unitary operator F (the 'phase' of D) and a densely defined positive operator |D| (the 'metric' part). If ( A , H , D
Spectral_triple
Number divisible only by 1 and itself
as mutually unbiased bases and symmetric informationally complete positive-operator-valued measures. The evolutionary strategy used by cicadas of the
Prime_number
Type of differential operator
partial differential equations, elliptic operators are differential operators that generalize the Laplace operator. They are defined by the condition that
Elliptic_operator
Second-order partial differential equation
Laplace operator, ∇ ⋅ {\displaystyle \nabla \cdot } is the divergence operator (also symbolized "div"), ∇ {\displaystyle \nabla } is the gradient operator (also
Laplace's_equation
1960 self-help book by Maxwell Maltz
pursued a means of helping them set the goal of a positive outcome through visualization of that positive outcome. Patients thinking that surgery will solve
Psycho-Cybernetics
mathematics, and specifically in operator theory, a positive-definite function on a group relates the notions of positivity, in the context of Hilbert spaces
Positive-definite function on a group
Positive-definite_function_on_a_group
Noncommutative geometric structure
sequence space j such that for every positive operator A belonging to J. Here μ: J+ → j+ is the map from a positive operator to its singular values. A singular
Singular_trace
Computing operation which compares two values
strcmp in C), a method (such as compareTo in Java), or an operator (such as the spaceship operator <=> in Perl, PHP and C++). Most processors have instruction
Three-way_comparison
Linear mathematical operator which translates a function
particular functional analysis, the shift operator, also known as the translation operator, is an operator that takes a function x ↦ f(x) to its translation
Shift_operator
Class of transformations that quantum systems and processes can undergo
of the density operator description of a quantum mechanical system. Rigorously, a quantum operation is a linear, completely positive map from the set
Quantum_operation
Mathematical method in calculus
integration by parts in operator theory is that it shows that the −∆ (where ∆ is the Laplace operator) is a positive operator on L 2 {\displaystyle L^{2}}
Integration_by_parts
Algebraic trace
_{i}(T)}{\log(N)}}} . The Dixmier trace Trω(T) of T is defined for positive operators T of L1,∞(H) to be Tr ω ( T ) = lim ω a N {\displaystyle \operatorname
Dixmier_trace
Topologies on operators on a Hilbert space
topology or strongest topology or strongest operator topology is defined by the family of seminorms pw(x) for positive elements w of B(H)*. It is stronger than
Operator_topologies
their polar decomposition is the operator corresponding to an element in the original real Lie group, while the positive part is the exponential of an imaginary
Invariant_convex_cone
In probability theory and ergodic theory, a Markov operator is an operator on a certain function space that conserves the mass (the so-called Markov property)
Markov_operator
Surjective bounded operator on a Hilbert space preserving the inner product
In functional analysis, a unitary operator is a surjective bounded operator on a Hilbert space that preserves the inner product. Non-trivial examples
Unitary_operator
structure operator. In algebraic geometry, positive definite (1,1)-forms arise as curvature forms of ample line bundles (also known as positive line bundles)
Positive_form
Foundational principle in quantum physics
challenge for quantum theories; some progress has been made using positive operator-valued measure concepts. In 1945, Leonid Mandelstam and Igor Tamm
Uncertainty_principle
Operator generalizing the Laplacian in differential geometry
In differential geometry, the Laplace–Beltrami operator is a generalization of the Laplace operator to functions defined on submanifolds in Euclidean space
Laplace–Beltrami_operator
that the positive self-adjoint operator |A| should be affiliated with M. However, by the spectral theorem, a positive self-adjoint operator commutes with
Affiliated_operator
Non-self-adjoint compact operator used to solve boundary value problems for the Laplacian
Neumann–Poincaré operator or Poincaré–Neumann operator, named after Carl Neumann and Henri Poincaré, is a non-self-adjoint compact operator introduced by
Neumann–Poincaré_operator
Mathematical operation with only one operand
Decrement: --x, x-- Positive: +x Negative: -x Ones' complement: ~x Logical negation: !x In the C family of languages, the following operators are unary: Increment:
Unary_operation
French). 23 (9): 219–247. (See also: Favard operators) Horová, Ivana (1968). "Linear positive operators of convex functions". Mathematica (Cluj). 10
Szász–Mirakyan_operator
Type of entropy in quantum theory
freedom. A density operator, the mathematical representation of a quantum state, is a positive semi-definite, self-adjoint operator of trace one acting
Von_Neumann_entropy
Loop that increases an initial effect
Positive feedback (exacerbating feedback, self-reinforcing feedback) is a process that occurs in a feedback loop where the outcome of a process reinforces
Positive_feedback
C(j) = j, where C denotes the Cesàro operator on sequences. In any two-sided ideal the difference between a positive operator and its diagonalisation is a sum
Commutator_subspace
Type o integral transform in mathematics
Hausdorff space X equipped with a positive Borel measure. If L2(X) is separable, and k belongs to L2(X × X), then the operator T : L2(X) → L2(X) defined by
Hilbert–Schmidt integral operator
Hilbert–Schmidt_integral_operator
*-algebra of bounded operators on a Hilbert space
*-algebra of bounded operators on a Hilbert space that is closed in the weak operator topology and contains the identity operator. It is a special type
Von_Neumann_algebra
by the normalized positive semidefinite matrices, i.e. by the density matrices. Measurements are identified with Positive Operator valued Measures (POVMs)
Generalized probabilistic theory
Generalized_probabilistic_theory
Result about when a matrix can be diagonalized
functional analysis, a spectral theorem is a result about when a linear operator or matrix can be diagonalized (that is, represented as a diagonal matrix
Spectral_theorem
Theorem in quantum mechanics
density operator is a positive-semidefinite operator on the Hilbert space whose trace is equal to 1. In the language of von Weizsäcker, a density operator is
Gleason's_theorem
mathematics, the Baskakov operators are generalizations of Bernstein polynomials, Szász–Mirakyan operators, and Lupas operators. They are defined by [ L
Baskakov_operator
4,553,068), and co-inventor of a quantum key receiver based on a positive operator valued measure (US Patent 5,999,285). His broad research interests
Howard_Brandt
Mathematical tool in quantum physics
(\rho _{ij})} be a positive semi-definite operator, see below. A density operator is a positive semi-definite, self-adjoint operator of trace one acting
Density_matrix
Mathematical abstraction of quantum measurement
_{x}{\mathcal {E}}_{x}(\rho )\right)=\operatorname {tr} (\rho )} for all positive operators ρ . {\displaystyle \rho .} Now for describing a measurement by an
Quantum_instrument
POSITIVE OPERATOR
POSITIVE OPERATOR
Boy/Male
Hindu
Positive, Suitable
Boy/Male
Indian
Positive Power
Boy/Male
Hindu
Positive, Suitable
Boy/Male
Hindu, Indian, Japanese
Yonit; Good; Positive
Boy/Male
Hindu, Indian
Positive
Boy/Male
Tamil
Positive, Suitable
Boy/Male
Tamil
Positive energy, Horseless
Boy/Male
Hindu
Positive energy, Horseless
Boy/Male
Indian, Tamil
Positive; The Lord Ganesh
Boy/Male
Hindu, Indian
Positive Thinking Person
Girl/Female
Tamil
Positive energy, Horseless
Girl/Female
Tamil
Position
Boy/Male
Bengali, Gujarati, Hindu, Indian, Kannada, Malayalam, Marathi, Mythological, Sanskrit, Tamil, Telugu, Traditional
Powerful; Positive Thinker; Self Confidence; Positive; Frank; Powerful Character of Mahabharat
Boy/Male
Tamil
Anirved | அநீரà¯à®µà¯‡à®¤
Positive, Courageous, Resilient, Independent
Anirved | அநீரà¯à®µà¯‡à®¤
Girl/Female
Hindu
Positive energy, Horseless
Girl/Female
Arabic, Australian, Muslim
Inspiring; Positive Attitude
Boy/Male
Tamil
Positive, Suitable
Boy/Male
Hindu, Indian, Tamil
Positive Energy
Boy/Male
Hindu, Indian
Positive Thinking
Boy/Male
Hindu
Positive, Courageous, Resilient, Independent
POSITIVE OPERATOR
POSITIVE OPERATOR
Girl/Female
Indian
Infinite, Endless, Eternal
Male
Arthurian
, a king of the Saxons.
Boy/Male
Hindu, Indian, Telugu
Lord Krishna
Boy/Male
Tamil
Honor
Surname or Lastname
English
English : variant spelling of Male.
Boy/Male
Hindu, Indian, Kannada, Malayalam, Marathi, Sanskrit, Telugu
A Manu
Male
Spanish
 Spanish pet form of Portuguese/Spanish José, PEPE means "(God) shall add (another son)." Compare with another form of Pepe.
Boy/Male
Indian
Help
Boy/Male
Indian, Punjabi, Sikh
A Person of Good Family
Boy/Male
Biblical
Naming; or astonishment; of God.
POSITIVE OPERATOR
POSITIVE OPERATOR
POSITIVE OPERATOR
POSITIVE OPERATOR
POSITIVE OPERATOR
a.
Hence: Not admitting of any doubt, condition, qualification, or discretion; not dependent on circumstances or probabilities; not speculative; compelling assent or obedience; peremptory; indisputable; decisive; as, positive instructions; positive truth; positive proof.
a.
Electro-positive.
n.
Hence: The ground which any one takes in an argument or controversy; the point of view from which any one proceeds to a discussion; also, a principle laid down as the basis of reasoning; a proposition; a thesis; as, to define one's position; to appear in a false position.
adv.
In a positive manner; absolutely; really; expressly; with certainty; indubitably; peremptorily; dogmatically; -- opposed to negatively.
n.
Relative place or standing; social or official rank; as, a person of position; hence, office; post; as, to lose one's position.
a.
Asserting a thing positively and authoritatively; positive; magisterial; hence, arrogantly authoritative; overbearing.
a.
Having a real position, existence, or energy; existing in fact; real; actual; -- opposed to negative.
n.
The positive plate of a voltaic or electrolytic cell.
n.
The state of being posited, or placed; the manner in which anything is placed; attitude; condition; as, a firm, an inclined, or an upright position.
v. t.
To indicate the position of; to place.
n.
A picture in which the lights and shades correspond in position with those of the original, instead of being reversed, as in a negative.
n.
The positive degree or form.
n.
The spot where a person or thing is placed or takes a place; site; place; station; situation; as, the position of man in creation; the fleet changed its position.
a.
Hence: Positive; metallic; basic; -- distinguished from negative, nonmetallic, or acid.
a.
Corresponding with the original in respect to the position of lights and shades, instead of having the lights and shades reversed; as, a positive picture.
a.
Definitely laid down; explicitly stated; clearly expressed; -- opposed to implied; as, a positive declaration or promise.
a.
Used in expressing a wish or permission as, volitive proposition.
a.
Derived from an object by itself; not dependent on changing circumstances or relations; absolute; -- opposed to relative; as, the idea of beauty is not positive, but depends on the different tastes individuals.
a.
Having the power of direct action or influence; as, a positive voice in legislation.
a.
Of or pertaining to punishment; involving, awarding, or inflicting punishment; as, punitive law or justice.