





PROJECT SUPPLEMENTAL BOOKS 

ARTICLES
Epperson, M. “Relational Realism and the Ontogenetic Universe: Subject, Object, and Ontological Process in Quantum Mechanics.” Angelaki 25:3 (2020)
R. Kastner, S. Kauffman, M. Epperson, "Taking Heisenberg's Potentia Seriously" International Journal of Quantum Foundations, 4:2 (2018) 158172 (See also Tom Siegfried's review article on this paper in Science News)
M. Epperson, “EventOntological Quantum Mechanics: A Process Theoretic Approach” in Physics and Speculative Philosophy: Potentiality and Modern Science. Eds. Timothy Eastman, Michael Epperson, and David Ray Griffin. Berlin: De Gruyter (2016)
E. Zafiris, "The Global Symmetry Group of Quantum Spectral Beams and Geometric Phase Factors," Advances in Mathematical Physics (2015)
Epperson, M. “The Common Sense of Quantum Theory: Exploring the Internal Relational Structure of SelfOrganization in Nature,” Coding as Literacy, Metalithicum 5. Ed. Vera Bühlmann and Ludger Hovestadt. Birkhäuser (2015)
E. Zafiris, V. Karakostas, “A Categorial Semantic Representation of Quantum Event Structures,” Foundations of Physics 43 (2013)
K. Bschir, M. Epperson, E. Zafiris, “Decoherence: A View from Topology,” Center for Philosophy and the Natural Sciences, California State University Sacramento (2014)
M. Epperson, “Quantum Mechanics and Relational Realism: Logical Causality and Wavefunction Collapse,” Process Studies, 38:2 (2009)
E. Zafiris, A. Mallios, “The Homological KählerDe Rham Differential Mechanism, Part I: Application in General Theory of Relativity,” Advances in Mathematical Physics (2011)
E. Zafiris, A. Mallios, “The Homological Kählerde Rham Differential Mechanism, Part II. SheafTheoretic Localization of Quantum Dynamics,” Advances in Mathematical Physics (2011)
P. Stamp, S. Takahashi, et al. “Decoherence in crystals of quantum molecular magnets.” Nature 476.7358 (2011): 7679
E. Zafiris, "Boolean information sieves: a localtoglobal approach to quantum information," International Journal of General Systems 39, No. 8 (2010): 873–895
M. Epperson, "Relational Realism: The Evolution of Ontology to Praxiology in the Philosophy of Nature." World Futures, 65:1, Routledge (2009): 1941
M. Epperson, “The Mechanics of Concrescence: Quantum Theory and Process Metaphysics,” Studia Whiteheadiana (Poland), Vol 4 (2010): 159190 



PERSONNEL 
Principal Investigator: 

Michael Epperson, Research Professor & Founding Director, Center for Philosophy and the Natural Sciences, College of Natural Sciences and Mathematics, California State University Sacramento 


CoInvestigators: 



Elias Zafiris 
Senior Research Fellow, Quantum Theory
Department of Mathematics & Institute of Mathematics
University of Athens 


Stuart Kauffman 
Institute for Systems Biology, Seattle and Professor Emeritus, Dept. of Biochemistry and Biophysics, University of Pennsylvania 


Karim Bschir 
Senior Research Fellow
Chair for Philosophy
Swiss Federal Institute of Technology, Zurich, Switzerland



Timothy Eastman 
NASAGoddard; Plasmas International 


Philip C.E. Stamp 
Professor, Condensed Matter Theory
Department of Physics and Astronomy
University of British Columbia
Director, Pacific Institute of Theoretical Physics 


Consultants: 



David Finkelstein 
Professor Emeritus, Quantum Theory
Department of Physics
Georgia Institute of Technology 


Roland Omnès 
Quantum Theorist
Laboratoire de Physique Théorique
Université de Paris XI, (Unité Mixte de Recherche, CNRS, UMR 8627) 

PROJECT SUMMARY
The quantum mechanics of large systems and related decoherence phenomena are crucial to current groundbreaking efforts in quantum information theory, quantum computing, and the relation of these to complex systems theory, where ‘classical reality’ is modeled as emergent from a more fundamental quantum mechanical description of nature. In recent wellregarded interpretations of quantum physics that explore various mechanisms of phase decoherence, including the consistent histories approach of Robert Griffiths (1984, 2002) and the work of Roland Omnès (1994), one finds a physical—i.e., not ‘merely philosophical’—distinction between the order of contingent causal relation and the order of necessary logical implication. Of particular import are recent experiments [1] on precessional decoherence in spin bath dynamics which, unlike oscillator bath and other environmental decoherence models [2] , entails no energy transfer between the bath and the measured system. Thus the conventional description of decoherencegenerating systemenvironment interactions, via an effective Hamiltonian, is arguably incomplete. That is to say, nondissipative decoherence cannot be simply reduced to the dynamics of efficient physical causality—the framework environmental decoherence has typically been fitted to. In this sense, nondissipative decoherence can be seen as exemplifying the concept of ‘logical conditioning of potentia’ in the relational realist interpretation of quantum mechanics [3], and supportive of that interpretation’s argument against the conventional presupposition of physical causal closure.
Moreover the decoherent histories formalism, in its pathintegral form, provides a spacetime formulation of quantum theory that is highly compatible with the mereotopological model of spatiotemporal extension proposed by Alfred North Whitehead. This implies the possibility of logicallycausally relating and defining probabilities for alternative potential spatiotemporal regions, whereas conventional quantum theory only permits the calculation of probabilities for alternative outcome states at definite moments of time.
In their recent book, Foundations of Relational Realism: A Topological Approach to Quantum Mechanics and the Philosophy of Nature (Lexington Books / Rowman & Littlefield, New York, 2013) the project’s principal investigators Michael Epperson and Elias Zafiris have examined the function of bivalent propositional logic in describing nondissipative intrinsic decoherence and quantum nonlocality (nonlocal logical causality) at the microscale, and suggest that there are important implications for the understanding of spacetime at the macroscale—namely the possibility of constructing a quantum mereotopological spacetime formalism that refines and expands the model proposed by Whitehead. Such a formalism would supply a novel approach to the problem of quantum gravity, understanding classical mechanics as emergent from quantum mechanics, and the formation of emergent complex adaptive systems given in the work of CoI Stuart Kauffman. With respect to the latter, for example, Zafiris notes that “in the arena of quantum cosmology, there is a fundamental necessity to understand why, on sufficiently large scales quantum theory admits an emergent description of the universe involving only a small number of dynamical variables, the ‘hydrodynamic variables,’ which obey deterministic evolution equations, and are related to the existence of conservation laws as well.”
Epperson has argued (2004, 2009, 2010) that nondissipative, intrinsic decoherence can be described in terms of logicalcausal quantum dynamics; that is, the logicalcausal order presupposed by the standard formalism (trace over of the density matrix, the decoherence functional, etc.) can be seen as a necessary presupposition of the physical dynamics, such that intrinsic decoherence—particularly the concept of ‘third party decoherence’—can be seen as a reflection of this presupposition. Indeed, since third party decoherence pertains to any quantum measurement interaction where both the system and tracedover environment are coconditioned, the appeal to dynamical logical causality would account for the current experimental difficulty in wholly eliminating decoherence from quantum measurement.
The experimental component of this project, modeled by CoI Philip Stamp, Professor, Condensed Matter Theory, Department of Physics, University of British Columbia and Founding Director of the Pacific Institute for Theoretical Physics, was a followup to recent work by S. Bertaina, B. Barbara, et al. (“Quantum Oscillations in a Molecular Magnet,” Nature, 453, 8 May 2008. See also, Stamp’s discussion of this experiment on page 167 of the same issue.) Initial work to this end has been published in Stamp, P., Takahashi, S. et al. “Decoherence in crystals of quantum molecular magnets.” Nature 476.7358 (2011): 7679.
The macroscale (spatiotemporal, cosmological) implications of these explorations of decoherence at the microscale are being examined by way of a Whiteheadian/Relational Realist interpretation of the decoherent histories QM formalism (cf. Epperson, 2004, and Epperson and Zafiris 2013). Again, the decoherent histories formalism allows for a spacetime formulation of quantum theory that is highly compatible with the mereotopological model of spatiotemporal extension proposed by Whiteheada settheoretic model that shows a great potential for refinement via the mathematics of Grothendieck topology and category/sheaf theory. This is crucial because the mathematical rigidity of the Hilbert space (as a topological vector space) does not allow a relativization analogous with the one of classical relativity theory on smooth manifolds. By contrast, a mereotopological/categorytheoretic reformulation of quantum logic in terms of Boolean localization systems (e.g., Booelan sheaves, per the work of CoI Elias Zafiris) achieves precisely such an objective by generalizing the smooth manifold construction in generic algebraic/categorical terms.
This makes it possible to formulate a framework of local/global or part/whole relations without the intervention of a spacetime classically conceived. On the contrary, the usual spacetime manifold and its metrical relations (imposing extra conditions like the lightcone causality relations) appear as emergent at a higher level than the more fundamental level of logical and algebraic partwhole relations. Epperson’s distinction between a) mereological/topological/logical relations, and b) physical/metrical/causal relations, is reflected precisely in Zafiris’ distinction between these two different levelsthe algebraic partwhole relations and the metrical spacetime relations, respectively where the latter can be seen as an emergent/metrical specialization of the former. The key issue to be explored is the problem of localization and the problem of passing from the local to the global in an extensive continuum. 

[1] Bertaina, S., Gamarelli, S., Mitra, T., Tsukerblat, B., Muller, A., & Barbara, B. (2008), “Quantum oscillations in a molecular magnet,” Nature, 453:8 May 2008.
[2] cf. for example, Caldeira, A. & Leggett, A. (1983). “Quantum tunneling in a dissipative system.” Annals of Physics, 149: 374456
[3] Epperson (2004, 2009)



PROJECT DESCRIPTION
Objectives
Interpretations of quantum physics such as those offered by Omnès and Griffiths derive the logical order of classical causality, in part, from the decoherence effect, whereby potential facts constitutive of a quantum mechanical system are logically ordered into potential, mutually consistent histories. Decoherence is thus given by these interpretations as a derivation of classical logical causality from the quantum mechanical correlation of the causal and logical orders. And indeed, there have been experiments by which the logical order of classical causality can be seen as deriving from the logical integrations of potentia yielded by decoherence. Caldeira and Leggett (1983) created a successful demonstration of such a derivation. Using the classical Lorentz oscillator model, they showed that the quantum interferences manifest by the oscillations were cancelled out via the decoherence effect. The latter, in other words, can be seen as introducing logical constraints upon the quantum system. Given sufficient time for decoherence to occur, the system becomes describable as a classical probability distribution in phase space. Moreover, observable consequences of coinvestigator David Finkelstein’s theory (as characterized, for instance, in Finkelstein et al., [2001] “Clifford Algebra as Quantum Language,” J. Math. Phys 42, 14891502) are discussed in the model of the oscillator in Finkelstein and ShiriGarakani, 2004c Finite Quantum Harmonic Oscillator.
Even more significant, recent experiments on precessional nondissipative decoherence in spin bath dynamics are arguably even better at exemplifying the concept of ‘logical conditioning of potentia’ in the relational realist interpretation of quantum mechanics; for unlike the oscillator bath and other environmental decoherence models, the phenomenon of precessional decoherence entails no energy transfer between the bath and the measured system. That is to say, nondissipative precessional, intrinsic, and ‘third party’ decoherence which we propose to investigate in this continuation of our project, cannot be simply reduced to the dynamics of efficient physical causality—the ‘causally closed’ framework environmental decoherence has typically been fitted to.
The fundamental question we will be exploring, then, is whether there are intrinsic sources of decoherence in Nature—i.e., sources that cannot be accounted for, in an experimental setting, solely via any of the known decoherence mechanisms. Experimental investigation of the hypothesis of intrinsic decoherence is as crucial to the enterprise of philosophy as it is to the enterprise of physics; for the implication is that decoherence, and the associated logical conditioning of physical causality by which the effects of decoherence are recognized, is inevitable. It does not, in other words, merely arise as an epiphenomenon from dissipative, purely efficient causal processes, as has been the popular understanding of environmental decoherence for a number of years. Dissipation and decoherence are indeed tied together in the oscillator bath models of the environment; but as mentioned above, and discussed further below, this result is not true for spin baths, where one can have decoherence with no dissipation, even at T = 0; and in the case of thirdparty decoherence there cannot possibly be any environmental dissipation, at any T, since there is no direct coupling to the environment. Thus there is no necessary connection between decoherence and dissipation in the real world, and no necessary reason for it to cease at T = 0. This is a problem of real practical interest right now, both for the construction of quantum information processing systems and for the standard physics of solids, and there is consequently a substantial worldwide quest underway exploring ways to eliminate environmental decoherence. Thus the question of ‘intrinsic’ sources of decoherence in Nature, impossible to eradicate, is crucial.
The hallmark feature of the concept of intrinsic decoherence is that it is inevitable—perhaps even arising as part of the basic structure of the universe. And thus the logical conditioning of physical causality, as evinced by the effect of decoherence upon quantum systems, can be envisioned similarly—as part of the basic structure of the universe (and perhaps part of the answer to the question of why the universe is accessible to reason in the first place.) Such intrinsic sources of decoherence in Nature, operating even at T = 0, would not only provide a way of explaining the ‘emergence of classical physics’ in fields ranging from quantum cosmology to condensed matter physics; they would also place a fundamental limit on the observability of quantum phenomena. This would limit the possibility of seeing macroscopic quantum phenomena, and also place fundamental limits on the superpositions required for quantum computing.
Possibilities for intrinsic decoherence mechanisms have already emerged from both low and
highenergy physics, and this is currently one of the most exciting frontiers of physics. Crucial experiments are required such as the one proposed herein. But if fitness is to be tested and evaluated among competing physicalmetaphysical interpretations of quantum mechanics—i.e., those that dualistically treat actuality & the causal order and potentiality & the logical order as separate or separable features of reality, versus the relational realist interpretation, which treats actuality and potentiality as dipolar, mutually implicative features of every quantum praxis event—it is equally crucial that the conception of experiment be sufficiently free of serious constraints imposed by any particular ontological commitment. This is especially important with respect to certain of these commitments that enjoy the status of ‘convention.’ Thus an emphasis on experimental testing, such as those discussed above, combined with reduced modeldependence, and a turn away from the typical conditioning influence of traditionally inherited ontological presuppositions, will be an important prescription for the development of metaphysically coherent interpretations of physical theories such as quantum physics. The EPR gedanken experiment, for example, was conceived by its authors via the conventional, inherited classical mechanisticmaterialistic ontology. But more recent EPRlike tests of quantum nonlocality, rather than being conceived as constricted to this ontology, were conceived to test the limitations of this ontology. 



EXPERIMENTAL PROPOSAL
We are currently into our second year of work, and are now in position to develop an experimental component with Philip Stamp at the University of British Columbia/Pacific Institute of Theoretical Physics, who has just joined our group as coInvestigator. Our goal is to develop an experiment that attempts to differentiate between precessional / spin bath decoherence and 'intrinsic' decoherence, so that the latter can be further elucidated.
Our work will build upon recent groundbreaking experiments on the mechanisms of decoherence in molecular magnets. In Bertaina et al., published last year (Nature 453: 8 May 2008see also in the same issue P.C.E. Stamp, “Quantum Information: Stopping the Rot” p.167, a discussion of the Bertaina experiment) three decoherence mechanisms were accounted for: Spin bath, lattice vibrations, and dipolar pairwise decoherence. The observed coherence time was 800 ns for the spin ½ transitions of the Vanadium molecule. It is proposed that if the experiment were performed at liquid He temperatures, with spinfree molecules, sufficiently separated by a surfactant to restrict dipolar pairwise decoherence, coherence time could be extended to 100 microseconds. Our own experimental work will proceed to test this and related hypotheses.
This experimental investigation is crucial for the relational realist interpretation of quantum mechanics, and its conception of logical causality, because spinbath / precessional decoherence involves no transfer of energy. It is entirely nondissipative, unlike the more common oscillator bath models that have been used in previous experiments. Nondissipative decoherence is arguably something 'deeper' than dissipative environmental decoherence via simple efficient physical causality, which is the framework environmental decoherence has typically been fitted to. Our goal, then, is to develop an experiment that attempts to differentiate between precessional / spin bath decoherence and other possible sources of 'intrinsic' decoherence, so that the latter can be further elucidated.
Our proposed experimental work will help shed light on, 1. how decoherence can be examined as a potential challenge to (or refinement of) Leggett's thesis of macrorealism (which would be a much needed blow to the conventional mechanisticmaterialistic paradigm); and 2. how decoherence—especially nondissipative decoherence seen in the spin bath, 3rd party, and 'intrinsic' conceptions—can be interpreted as a physical exemplification of 'logical causality' via ‘logicalrelational decoherence.’ In this regard, decoherence might be seen as implying a logically governed conditioning of physical causality at the level of microphysical reality—one that could account for the tacitly presupposed correlation of the causal and logical orders at the classical level as an emergent phenomenon.
Since the correlation of the causal and logical orders has been a centuriesold problem in natural philosophy, the obvious relevance of the logical order to decoherence warrants careful study. Possible implications include new understandings of: 1. the quantum measurement problem, 2. the supposed quantumclassical boundary, 3. relating the asymmetrical logical order to the asymmetrical cosmological arrow, thermodynamic arrow, and quantum arrow (to the extent that the latter is asymmetrical, for example, via Von Neumann’s Process 1); and 4, the conception of classical physics as ‘emergent’ from quantum physics, via the decoherence effect.
With respect to the latter, one might focus on the more physical question of how classical quasideterministic behavior emerges for large systems, and/or how quasiclassical stochastic behavior emerges, even for small systems. Coinvestigator Philip Stamp writes, “a proper answer to this question requires understanding the real decoherence mechanisms operating in Nature and that these are not so simple, or necessarily completely understood. Thus we do not yet have a theory which derives classical physics from quantum physics solely using ideas from decoherence, even though we do have some derivations of classical behaviour within certain models. It is important to note that in some other models one can actually find nonclassical behavior emerging in the largescale dynamics, because of decoherence (this happens, for example, when one is dealing with a spin bath environment (Prokof’ev & Stamp, 2006)). Thus there is nothing inevitable about classical behaviour!”
“It is always remarkable when a combination of theory and experiment has larger
philosophical consequences. Perhaps the most dramatic example in recent times has been
the impact of Bell’s inequalities, where a set of experiments in atomic physics was able to
rule out a whole class of possible theories about Nature, and in doing so, consign a widely
accepted philosophical view about ‘reality’ to the dustbin. The fascinating prospect is that
future experiments at low temperatures in condensed matter systems looking for
‘intrinsic decoherence’ may have a similar impact.”
 Philip C.E. Stamp 
The idea of intrinsic decoherence in Nature is implicit in some theories of hidden variables, and also in the 'nonlinear' adaptations of quantum mechanics by Ghirardi, Pearle, et al. (1986, 1990). More recently it has been widely appreciated that any sign of 'intrinsic decoherence' in Nature, or for that matter any breakdown of quantum mechanics, is almost certainly going to happen in systems with large numbers of degrees of freedom. More recent ideas therefore focus on this. The recent ideas of 't Hooft (1999, 2001) are very interesting in this respect; he points out that if one believes that the holographic principle really does apply (and it is now a pretty central part of quantum gravity), then genuine entanglement in Nature cannot involve more than 10^{120} degrees of freedom, since this is the size of the Hilbert space allowed by this principle. However any experiments to check out ideas like this are dogged by the fact that almost all physical systems in Nature show far more decoherence than theory predicts (often at least 3 orders of magnitude more). The reason for this is pretty obvious: there are many sources of 'junk decoherence,' coming from defects, nuclear spins, dislocations, charge fluctuators, etc., in either physical systems of interest, or in surrounding parts of the experimental cell, or even in the measuring system. This 'junk' is typically described by models of '2level systems', and the decoherence from them is described by the 'spin bath' model of environmental decoherence (Prokof'ev and Stamp, Rep Prog Phys 69, 669 (2000)).
The best systems to initially do decoherence tests in are thus the ones (i) in which one has a large number of degrees of freedom, and (ii) in which decoherence processes are understood best. The only systems that have so far shown agreement between experiment and theoretical predictions, and which involve large numbers of degrees of freedom, are largespin magnetic molecules. Those that have been tested are the V15 molecule (Bertaina et al., Nature 2008), and the Fe8 molecules (Takahashi et al., preprint about to be issued); in both cases, experiment agrees with theoretical prediction to within a relatively small experimental error. The Fe8 molecule has over 10^{50} degrees of freedom in the nuclear bath; the lowT quantum dynamics of this system is entirely governed by the coupled dynamics of the electron spins with these nuclear spins, with the phonon bath, and with other molecules (with photons playing a secondary role).
In unpublished work the BertainaBarbara group has now also checked out the role of dipolar interactions between the V15 molecules, by varying the distance separating the molecules. Theory and experiment still agree. In both of these systems (and also in related systems like the Erbium tungstenates, or the LiHoF system, where one deals with a large Rare Earth spin, and one also has a very good handle on the experimental systems [here the number of degrees of freedom is much smaller however]), one can therefore look for a key signature of ‘intrinsic decoherence,’ where it is most likely to show up: in the dynamics of decoherence once entanglement has been set up between 2 or more of these molecules.
There as yet are no theoretical works, with or without predictions, exploring this important hypothesis. So the first step would be to give a quantitative analysis of what one would expect in the coupled dynamics of such entanglement experiments. This would require a calculation of the coupled dynamics of the 2 molecules; these couple to each other purely via magnetic dipolar interactions (very well understood) and each couples to nuclear spins in their surroundings (all the nuclear species are known, as are all the relevant hyperfine couplings, to very high accuracybetter than one part in 10^3 in most cases). There is also the coupling to photons (understood exactly) and to phonons (we know this very well for V15, for Fe8, and for the LiHo system, because of existing very thorough studies).
These calculations would predict the timecorrelations of the coupled molecules, and then the prediction of what would be seen in Rabi experiments, ESR experiments, and in spin echo experiments. At the same time it would be terribly useful to do NMR on the nuclear spins, to check that they were behaving as expected (the nuclear spins cause almost all the decoherence, and while they are doing this their dynamics is strongly modified).
The experimental testing of ideas of intrinsic decoherence in Nature requires measuring the timedependent entanglement between the molecules or rareearth spins. The main problem here is that no single experimental group possesses all the apparatus to do these experiments, which work at quite different frequencies. What typically happens in such a situation is that the different experiments are done in different research centers by one collaboration, with different students or postdocs working in the different centers. Thus the ESR and Rabi experiments could be done in one center, and the spin echo and NMR experiments in another).
More detail on the experimental work will follow once the theoretical studies have made it clear exactly what has to be measured. However it is already clear that separate experiments will be necessary at microwave (120 GHz) and ESR (100300 GHz frequencies), as well as measurements of T_1 and T_2 on the nuclear spins. These may have to be supplemented by measurements of spinphonon couplings. No equipment costs are anticipated, although sometimes if large facilities are being used—for example, to do ESR and spin echo experiments at low T (below 50 mK) and high magnetic field (around 10T)—one may need to use large facilities, and there may be extra costs involved if the group does not have user privileges.
PHILOSOPHICAL IMPLICATIONS
In recent wellregarded interpretations of quantum physics that explore various mechanisms of phase decoherence, including the consistent histories approach of Robert Griffiths (1984, 2002) and the work of Roland Omnès (1994), we have seen careful investigations into the physical (i.e., not “merely philosophical”) distinction between the order of contingent causal relation and the order of necessary logical implication. Of particular import are recent experiments on precessional decoherence in spin bath dynamics which, unlike oscillator bath and other environmental decoherence models, entails no energy transfer between the bath and the measured system. Thus the conventional description of decoherencegenerating systemenvironment interactions, via an effective Hamiltonian, is arguably incomplete. This project focuses on the function of bivalent propositional logic in describing intrinsic decoherence at the microscale, and explores the implications for complex adaptive systems theory at the macroscale (e.g., the ‘emergence’ of classical mechanics from quantum mechanics) as given in the work of CPNS Fellow Stuart Kauffman, Professor of Biological Sciences and Physics, and Director, Institute for Biocomplexity and Informatics (IBI), University of Calgary.
The PI has argued that nondissipative, intrinsic decoherence can be described in terms of logicalcausal quantum dynamics; that is, the logicalcausal order presupposed by the standard formalism (trace over of the density matrix, the decoherence functional, etc.) can be seen as a necessary presupposition of the physical dynamics, such that thirdparty decoherence can be seen as a reflection of this presupposition. Indeed, since thirdparty decoherence pertains to any quantum measurement interaction where both the system and tracedover environment are coconditioned, the appeal to dynamical logical causality would account for the current experimental difficulty in wholly eliminating decoherence from quantum measurement (Zurek 2003, 715775).
In the broadest sense, quantum theoretical descriptions of the measurement of ‘objects’ by ‘subjects’ always yields a linear superposition of possible objective states; yet the actual measurement interaction always terminates with a unique ‘measured object’ in a definite state. Nondissipative decoherence can be understood as that aspect of the dynamics whereby the logical principles of NonContradiction (PNC) and the Excluded Middle (PEM) are always satisfied in the practice of quantum mechanics, without being in any way accounted for by the quantum theory itself.
The description of the logical structure of quantum theory given above emphasizes the importance in conventional orthodox quantum theory of Process 1 interventions and the phenomenon of nondissipative decoherence with which these interventions can be associated. As discussed above, they are interventions from outside the scope of the effective Hamiltonian—that is, beyond the dynamics given by the known mathematically described physical processes. The effects of these logically conditioned ‘interventions’ (as described by von Neumann) are specified by the orthodox vN rules, but the process that fixes the selected projection operator P is not specified by any yetknown law or rule. The principle of the causal closure of the physical is, as evinced by the phenomenon of intrinsic ‘logicalrelational’ decoherence, not validated by the known rules of contemporary quantum physics.
It is clear, then, that the logical presuppositions and implications underlying the mathematical formalism by which quantum decoherence is typically described, must be further explored. CoInvestigator David Finkelstein has, to this end, shown that the relation between the logical and causal orders in quantum measurement is fully illustrated in the simplest model, Peano’s. This is based on a successor operation ι converting any integer “moment” to the next, n to ι n = n + 1. Peano later generalized ι to the unitsetgenerating operation ι in his set theory, converting any set s of any cardinality into the unit set ι s = {s}; we call this unition. The Peano causal order ι presupposes a logical order represented by the inclusion relation
holding between any set
regarded as defining a predicate or class of integers, and any subset s’of s (Finkelstein, 2002).
The quantum theory of Bohr and Heisenberg was the first physical theory to transcend the mechanical notion of absolute truth implicit in mathematics; Heisenberg called it ‘nonobjective.’ Like an integer, physical systems seem to have maximal descriptions. Unlike an integer, these are incomplete; every predicate has complementary ones. Bohr and Von Neumann respectively renounced and revised classical logic in formulating quantum theory. We see this as renouncing ontology (theory of being) for a praxiology (theory of acting); this is not an ‘interpretation’ of quantum theory but rather a ‘paraphrase.’ Since all actual observations make changes in the system beyond our control, we do not assume that a system has an absolute ontology, except as a singular limit
but only an absolute praxiology, a network of quantum processes represented by an operator algebra associated with the system.
Most quantum theory to date has retained the classical theory of the causal order and an absolute spacetime, projecting these prequantum concepts into the quantum microcosm in what has long been recognized as unphysical and probably a failure of the theorist's imagination. Such mixed quantum/classical field theories are structurally unstable and singular as well as false to actual practice. They challenge us to reconstruct the physical theory of the causal order based on explicit linkages with the logical order.
Just as classical unition ι (taken with union) generates classical set theory, a quantum
unition operator ι generates a quantum set theory rich enough for field theory. Like classical set theory, this quantum set theory comes with no manual for building a physical theory with its tools. This is provided by a correspondence principle generalizing Bohr’s, which is implicit in a suggestion by Irving Segal: Presentday singular physical theories are singular limits of a regular physical theory. Slight errors in the commutation relations have converted simple Lie algebras into nearby nonsimple ones.
This suggests that a suitable Lie algebraic (i.e. the algebra characterizing a physical theory’s transformations, as idealized in an infinitesimal limit) simplification can restore the hypothetical regular theory (i.e., a theory devoid of singularities which are denotive of a theory’s failure to give definite information.) This is an extension of canonical quantization; one may call it simplification quantization. One way to implement it is to move physical theories from their singular foundations in classical set theory onto the regular logical foundations of quantum set theory, which provides the necessary variety of simple Lie algebras. ‘Simplification quantization’ regularizes singularities that have eluded canonical quantization, while maintaining agreement with experiment. Simplification quantizations of gauge theory in general and of the gravitational theory of the causal order in particular are underway by Finkelstein and consultant Mohsen ShiriGarakani.
This hypothesis provides an origin for the important Lie algebras of quantum physics, including the Lorentz, Heisenberg, Poincaré, and unitary ones. The basic Lie algebras define the statistics of quantum aggregates. These then generate kinematical algebras—i.e., algebras characterizing all possible dynamical outcomes of a quantum system, as underwritten by the theory. Finally, the operators in kinematical algebras that are symmetries of organized modes like condensates make up the symmetry groups and Lie algebras. In this approach, there are no truly fundamental symmetries in nature (i.e., dynamics that do not fundamentally presuppose logical asymmetry). Empirical symmetries tell us about the symmetry of some organized substratum and are contingent upon that organization. Spacetime curvature and classical gravity can now be regarded as residual effects of the quantum noncommutativity of a simple spacetimeenergymomentum Lie algebra near the singular limit of classical spacetime.
The Dipolar Relational Realist Interpretation of Quantum Mechanics
(see Epperson and Zafiris, 2013)
This interpretation begins with Heisenberg’s suggestion that apart from its epistemic significance, there is a sense in which the wave function must be understood to entail at least some ontological significance; for the potentia it describes, while not physically 'actual,' are nevertheless ‘real’ to some extent given that their probability valuations yield ‘real’ physical outcomes. And indeed, Heisenberg would later insist upon the fundamental reality and function of potentia in this regard. For him, potentia are not merely epistemic, statistical approximations of an underlying veiled reality of predetermined facts; potentia are, rather, ontologically fundamental constituents of nature. They are things “standing in the middle between the idea of an event and the actual event, a strange kind of physical reality just in the middle between possibility and reality.” (1958, 41) Elsewhere, Heisenberg writes that the correct interpretation of quantum mechanics requires that one consider the concept of “probability as a new kind of ‘objective’ physical reality. This probability concept is closely related to the concept of natural philosophy of the ancients such as Aristotle; it is, to a certain extent, a transformation of the old ‘potentia’ concept from a qualitative to a quantitative idea.” (1955, 12)
The relational realist interpretation of quantum mechanics begins with this conception of ontologically significant potentia—‘real’ apart from their actualizations, but ‘nonactual’ until actualized quantum mechanically. Within that context, this interpretation incorporates foundational features of various theoretical programs that explicitly explore the phenomenon of quantum decoherence as a process integral to quantum mechanical actualization of potentia (i.e., ‘wave function collapse’): In particular, the work of Wojciech Zurek, Roland Omnès, Robert Griffiths, and Murray GellMann & James Hartle. A great deal of experimental work has been committed to the study of quantum decoherence in recent years, and it has become a robust topic of inquiry in physics. While there is as yet no empirically validated ‘generic’ model for decoherence, the basic features of the theory have been sufficiently established to warrant careful philosophical exploration. The dipolar relational realist interpretation is one such exploration.
By this interpretation, the quantum mechanical actualization of potentia is defined as a decoherencedriven process by which each actualization (in ‘orthodox’ terms, each measurement outcome) is conditioned both by physical and logical relations with the actualities conventionally demarked as ‘environmental’ or external to that particular outcome. But by the relational realist interpretation, the actualizationinprocess is understood as internally related to these ‘environmental’ data per the formalism of quantum decoherence. The concept of ‘actualization via wave function collapse’ is accounted for solely by virtue of these relations, and thus requires no ‘external’ physicaldynamical trigger—the Gaussian hits of GRW, acts of conscious observation, etc. By the relational realist interpretation, it is the physical and logical relations among quantum actualities (quantum ‘final real things’) that drives the process of decoherence and, via the latter, the actualization of potentia. In this regard, the relational realist interpretation of quantum mechanics is a praxiological interpretation; that is, these physical and logical relations are ontologically active relations, contributing not just to the epistemic coordination of quantum actualizations, but to the process of actualization itself.
The wave function / density matrix represents the totality of potential relations for that actualizationinprocess—a coherent superposition of both logical and illogical potential relations, represented by the diagonal and offdiagonal terms of the density matrix, respectively. The latter, for example, would represent relations violating the Principle of NonContradiction (PNC), the theoretical actualization of which has been famously represented by the concept of an ‘actual’ Schrödinger Cat, both alive and dead at the same time.
As described via von Neumann’s ‘Process 1’ the process of quantum mechanical actualization/state evolution entails a ‘reduction’ of this density matrix whereby the ‘illogical,’ offdiagonal terms are eliminated from the coherent superposition, rendering it ‘decoherent.’ The diagonal terms which survive this logical conditioning each represent a potential outcome actualization as before, but with an important new qualification: They are now valuated as probabilities and as such satisfy a second presupposed logical desideratum—the Principle of the Excluded Middle (PEM). Thus, the probable outcome states of the reduced density matrix are both mutually exclusive in satisfaction of PNC (i.e., at most, one will be actualized), and exhaustive in satisfaction of PEM (i.e., at least one will be actualized), since the probabilities for each possible outcome state must sum to unity.
Von Neumann’s nonunitary ‘Process 1’ evolution, as a formal aspect of environmental decoherence (Zurek, 2003), reflects a fundamental logical asymmetry underlying the symmetrical unitary evolution. In von Neumann’s nonrelativistic formulation the density operator ρ evolves in time, and ρ(t) represents the state of the system S at time t. The state S at time t is considered to exist over the subset of the set of spacetime points (x’, y’, z’, t’) for which t’= t. The quantum dynamical law of evolution asserts that for an isolated system S, ρ(t’) = exp –iH(t’t) ρ(t) exp iH(t’t), where H is the Hamiltonian operator, here assumed to be time independent. This dynamical law holds except at a discrete set of times at which Process 1 decoherence occurs, when the density matrix is reduced to a set of logical bivalent truth propositions derived from the logically conditioned relations between the system, detector, and environment (as reflected by the preferred/pointer basis). Each such proposition is associated with a pair of projection operators P and P’ = (1P), and is represented mathematically by the Process 1 action ρ à ρ’ = PρP + P’ρP’. The probability that a proposition PρP is actualized is Trace PρP/ Trace ρ.
Again, the probable outcome states of the reduced density matrix are both mutually exclusive in satisfaction of PNC and exhaustive in satisfaction of PEM, since the probabilities for each possible outcome state must sum to unity.
Perhaps most important, the explicit acknowledgement of PEM as a logical desideratum of quantum mechanics, presupposed by the very concept of probability as absolutely fundamental to the mechanics, obviates the need for some physical dynamical ‘mechanism’ that actualizes the final, unique outcome state from among the reduced matrix of probable states. The actualization of one probable state is presupposed by the logical, probabilistic nature of the mechanics and the mathematics by which the mechanics are described; the fact of a unique outcome need not (and indeed, logically cannot) be accounted for by the mechanics which necessarily presuppose it. Likewise, quantum mechanics cannot account for the existence of unique, actual, systemdetectorenvironment states prior to measurement, similarly presupposed by the theory. In the same way that we easily stipulate the actual existence of the systemdetectorenvironment as a presupposition for the very possibility of measurement, a unique actual outcome subsequent to measurement is similarly presupposed by quantum mechanical measurement. The fact that such measurement yields a set of probabilityvaluated outcome states alone guarantees the actualization of one of those states.
Put another way, quantum mechanics can no more account for the existence of unique actuality via some purely efficient ‘cause of wave function collapse’ than classical mechanics can account for the existence of matter via descriptions of motion and inertia. Unique actual existence characterized by logically conditioned causality—explicitly acknowledged in the relational realist interpretation—is a presupposition of both quantum and classical mechanics. The difference is that classical mechanics provided philosophers of the early modern period no readily discernable indication of how the order of physical causal relation correlated with the order of logical implication. The resulting philosophical proposals either attempted to reduce the logical order to the physical causal order (e.g., the philosophy of Locke), to reduce the causal order to the logical order (e.g., Spinoza), to depict the correlation of the logical and causal orders as a schematization by which we experience the otherwise transcendent ‘things in themselves’ (e.g., Kant), or to deny the necessary presupposition of either order (e.g., Hume).
Like classical mechanics, quantum mechanics raises the same issue and has generated analogous philosophical approaches: The GRW approach generally comports with the philosophy of Locke, the transcendent realist approaches of Bohr and Everett generally comport with the philosophy of Kant, etc. The advantage of the relational realist interpretation and its reliance upon the concept of logically conditioned decoherence is that it offers a more detailed proposal for how, precisely, the logical order correlates with the physicalcausal order as exemplified by modern quantum mechanics. It does so by way of describing quantum actualities, quantum ‘things in themselves,’ as fundamental becomings rather than fundamental beings. Quantum mechanics, when interpreted via those approaches that explicitly acknowledge the process of decoherence, exemplifies three primary features of these quantum actualizations:
1) They are fundamentally relational, not just in ad hoc epistemic terms of ‘measuring apparatus’ and ‘measured system’ but also at the ontological/substance level of quantum actualities, such that quantum mechanical actualities both internally and externally ‘environmental’ to ‘system’ and ‘detector’ are involved. In this way, all actualities within the closed system of the universe are considered in logical relation quantum mechanically, thus allowing for a coherent ontological (universal) interpretation.
2) These quantum mechanical relations are logically governed potential integrations. It is the explicit incorporation of these relations into logical equivalence classes, relative to a particular actualization, with its particular preferred basis, that provides sufficient degrees of freedom for a logical negative selection process. This process is represented mathematically by the trace over, elimination of offdiagonal terms, and by reduction to the reduced density matrix with its mutually exclusive and exhaustive probabilityvaluated potential outcome states.
3) The logical integrations of coherent, superposed potentia into the decoherent, mutually exclusive and exhaustive probable outcome states represented by the reduced matrix can be correlated with von Neumann’s Process 1; and likewise, the physical fact of unitary evolution to a unique outcome state can be correlated with his Process 2. Thus the logical features of Process 1 and the physical features of Process 2 are mutually implicative in every quantum mechanical actualization, and it is in this sense that every such actualization is a dipolar (logical and physical) relational ‘becoming.’
There have been two major criticisms of interpretations of quantum mechanics grounded in the concept of decoherence. The first is that they do not ‘physically account for’ wave function collapse—that is, the actualization of a unique outcome state from among the menu of probable outcome states represented by the reduced density matrix. One answer to this criticism was given above: namely that such actualization is a logical presupposition inherent in the fact that the potential outcome states represented by the reduced density matrix are probabilityvaluated outcomes, mutually exclusive (in satisfaction of PNC) and exhaustive (in satisfaction of PEM). It is because of these two logical desiderata that some actual outcome is guaranteed (by PEM) and that (by PNC) it will not be some actualized superposition—i.e., an actualized Schrödinger Cat. Thus the fact that quantum mechanics terminates in probabilities rather than unique actualities is no theoretical deficiency or evidence of ‘incompleteness.’ Nevertheless, the inability of decoherencebased interpretations to ‘account for actuality’ remains a source of criticism. This is likely driven in large measure by the fact that the ‘problem’ of wave packet collapse is an infamous one, and its solution by simple denial on logical grounds rings of sophistry for many physicists.
Regardless, the argument remains: First, it is ultimately unreasonable to suppose that quantum mechanics could ever ‘account’ for either 1) the fact of ‘actuality’ which it necessarily presupposes; or 2) the fact that this actuality is logically conditioned, which the theory also necessarily presupposes. Physicist Roland Omnès, whose approach to quantum mechanics can be said to fall within the dipolar relational realist category, puts it thus: “One may consider that the inability of the quantum theory to offer an explanation, a mechanism, or a cause for actualization is in some sense a mark of its achievement. This is because it would otherwise reduce reality to bare mathematics.” (494) Indeed, one could argue that it is typically when fundamental physics reaches beyond its proper task of describing nature and presumes to explain nature—i.e., account for its existence—that it encounters problems of philosophical incoherence.
Second, capitalizing on the logical features of quantum mechanics in the manner proposed by the various decoherencebased interpretations is in no way a sophistic maneuver given that these same logical features are unavoidably implicit in every aspect of the quantum theory—both the mathematics by which the theory is described, but also, equally important, in the logical nature of physical causality. Advocates of decoherencebased interpretations of quantum mechanics simply make use of logical principles that are already presupposed by the quantum theory and universally evinced in every scientific theory of physical causality. The only difference is that rather than merely stipulating the logical nature of physical causality (or worse, pretending that the scientific enterprise is not founded upon this stipulation as an article of faith), the decoherencebased interpretations explicitly acknowledge and capitalize upon the presupposition of logical causality, applying it mathematically to the ‘problem’ of wave function collapse.
Wojciech Zurek (2003), for example, referring to a paper by Richard Cox (Cox, R. T., 1946, Am. J. Phys. 14 113) emphasizes that the theory of probability as it is employed in quantum mechanics presupposes the laws of Boolean logic. Zurek writes:
Intuitively, this is a very appealing demand. Probability emerges as an extension of the twovalued logic into a continuum of the “degrees of certainty.” The assumption that one should be able to carry classical reasoning concerning “events” and get consistent estimates of the conditional degree of certainty leads to algebraic rules which must be followed by the measure of the degree of certainty.
This implies that an information processing observer who employs classical logic states and classical memory states which do not interfere will be forced to adopt calculus of probabilities essentially identical to what we have grown accustomed to. In particular, likelihood of c and b (i.e., “proposition c · b”) will obey a multiplication theorem:
μ (c · ba) = μ (cb · a) μ (ba) .
Above μ(ba) designates a conditional likelihood of b given that a is
certain. Moreover, μ should be normalized:
μ (ab) + μ (∼ ab) = 1 ,
where ~ a is the negation of the proposition a. Finally, likelihood
of c or b
(c ∪ b) is:
μ (c ∪ ba) = μ(ca) + μ(ba) − μ(c · ba) ,
which is the ordinary rule for the probability that at least one of two events will occur.
In short, if classical Boolean logic is valid, then the ordinary probability theory follows. We are halfway through our argument, as we have not yet established the connection between the μ’s and the state vectors. But it is important to point out that the assumption of the validity of Boolean logic in the derivation involving quantum theory is nontrivial. As was recognized by Birkhoff and von Neumann, (Birkhoff, G., and von Neumann, J., 1936, Ann. Math. 37, 823843) the distributive law a · (b∪c) = (a · b) ∪ (a · c) is not valid for quantum systems. Without this law, the rule for the likelihood of the logical sum of alternatives, Eqs. (26), (27) would not have held. The physical culprit is quantum interference, which, indeed, invalidates probability sum rules (as is well appreciated in the examples such as the double slit experiment). Decoherence destroys interference between the einselected states [states ‘superselected’ via their environmental relations]. Thus, with decoherence, Boolean logic, and, consequently, classical probability calculus with its sum rules are recovered… Thus, starting from an assumption about the validity of classical logic (i.e., absence of interference) we have arrived, first, at the sum rule for probabilities and, subsequently, at the Born’s formula. (1998, 1213)
The second major criticism of the decoherencebased approaches is that although the phenomenon of quantum decoherence can be and has been rigorously studied in the laboratory setting, it remains unclear what, precisely, generates decoherence—that is, what are the physical relata that generate the required degrees of freedom necessary for logical integration and negative selection of the offdiagonal terms? Typically, decoherence is understood to be ‘induced’ by phase correlations between system and ‘environment.’ Spin baths and oscillator baths are two types of experimental arrangements that have been employed to test environmental decoherence. The difficulty is that a number of experiments have yielded decoherence rates that far exceed those predicted by the usual environmental decoherence models—i.e., those restricted to ‘external’ physical interactions.
This has led some theorists to explore the notion of intrinsic or ‘internally environmental’ relata that, when added to externally environmental relations, might account for the observed decoherence rates. Philosophically, this idea of ‘intrinsic’ sources of decoherence implies the possibility of a substancedefinitive conception of decoherence such as that proposed by the relational realist interpretation of quantum mechanics—sources that can be described ontologically as Nature’s ultimate constituent ‘final real things.’ The relational realist depiction of the latter as quantum mechanical ‘becomings,’ discussed above, is certainly compatible with the physical theory of ‘intrinsic decoherence.’
CoInvestigator P.C.E. Stamp writes:
By ‘intrinsic’ sources [of decoherence in Nature] is meant sources which are inevitable in the world as it is, not arising from dissipative processes and perhaps even arising as part of the basic structure of the universe.
Such intrinsic sources of decoherence in Nature, operating even at T=0, would not only provide a way of explaining the ‘emergence of classical physics’ in fields ranging from quantum cosmology to condensed matter physics; they would also place a fundamental limit on the observability of quantum phenomena. This would limit the possibility of seeing macroscopic quantum phenomena, and also place fundamental limits on the superpositions required for quantum computing.
Possibilities for intrinsic decoherence mechanisms have already emerged from both low and highenergy physics. From lowenergy physics there has been a suggestion that zero point modes of continuous quantum fields (in particular, the photon field) could cause T=0 decoherence. This has, for example, been suggested as an explanation of the decoherence saturation at low T in mesoscopic conductors (Mohanty et al., 1997)… (490)
To the extent that the decoherencebased interpretations of quantum mechanics are at least sufficiently developed to have generated rigorous experimental testing, likewise the philosophical implications of the general principles of the se interpretations are equally worthy of careful exploration. In Epperson 2004, I proposed that the philosophical innovations inherent in the decoherencebased interpretations correlate closely with those proposed by Alfred North Whitehead in Process and Reality. It must be emphasized, however, that my exploration of these correlations was and is not intended as an ‘explanatory’ scheme by which either Whitehead’s metaphysics or the quantum theory can be ‘properly’ understood, each in terms of the other. What I explore, rather, is simply the proposition that the fundamental features of Whitehead’s speculative metaphysical scheme and his conception of dipolar actuality can be seen as exemplified in those interpretations of quantum mechanics that make use of the decoherence effect. Circularity of validation—whether the physics is to be understood as validating the metaphysics or vice versa—is avoided by acknowledging, in a speculative philosophical context, that the first principles common to both are necessarily presupposed within the proposition and thus incapable of simple proof by deduction or demonstration. These first principles, both logical and ontological, constitute the starting point for exploration, not the end point of explanation.
But beyond merely exploring this proposition, I do attempt to argue for its fitness to the task of interpreting quantum mechanics. I offer this argument in the same speculative philosophical spirit in which Whitehead argued for the fitness of his metaphysical scheme to the task of understanding (though not ‘explaining’) nature—not by the ‘provability’ of his first principles via deduction or demonstration, but by their evaluation against the metrics of coherence and empirical adequacy.
In the most general terms, both decoherencebased interpretations and relational realist philosophy depict the following:
1. Fundamental substance defined as quantum facts whose actualization is predicated upon internal relations with an environment of antecedently settled quantum facts—the data of the settled world. These relations are both causalphysical, and logicalconceptual in that the physical relations are, via the process of quantum decoherence, logically conditioned and thus productive of an integrated objectification. Thus each quantum actualizationoffact, when considered as a substantial ‘thinginitself’ evinces both a physicalcausal pole and a logicalconceptual pole. The term ‘dipolar’ signifies the fact that the physical and logical features of a quantum mechanical becoming are mutually implicative in quantum mechanical actualizations.
2. The internal relations with the dative environment are logically integrated, first into a ‘pure state’ comprising superdenumerable potential outcome states. These integrations are then further integrated into coarsegrained equivalence classes. A negative selection process conditioned by the logical principle of NonContradiction and fuelled by the massive degrees of freedom yielded by environmental relations (both physicaldissipative and logical nondissipative), eliminates potentia logically incapable of integration. This is represented by the cancellation of offdiagonal terms and the evolution of the density matrix to the reduced state.
3. This integration, described by von Neumann’s Process 1, results in a probability ‘valuation’ of the remaining potential outcome states. By the Principle of the Excluded Middle, one of these probabilityvaluated potential outcome states/subjective forms will be actualized, in accord with its valuation—i.e., its probability amplitude.
When actualized, the occasion has its causal efficacy upon subsequent actualizations; and likewise, its process of actualization is affected by both 1) its causal physical relations with the actualities ‘physically’ prior to it in terms of spatiotemporal extensiveness—i.e., within its backward lightcone, per the restrictions of relativity theory. Physical antecedence is reflected, for example, in the statement ‘p causes q’; and 2) its logical relations with those actualities ‘logically’ prior to it, per the restrictions of the Principle of NonContradiction, among other logical restrictions. Logical antecedence is reflected in the statement ‘p then q.’
Each actual occasion is thus fundamentally a unit of relation. In the process of actualization, the becoming occasion is internally related to its dative world of antecedently actualized quantum facts, and these relations are both causally and logically integrated; and since the actualization is internally related to its dative world, the relations form potential histories subsuming both the becoming quantum fact and its dative world.
Thus, another philosophically problematic conceptual pair, ‘unity’ and ‘diversity’ are also brought into coherence via mutual implication. “The many,” writes Whitehead, “become one, and are increased by one. In their natures, entities are disjunctively ‘many’ in process of passage into conjunctive unity.” (21) These integrations are always logically governed, such that upon actualization via decoherence, the quantum fact is related to the world in a manner free of violations of the Principle of NonContradiction, or any other such violation of the logical order. Writ large, the universe is thus described as a networked system of serial routes or ‘histories’ (Griffiths, 1984 and 2002) of quantum facts; the integrative internal relations of every actualization constitutive of each route are logically governed such that the orders of causal relation and logical implication are correlated (again, this is a speculative presupposition grounded in the concept of the dipolar actual occasion).
Those interpretations of quantum mechanics that make use of the decoherence effect are unique in their reliance upon the explicit operation of two categories of first principles, ontological and logical. The ontological first principle is that which categorizes actuality and potentiality as two species of reality—a long overdue rehabilitation of Aristotle’s signature improvement of the Parmenidean worldview, which depicted ‘becoming’ as pure illusion. The logical first principles are PNC and PEM, without whose presupposition the correlation of causal relation and logical implication would remain wholly unfounded. Science requires that these conclusions follow both causally and logically from premises and not merely by conjunction, either random or constant; quantum mechanics, by the Heisenberg uncertainty principle, requires that the final outcome state be not only subsequent to the evolution but causally and logically consequent of it.
From the Emergence of Classicality
To the Emergence of Complex Adaptive Systems
In collaboration with CoI and CPNS Fellow Stuart Kauffman, Professor of Biological Sciences and Physics, and Director, Institute for Biocomplexity and Informatics (IBI), University of Calgary, we will examine the function of bivalent propositional logic in describing intrinsic decoherence at the microscale, and explore the implications for complex adaptive systems theory at the macroscale (e.g., the ‘emergence’ of classical mechanics from quantum mechanics).
We will investigate the ways in which Kauffman’s work on biological adaptive complexity might find a robust philosophical and physical foundation in the relational realist approach to quantum logical causality—a modern rehabilitation of the process eventontology of Whitehead. Among the topics to be explored will be the relationship between the Whiteheadian spacetime mereotopology described by the relational realist interpretation, and possible topological models describing Kauffman’s conception of evolving selective complexity in nature.
More broadly, we will undertake the development of a rigorous philosophicalphysical model that accommodates both 1. the phenomenon of natural selforganization (cf. the Kauffman Models); and 2. the phenomenon of natural selection. Though there are interpretations of quantum mechanics that can be applied to the task of modeling selforganization (i.e., complexity) in nature, there are as yet no interpretations that can adequately accommodate the phenomenon of selective complexity exemplified by Darwinian evolution. And likewise, though Darwinism offers a robust, empirically validated model for natural selection, it does not accommodate the phenomenon of selforganization. Kauffman thus writes that we must seek to “broaden evolutionary theory to describe what happens when selection acts on systems that already have robust selforganizing properties. This body of theory simply does not exist.”
Epperson suggests that the logicalcausal, praxiological formalism of the relational realist interpretation of quantum mechanics might provide a basic framework for such a theory—particularly when explored in the context of Whitehead’s Philosophy of Organism. The latter entails a rigorous schematization of both natural selforganization and natural selection in terms of fundamental relational, eventontological processes; and recent work (Epperson 2004) has shown that the formalism by which Whitehead describes these processes is precisely reflected in modern, decoherencebased interpretations of quantum mechanics (cf. Robert Griffiths, 1984, 2002; Roland Omnès, 1994, and Murray GellMann, 1997.) A key goal of the relational realist program is to develop a descriptive scheme by which both these quantum mechanical features of nature and its selforganizing selective complexity are accommodatedboth in terms of philosophical coherence and empirical adequacy.
APPLICATIONS
A CategoryTheoretic Mereotopological Model of Quantum Spacetime
See the following project publications:
E. Zafiris, A. Mallios, “The Homological KählerDe Rham Differential Mechanism, Part I: Application in General Theory of Relativity,” Advances in Mathematical Physics (2011)
E. Zafiris, A. Mallios, “The Homological Kählerde Rham Differential Mechanism, Part II. SheafTheoretic Localization of Quantum Dynamics,” Advances in Mathematical Physics (2011)
M. Epperson, E. Zafiris, Foundations of Relational Realism: A Topological Approach to Quantum Mechanics and the Philosophy of Nature. Lexington Books / Rowman & Littlefield, New York (2013)
The quantum decoherent histories formalism, in its pathintegral form, provides a spacetime formulation of quantum theory that is highly compatible with the mereotopological model of spatiotemporal extension proposed by Alfred North Whitehead. This is crucial because the mathematical rigidity of the Hilbert space (as a topological vector space) does not allow a relativization analogous with the one of classical relativity theory on smooth manifolds. By contrast, a mereotopological/categorytheoretic reformulation of quantum logic in terms of Boolean localization systems (Booelan sheaves, per the work of CoI Elias Zafiris) achieves precisely such an objective by generalizing the smooth manifold construction in generic algebraic/categorical terms.
This makes it possible to formulate a framework of local/global or part/whole relations without the intervention of a spacetime classically conceived. On the contrary, the usual spacetime manifold and its metrical relations (imposing extra conditions like the lightcone causality relations) appear as emergent at a higher level than the more fundamental level of logical and algebraic partwhole relations. Epperson’s distinction between a) mereological/topological/logical relations, and b) physical/metrical/causal relations, is reflected precisely in Zafiris’ distinction between these two different levelsthe algebraic partwhole relations and the metrical spacetime relations, respectively where the latter can be seen as an emergent/metrical specialization of the former. The key issue to be explored is the problem of localization and the problem of passing from the local to the global in an extensive continuum.
Note that these problems are not metrical but mereotopological. The emergent metrical relations of classical relativity theory presuppose a pointwise localization on a smooth manifold and the metric is a (local) expression of the simultaneity conventions imposed by the constancy of the speed of light. But in the quantum theoretic level, the assumption of pointwise localization of events is not feasible unless a measurement context has been specified and also a specific type of measurement has been performed.
In Whitehead's language this is reflected in the distinction between genetic division (presupposing a generic/algebraic type of localization) and coordinate division (like the one of the classical spacetime manifold endowed with a semiRiemannian metric and dictating the lightcone causality relations). Since now we can prove that the latter is an emergent form of the more fundamental former division, there is no tension between the fundamental mereological order of the extensive continuum (modeled in terms of CoI Elias Zafiris’s sheaftheoretic topos
model) and the more special spatiotemporal causal extensive order pertinent to a pointwise localized and metricized continuum. This has fundamental consequences for the interpretation of the mechanism of differential extensive analysis, which is crucial for physics since it captures the dynamical relations in an extensive continuum of events.
In Process and Reality and other works, Alfred North Whitehead developed the basic conceptual framework for this mereotopological understanding of spacetime, which he termed ‘The Theory of Extensive Abstraction.’ The formal categorical/algebraic formulation we propose herein, however, permits us to refine and integrate these ideas into modern quantum theory via, in particular, the decoherent histories formalism.
A Topological, SheafTheoretic Explication of Quantum Geometric Phases
By Analysis of Experimental Data on the AharonovBohm Effect, the Pancharatnam Phase, and the Quantum Hall Effect, Toward a Unified Interpretation
White Paper 

Current Publication: E. Zafiris, "The Global Symmetry Group of Quantum Spectral Beams and Geometric Phase Factors," Advances in Mathematical Physics (2015)
Foundations of Relational Realism (Lexington Books / Rowman & Littlefield, 2013) represents the capstone of our initial project, along with a number of published papers and conference presentations. With this foundational work in place, our next step is to demonstrate the experimental applicability of this sheaf theoretic quantum formalism and its philosophical conceptual framework—viz. its advantages both in terms of prediction and interpretation of data. To that end, for 201315, we propose to apply the relational realist framework to the task of explicating the wellknown but poorly understood problem of quantum geometric phases. We will do so by analysis of experimental data on the AharonovBohm Effect, the Pancharatnam Phase, and the Quantum Hall Effect, toward a unified interpretation of all three.
"Knowledge of the classical electromagnetic field acting locally on a particle is not sufficient to predict its quantummechanical behavior... For a long time it was believed that A [the vector potential] was not a ‘real’ field... There are phenomena involving quantum mechanics which show that in fact A is a ‘real’ field in the sense that we have defined it... E and B [electromagnetic fields] are slowly disappearing from the modern expression of physical laws; they are being replaced by A [the vector potential] and [the scalar potential].”
Richard Feynman
The Feynman Lectures on Physics
"We believe that the concept of a geometric phase, repeating the history of the group concept, will eventually ﬁnd so may realizations and applications in physics that it will repay study for its own sake, and become part of the lingua franca."
A. Shapere and F. Wilczek
In a groundbreaking paper published in the mid1980’s, Sir M. Berry discovered that a quantum system undergoing a slowly evolving (adiabatic) cyclic evolution retains a “memory” of its motion after coming back to its original physical state. This “memory” is expressed by means of a complex phase factor in the wavefunction of the system, called Berry’s phase or the geometric phase. The main idea is that a quantum system in a slowly changing environment displays a history dependent geometric effect: When the environment returns to its original state, the system also does, but for an additional phase.
The Berry phase is a complex number of modulus one and is experimentally observable. The two most important properties of the geometric phase are [1] that it is a statistical object, and [2] it can be measured only relatively. Thus it becomes observable by comparing the evolution of two distinct statistical ensembles of systems through their interference pattern. The Berry phase is called ‘geometric’ because it depends solely on the topology of the pathway along which the system evolves and neither on the temporal metric duration of the evolution nor on the dynamics that is applied to the system.
After Berry’s initial experimental discovery of the geometric phase, it has been demonstrated that it also exists for nonadiabatic evolutions and even for sequences of measurements. All these experimental observations of the geometric phase phenomenon, including the AharonovBohm, Pancharatnam, and Quantum Hall effects—as well as features of molecular and nuclear spectra, vortices occurring in superfluid helium, and even chemical reactions—help to emphasize its purely topological nature. In this way, the geometric phase observable initiated a tremendous surge of experimental research across a diverse range of physics disciplines establishing surprising connections among a number of apparently disparate phenomena—again, viz. the AharonovBohm effect, its molecular physics analogue by Mead and Truhlar, polarization optics effects, and the Quantum Hall effect. Thus, we expect that a unified topological approach to the study, description and interpretation of all these experimentally wellestablished geometric phase phenomena will shed light on their nature, lead to predictions of new effects of a similar type, and even provide a paradigm for applications in areas beyond the strict domain of natural sciences.
The novel topological approach to quantum mechanics we present in Foundations of Relational Realism, in the context of our overall Fetzer research project publications, provides a promising candidate for evaluating consistently the experimental data of geometric phases observed in all the above experiments. Such an evaluation would demonstrate our work’s applicability to diverse quantum phenomena, explicated via the lens of a unifying topological theoretical framework, which is based on the powerful modern mathematical methods of category theory and sheaf theory.
The application of our topological formalism to the analysis of experimental data, carrying with it an associated unifying realistic interpretation of geometric phase phenomena, thus constitutes a natural continuation and experimental substantiation of our previous research program. The basic principle underlying the crucial explanatory role of this approach in relation to geometric phases is the following: Whenever a global physical system is partitioned into local parts and one attempts to describe a subsystem in isolation, the influence and connectivity of the others is manifested through geometric phase effects of a pure topological origin.
The pervasiveness throughout the natural sciences of this partwhole methodology accounts for the ubiquity of the geometric phase effect, but not its explanation. We propose to solve this problem via our realistic mereotopological formalism and conceptual framework. To that end, the precise mathematical notion which captures the topological origin of geometric phases is the anholonomy of a connection on a sheaf modeling the structure of events. The notion of a sheaf connection provides the technical means for describing the process of parallel transport of the state vector of a system along a curve on the space of the control variables. The particular transformation undergone by the state vector when it is paralleltransported along a closed curve is called the anholonomy of the sheaf connection. Thus, the anholonomy describes the state vector transformation induced by cyclic changes (loops) in the controlling variables. A simple intuitive example from macroscopic geometry is provided by the rotation of a vector when paralleltransported along a closed path on a curved surface. The topological nature of the effect is realized by the fact that if the parallel transport of a vector takes place along a closed path on a plane, the vector comes back unchanged; whereas if it takes place along a closed path on a sphere it gets rotated by an angle, which is measured precisely by the anholonomy of the connection.
Sample of Experiments Analyzed
Yano, S. and Yamada, H. (1986). “Evidence for AharonovBohm Effect with Magnetic Field Completely Shielded from Electron Wave” Physical Review Letters, 56 (8): 792795
Osakabe, N; et al. (1986). “Experimental confirmation of Aharonov–Bohm effect using a toroidal magnetic field confined by a superconductor”. Physical Review A 34 (2): 815–822.
Webb, RA; Washburn, S; Umbach, CP; Laibowitz, RB (1985). “Observation of h/e Aharonov–Bohm Oscillations in NormalMetal Rings”. Physical Review Letters 54 (25): 2696–2699
Schönenberger, C; Bachtold, Adrian; Strunk, Christoph; Salvetat, JeanPaul; Bonard, JeanMarc; Forró, Laszló; Nussbaumer, Thomas (1999). “Aharonov–Bohm oscillations in carbon nanotubes”. Nature 397 (6721): 673.
van Oudenaarden, A; Devoret, Michel H.; Nazarov, Yu. V.; Mooij, J. E. (1998). “Magnetoelectric Aharonov–Bohm effect in metal rings”. Nature 391 (6669): 768.
Pancharatnam, S. Proc. Indian Acad. Sci. A44, 247−262 (1956); reprinted in Collected Works of S. Pancharatnam (Oxford Univ. Press, 1975)
Anandan, J. “The Geometric Phase,” Nature 360, 307  313 (26 November 1992)
Tomita, A. & Chiao, R. Y. “Observation of Berry's Topological Phase by Use of an Optical Fiber” Phys. Rev. Lett. 57, 937−940 (1986)
Hsieh, D.; Qian, D.; Wray, L.; Xia, Y.; Hor, Y. S.; Cava, R. J.; Hasan, M. Z. (2008). “A topological Dirac insulator in a quantum spin Hall phase”. Nature 452 (7190): 970–974.
Baumgartner, A.; Ihn, T.; Ensslin, K.; Maranowski, K.; Gossard, A. (2007). “Quantum Hall effect transition in scanning gate experiments”. Physical Review B 76 (8)
References
Aharonov, Y. & Bohm, D. Phys. Rev. 115, 485−491 (1959). 
Berry, M. V. Proc. R. Soc. A392, 45−57 (1984). 
Aharonov, Y. & Anandan, J. Phys. Rev. Lett. 58, 1593−1596 (1987). 
Anandan, J. & Aharonov, Y. Phys. Rev. D38, 1863−1870 (1988). 
Pancharatnam, S. Proc. Indian Acad. Sci. A44, 247−262 (1956); reprinted in Collected Works of S. Pancharatnam (Oxford Univ. Press, 1975). 
Anandan, J. & Stodolsky, L. Phys. Rev. D35, 2597−2600 (1987). 
Anandan, J. Phys. Lett. A129, 201−207 (1988). 
Kugler, M. & Shtrikman, S. Phys. Rev. D37, 934−937 (1988). 
Hannay, J. H. J. Phys. A18, 221−230 (1985). 
Berry, M. V. J. Phys. A18, 15−27 (1985). 
Berry, M. V. & Hannay, J. H. J. Phys. A21, L325−L331 (1988). 
Berry, M. V. J. mod. Opt. 34, 1401−1407 (1987). 
Ramaseshan, S. & Nityananda, R. Current Science 55, 1225−1226 (1986). 
Samuel, J. & Bhandari, R. Phys. Rev. Lett. 60, 2339−2342 (1988). 
Simon, B. Phys. Rev. Lett. 51, 2167−2170 (1983). 
Herzberg, G. & LonguetHiggins, H. C. Disc. Farad. Soc. 35, 77−82 (1963). 
Stone, A. J. Proc. R. Soc. Lond. A351, 141−150 (1976). 
Mead, C. A. & Truhlar, D. G. J. chem. Phys. 70, 2284−2296 (1979). 
Moody, J., Shapere, A. & Wilczek, F. in Geometric Phases in Physics (eds Shapere, A. & Wilczek, F.) 160−183 (World Scientific, Singapore, 1989). 
Bitter, T. & Dubbers, D. Phys. Rev. Lett. 59, 251−254 (1987).  
Suter, D., Chingas, G. R. Harris & Pines, A. Molec. Phys. 61, 1327−1340 (1987). 
Tycko, R. Phys. Rev. Lett. 58, 2281−2284 (1987). 
Suter, D., Mueller, K. T. & Pines, A. Phys. Rev. Lett. 60, 1218−1220 (1988). 
Chiao, R. Y. & Wu, Y. Phys. Rev. Lett. 57, 933−936 (1986). 
Tomita, A. & Chiao, R. Y. Phys. Rev. Lett. 57, 937−940 (1986). 
Berry, M. V. Nature 326, 277−278 (1987). 
Rytov, S. M. Dokl. Akad. Nauk. XVIII, 263 (1938); reproduced in Topological Phases in Quantum Theory (eds Markovski, B. & Vinitsky, S. I.) (World Scientific, Singapore, 1989). 
Haldane, F. D. M. Phys. Rev. Lett. 59, 1788 (1987). 
Geometric Phases in Physics (eds Shapere, A. & Wilczek, F.) (World Scientific, Singapore, 1989). 
Zwanziger, J. W., Koenig, M. & Pines, A. A. Rev. phys. Chem. 41, 601−646 (1990). 



WORKS CITED AND BIBLIOGRAPHY:
Aristotle, and McKeon, Richard. 1941. The basic works of Aristotle. Random House.
Bohm, David. 1952, Phys Rev. 85: 166,180.
Bohm, David, Hiley, B.J. 1993. The Undivided Universe: An Ontological Interpretation of Quantum Theory. London: Routeledge.
Bohr, Niels. 1949. “Discussion with Einstein,” in Albert Einstein: PhilosopherScientist, Paul Arthur
Schilpp, ed. New York: Harper, 210.
_____. 1958. Atomic physics and human knowledge. New York: Wiley.
Caldeira, A. & Leggett, A. (1983). “Quantum tunneling in a dissipative system.” Annals of Physics, 149: 374456
Cox, R. T., 1946. Am. J. Phys. 14 113.
De Broglie, N. 1923. “Recherches sur la theorie des Quanta.” University of Paris, 1924. English translation published as “Phase Waves of Louis de Broglie.” Am. J. Phys. vol. 40 no. 9, pp. 13151320, September, 1972
Epperson, Michael & E. Zafiris (2013) Foundations of Relational Realism: A Topological Approach to Quantum Mechanics and the Philosophy of Nature. New York: Lexington Books / Rowman & Littlefield.
Epperson, Michael (2004.) Quantum mechanics and the philosophy of Alfred North Whitehead. American philosophy series, no. 14. New York: Fordham University Press.
_____. 2009. “Relational Realism: The Evolution of Ontology to Praxiology in the Philosophy of Nature.” World Futures, 65,1:1941
_____. 2009. “Quantum Mechanics and Relational Realism: Logical Causality and Wave Function Collapse”. Process Studies 38:2
Everett, Hugh. 1957. “‘Relative State’ Formulation of Quantum Mechanics.” Rev. Mod. Phys. 29: 454462
GellMann, Murray, Hartle, James. 1994. "Strong Decoherence" Contribution to the Proceedings of the 4th Drexel Symposium on Quantum NonIntegrabilityThe QuantumClassical Correspondence, Drexel University
GellMann, Murray. 1994. The Quark and the Jaguar: Adventures in the Simple and the Complex. New York: W.H. Freeman and Company
Ghirardi, G. C., Rimini, A., Weber, T. (1986). “Unified dynamics for microscopic and macroscopic systems”, Phys. Rev. D 34, 470491
Ghirardi, G. C., Grassi, R., & Rimini, A. (1990). Continuousspontaneousreduction model involving gravity. Physical Review A, 42, 1057–1064.
Ghirardi, G. C., Pearle, P., & Rimini, A. (1990). Markov processes in Hilbert space and continuous spontaneous localization of systems of identical particles. Physical Review A, 42, 78–89.
Ghirardi, G.C. 2004. “Sneaking a look at God’s cards” in Unraveling the mysteries of quantum mechanics. Princeton University Press: 406
Griffiths, Robert J. 1984. Stat Phys. 36: 219.
_____. 2002. Consistent quantum theory. Cambridge: Cambridge University Press.
Hartle, J. and Hawking, S. 1983. “The Wave Function of the Universe.” Physical Review D 28: 29602975
Heisenberg, Werner. 1955. “The Development of the Interpretation of the Quantum Theory” in Niels Bohr and the Development of Physics, Wolfgang Pauli, ed. New York: McGrawHill, 12
_____. 1958. Physics and Philosophy. New York: Harper Torchbooks
Mohanty, P., Jariwala, E.M.Q. and Webb, R.A., 1997 “Intrinsic decoherence in mesoscopic systems,” Physical Review Letters 78: 3366–3369.
Myatt, C. J., King, B. E., Turchette, Q. A., Sackett, C. A., Kielpinski, D., Itano, W. M., et al. 2000. “Decoherence of quantum superpositions through coupling to engineered reservoirs.” Nature, 403, 269–273.
Omnès, Roland. 1994. The Interpretation of Quantum Mechanics. Princeton: Princeton University Press.
Plato, and John Henry McDowell. 1973. Theaetetus. Clarendon Plato series. Oxford: Clarendon Press
Stamp, P.C.E. 2006. “The Decoherence Puzzle” Studies in History and Philosophy of Modern Physics 37:490
Stapp, Henry P. 2007. Mindful universe: quantum mechanics and the participating observer. The frontiers collection. Berlin: Springer.
’t Hooft, G. (1999). Quantum gravity as a dissipative deterministic system. Classical and Quantum Gravity Class, 16(10), 3263–3279.
’t Hooft, G. (2001, May 11). Quantum mechanics and determinism. hepth/0105105, Retrieved February 18, 2006 from hhttp://arxiv.org/abs/hepth/0105105i.
Von Neumann, John. 1955. Mathematical Foundations of Quantum Mechanics. Princeton: Princeton University Press
Whitehead, Alfred North. 1929. Process and Reality: An Essay in Cosmology. Cambridge University Press. (Corrected Edition, D. Griffin, D. Sherburne, ed. New York: Free Press, 1978.)
Wigner, E. 1961. “Remarks on the mindbody problem” in The Scientist Speculates, I.J. Good, ed. London: Heinemann
_____. 1967. Symmetries and Reflections. Bloomington: Indiana University Press.
Zurek, Wojciech. 1991. “Decoherence and the Transition from the Quantum to the Classical” Physics Today, 44, 10:36
_____. 1998. “Decoherence, einselection, and the existential interpretation.” Phil.Trans.Roy.Soc.Lond. A356:17931820
_____. 2003. “Decoherence, einselection, and the quantum origins of the classical.” Reviews of Modern Physics, 75:715–785.
E. Zafiris, A. Mallios, “The Homological KählerDe Rham Differential Mechanism, Part I: Application in General Theory of Relativity,” Advances in Mathematical Physics (2011)
E. Zafiris, A. Mallios, “The Homological Kählerde Rham Differential Mechanism, Part II. SheafTheoretic Localization of Quantum Dynamics,” Advances in Mathematical Physics (2011)
Zafris, E. and J. J. Halliwell, `Decoherent Histories Approach to the Arrival Time Problem' Phys. Rev. D57 3351 (1998), quantph/9706045.
Zafiris, E. ‘Incorporation of Spacetime Symmetries in Einstein's Field Equations', J. Math. Phys. 38 (11), 5854, (1997), grqc/9710103.
_____`On Quantum Event Structures. Part I: The Categorical Scheme', Foundations of Physics Letters 14(2), (2001).
_____`On Quantum Event Structures. Part II: Interpretational Aspects', Foundations of Physics Letters 14(2), (2001).
_____`Probing Quantum Structure Through Boolean Localization Systems', International Journal of Theoretical Physics 39, (12) (2000).
_____`Boolean Coverings of Quantum Observable Structure: A Setting for an Abstract Differential Geometric Mechanism ', Journal of Geometry and Physics 50, 99 (2004), mathph/0306045.
_____`On Quantum Event Structures. Part III: Object of Truth Values ', Foundations of Physics Letters 17(5), (2004).
_____`Quantum Event Structures from the perspective of Grothendieck Topoi', Foundations of Physics 34(7), (2004).
_____`Interpreting Observables in a Quantum World from the Categorial Standpoint ', International Journal of Theoretical Physics 43, (1) (2004).
_____`Complex Systems from the perspective of Category Theory: I. Functioning of the Adjunction Concept ', Axiomathes 15, (1) (2005), PITTPHILSCI 1236.
_____`Complex Systems from the perspective of Category Theory: II. Covering Systems and Sheaves ', Axiomathes 15, (2) (2005), PITTPHILSCI 1237.
_____`CategoryTheoretic Analysis of the Notion of Complementarity for Quantum Systems', International Journal of General Systems, 35, (1) (2006).
_____`SheafTheoretic Representation of Quantum Measure Algebras', Journal of Mathematical Physics 47, 092103 (2006).
_____`Generalized Topological Covering Systems on Quantum Events Structures', Journal of Physics A: Mathematical and General 39, (2006).
_____`ToposTheoretic Classification of Quantum Events Structures in terms of Boolean Reference Frames', International Journal of Geometric Methods in Modern Physics, 3 (8) (2006).
_____`A SheafTheoretic Topos Model of the Physical Continuum and its Cohomological Observable Dynamics', International Journal of General Systems, 38, (1) (2009).
SELECTED BIBLIOGRAPHY
Bertaina, S., Gamarelli, S., Mitra, T., Tsukerblat, B., Muller, A., & Barbara, B. (2008), “Quantum oscillations in a molecular magnet,” Nature, 453:8 May 2008.
Epperson, Michael (2004), Quantum Mechanics and the Philosophy of Alfred North Whitehead, New York: Fordham University Press
_____ 2009 “Relational Realism: The Evolution of Ontology to Praxiology”. World Futures 65:1, 1941.
_____ (forthcoming) “Quantum Mechanics and Relational Realism: Logical Causality and Wave Function Collapse”. Process Studies 38.
Finkelstein, David (2002), Quantum Relativity: A Synthesis of the Ideas of Einstein and Heisenberg, Berlin: SpringerVerlag
GellMann, Murray, Hartle, James (1994), "Strong Decoherence" Contribution to the Proceedings of the 4th Drexel Symposium on Quantum NonIntegrabilityThe QuantumClassical Correspondence, Drexel University
Griffiths, R. B., & Omnes, R. (1999). “Consistent Histories and Quantum Measurements.” Physics Today. 52 (8), 26.
Griffiths, R. 1984. “Consistent histories and the interpretation of quantum mechanics”. Journal of Statistical Physics 36: 219–272.
_____. (2002), Consistent quantum theory. Cambridge: Cambridge University Press.
Kauffman, S. 1969. "Metabolic stability and epigenesis in randomly constructed genetic nets”. Journal of Theoretical Biology 22: 437467.
_____ 1991. "Antichaos and Adaptation". Scientific American, August 1991.
_____ 1993. Origins of Order: SelfOrganization and Selection in Evolution. Oxford University Press.
_____ 1995. At Home in the Universe. Oxford University Press.
_____ 2000. Investigations. Oxford University Press.
_____ 2004. "Prolegomenon to a General Biology". In: W. A. Dembski, M. Ruse (eds.), Debating Design: From Darwin to DNA. Cambridge University Press.
_____ 2004. "Autonomous Agents". In: J. D. Barrow, P.C.W. Davies, and C. L. Harper Jr. (eds.), Science and Ultimate Reality: Quantum Theory, Cosmology, and Complexity. Cambridge University Press.
Mohanty, P., Jariwala, E.M.Q. and Webb, R.A. (1997), “Intrinsic decoherence in mesoscopic systems,” Physical Review Letters 78: 3366–3369.
Myatt, C. J., King, B. E., Turchette, Q. A., Sackett, C. A., Kielpinski, D., Itano, W. M., et al. (2000), “Decoherence of quantum superpositions through coupling to engineered reservoirs.” Nature, 403, 269–273.
Omnès, Roland (1994), The Interpretation of Quantum Mechanics. Princeton, N.J.: Princeton University Press
_____. (2002). “Fundamental concepts  Decoherence, irreversibility, and selection by decoherence of exclusive quantum states with definite probabilities” (18 pages). Physical Review. A. 65 (5), 52119.
_____. (2005). “Model of quantum reduction with decoherence” (8 pages). Physical Review. D, Particles and Fields. 71 (5), 65011.
_____. (2005). Converging realities: Toward a common philosophy of physics and mathematics. Princeton, N.J.: Princeton University Press.
_____. (2006). “Decoherence and Reduction.” arXiv: quantph/0604130v1 18 Apr 2006
_____. (2008) “Possible derivation of wave function reduction from the basic quantum principles.” arXiv:0712.0730v2 [quantph] 19 Feb 2008
Stamp, P.C.E. & Tupitsyn, I.S. (2004) “Coherence window in the dynamics of quantum nanomagnets.” Phys. Rev. B 69, 014401.
Stapp, Henry (2007), The Mindful Universe. Berlin: SpringerVerlag
Whitehead, A. N. 1978. Process and Reality. An Essay in Cosmology. New York: Free Press.
Zafris, E. and J. J. Halliwell, `Decoherent Histories Approach to the Arrival Time Problem' Phys. Rev. D57 3351 (1998), quantph/9706045.
Zafiris, E. ‘Incorporation of Spacetime Symmetries in Einstein's Field Equations', J. Math. Phys. 38 (11), 5854, (1997), grqc/9710103.
_____`On Quantum Event Structures. Part I: The Categorical Scheme', Foundations of Physics Letters 14(2), (2001).
_____`On Quantum Event Structures. Part II: Interpretational Aspects', Foundations of Physics Letters 14(2), (2001).
_____`Probing Quantum Structure Through Boolean Localization Systems', International Journal of Theoretical Physics 39, (12) (2000).
_____`Boolean Coverings of Quantum Observable Structure: A Setting for an Abstract Differential Geometric Mechanism ', Journal of Geometry and Physics 50, 99 (2004), mathph/0306045.
_____`On Quantum Event Structures. Part III: Object of Truth Values ', Foundations of Physics Letters 17(5), (2004).
_____`Quantum Event Structures from the perspective of Grothendieck Topoi', Foundations of Physics 34(7), (2004).
_____`Interpreting Observables in a Quantum World from the Categorial Standpoint ', International Journal of Theoretical Physics 43, (1) (2004).
_____`Complex Systems from the perspective of Category Theory: I. Functioning of the Adjunction Concept ', Axiomathes 15, (1) (2005), PITTPHILSCI 1236.
_____`Complex Systems from the perspective of Category Theory: II. Covering Systems and Sheaves ', Axiomathes 15, (2) (2005), PITTPHILSCI 1237.
_____`CategoryTheoretic Analysis of the Notion of Complementarity for Quantum Systems', International Journal of General Systems, 35, (1) (2006).
_____`SheafTheoretic Representation of Quantum Measure Algebras', Journal of Mathematical Physics 47, 092103 (2006).
_____`Generalized Topological Covering Systems on Quantum Events Structures', Journal of Physics A: Mathematical and General 39, (2006).
_____`ToposTheoretic Classification of Quantum Events Structures in terms of Boolean Reference Frames', International Journal of Geometric Methods in Modern Physics, 3 (8) (2006).
_____`A SheafTheoretic Topos Model of the Physical Continuum and its Cohomological Observable Dynamics', International Journal of General Systems, 38, (1) (2009).
Zurek, Wojciech (2003), “Decoherence, einselection, and the quantum origins of the classical.” Reviews of Modern Physics, 75:715–785. 









