Difference between revisions of "Logic of medical language: Introduction to quantum-like probability in the masticatory system"

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Returning to the case of the cat, however, it should be noted that the above description is incorrect<ref>Stefan Rinner, Ernst Werner: [https://arxiv.org/pdf/0705.2935.pdf ''On the role of entanglement in Schrödinger's cat paradox''], Central European Journal of Physics 02/2008; 6(1):178-183</ref>. The same conclusion of Schrödinger, who nevertheless never uses the term "paradox", is expressed in very different terms: Schrödinger refers to the ''' wave function of the whole system ''', not to that of the cat. In fact, quantum theory states that the atom + cat system is described by the quantum correlation state.
Returning to the case of the cat, however, it should be noted that the above description is incorrect<ref>Stefan Rinner, Ernst Werner: [https://arxiv.org/pdf/0705.2935.pdf ''On the role of entanglement in Schrödinger's cat paradox''], Central European Journal of Physics 02/2008; 6(1):178-183</ref>. The same conclusion of Schrödinger, who nevertheless never uses the term "paradox", is expressed in very different terms: Schrödinger refers to the ''' wave function of the whole system ''', not to that of the cat. In fact, quantum theory states that the atom + cat system is described by the quantum correlation state.


<math>|A, G \rangle = \frac{1}{\sqrt{2}} \, \left( | \textrm{atom} \; \textrm{lapsed,} \; \textrm{cat} \; \textrm{mdead} \rangle +  | \textrm{atom} \; \textrm{non} \; \textrm{lapsed,} \; \textrm{cat} \; \textrm{live} \rangle \right). </math>
<math>|A, G \rangle = \frac{1}{\sqrt{2}} \, \left( | \textrm{atom} \; \textrm{lapsed,} \; \textrm{cat} \; \textrm{dead} \rangle +  | \textrm{atom} \; \textrm{non} \; \textrm{lapsed,} \; \textrm{cat} \; \textrm{live} \rangle \right). </math>




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