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  • 06:44, 11 November 2022 diff hist +3,575 N Store:EMfr03Created page with "=== Sclerosi multipla e riflessi trigeminali === Dobbiamo fare un ulteriore attenzione premessa che riguarda la demilienizzazione assonale nelle sclerosi multiple. Da uno studio di Joanna Kamińska et el.<ref>Joanna Kamińska, Olga M Koper, Kinga Piechal, Halina Kemona . [https://pubmed.ncbi.nlm.nih.gov/28665284/ Multiple sclerosis - etiology and diagnostic potential].Postepy Hig Med Dosw. 2017 Jun 30;71(0):551-563.doi: 10.5604/01.3001.0010.3836. </ref> si evince che..."
  • 06:43, 11 November 2022 diff hist +3,575 N Store:EMit03Created page with "=== Sclerosi multipla e riflessi trigeminali === Dobbiamo fare un ulteriore attenzione premessa che riguarda la demilienizzazione assonale nelle sclerosi multiple. Da uno studio di Joanna Kamińska et el.<ref>Joanna Kamińska, Olga M Koper, Kinga Piechal, Halina Kemona . [https://pubmed.ncbi.nlm.nih.gov/28665284/ Multiple sclerosis - etiology and diagnostic potential].Postepy Hig Med Dosw. 2017 Jun 30;71(0):551-563.doi: 10.5604/01.3001.0010.3836. </ref> si evince che..."
  • 06:42, 11 November 2022 diff hist 0 N File:Scwannoma.jpegcurrent
  • 06:41, 11 November 2022 diff hist +3,528 N Store:EMes02Created page with "=== Scwannoma vestibolare e trigeminale === Lo spasmo emifacciale secondario dovuto a schwannoma vestibolare è molto raro. U_no studio di S Peker et al.<ref>S Peker, K Ozduman, T Kiliç, M N Pamir. [https://pubmed.ncbi.nlm.nih.gov/15346321/ Relief of hemifacial spasm after radiosurgery for intracanalicular vestibular schwannoma.] Minim Invasive Neurosurg. 2004 Aug;47(4):235-7. doi: 10.1055/s-2004-818485. </ref> è stato il primo caso riportato di spasmo emifacciale re..."
  • 06:40, 11 November 2022 diff hist +3,528 N Store:EMde02Created page with "=== Scwannoma vestibolare e trigeminale === Lo spasmo emifacciale secondario dovuto a schwannoma vestibolare è molto raro. U_no studio di S Peker et al.<ref>S Peker, K Ozduman, T Kiliç, M N Pamir. [https://pubmed.ncbi.nlm.nih.gov/15346321/ Relief of hemifacial spasm after radiosurgery for intracanalicular vestibular schwannoma.] Minim Invasive Neurosurg. 2004 Aug;47(4):235-7. doi: 10.1055/s-2004-818485. </ref> è stato il primo caso riportato di spasmo emifacciale re..."
  • 06:40, 11 November 2022 diff hist +3,528 N Store:EMfr02Created page with "=== Scwannoma vestibolare e trigeminale === Lo spasmo emifacciale secondario dovuto a schwannoma vestibolare è molto raro. U_no studio di S Peker et al.<ref>S Peker, K Ozduman, T Kiliç, M N Pamir. [https://pubmed.ncbi.nlm.nih.gov/15346321/ Relief of hemifacial spasm after radiosurgery for intracanalicular vestibular schwannoma.] Minim Invasive Neurosurg. 2004 Aug;47(4):235-7. doi: 10.1055/s-2004-818485. </ref> è stato il primo caso riportato di spasmo emifacciale re..."
  • 06:40, 11 November 2022 diff hist +3,528 N Store:EMit02Created page with "=== Scwannoma vestibolare e trigeminale === Lo spasmo emifacciale secondario dovuto a schwannoma vestibolare è molto raro. U_no studio di S Peker et al.<ref>S Peker, K Ozduman, T Kiliç, M N Pamir. [https://pubmed.ncbi.nlm.nih.gov/15346321/ Relief of hemifacial spasm after radiosurgery for intracanalicular vestibular schwannoma.] Minim Invasive Neurosurg. 2004 Aug;47(4):235-7. doi: 10.1055/s-2004-818485. </ref> è stato il primo caso riportato di spasmo emifacciale re..."
  • 06:38, 11 November 2022 diff hist +2,712 N Store:EMes01Created page with "== Introduzione == Prima di entrare nel vivo della discussione riguardante la patologia della nostra paziente Mary Poppins quella che dai capitoli precedenti sembra di tipo neuromotriia ed in particolare un 'Spasmo emimasticatorio' dovremmo focalizzare alcuni punti selettivi che ci aiuteranno a comprendere l'importanza dello excursus dei capitoli precedenti per finire al determinante processo di decriptazione del segnale. Cominciamo con il dire che non è tanto comples..."
  • 06:37, 11 November 2022 diff hist +2,712 N Store:EMde01Created page with "== Introduzione == Prima di entrare nel vivo della discussione riguardante la patologia della nostra paziente Mary Poppins quella che dai capitoli precedenti sembra di tipo neuromotriia ed in particolare un 'Spasmo emimasticatorio' dovremmo focalizzare alcuni punti selettivi che ci aiuteranno a comprendere l'importanza dello excursus dei capitoli precedenti per finire al determinante processo di decriptazione del segnale. Cominciamo con il dire che non è tanto comples..."
  • 06:37, 11 November 2022 diff hist +2,712 N Store:EMfr01Created page with "== Introduzione == Prima di entrare nel vivo della discussione riguardante la patologia della nostra paziente Mary Poppins quella che dai capitoli precedenti sembra di tipo neuromotriia ed in particolare un 'Spasmo emimasticatorio' dovremmo focalizzare alcuni punti selettivi che ci aiuteranno a comprendere l'importanza dello excursus dei capitoli precedenti per finire al determinante processo di decriptazione del segnale. Cominciamo con il dire che non è tanto comples..."
  • 06:35, 11 November 2022 diff hist +2,712 N Store:EMit01Created page with "== Introduzione == Prima di entrare nel vivo della discussione riguardante la patologia della nostra paziente Mary Poppins quella che dai capitoli precedenti sembra di tipo neuromotriia ed in particolare un 'Spasmo emimasticatorio' dovremmo focalizzare alcuni punti selettivi che ci aiuteranno a comprendere l'importanza dello excursus dei capitoli precedenti per finire al determinante processo di decriptazione del segnale. Cominciamo con il dire che non è tanto comples..."
  • 06:27, 11 November 2022 diff hist +20,578 N Spasmo emimasticatorioCreated page with "{{transl|it}} left|200x200px Questo capitolo e la serie di sub capitoli saranno dedicati principalmente al caso clinico della nostra povera paziente Mary Poppins che ha dovuto aspettare ben 10 anni per avere una diagnosi certa e dettagliata di Spasmo Emimasticatorio trovandosi tra due fuochi quello del contesto odontoiatrico, e quello neurologico oltre tutte le altre branche della medicina incontrate nel percorso clinico tipo la derma..."
  • 19:51, 10 November 2022 diff hist −17 Store:QLMit03→‎Observazioni
  • 05:33, 10 November 2022 diff hist +3,499 N Store:QLMfr09Created page with "==4. Quantum instruments from the scheme of indirect measurements== The basic model for construction of quantum instruments is based on the scheme of indirect measurements. This scheme formalizes the following situation: measurement’s outputs are generated via interaction of a system <math>S</math> with a measurement apparatus <math>M</math> . This apparatus consists of a complex physical device interacting with <math>S</math> and a pointer that shows the result of me..."
  • 05:33, 10 November 2022 diff hist +3,465 N Store:QLMfr04Created page with "==2. Classical versus quantum probability== CP was mathematically formalized by Kolmogorov (1933)<ref name=":2" /> This is the calculus of probability measures, where a non-negative weight <math>p(A)</math> is assigned to any event <math>A</math>. The main property of CP is its additivity: if two events <math>O_1, O_2</math> are disjoint, then the probability of disjunction of these events equals to the sum of probabilities: {| width="80%" | |- | width="33%" | ..."
  • 05:30, 10 November 2022 diff hist +1,768 N Modélisation de type quantique en biologie avec des systèmes et des instruments quantiques ouvertsCreated page with "{{transl|en}} {{FR | Title = Quantum-like modeling in biology with open quantum systems and instruments | author1 = Irina Basieva | author2 = Andrei Khrennikov | author3 = Masanao Ozawa | Source = https://pubmed.ncbi.nlm.nih.gov/33347968/<!-- where this work comes from or where was it was retrieved (URL) --> | Original = <!-- link to the original screenshot or PDF print from the retrieval --> | Date = 2021<!-- date of the original work, when the author/s publish..."
  • 05:28, 10 November 2022 diff hist +1,768 N Modellazione quantistica in biologia con sistemi e strumenti quantistici apertiCreated page with "{{transl|en}} {{FR | Title = Quantum-like modeling in biology with open quantum systems and instruments | author1 = Irina Basieva | author2 = Andrei Khrennikov | author3 = Masanao Ozawa | Source = https://pubmed.ncbi.nlm.nih.gov/33347968/<!-- where this work comes from or where was it was retrieved (URL) --> | Original = <!-- link to the original screenshot or PDF print from the retrieval --> | Date = 2021<!-- date of the original work, when the author/s publish..."
  • 05:24, 10 November 2022 diff hist −22,375 Quantum-like modeling in biology with open quantum systems and instruments - enReplaced content with "{{transl|en}} {{FR | Title = Quantum-like modeling in biology with open quantum systems and instruments | author1 = Irina Basieva | author2 = Andrei Khrennikov | author3 = Masanao Ozawa | Source = https://pubmed.ncbi.nlm.nih.gov/33347968/<!-- where this work comes from or where was it was retrieved (URL) --> | Original = <!-- link to the original screenshot or PDF print from the retrieval --> | Date = 2021<!-- date of the original work, when the author/s pub..." Tag: Replaced
  • 05:23, 10 November 2022 diff hist +4,730 N Store:QLMes18Created page with "===11.3. Psychological functions=== Now, we turn to the model presented in Section 10. A neural network is modeled as a compound quantum system; its state is presented in tensor product of single-neuron state spaces. Brain’s functions perform self-measurements modeled within theory of open quantum systems. (There is no need to consider state’s collapse.) State’s dynamics of some brain’s function (psychological function) <math>F</math> is described by the quantum..." current
  • 05:23, 10 November 2022 diff hist +4,730 N Store:QLMde18Created page with "===11.3. Psychological functions=== Now, we turn to the model presented in Section 10. A neural network is modeled as a compound quantum system; its state is presented in tensor product of single-neuron state spaces. Brain’s functions perform self-measurements modeled within theory of open quantum systems. (There is no need to consider state’s collapse.) State’s dynamics of some brain’s function (psychological function) <math>F</math> is described by the quantum..."
  • 05:23, 10 November 2022 diff hist 0 m Store:QLMfr18Gianfranco moved page Store:QLMfr8 to Store:QLMfr18 without leaving a redirect current
  • 05:23, 10 November 2022 diff hist +4,730 N Store:QLMfr18Created page with "===11.3. Psychological functions=== Now, we turn to the model presented in Section 10. A neural network is modeled as a compound quantum system; its state is presented in tensor product of single-neuron state spaces. Brain’s functions perform self-measurements modeled within theory of open quantum systems. (There is no need to consider state’s collapse.) State’s dynamics of some brain’s function (psychological function) <math>F</math> is described by the quantum..."
  • 05:22, 10 November 2022 diff hist +4,730 N Store:QLMit18Created page with "===11.3. Psychological functions=== Now, we turn to the model presented in Section 10. A neural network is modeled as a compound quantum system; its state is presented in tensor product of single-neuron state spaces. Brain’s functions perform self-measurements modeled within theory of open quantum systems. (There is no need to consider state’s collapse.) State’s dynamics of some brain’s function (psychological function) <math>F</math> is described by the quantum..."
  • 05:22, 10 November 2022 diff hist +4,730 N Store:QLMen18Created page with "===11.3. Psychological functions=== Now, we turn to the model presented in Section 10. A neural network is modeled as a compound quantum system; its state is presented in tensor product of single-neuron state spaces. Brain’s functions perform self-measurements modeled within theory of open quantum systems. (There is no need to consider state’s collapse.) State’s dynamics of some brain’s function (psychological function) <math>F</math> is described by the quantum..."
  • 05:22, 10 November 2022 diff hist +10,228 N Store:QLMes17Created page with "==11. Compound biosystems== ===11.1. Entanglement of information states of biosystems=== The state space <math>{\mathcal{H}}</math> of the biosystem <math>S</math> consisting of the subsystems <math>S_j,j=1,2,....n</math>, is the tensor product of subsystems’ state spaces<math>{\mathcal{H}}_j</math> , so {| width="80%" | |- | width="33%" |'''<big>*</big>''' | width="33%" |<math>\Im=\Im_1\otimes....\otimes\Im_n</math> | width="33%" align="right" |<math>(31)</math>..." current
  • 05:21, 10 November 2022 diff hist +10,228 N Store:QLMde17Created page with "==11. Compound biosystems== ===11.1. Entanglement of information states of biosystems=== The state space <math>{\mathcal{H}}</math> of the biosystem <math>S</math> consisting of the subsystems <math>S_j,j=1,2,....n</math>, is the tensor product of subsystems’ state spaces<math>{\mathcal{H}}_j</math> , so {| width="80%" | |- | width="33%" |'''<big>*</big>''' | width="33%" |<math>\Im=\Im_1\otimes....\otimes\Im_n</math> | width="33%" align="right" |<math>(31)</math>..."
  • 05:21, 10 November 2022 diff hist +10,228 N Store:QLMfr17Created page with "==11. Compound biosystems== ===11.1. Entanglement of information states of biosystems=== The state space <math>{\mathcal{H}}</math> of the biosystem <math>S</math> consisting of the subsystems <math>S_j,j=1,2,....n</math>, is the tensor product of subsystems’ state spaces<math>{\mathcal{H}}_j</math> , so {| width="80%" | |- | width="33%" |'''<big>*</big>''' | width="33%" |<math>\Im=\Im_1\otimes....\otimes\Im_n</math> | width="33%" align="right" |<math>(31)</math>..." current
  • 05:21, 10 November 2022 diff hist +10,228 N Store:QLMit17Created page with "==11. Compound biosystems== ===11.1. Entanglement of information states of biosystems=== The state space <math>{\mathcal{H}}</math> of the biosystem <math>S</math> consisting of the subsystems <math>S_j,j=1,2,....n</math>, is the tensor product of subsystems’ state spaces<math>{\mathcal{H}}_j</math> , so {| width="80%" | |- | width="33%" |'''<big>*</big>''' | width="33%" |<math>\Im=\Im_1\otimes....\otimes\Im_n</math> | width="33%" align="right" |<math>(31)</math>..."
  • 05:21, 10 November 2022 diff hist +10,228 N Store:QLMen17Created page with "==11. Compound biosystems== ===11.1. Entanglement of information states of biosystems=== The state space <math>{\mathcal{H}}</math> of the biosystem <math>S</math> consisting of the subsystems <math>S_j,j=1,2,....n</math>, is the tensor product of subsystems’ state spaces<math>{\mathcal{H}}_j</math> , so {| width="80%" | |- | width="33%" |'''<big>*</big>''' | width="33%" |<math>\Im=\Im_1\otimes....\otimes\Im_n</math> | width="33%" align="right" |<math>(31)</math>..."
  • 05:19, 10 November 2022 diff hist +7,471 N Store:QLMes16Created page with "==9. Epigenetic evolution within theory of open quantum systems== In paper (Asano et al., 2012b), a general model of the epigenetic evolution unifying neo-Darwinian with neo-Lamarckian approaches was created in the framework of theory of open quantum systems. The process of evolution is represented in the form of ''adaptive dynamics'' given by the quantum(-like) master equation describing the dynamics of the information state of epigenome in the process of interaction wi..." current
  • 05:19, 10 November 2022 diff hist +7,471 N Store:QLMde16Created page with "==9. Epigenetic evolution within theory of open quantum systems== In paper (Asano et al., 2012b), a general model of the epigenetic evolution unifying neo-Darwinian with neo-Lamarckian approaches was created in the framework of theory of open quantum systems. The process of evolution is represented in the form of ''adaptive dynamics'' given by the quantum(-like) master equation describing the dynamics of the information state of epigenome in the process of interaction wi..."
  • 05:19, 10 November 2022 diff hist +7,471 N Store:QLMfr16Created page with "==9. Epigenetic evolution within theory of open quantum systems== In paper (Asano et al., 2012b), a general model of the epigenetic evolution unifying neo-Darwinian with neo-Lamarckian approaches was created in the framework of theory of open quantum systems. The process of evolution is represented in the form of ''adaptive dynamics'' given by the quantum(-like) master equation describing the dynamics of the information state of epigenome in the process of interaction wi..." current
  • 05:19, 10 November 2022 diff hist +7,471 N Store:QLMit16Created page with "==9. Epigenetic evolution within theory of open quantum systems== In paper (Asano et al., 2012b), a general model of the epigenetic evolution unifying neo-Darwinian with neo-Lamarckian approaches was created in the framework of theory of open quantum systems. The process of evolution is represented in the form of ''adaptive dynamics'' given by the quantum(-like) master equation describing the dynamics of the information state of epigenome in the process of interaction wi..."
  • 05:18, 10 November 2022 diff hist +7,471 N Store:QLMen16Created page with "==9. Epigenetic evolution within theory of open quantum systems== In paper (Asano et al., 2012b), a general model of the epigenetic evolution unifying neo-Darwinian with neo-Lamarckian approaches was created in the framework of theory of open quantum systems. The process of evolution is represented in the form of ''adaptive dynamics'' given by the quantum(-like) master equation describing the dynamics of the information state of epigenome in the process of interaction wi..."
  • 05:16, 10 November 2022 diff hist −21,304 Quantum-like modeling in biology with open quantum systems and instruments - en
  • 05:16, 10 November 2022 diff hist +6,383 N Store:QLMes15Created page with "===8.3. Operation of biological functions through decoherence=== To make the previous considerations concrete, let us consider a pure quantum state as the initial state. Suppose that a biological function  <math>F</math> is dichotomous, <math>F=0,1 </math>, and it is symbolically represented by the Hermitian operator that is diagonal in orthonormal basis <math>|0\rangle</math>,<math>|1\rangle</math> . (We consider the two dimensional state space — the qubit space.) Le..." current
  • 05:16, 10 November 2022 diff hist +6,383 N Store:QLMde15Created page with "===8.3. Operation of biological functions through decoherence=== To make the previous considerations concrete, let us consider a pure quantum state as the initial state. Suppose that a biological function  <math>F</math> is dichotomous, <math>F=0,1 </math>, and it is symbolically represented by the Hermitian operator that is diagonal in orthonormal basis <math>|0\rangle</math>,<math>|1\rangle</math> . (We consider the two dimensional state space — the qubit space.) Le..."
  • 05:16, 10 November 2022 diff hist +6,383 N Store:QLMfr15Created page with "===8.3. Operation of biological functions through decoherence=== To make the previous considerations concrete, let us consider a pure quantum state as the initial state. Suppose that a biological function  <math>F</math> is dichotomous, <math>F=0,1 </math>, and it is symbolically represented by the Hermitian operator that is diagonal in orthonormal basis <math>|0\rangle</math>,<math>|1\rangle</math> . (We consider the two dimensional state space — the qubit space.) Le..."
  • 05:15, 10 November 2022 diff hist +6,383 N Store:QLMit15Created page with "===8.3. Operation of biological functions through decoherence=== To make the previous considerations concrete, let us consider a pure quantum state as the initial state. Suppose that a biological function  <math>F</math> is dichotomous, <math>F=0,1 </math>, and it is symbolically represented by the Hermitian operator that is diagonal in orthonormal basis <math>|0\rangle</math>,<math>|1\rangle</math> . (We consider the two dimensional state space — the qubit space.) Le..."
  • 05:15, 10 November 2022 diff hist +6,383 N Store:QLMen15Created page with "===8.3. Operation of biological functions through decoherence=== To make the previous considerations concrete, let us consider a pure quantum state as the initial state. Suppose that a biological function  <math>F</math> is dichotomous, <math>F=0,1 </math>, and it is symbolically represented by the Hermitian operator that is diagonal in orthonormal basis <math>|0\rangle</math>,<math>|1\rangle</math> . (We consider the two dimensional state space — the qubit space.) Le..."
  • 05:14, 10 November 2022 diff hist +3,960 N Store:QLMes14Created page with "===8.2. Biological functions in the quantum Markov framework=== We turn to the open system dynamics with the GKSL-equation. In our modeling, Hamiltonian  <math>\widehat{\mathcal{H}}</math> and Lindbladian  <math>\widehat{{L}}</math> represent some special ''biological function'' <math>F</math> (see Khrennikov et al., 2018) for details. Its functioning results from interaction of internal and external information flows. In Sections 10, 11.3,  <math>F</math> is some ''..." current
  • 05:14, 10 November 2022 diff hist +3,960 N Store:QLMde14Created page with "===8.2. Biological functions in the quantum Markov framework=== We turn to the open system dynamics with the GKSL-equation. In our modeling, Hamiltonian  <math>\widehat{\mathcal{H}}</math> and Lindbladian  <math>\widehat{{L}}</math> represent some special ''biological function'' <math>F</math> (see Khrennikov et al., 2018) for details. Its functioning results from interaction of internal and external information flows. In Sections 10, 11.3,  <math>F</math> is some ''..."
  • 05:14, 10 November 2022 diff hist +3,960 N Store:QLMfr14Created page with "===8.2. Biological functions in the quantum Markov framework=== We turn to the open system dynamics with the GKSL-equation. In our modeling, Hamiltonian  <math>\widehat{\mathcal{H}}</math> and Lindbladian  <math>\widehat{{L}}</math> represent some special ''biological function'' <math>F</math> (see Khrennikov et al., 2018) for details. Its functioning results from interaction of internal and external information flows. In Sections 10, 11.3,  <math>F</math> is some ''..."
  • 05:13, 10 November 2022 diff hist +3,960 N Store:QLMit14Created page with "===8.2. Biological functions in the quantum Markov framework=== We turn to the open system dynamics with the GKSL-equation. In our modeling, Hamiltonian  <math>\widehat{\mathcal{H}}</math> and Lindbladian  <math>\widehat{{L}}</math> represent some special ''biological function'' <math>F</math> (see Khrennikov et al., 2018) for details. Its functioning results from interaction of internal and external information flows. In Sections 10, 11.3,  <math>F</math> is some ''..."
  • 05:13, 10 November 2022 diff hist +3,960 N Store:QLMen14Created page with "===8.2. Biological functions in the quantum Markov framework=== We turn to the open system dynamics with the GKSL-equation. In our modeling, Hamiltonian  <math>\widehat{\mathcal{H}}</math> and Lindbladian  <math>\widehat{{L}}</math> represent some special ''biological function'' <math>F</math> (see Khrennikov et al., 2018) for details. Its functioning results from interaction of internal and external information flows. In Sections 10, 11.3,  <math>F</math> is some ''..."
  • 05:12, 10 November 2022 diff hist +3,900 N Store:QLMfr13Created page with "==8. Open quantum systems: interaction of a biosystem with its environment== As was already emphasized, any biosystem <math>S</math> is fundamentally open. Hence, dynamics of its state has to be modeled via an interaction with surrounding environment <math> \varepsilon</math>. The states of  <math>S</math> and <math> \varepsilon</math> are represented in the Hilbert spaces <math>\mathcal{H}</math> and <math>\mathcal{H}</math>. The compound system <math>S+\varepsilon</..."
  • 05:12, 10 November 2022 diff hist +3,900 N Store:QLMde13Created page with "==8. Open quantum systems: interaction of a biosystem with its environment== As was already emphasized, any biosystem <math>S</math> is fundamentally open. Hence, dynamics of its state has to be modeled via an interaction with surrounding environment <math> \varepsilon</math>. The states of  <math>S</math> and <math> \varepsilon</math> are represented in the Hilbert spaces <math>\mathcal{H}</math> and <math>\mathcal{H}</math>. The compound system <math>S+\varepsilon</..."
  • 05:11, 10 November 2022 diff hist +3,900 N Store:QLMit13Created page with "==8. Open quantum systems: interaction of a biosystem with its environment== As was already emphasized, any biosystem <math>S</math> is fundamentally open. Hence, dynamics of its state has to be modeled via an interaction with surrounding environment <math> \varepsilon</math>. The states of  <math>S</math> and <math> \varepsilon</math> are represented in the Hilbert spaces <math>\mathcal{H}</math> and <math>\mathcal{H}</math>. The compound system <math>S+\varepsilon</..."
  • 05:11, 10 November 2022 diff hist +3,900 N Store:QLMen13Created page with "==8. Open quantum systems: interaction of a biosystem with its environment== As was already emphasized, any biosystem <math>S</math> is fundamentally open. Hence, dynamics of its state has to be modeled via an interaction with surrounding environment <math> \varepsilon</math>. The states of  <math>S</math> and <math> \varepsilon</math> are represented in the Hilbert spaces <math>\mathcal{H}</math> and <math>\mathcal{H}</math>. The compound system <math>S+\varepsilon</..."
  • 05:11, 10 November 2022 diff hist +3,900 N Store:QLMes13Created page with "==8. Open quantum systems: interaction of a biosystem with its environment== As was already emphasized, any biosystem <math>S</math> is fundamentally open. Hence, dynamics of its state has to be modeled via an interaction with surrounding environment <math> \varepsilon</math>. The states of  <math>S</math> and <math> \varepsilon</math> are represented in the Hilbert spaces <math>\mathcal{H}</math> and <math>\mathcal{H}</math>. The compound system <math>S+\varepsilon</..." current

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