PlanetPhysics/Quantum Super Operators

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This is a topic on quantum super-operators (or superoperators).

Time and Microentropy: Irreversibility in Open Systems

A significant part of the scientific and philosophical [[../Work/|work]] of Ilya Prigogine has been devoted to the dynamical meaning of phenomenal/physical irreversibility expressed in terms of the second law of [[../Thermodynamics/|Thermodynamics]] and [[../QuantumStatisticalTheories/|quantum statistical mechanics]]. For [[../SimilarityAndAnalogousSystemsDynamicAdjointnessAndTopologicalEquivalence/|systems]] with strong enough instability of [[../CosmologicalConstant/|motion]] the [[../PreciseIdea/|concept]] of phase space trajectories is no longer meaningful and the dynamical description has to be replaced by the motion of distribution [[../Bijective/|functions]] on the phase space. The viewpoint is that [[../SpaceTimeQuantizationInQuantumGravityTheories/|quantum theory]] produces a more coherent [[../Bijective/|type]] of motion than in the classical setting and the quantum effects induce correlations between neighbouring classical trajectories in phase space.

Quantum Super-Operators

Prigogine's idea (1980) is to associate a macroscopic [[../ThermodynamicLaws/|entropy]] (or Lyapounov function) with a microscopic entropy (quantum) super--operator $M$. Here the time--parametrized distribution functions ${\rho }_t$ are regarded as densities in phase space such that the [[../NormInducedByInnerProduct/|inner product]] $⟨{\rho }_t,M{\rho }_t⟩$ varies monotonously with $t$ as the functions ${\rho }_t$ evolve in accordance with Liouville's equation (Prigogine, 1980; Misra et al, 1979). For well defined systems for which the super-operators $M$ exist, a time super-operator $T$ (`age' or `internal time') can also be introduced. (For the precise details, the reader is referred to Misra et al. 1979). Furthermore, the equations of motion with randomness at the microscopic level then emerge as irreversibility on the macroscopic level. However, unlike the usual [[../QuantumOperatorAlgebra5/|quantum operators]] representing [[../QuantumSpinNetworkFunctor2/|observables]], the $M$ super-operators are non-Hermitian [[../QuantumOperatorAlgebra4/|operators]], (i.e., they are not self-adjoint, $M$ $\ne$M* ).

However, there are certain provisions that have to be made in terms of the [[../CohomologyTheoryOnCWComplexes/|spectrum]] of the [[../Hamiltonian2/|Hamiltonian]] $H$ for M to be properly defined: if $H$ has a pure point spectrum, then $M$ does not exist, and likewise, if $H$ has a continuous but bounded spectrum then $M$ cannot exist. Thus, the super-operator $M$ cannot exist in the case of only finitely extended systems containing only a finite number of [[../Particle/|particles]]. Furthermore, the super-operator $M$ cannot preserve the class of `[[../PureState/|pure states]]' since it is non-factorizable. The distinction between pure states (represented by [[../Vectors/|vectors]] in a [[../NormInducedByInnerProduct/|Hilbert space]]) and [[../PureState/|mixed states]] (represented by density operators) is thus lost in the process of measurement. In other words, the distinction between pure and mixed states is lost in a quantum system for which the algebra of observables can be extended to include a new dynamical variable representing the non-equilibrium entropy. In this way, one may formulate the second law of thermodynamics in terms of $M$ for quantum mechanical systems. Let us mention that the time [[../QuantumSpinNetworkFunctor2/|operator]] $T$ represents `internal time' and the usual, `secondary' time in quantum [[../NewtonianMechanics/|dynamics]] is regarded as an average over $T$. When $T$ reduces to a trivial operator the usual concept of time is recovered $T\rho (x,v,t)=t\rho (x,v,t)$, and thus time in the usual sense is conceived as an average of the individual times as registered by the observer. Given the latter's ability to distinguish between between future and past, a self-consistent scheme may be summarized in the following [[../TrivialGroupoid/|diagram]] (Prigogine, 1980):

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for which `irreversibility' occurs as the intermediary in the following sequence: $=Dynamics=⟹=Irreversibility=⟹=Dissipativestructures=$

(Note however that certain quantum theorists, as well as [[../AlbertEinstein/|Einstein]], regarded the irreversibility of time as an `illusion' caused by statistical averaging. Others-- operating with minimal [[../CategoricalGroupRepresentation/|representations]] in [[../LQG2/|quantum logic]] for finite quantum systems-- go further still by denying that there is any need for real time to appear in the formulation of quantum theory.)

The importance of the above diagram will become fully apparent in the context of [[../IsomorphicObjectsUnderAnIsomorphism/|section]] 4 , where we discuss living organisms in terms of open systems that by definition are irreversible, and also have highly complex (generic) dynamics supported by dissipative structures which may have come into existence through `symmetry breaking' , as explained in further detail by Baianu and Poli, 2008, in this [[../Volume/|volume]], and also briefly in the next subsection. This diagram sketches four major pieces from the puzzle of the emergence/origin of life on earth, without however coming very close to completing this puzzle; thus, Prigogine's subtle concepts of microscopic time and micro--entropy super--operators may allow us to understand how life originated on earth several billion years ago, and also how organisms function and survive today. They also provide a partial answer to subtle quantum genetics and fundamental evolutionary dynamics questions asked by Schr\"{o}dinger-- one of the great founders of quantum `[[../CosmologicalConstant2/|wave]] [[../Mechanics/|mechanics]]' in his widely read book "What is Life?" Other key answers to the latter's question were recently provided by Robert Rosen (2000) in his popular book ``Essays on Life Itself.", unfortunately without any possibility of continuation or of reaching soon the `ultimate' or complete answer. Schr\"{o}dinger's suggestion that living organisms "feed on 'negative entropy'...," was at least in part formalized by Prigogine's super-operators, such as $M$. This theory is in great need of further developments that he could not complete during his lifespan; such developments may also include several of Rosen 's (2000) suggestions and will apparently require a categorical and Higher Dimensional [[../CoIntersections/|algebraic]], non--Abelian theory of irreversible thermodynamics, as well as a quantum--mechanical statistics of [[../ThermodynamicLaws/|open systems]] that are capable of autopoiesis,that is, living organisms.

One notes that Albert Einstein would have discarded such notions along with the standard [[../QuantumParadox/|quantum mechanics]] formulation it is interesting that no imaginary experiments have been designed so far to test the reality of quantum super-operators.