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		<summary type="html">&lt;p&gt;Repair Quantum Collection B backlink template&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Quantum book backlink|Foundations}}&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Quantum probability&amp;#039;&amp;#039;&amp;#039; was developed in the 1980s as a noncommutative analog of the Kolmogorovian theory of stochastic processes.&amp;lt;ref name=Accardi82&amp;gt;{{cite journal&lt;br /&gt;
 |author1=L. Accardi |author2=A. Frigerio |author3=J.T. Lewis  |last-author-amp=yes | title = Quantum stochastic processes&lt;br /&gt;
 | journal = Publ. Res. Inst. Math. Sci.&lt;br /&gt;
 | volume = 18&lt;br /&gt;
 | year = 1982&lt;br /&gt;
 | pages = 97–133&lt;br /&gt;
 | issue = 1&lt;br /&gt;
 | doi = 10.2977/prims/1195184017&lt;br /&gt;
| url = https://art.torvergata.it/bitstream/2108/83328/1/Ac84_Quantum%20Stochastic%20Processes.pdf&lt;br /&gt;
 }}&amp;lt;/ref&amp;gt;&amp;lt;ref name=Hudson-Parthasarathy84&amp;gt;{{cite journal&lt;br /&gt;
 | author = R.L. Hudson, K.R. Parthasarathy&lt;br /&gt;
 | title = Quantum Ito&amp;#039;s formula and stochastic evolutions&lt;br /&gt;
 | journal = Comm. Math. Phys.&lt;br /&gt;
 | volume = 93&lt;br /&gt;
 | year = 1984&lt;br /&gt;
 | pages = 301–323&lt;br /&gt;
 | issue = 3&lt;br /&gt;
 | bibcode = 1984CMaPh..93..301H&lt;br /&gt;
 | last2 = Parthasarathy&lt;br /&gt;
 | doi = 10.1007/BF01258530&lt;br /&gt;
}}&amp;lt;/ref&amp;gt;&amp;lt;ref name=Parthasarathy92&amp;gt;{{cite book&lt;br /&gt;
 | author = K.R. Parthasarathy&lt;br /&gt;
 | title = An introduction to quantum stochastic calculus&lt;br /&gt;
 | series = Monographs in Mathematics&lt;br /&gt;
 | volume = 85&lt;br /&gt;
 | publisher = Birkhäuser Verlag&lt;br /&gt;
 | location = Basel&lt;br /&gt;
 | year = 1992&lt;br /&gt;
}}&amp;lt;/ref&amp;gt;&amp;lt;ref name=Voiculescu92&amp;gt;{{cite book&lt;br /&gt;
 |author1=D. Voiculescu |author2=K. Dykema |author3=A. Nica | title = Free random variables. A noncommutative probability approach to free products with applications to random matrices, operator algebras and harmonic analysis on free groups&lt;br /&gt;
 | series = CRM Monograph Series&lt;br /&gt;
 | volume = 1&lt;br /&gt;
 | publisher = American Mathematical Society&lt;br /&gt;
 | location = Providence, RI&lt;br /&gt;
 | year = 1992&lt;br /&gt;
}}&amp;lt;/ref&amp;gt;&amp;lt;ref name=Meyer93&amp;gt;{{cite book&lt;br /&gt;
 | author = P.-A. Meyer&lt;br /&gt;
 | title = Quantum probability for probabilists&lt;br /&gt;
 | series = Lecture Notes in Mathematics&lt;br /&gt;
 | volume = 1538&lt;br /&gt;
 | year = 1993&lt;br /&gt;
}}&amp;lt;/ref&amp;gt; One of its aims is to clarify the mathematical foundations of [[Physics:Quantum mechanics|quantum theory]] and its statistical interpretation.&amp;lt;ref name=Neumann29&amp;gt;{{cite journal&lt;br /&gt;
 | author = John von Neumann&lt;br /&gt;
 | title = Allgemeine Eigenwerttheorie Hermitescher Funktionaloperatoren&lt;br /&gt;
 | journal = Mathematische Annalen&lt;br /&gt;
 | volume = 102&lt;br /&gt;
 | pages = 49–131&lt;br /&gt;
 | year = 1929&lt;br /&gt;
 | doi=10.1007/BF01782338&lt;br /&gt;
}}&amp;lt;/ref&amp;gt;&amp;lt;ref name=Neumann32&amp;gt;{{cite book&lt;br /&gt;
 | author = John von Neumann&lt;br /&gt;
 | title = Mathematische Grundlagen der Quantenmechanik&lt;br /&gt;
 | series = Die Grundlehren der Mathematischen Wissenschaften, Band 38&lt;br /&gt;
 | location = Berlin&lt;br /&gt;
 | publisher = Springer&lt;br /&gt;
 | year = 1932&lt;br /&gt;
}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
A significant recent application to [[Physics:Physics|physics]] is the dynamical solution of the quantum measurement problem,&amp;lt;ref name=Belavkin95&amp;gt;{{cite journal&lt;br /&gt;
 | author = V. P. Belavkin&lt;br /&gt;
 | title = A Dynamical Theory of Quantum Measurement and Spontaneous Localization&lt;br /&gt;
 | journal = Russian Journal of Mathematical Physics&lt;br /&gt;
 | volume = 3&lt;br /&gt;
 | year = 1995&lt;br /&gt;
 | pages = 3–24&lt;br /&gt;
 | arxiv =  math-ph/0512069 |bibcode = 2005math.ph..12069B&lt;br /&gt;
 | issue = 1 }}&amp;lt;/ref&amp;gt;&amp;lt;ref name=Belavkin2000&amp;gt;{{cite journal&lt;br /&gt;
 | author = V. P. Belavkin&lt;br /&gt;
 | title = Dynamical Solution to the Quantum Measurement Problem, Causality, and Paradoxes of the Quantum Century&lt;br /&gt;
 | journal = Open Systems and Information Dynamics&lt;br /&gt;
 | volume = 7&lt;br /&gt;
 | pages = 101–129&lt;br /&gt;
 | year = 2000&lt;br /&gt;
 | doi = 10.1023/A:1009663822827&lt;br /&gt;
 | arxiv = quant-ph/0512187&lt;br /&gt;
 | issue = 2}}&amp;lt;/ref&amp;gt; by giving constructive models of quantum observation processes which resolve many famous paradoxes of [[Physics:Quantum mechanics|quantum mechanics]].&lt;br /&gt;
&lt;br /&gt;
Some recent advances are based on [[Belavkin equation|quantum filtering]]&amp;lt;ref name=Belavkin99&amp;gt;{{cite journal&lt;br /&gt;
 | author = V. P. Belavkin&lt;br /&gt;
 | title = Measurement, filtering and control in quantum open dynamical systems&lt;br /&gt;
 | journal = Reports on Mathematical Physics&lt;br /&gt;
 | volume = 43&lt;br /&gt;
 | pages = A405–A425&lt;br /&gt;
 | year = 1999&lt;br /&gt;
 | doi = 10.1016/S0034-4877(00)86386-7&lt;br /&gt;
 | arxiv = quant-ph/0208108|bibcode = 1999RpMP...43A.405B&lt;br /&gt;
 | issue = 3 | citeseerx = 10.1.1.252.701&lt;br /&gt;
 }}&amp;lt;/ref&amp;gt; and feedback control theory as applications of [[Quantum stochastic calculus|quantum stochastic calculus]].&lt;br /&gt;
&lt;br /&gt;
== Orthodox quantum mechanics ==&lt;br /&gt;
Orthodox [[Physics:Quantum mechanics|quantum mechanics]] has two seemingly contradictory mathematical descriptions:&lt;br /&gt;
&lt;br /&gt;
# deterministic [[Unitary operator|unitary]] [[Time evolution|time evolution]] (governed by the [[Physics:Schrödinger equation|Schrödinger equation]]) and&lt;br /&gt;
# [[Stochastic|stochastic]] (random) wavefunction collapse.&lt;br /&gt;
&lt;br /&gt;
Most physicists are not concerned with this apparent problem. Physical intuition usually provides the answer, and only in unphysical systems (e.g., [[Physics:Schrödinger&amp;#039;s cat|Schrödinger&amp;#039;s cat]], an isolated atom) do paradoxes seem to occur.&lt;br /&gt;
&lt;br /&gt;
Orthodox quantum mechanics can be reformulated in a quantum-probabilistic framework, where [[Belavkin equation|quantum filtering]] theory (see Bouten et al.&amp;lt;ref&amp;gt;{{Cite journal|last=Bouten|first=Luc|last2=Van Handel|first2=Ramon|last3=James|first3=Matthew R.|date=2007|title=An Introduction to Quantum Filtering|journal=SIAM Journal on Control and Optimization|language=en-US|volume=46|issue=6|pages=2199–2241|doi=10.1137/060651239|issn=0363-0129|arxiv=math/0601741}}&amp;lt;/ref&amp;gt;&amp;lt;ref name=Bouten2009&amp;gt;{{cite journal&lt;br /&gt;
 |author1=Luc Bouten |author2=Ramon van Handel |author3=Matthew R. James | title = A discrete invitation to quantum filtering and feedback control&lt;br /&gt;
 | journal = SIAM Review&lt;br /&gt;
 | volume = 51&lt;br /&gt;
 | pages = 239–316&lt;br /&gt;
 | year = 2009&lt;br /&gt;
 | doi = 10.1137/060671504&lt;br /&gt;
 | arxiv = math/0606118&lt;br /&gt;
|bibcode = 2009SIAMR..51..239B&lt;br /&gt;
 | issue = 2 }}&amp;lt;/ref&amp;gt; for introduction or [[Biography:Viacheslav Belavkin|Belavkin]], 1970s&amp;lt;ref name=&amp;quot;Belavkin72&amp;quot;&amp;gt;{{cite journal|author=V. P. Belavkin|year=1972–1974|title=Optimal linear randomized filtration of quantum boson signals|url=|journal=Problems of Control and Information Theory|volume=3|issue=1|pages=47–62|via=}}&amp;lt;/ref&amp;gt;&amp;lt;ref name=Belavkin75&amp;gt;{{cite journal&lt;br /&gt;
 | author = V. P. Belavkin&lt;br /&gt;
 | title = Optimal multiple quantum statistical hypothesis testing&lt;br /&gt;
 | journal = Stochastics&lt;br /&gt;
 | volume = 1&lt;br /&gt;
 | issue = 1–4&lt;br /&gt;
 | pages = 315–345&lt;br /&gt;
 | year = 1975&lt;br /&gt;
 | doi = 10.1080/17442507508833114&lt;br /&gt;
}}&amp;lt;/ref&amp;gt;&amp;lt;ref name=Belavkin78&amp;gt;{{cite journal&lt;br /&gt;
 | author = V. P. Belavkin&lt;br /&gt;
 | title = Optimal quantum filtration of Makovian signals [In Russian]&lt;br /&gt;
 | journal = Problems of Control and Information Theory&lt;br /&gt;
 | volume = 7&lt;br /&gt;
 | pages = 345–360&lt;br /&gt;
 | year = 1978&lt;br /&gt;
 | issue = 5&lt;br /&gt;
}}&amp;lt;/ref&amp;gt;) gives the natural description of the measurement process. This new framework encapsulates the standard postulates of quantum mechanics, and thus all of the science involved in the orthodox postulates.&lt;br /&gt;
&lt;br /&gt;
=== Motivation ===&lt;br /&gt;
In classical [[Probability theory|probability theory]], information is summarized by the [[Sigma-algebra|sigma-algebra]] &amp;#039;&amp;#039;F&amp;#039;&amp;#039; of events in a classical [[Probability space|probability space]] (Ω, &amp;#039;&amp;#039;F&amp;#039;&amp;#039;,&amp;#039;&amp;#039;&amp;#039;P&amp;#039;&amp;#039;&amp;#039;). For example, &amp;#039;&amp;#039;F&amp;#039;&amp;#039; could be the σ-algebra σ(&amp;#039;&amp;#039;X&amp;#039;&amp;#039;) generated by a [[Random variable|random variable]] &amp;#039;&amp;#039;X&amp;#039;&amp;#039;, which contains all the information on the values taken by &amp;#039;&amp;#039;X&amp;#039;&amp;#039;. We wish to describe quantum information in similar algebraic terms, in such a way as to capture the non-commutative features and the information made available in an experiment. The appropriate algebraic structure for observables, or more generally operators, is a [[*-algebra|*-algebra]]. A (unital) *- algebra is a complex vector space &amp;#039;&amp;#039;A&amp;#039;&amp;#039; of operators on a Hilbert space &amp;#039;&amp;#039;H&amp;#039;&amp;#039; that&lt;br /&gt;
&lt;br /&gt;
* contains the identity &amp;#039;&amp;#039;I&amp;#039;&amp;#039; and&lt;br /&gt;
* is closed under composition (a multiplication) and adjoint (an involution &amp;lt;sup&amp;gt;*&amp;lt;/sup&amp;gt;): &amp;#039;&amp;#039;a&amp;#039;&amp;#039; ∈ &amp;#039;&amp;#039;A&amp;#039;&amp;#039; implies &amp;#039;&amp;#039;a&amp;#039;&amp;#039;&amp;lt;sup&amp;gt;*&amp;lt;/sup&amp;gt; ∈ &amp;#039;&amp;#039;A&amp;#039;&amp;#039;.&lt;br /&gt;
&lt;br /&gt;
A state &amp;#039;&amp;#039;&amp;#039;P&amp;#039;&amp;#039;&amp;#039; on &amp;#039;&amp;#039;A&amp;#039;&amp;#039; is a linear functional &amp;#039;&amp;#039;&amp;#039;P&amp;#039;&amp;#039;&amp;#039; : &amp;#039;&amp;#039;A&amp;#039;&amp;#039; → &amp;#039;&amp;#039;&amp;#039;C&amp;#039;&amp;#039;&amp;#039; (where &amp;#039;&amp;#039;&amp;#039;C&amp;#039;&amp;#039;&amp;#039; is the field of complex numbers) such that 0 ≤ &amp;#039;&amp;#039;&amp;#039;P&amp;#039;&amp;#039;&amp;#039;(&amp;#039;&amp;#039;a&amp;#039;&amp;#039;&amp;lt;sup&amp;gt;*&amp;lt;/sup&amp;gt; &amp;#039;&amp;#039;a&amp;#039;&amp;#039;) for all &amp;#039;&amp;#039;a&amp;#039;&amp;#039; ∈ &amp;#039;&amp;#039;A&amp;#039;&amp;#039; (positivity) and &amp;#039;&amp;#039;&amp;#039;P&amp;#039;&amp;#039;&amp;#039;(&amp;#039;&amp;#039;I&amp;#039;&amp;#039;) = 1 (normalization). A projection is an element &amp;#039;&amp;#039;p&amp;#039;&amp;#039; ∈ &amp;#039;&amp;#039;A&amp;#039;&amp;#039; such that &amp;#039;&amp;#039;p&amp;#039;&amp;#039;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt; = &amp;#039;&amp;#039;p&amp;#039;&amp;#039; = &amp;#039;&amp;#039;p&amp;#039;&amp;#039;&amp;lt;sup&amp;gt;*&amp;lt;/sup&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== Mathematical definition ==&lt;br /&gt;
The basic definition in quantum probability is that of a quantum probability space, sometimes also referred to as an algebraic or noncommutative probability space.&lt;br /&gt;
 &lt;br /&gt;
:&amp;#039;&amp;#039;&amp;#039;Definition : Quantum probability space.&amp;#039;&amp;#039;&amp;#039;&lt;br /&gt;
&lt;br /&gt;
A quantum probability space is a pair (&amp;#039;&amp;#039;A&amp;#039;&amp;#039;, &amp;#039;&amp;#039;&amp;#039;P&amp;#039;&amp;#039;&amp;#039;), where &amp;#039;&amp;#039;A&amp;#039;&amp;#039; is a [[*-algebra|*-algebra]] and &amp;#039;&amp;#039;&amp;#039;P&amp;#039;&amp;#039;&amp;#039; is a state.&lt;br /&gt;
&lt;br /&gt;
This definition is a generalization of the definition of a probability space in Kolmogorovian probability theory, in the sense that every (classical) probability space gives rise to a quantum probability space if &amp;#039;&amp;#039;A&amp;#039;&amp;#039; is chosen as the *-algebra of almost everywhere bounded complex-valued measurable functions{{citation needed|date=March 2018}}.&lt;br /&gt;
&lt;br /&gt;
The idempotents &amp;#039;&amp;#039;p&amp;#039;&amp;#039; ∈ &amp;#039;&amp;#039;A&amp;#039;&amp;#039; are the events in &amp;#039;&amp;#039;A&amp;#039;&amp;#039;, and &amp;#039;&amp;#039;&amp;#039;P&amp;#039;&amp;#039;&amp;#039;(&amp;#039;&amp;#039;p&amp;#039;&amp;#039;) gives the probability of the event &amp;#039;&amp;#039;p&amp;#039;&amp;#039;.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== External links ==&lt;br /&gt;
* [https://sites.google.com/site/associationqp/home Association for Quantum Probability and Infinite Dimensional Analysis (AQPIDA)]&lt;br /&gt;
&lt;br /&gt;
{{Quantum mechanics topics|state=expanded}}&lt;br /&gt;
[[Category:Quantum mechanics]]&lt;br /&gt;
[[Category:Exotic probabilities]]&lt;br /&gt;
&lt;br /&gt;
{{Sourceattribution|Quantum probability|1}}&lt;/div&gt;</summary>
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