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{{Short description|Quantum Collection topic on Quantum Projective measurement}}
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A '''projective measurement''' (also called a '''von Neumann measurement''') is a fundamental type of measurement in [[quantum mechanics]] in which the state of a system is projected onto an eigenstate of an observable.<ref name=Neumann>{{cite book |last=von Neumann |first=John |title=Mathematical Foundations of Quantum Mechanics |year=1932}}</ref>
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'''Projective measurement''' a projective measurement (also called a von Neumann measurement) is a fundamental type of measurement in quantum mechanics in which the state of a system is projected onto an eigenstate of an observable. Projective measurements represent the simplest and most idealized form of quantum measurement and form the basis for more general frameworks such as positive operator-valued measurements (POVMs) and quantum instruments. A projective measurement (also called a von Neumann measurement) is a fundamental type of measurement in quantum mechanics in which the state of a system is projected onto an eigenstate of an observable. Projective measurements represent the simplest and most idealized form of quantum measurement and form the basis for more general frameworks such as positive operator-valued measurements (POVMs) and quantum instruments. Let an observable be represented by a self-adjoint operator with spectral decomposition
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Projective measurements represent the simplest and most idealized form of quantum measurement and form the basis for more general frameworks such as [[positive operator-valued measurement]]s (POVMs) and quantum instruments.<ref name=Nielsen>{{cite book |last1=Nielsen |first1=Michael A. |last2=Chuang |first2=Isaac L. |title=Quantum Computation and Quantum Information |publisher=Cambridge University Press |year=2010}}</ref>
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[[File:Quantum_projective_measurement_collapse_yellow.jpg|thumb|280px|Quantum Projective measurement.]]
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[[File:Quantum_projective_measurement_collapse_yellow.jpg|thumb|400px|Projective measurement: a quantum state collapses onto one of the orthogonal eigenstates of the observable, yielding a definite outcome.]]
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== Definition ==
== Definition ==
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where <math>\rho</math> is the state of the system.<ref name=Nielsen/>
where <math>\rho</math> is the state of the system.<ref name=Nielsen>{{cite book |last1=Nielsen |first1=Michael A. |last2=Chuang |first2=Isaac L. |title=Quantum Computation and Quantum Information |publisher=Cambridge University Press |year=2010}}</ref>


After the measurement, the state collapses to
After the measurement, the state collapses to
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This process is known as the '''projection postulate'''.<ref name=Neumann/>
This process is known as the '''projection postulate'''.<ref name=Neumann>{{cite book |last=von Neumann |first=John |title=Mathematical Foundations of Quantum Mechanics |year=1932}}</ref>


== Physical interpretation ==
== Physical interpretation ==
Projective measurements correspond to ideal measurements in which the system is sharply projected onto an eigenstate of the observable. They are often associated with textbook examples such as spin measurements using a [[Stern–Gerlach experiment]].<ref name=Nielsen/>
Projective measurements correspond to ideal measurements in which the system is sharply projected onto an eigenstate of the observable. They are often associated with textbook examples such as spin measurements using a Stern–Gerlach experiment.<ref name=Nielsen/>


However, real physical measurements are often more general and cannot always be described by simple projection operators.
However, real physical measurements are often more general and cannot always be described by simple projection operators.
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Projective measurements are a special case of more general measurement frameworks:
Projective measurements are a special case of more general measurement frameworks:


* A [[positive operator-valued measurement]] (POVM) generalizes projective measurements by allowing non-orthogonal measurement operators.<ref name=Nielsen/>
* A positive operator-valued measurement (POVM) generalizes projective measurements by allowing non-orthogonal measurement operators.<ref name=Nielsen/>
* A '''quantum instrument''' provides a full description of a measurement, including both the classical outcome and the post-measurement quantum state.
* A '''quantum instrument''' provides a full description of a measurement, including both the classical outcome and the post-measurement quantum state.


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{{#invoke:PhysicsQC|tocHeadingAndList|Physics:Quantum basics/See also}}
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== References ==
= References =
{{reflist|3}}
{{reflist|3}}


{{Author|Harold Foppele}}
{{Author|Harold Foppele}}
{{Sourceattribution|Physics:Quantum Projective measurement|1}}
{{Sourceattribution|Physics:Quantum Projective measurement|1}}

Latest revision as of 00:31, 24 May 2026

← Previous : Measurement operators
Next : POVM →

Projective measurement a projective measurement (also called a von Neumann measurement) is a fundamental type of measurement in quantum mechanics in which the state of a system is projected onto an eigenstate of an observable. Projective measurements represent the simplest and most idealized form of quantum measurement and form the basis for more general frameworks such as positive operator-valued measurements (POVMs) and quantum instruments. A projective measurement (also called a von Neumann measurement) is a fundamental type of measurement in quantum mechanics in which the state of a system is projected onto an eigenstate of an observable. Projective measurements represent the simplest and most idealized form of quantum measurement and form the basis for more general frameworks such as positive operator-valued measurements (POVMs) and quantum instruments. Let an observable be represented by a self-adjoint operator with spectral decomposition

Quantum Projective measurement.

Definition

Let an observable be represented by a self-adjoint operator with spectral decomposition

A=iaiPi,

where Pi are orthogonal projection operators satisfying

PiPj=δijPi,iPi=I.

A projective measurement yields outcome ai with probability

p(i|ρ)=tr(Piρ),

where ρ is the state of the system.[1]

After the measurement, the state collapses to

ρi=PiρPitr(Piρ).

This process is known as the projection postulate.[2]

Physical interpretation

Projective measurements correspond to ideal measurements in which the system is sharply projected onto an eigenstate of the observable. They are often associated with textbook examples such as spin measurements using a Stern–Gerlach experiment.[1]

However, real physical measurements are often more general and cannot always be described by simple projection operators.

Relation to POVMs and quantum instruments

Projective measurements are a special case of more general measurement frameworks:

  • A positive operator-valued measurement (POVM) generalizes projective measurements by allowing non-orthogonal measurement operators.[1]
  • A quantum instrument provides a full description of a measurement, including both the classical outcome and the post-measurement quantum state.

In this broader framework, projective measurements correspond to the case where the measurement operators are orthogonal projections and the post-measurement state follows directly from the projection.

See also

Table of contents (217 articles)

Index

Full contents

References

  1. 1.0 1.1 1.2 Nielsen, Michael A.; Chuang, Isaac L. (2010). Quantum Computation and Quantum Information. Cambridge University Press. 
  2. von Neumann, John (1932). Mathematical Foundations of Quantum Mechanics. 


Author: Harold Foppele


Source attribution: Physics:Quantum Projective measurement