Open Quantum Systems II The Markovian Approach

Understanding dissipative dynamics of open quantum systems remains a challenge in mathematical physics. This problem is relevant in various areas of fundamental and applied physics. From a mathematical point of view, it involves a large body of knowledge.

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    

         

                                                                                                                                                                                                                              

   

 

 





                                                                                                                                                                                                   

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