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&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Short description|Fundamental problem concerning the emergence of definite outcomes in quantum measurements}}&lt;br /&gt;
&lt;br /&gt;
{{Quantum book backlink|Conceptual and interpretations}}&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Quantum Measurement problem&amp;#039;&amp;#039;&amp;#039; is a central conceptual issue in [[Physics:Quantum mechanics|quantum mechanics]] concerning how definite outcomes arise from probabilistic quantum states. While the [[Physics:Wave function|wave function]] evolves deterministically according to the [[Physics:Schrödinger equation|Schrödinger equation]], measurements yield single, definite results rather than superpositions.&amp;lt;ref name=&amp;quot;Weinberg1998&amp;quot;&amp;gt;{{cite book |title=The Oxford History of the Twentieth Century |first=Steven |last=Weinberg |year=1998 |publisher=Oxford University Press |isbn=0-19-820428-0}}&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Zurek2003&amp;quot;&amp;gt;{{cite journal |last=Zurek |first=Wojciech H. |title=Decoherence, einselection, and the quantum origins of the classical |journal=Reviews of Modern Physics |volume=75 |issue=3 |pages=715–775 |year=2003 |doi=10.1103/RevModPhys.75.715}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This raises the fundamental question: how does a superposition of many possible outcomes reduce to a single observed reality?&lt;br /&gt;
[[File:Quantum_measurement_problem.jpg|thumb|400px|Conceptual illustration of the quantum measurement problem: a superposed quantum state yielding a single classical outcome upon observation, often represented by Schrödinger’s cat.]]&lt;br /&gt;
&lt;br /&gt;
== Deterministic evolution vs measurement ==&lt;br /&gt;
&lt;br /&gt;
In quantum theory, the state of a system is described by a wave function that evolves deterministically:&lt;br /&gt;
&lt;br /&gt;
* Continuous, unitary evolution governed by the Schrödinger equation  &lt;br /&gt;
* Linear superposition of multiple possible states  &lt;br /&gt;
&lt;br /&gt;
However, measurement introduces:&lt;br /&gt;
&lt;br /&gt;
* A single definite outcome  &lt;br /&gt;
* Apparent discontinuity (often called [[Physics:Wave function collapse|wave function collapse]])  &lt;br /&gt;
&lt;br /&gt;
This mismatch between continuous evolution and discrete measurement outcomes defines the measurement problem.&amp;lt;ref name=&amp;quot;Weinberg2005&amp;quot;&amp;gt;{{cite journal |last=Weinberg |first=Steven |title=Einstein&amp;#039;s Mistakes |journal=Physics Today |volume=58 |issue=11 |pages=31–35 |year=2005 |doi=10.1063/1.2155755}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Schrödinger’s cat paradox ==&lt;br /&gt;
&lt;br /&gt;
The measurement problem is famously illustrated by [[Physics:Schrödinger&amp;#039;s cat|Schrödinger’s cat]]:&lt;br /&gt;
&lt;br /&gt;
* A quantum event (e.g., radioactive decay) determines the fate of a cat  &lt;br /&gt;
* Before observation, the system exists in a superposition  &lt;br /&gt;
* The cat is simultaneously “alive” and “dead” in the formalism  &lt;br /&gt;
&lt;br /&gt;
Yet observation always yields a definite state, raising the question:&lt;br /&gt;
&lt;br /&gt;
→ How do probabilities become actual outcomes?&lt;br /&gt;
&lt;br /&gt;
== Major interpretations ==&lt;br /&gt;
&lt;br /&gt;
Different interpretations of quantum mechanics provide distinct resolutions:&lt;br /&gt;
&lt;br /&gt;
=== Copenhagen-type interpretations ===&lt;br /&gt;
&lt;br /&gt;
The [[Physics:Copenhagen interpretation|Copenhagen interpretation]] posits:&lt;br /&gt;
&lt;br /&gt;
* Measurement causes collapse of the wave function  &lt;br /&gt;
* The wave function encodes probabilistic knowledge  &lt;br /&gt;
&lt;br /&gt;
However, the mechanism of collapse remains undefined.&amp;lt;ref&amp;gt;{{cite journal |last1=Schlosshauer |first1=Maximilian |last2=Kofler |first2=Johannes |last3=Zeilinger |first3=Anton |title=A snapshot of foundational attitudes toward quantum mechanics |journal=Studies in History and Philosophy of Science Part B |volume=44 |issue=3 |pages=222–230 |year=2013 |doi=10.1016/j.shpsb.2013.04.004}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Many-worlds interpretation ===&lt;br /&gt;
&lt;br /&gt;
The [[Physics:Many-worlds interpretation|many-worlds interpretation]] removes collapse entirely:&lt;br /&gt;
&lt;br /&gt;
* The universal wave function always evolves deterministically  &lt;br /&gt;
* Measurement creates branching worlds  &lt;br /&gt;
* All outcomes occur in separate branches  &lt;br /&gt;
&lt;br /&gt;
A key challenge is deriving the [[Physics:Born rule|Born rule]] for probabilities.&amp;lt;ref&amp;gt;{{cite encyclopedia |last=Kent |first=Adrian |title=One world versus many |year=2010 |publisher=Oxford University Press}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== de Broglie–Bohm theory ===&lt;br /&gt;
&lt;br /&gt;
The [[Physics:De Broglie–Bohm theory|pilot-wave theory]] introduces hidden variables:&lt;br /&gt;
&lt;br /&gt;
* Particles have definite trajectories  &lt;br /&gt;
* The wave function guides motion  &lt;br /&gt;
* Apparent collapse emerges dynamically  &lt;br /&gt;
&lt;br /&gt;
No fundamental collapse occurs.&amp;lt;ref&amp;gt;{{cite book |last=Goldstein |first=Sheldon |title=Bohmian Mechanics |year=2017 |publisher=Stanford Encyclopedia of Philosophy}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Objective-collapse models ===&lt;br /&gt;
&lt;br /&gt;
[[Physics:Objective-collapse theory|Objective-collapse theories]] modify quantum dynamics:&lt;br /&gt;
&lt;br /&gt;
* Collapse occurs spontaneously  &lt;br /&gt;
* Governed by stochastic nonlinear terms  &lt;br /&gt;
* Predict experimentally testable deviations  &lt;br /&gt;
&lt;br /&gt;
Example: [[Physics:Ghirardi–Rimini–Weber theory|GRW theory]].&amp;lt;ref&amp;gt;{{cite journal |last1=Bassi |first1=Angelo |last2=Lochan |first2=Kinjalk |last3=Satin |first3=Seema |last4=Singh |first4=Tejinder P. |last5=Ulbricht |first5=Hendrik |title=Models of wave-function collapse |journal=Reviews of Modern Physics |volume=85 |issue=2 |pages=471–527 |year=2013 |doi=10.1103/RevModPhys.85.471}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Role of decoherence ==&lt;br /&gt;
&lt;br /&gt;
[[Physics:Quantum decoherence|Quantum decoherence]] provides a partial resolution:&lt;br /&gt;
&lt;br /&gt;
* Interaction with the environment suppresses interference  &lt;br /&gt;
* Quantum probabilities become classical probabilities  &lt;br /&gt;
* Explains emergence of classical behavior  &lt;br /&gt;
&lt;br /&gt;
However:&lt;br /&gt;
&lt;br /&gt;
* Decoherence does **not** produce actual collapse  &lt;br /&gt;
* It does not fully solve the measurement problem  &lt;br /&gt;
&lt;br /&gt;
It instead explains why classical outcomes appear stable.&amp;lt;ref name=&amp;quot;Schlosshauer2005&amp;quot;&amp;gt;{{cite journal |last=Schlosshauer |first=Maximilian |title=Decoherence, the measurement problem, and interpretations of quantum mechanics |journal=Reviews of Modern Physics |volume=76 |pages=1267–1305 |year=2005 |doi=10.1103/RevModPhys.76.1267}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Conceptual significance ==&lt;br /&gt;
&lt;br /&gt;
The measurement problem highlights a deep divide:&lt;br /&gt;
&lt;br /&gt;
* Quantum reality: superpositions and probabilities  &lt;br /&gt;
* Classical reality: definite outcomes  &lt;br /&gt;
&lt;br /&gt;
It remains one of the most important unresolved issues in the foundations of physics, closely linked to:&lt;br /&gt;
&lt;br /&gt;
* [[Physics:Interpretations of quantum mechanics|Interpretations of quantum mechanics]]  &lt;br /&gt;
* [[Physics:Quantum decoherence|Decoherence theory]]  &lt;br /&gt;
* [[Physics:Quantum information theory|Quantum information]]  &lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
{{#invoke:PhysicsQC|tocHeadingAndList|Physics:Quantum basics/See also}}&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist|3}}&lt;br /&gt;
&lt;br /&gt;
[[author|Harold Foppele}}&lt;br /&gt;
{{Sourceattribution|Physics:Quantum Measurement problem|1}}&lt;/div&gt;</summary>
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