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=== Implicate orders, pre-space and algebraic structures ===
=== Implicate orders, pre-space and algebraic structures ===
Much of Bohm and Hiley's work in the 1970s and 1980s has expanded on the notion of [[Implicate and explicate order according to David Bohm|implicate, explicate and generative orders]] proposed by Bohm.<ref name="bohm-hiley-stuart-1970">David Bohm, Basil J. Hiley, Allan E. G. Stuart: ''On a new mode of description in physics'', International Journal of Theoretical Physics, vol.&nbsp;3, no.&nbsp;3, 1970, pp.&nbsp;171–183, {{doi|10.1007/BF00671000}}, [http://www.springerlink.com/content/l2474245pw272842/ abstract]</ref><ref>David Bohm: ''Quantum theory as an indication of a new order in physics. B. Implicate and explicate order in physical law'', Foundations of Physics, vol.&nbsp;3, no.&nbsp;2, 1973, pp.&nbsp;139-168, {{doi|10.1007/BF00708436}}</ref> This concept is described in the books ''[[Wholeness and the Implicate Order]]''<ref>David Bohm: ''[[Wholeness and the Implicate Order]]'', 1980</ref> by Bohm and ''[[Science, Order, and Creativity]]'' by Bohm and [[F. David Peat]].<ref>David Bohm, F. David Peat: ''[[Science, Order, and Creativity]]'', 1987</ref> The mathematics underlying this approach have been developed by the Birkbeck group over the last decennies.
Much of Bohm and Hiley's work in the 1970s and 1980s has expanded on the notion of [[Implicate and explicate order according to David Bohm|implicate, explicate and generative orders]] proposed by Bohm.<ref name="bohm-hiley-stuart-1970">David Bohm, Basil J. Hiley, Allan E. G. Stuart: ''On a new mode of description in physics'', International Journal of Theoretical Physics, vol.&nbsp;3, no.&nbsp;3, 1970, pp.&nbsp;171–183, {{doi|10.1007/BF00671000}}, [http://www.springerlink.com/content/l2474245pw272842/ abstract]</ref><ref>David Bohm: ''Quantum theory as an indication of a new order in physics. B. Implicate and explicate order in physical law'', Foundations of Physics, vol.&nbsp;3, no.&nbsp;2, 1973, pp.&nbsp;139-168, {{doi|10.1007/BF00708436}}</ref> This concept is described in the books ''[[Wholeness and the Implicate Order]]''<ref>David Bohm: ''[[Wholeness and the Implicate Order]]'', 1980</ref> by Bohm and ''[[Science, Order, and Creativity]]'' by Bohm and [[F. David Peat]].<ref>David Bohm, F. David Peat: ''[[Science, Order, and Creativity]]'', 1987</ref> The theoretical framework underlying this approach has been developed by the Birkbeck group over the last decennies.


In 1981, Bohm and Hiley introduced the "characteristic matrix", a non-Hermitian extension of the [[density matrix]]. The Wigner and Moyal transformation of the characteristic matrix yields a complex function, for which the dynamics can be described in terms of a (generalized) [[Liouville equation]] with the aid of a matrix operating in [[phase space]], leading to eigenvalues that can be identified with stationary states of motion. From the characteristic matrix, they constructed a further matrix that has only non-negative eigenvalues which can thus be interpreted as a quantum "statistical matrix". Bohm and Hiley thus demonstrated a relation between the [[Wigner quasi-probability distribution|Wigner–Moyal approach]] and Bohm's theory of an implicate order that allows to avoid the problem of [[Negative probability|negative probabilities]]. They noted that this work stands in close connection with [[Ilya Prigogine]]'s proposal of a Liouville space extension of quantum mechanics.<ref name="bohm-hiley-1981">D. Bohm, B. J. Hiley: ''On a quantum algebraic approach to a generalized phase space'', Foundations of Physics, vol.&nbsp;11, no.&nbsp;3–4, pp.&nbsp;179–203, 1981, {{doi|10.1007/BF00726266}}, [http://www.springerlink.com/content/u625hv8q8321m175/ abstract]/[http://www.springerlink.com/content/u625hv8q8321m175/fulltext.pdf full text]</ref>
In 1981, Bohm and Hiley introduced the "characteristic matrix", a non-Hermitian extension of the [[density matrix]]. The Wigner and Moyal transformation of the characteristic matrix yields a complex function, for which the dynamics can be described in terms of a (generalized) [[Liouville equation]] with the aid of a matrix operating in [[phase space]], leading to eigenvalues that can be identified with stationary states of motion. From the characteristic matrix, they constructed a further matrix that has only non-negative eigenvalues which can thus be interpreted as a quantum "statistical matrix". Bohm and Hiley thus demonstrated a relation between the [[Wigner quasi-probability distribution|Wigner–Moyal approach]] and Bohm's theory of an implicate order that allows to avoid the problem of [[Negative probability|negative probabilities]]. They noted that this work stands in close connection with [[Ilya Prigogine]]'s proposal of a Liouville space extension of quantum mechanics.<ref name="bohm-hiley-1981">D. Bohm, B. J. Hiley: ''On a quantum algebraic approach to a generalized phase space'', Foundations of Physics, vol.&nbsp;11, no.&nbsp;3–4, pp.&nbsp;179–203, 1981, {{doi|10.1007/BF00726266}}, [http://www.springerlink.com/content/u625hv8q8321m175/ abstract]/[http://www.springerlink.com/content/u625hv8q8321m175/fulltext.pdf full text]</ref> They extended this approach further to relativistic phase space using results of [[Mario Schönberg]].<ref>D. Bohm, B.J. Hiley, ''Relativisitic phase space arising out of Dirac algebra'', in Old and New Questions in Physics, Cosmology, Philosophy and Theoretical Biology, A. van der Merwe (ed.), pp.&nbsp;67-76, Plenum Press, New York</ref> Their approach was subsequently applied by [[Peter R. Holland]] to [[fermion]]s and by Alves O. Bolivar to [[boson]]s.<ref>P.R. Holland: ''Relativistic algebraic spinors and quantum motions in phase space'', Foundations of Physics, vol&nbsp;16, no.&nbsp;8, 1986, pp.&nbsp;701-719 {{DOI|10.1007/BF00735377}}</ref><ref>A.O. Bolivar: ''Classical limit of bosons in phase space'', Physica A: Statistical Mechanics and its Applications, vol.&nbsp;315, no.&nbsp;3–4, December 2002, pp.&nbsp;601–615</ref>


As of 1980, Hiley and his co-worker Fabio A. M. Frescura expanded on the notion of an ''implicate order'' by building on the work of [[Fritz Sauter]] and [[Marcel Riesz]] who had identified [[spinor]]s with [[left ideal]]s of an algebra. Frescura and Hiley, in turn, described the spinor using algebraic approaches that had been developed in the 19th century by the mathematicians [[Hermann Grassmann|Grassmann]], [[William Rowan Hamilton|Hamilton]], and [[William Kingdon Clifford|Clifford]].<ref name="frescura-hiley-1980a">F. A. M. Frescura, B. J. Hiley: ''The implicate order, algebras, and the spinor'', Foundations of Physics , Volume 10, Numbers 1-2, pp.&nbsp;7-31, 1980, {{doi|10.1007/BF00709014}} ([http://www.springerlink.com/content/t14h376854642283/ abstract])</ref><ref name="frescura-hiley-1980b">F. A. M. Frescura and B. J. Hiley: ''The algebraization of quantum mechanics and the implicate order'', Foundations of Physics, Volume 10, Numbers 9-10, 1980, pp.&nbsp;705-722, {{doi|10.1007/BF00708417}} ([http://www.springerlink.com/content/l4r6x12466901l81/ abstract])</ref><ref name="frescura-hiley-1981">F. A. M. Frescura, B. J. Hiley: ''Geometric interpretation of the Pauli spinor'', American Journal of Physics, February 1981, Volume 49, Issue 2, pp.&nbsp;152 ([http://ajp.aapt.org/resource/1/ajpias/v49/i2/p152_s1 abstract])</ref> In 1984, they suggested that an implicate order could be carried by an algebra, with the explicate order being contained in the various [[Algebra representation|representations]] of this algebra.<ref name="frescura-hiley-1984">F. A. M. Frescura, B. J. Hiley: [http://www.bbk.ac.uk/tpru/BasilHiley/P12FrescandHiley3.pdf Algebras, quantum theory and pre-space], p.&nbsp;3–4 (published in Revista Brasileira de Fisica, Volume Especial, Julho 1984, Os 70 anos de Mario Schonberg, pp. 49-86)</ref> Bohm and Hiley expanded on the concept that "relativistic quantum mechanics can be expressed completely through the interweaving of three basic algebras, the bosonic, the fermionic and the Clifford" and that in this manner "the whole of relativisic quantum mechanics can also be put into an implicate order" as suggested in earlier publications of David Bohm of 1973 and 1980.<ref name="generalization-of-the-twistor-1984">D. Bohm, B. J. Hiley: ''Generalisation of the twistor to Clifford algebras as a basis for geometry'', published in Revista Brasileira de Fisica, Volume Especial, Os 70 anos de Mario Schönberg, pp.&nbsp;1-26, 1984 ([http://www.birkbeck.ac.uk/tpru/BasilHiley/PS16Twistors.pdf PDF])</ref> On this basis, they expressed the [[twistor theory]] of Penrose as a [[Clifford algebra]], thereby describing structure and forms of ordinary space as an explicit order that unfolds from an implicate order, the latter constituting a ''pre-space''.<ref name="generalization-of-the-twistor-1984"/> The spinor is described mathematically as an [[Ideal (ring theory)|ideal]] in the [[Pauli algebra|Pauli Clifford algebra]], the twistor as an ideal in the [[Conformal geometric algebra|conformal Clifford algebra]].<ref>B. J. Hiley, F. David Peat: ''General Introduction: The development of Bohm's ideas from plasma to the implicate order'', in: Basil . Hiley, F. David Peat (eds.): ''Quantum implications: essays in honour of David Bohm'', Routledge, 1987, ISBN 0-415-06960-2, pp.&nbsp;1–32, therein: [http://books.google.com/books?id=Avvxbw-NONYC&pg=PA25 p. 25]</ref> In a preprint that remained unpublished for many years, Bohm, P.G. Davies and Hiley presented their algebraic approach in context with the work of [[Arthur Stanley Eddington]]. With their approach based on [[idempotent]]s of an algebra, they "incorporate [[Niels Bohr|Bohr]]'s notion of ‘wholeness’ and [[Bernard d'Espagnat|d'Espagnat]]'s concept of ‘non-separability’ in a very basic way".<ref>D.J. Bohm, P.G. Davies, B.J. Hiley: ''Algebraic Quantum Mechanics and Pregeometry'', 1981, [http://arxiv.org/abs/quant-ph/0612002 arXiv:quant-ph/0612002] (submitted 30 November 2006), and its introductory note by B. Hiley: ''Quantum Space‐Times: An Introduction to “Algebraic Quantum Mechanics and Pregeometry”'', AIP Conference Proceedings 810, pp. 312-313, {{DOI|10.1063/1.2158734}}</ref>
As of 1980, Hiley and his co-worker Fabio A. M. Frescura expanded on the notion of an ''implicate order'' by building on the work of [[Fritz Sauter]] and [[Marcel Riesz]] who had identified [[spinor]]s with [[left ideal]]s of an algebra. Frescura and Hiley, in turn, described the spinor using algebraic approaches that had been developed in the 19th century by the mathematicians [[Hermann Grassmann|Grassmann]], [[William Rowan Hamilton|Hamilton]], and [[William Kingdon Clifford|Clifford]].<ref name="frescura-hiley-1980a">F. A. M. Frescura, B. J. Hiley: ''The implicate order, algebras, and the spinor'', Foundations of Physics , Volume 10, Numbers 1-2, pp.&nbsp;7-31, 1980, {{doi|10.1007/BF00709014}} ([http://www.springerlink.com/content/t14h376854642283/ abstract])</ref><ref name="frescura-hiley-1980b">F. A. M. Frescura and B. J. Hiley: ''The algebraization of quantum mechanics and the implicate order'', Foundations of Physics, Volume 10, Numbers 9-10, 1980, pp.&nbsp;705-722, {{doi|10.1007/BF00708417}} ([http://www.springerlink.com/content/l4r6x12466901l81/ abstract])</ref><ref name="frescura-hiley-1981">F. A. M. Frescura, B. J. Hiley: ''Geometric interpretation of the Pauli spinor'', American Journal of Physics, February 1981, Volume 49, Issue 2, pp.&nbsp;152 ([http://ajp.aapt.org/resource/1/ajpias/v49/i2/p152_s1 abstract])</ref> In 1984, they suggested that an implicate order could be carried by an algebra, with the explicate order being contained in the various [[Algebra representation|representations]] of this algebra.<ref name="frescura-hiley-1984">F. A. M. Frescura, B. J. Hiley: [http://www.bbk.ac.uk/tpru/BasilHiley/P12FrescandHiley3.pdf Algebras, quantum theory and pre-space], p.&nbsp;3–4 (published in Revista Brasileira de Fisica, Volume Especial, Julho 1984, Os 70 anos de Mario Schonberg, pp. 49-86)</ref> Bohm and Hiley expanded on the concept that "relativistic quantum mechanics can be expressed completely through the interweaving of three basic algebras, the bosonic, the fermionic and the Clifford" and that in this manner "the whole of relativisic quantum mechanics can also be put into an implicate order" as suggested in earlier publications of David Bohm of 1973 and 1980.<ref name="generalization-of-the-twistor-1984">D. Bohm, B. J. Hiley: ''Generalisation of the twistor to Clifford algebras as a basis for geometry'', published in Revista Brasileira de Fisica, Volume Especial, Os 70 anos de Mario Schönberg, pp.&nbsp;1-26, 1984 ([http://www.birkbeck.ac.uk/tpru/BasilHiley/PS16Twistors.pdf PDF])</ref> On this basis, they expressed the [[twistor theory]] of Penrose as a [[Clifford algebra]], thereby describing structure and forms of ordinary space as an explicit order that unfolds from an implicate order, the latter constituting a ''pre-space''.<ref name="generalization-of-the-twistor-1984"/> The spinor is described mathematically as an [[Ideal (ring theory)|ideal]] in the [[Pauli algebra|Pauli Clifford algebra]], the twistor as an ideal in the [[Conformal geometric algebra|conformal Clifford algebra]].<ref>B. J. Hiley, F. David Peat: ''General Introduction: The development of Bohm's ideas from plasma to the implicate order'', in: Basil . Hiley, F. David Peat (eds.): ''Quantum implications: essays in honour of David Bohm'', Routledge, 1987, ISBN 0-415-06960-2, pp.&nbsp;1–32, therein: [http://books.google.com/books?id=Avvxbw-NONYC&pg=PA25 p. 25]</ref> In a preprint that remained unpublished for many years, Bohm, P.G. Davies and Hiley presented their algebraic approach in context with the work of [[Arthur Stanley Eddington]]. With their approach based on [[idempotent]]s of an algebra, they "incorporate [[Niels Bohr|Bohr]]'s notion of ‘wholeness’ and [[Bernard d'Espagnat|d'Espagnat]]'s concept of ‘non-separability’ in a very basic way".<ref>D.J. Bohm, P.G. Davies, B.J. Hiley: ''Algebraic Quantum Mechanics and Pregeometry'', 1981, [http://arxiv.org/abs/quant-ph/0612002 arXiv:quant-ph/0612002] (submitted 30 November 2006), and its introductory note by B. Hiley: ''Quantum Space‐Times: An Introduction to “Algebraic Quantum Mechanics and Pregeometry”'', AIP Conference Proceedings 810, pp. 312-313, {{DOI|10.1063/1.2158734}}</ref>

Revision as of 20:26, 28 October 2012

Basil J. Hiley, born 1935, is a British quantum physicist and professor emeritus of the University of London.

Long-time co-worker of David Bohm, Hiley is known for his work with Bohm on implicate orders and for his work on algebraic descriptions of quantum physics in terms of underlying symplectic and orthogonal Clifford algebras.[1] Hiley co-authored the book The Undivided Universe with David Bohm, which is considered the main reference for Bohm's interpretation of quantum theory.

The work of Bohm and Hiley has been characterized as primarily addressing the question "whether we can have an adequate conception of the reality of a quantum system, be this causal or be it stochastic or be it of any other nature" and meeting the scientific challenge of providing a mathematical description of quantum systems that matches the idea of an implicate order.[2]

Education and career

Basil Hiley was born 1935 in Burma, where his father worked for the military for the British Raj. He came to Hampshire, England, at the age of twelve, where he attended high school. His imagination with regard to science was spurred by his teachers at secondary school and by books, in particular The Mysterious Universe by James Hopwood Jeans and Mr Tompkins in Wonderland by George Gamow.[3]

Hiley performed undergraduate studies at King's College London.[3] He published a paper in 1961 on the random walk of a macromolecule,[4] followed by further papers on the Ising model,[5] and on lattice constant systems defined in graph theoretical terms.[6] In 1962 he obtained his PhD from King's College in condensed matter physics, more specifically on cooperative phenomena in ferromagnets and long chain polymer models, under the supervision of Cyril Domb and Michael Fisher.[7][8]

Hiley first met met David Bohm during a week-end meeting organized by the student society of King's College at Cumberland Lodge, where Bohm held a lecture. In 1961 Hiley was appointed assistant lecturer at Birkbeck College, where Bohm had taken the chair of Theoretical Physics shortly before.[3] Hiley was interested to investigate how physics could be based on a notion of process, and he found that David Bohm held similar ideas.[9] He reports that during the seminars he held together with Roger Penrose he was particularly fascinated by John Wheeler’s "sum over three geometries" ideas that he was using to quantise gravity.[7]

He worked with David Bohm over many years on fundamental problems of theoretical physics.[10] Initially Bohm's model of 1952 did not feature in their discussions; this changed when Hiley asked himself whether the "Einstein-Schrödinger equation", as Wheeler called it, might be found by studying the full implications of that model.[7] They worked together closely for three decades. Together they wrote many publications and the book The Undivided Universe: An Ontological Interpretation of Quantum Theory, published 1993, which is now considered the major reference for Bohm's interpretation of quantum theory.[11]

In 1995, Basil Hiley was appointed to a chair in physics at Birkbeck College at the University of London.[12]

Work

Quantum potential and active information

In the 1970s Bohm, Hiley and co-workers at Birkbeck college expanded further on the theory presented by David Bohm in 1952.[13] They suggested to re-express the field equations of physics in a way that is independent of their spacetime description.[14] They interpreted Bell's theorem as a test of spontaneous localization, meaning a tendency of a many-body system to factorize into a product of localized states of its constituent particles, pointing out that such spontaneous localization removes the need for a fundamental role of the measuring apparatus in quantum theory.[15] They proposed that the fundamental new quality introduced by quantum physics is non-locality.[16][17] In 1975, they presented how in the causal interpretation of the quantum theory introduced by Bohm in 1952 the concept of a quantum potential leads to the notion of an "unbroken wholeness of the entire universe", and they proposed possible routes to a generalization of the approach to relativity by means of a novel concept of time.[16]

Bohm trajectories under the influence of the quantum potential, at the example of an electron going through the two-slit experiment. The resultant trajectories were first presented by Philippidis, Dewdney and Hiley in 1979.[18]

By performing numeric computations on the basis of the quantum potential, Chris Philippidis, Chris Dewdney and Basil Hiley used computer simulations to deduce ensembles of particle trajectories that could account for the interference fringes in the double-slit experiment[19] and worked out descriptions of scattering processes.[20] Their work renewed the interests of physicists in the Bohm interpretation of quantum physics.[21] In 1979, Bohm and Hiley discussed the Aharonov-Bohm effect which had recently found experimental confirmation.[22] They called attention to the importance of the early work of Louis de Broglie on pilot waves, emphasizing his insight and physical intuition and stating that developments based on his ideas aimed at a better understanding than mathematical formalism alone.[23] They offered ways of understanding quantum non-locality and the measurement process,[24][25][26][27] the limit of classicality,[28] interference and quantum tunneling.[29]

They showed how in the Bohm model, introducing the concept of active information, the measurement problem and the collapse of the wave function, could be understood in terms of the quantum potential approach, and that this approach could be extended to relativistic quantum field theories.[27] They described the measurement process and the impossibility of measuring position and momentum simultaneously as follows: "The ѱ field itself changes since it must satisfy the Schrödinger equation, which now contains the interaction between the particle and apparatus, and it is this change that makes it impossible to measure position and momentum together".[30] The collapse of the wave function of the Copenhagen interpretation of quantum theory is explained in the quantum potential approach by the demonstration that information can become inactive[31] in the sense that from then on "all the packets of the multi-dimensional wave function that do not correspond to the actual result of measurement have no effect on the particle".[32]

With P.N. Kaloyerou, Hiley extended the quantum potential approach to quantum field theory in Minkowski spacetime.[33][34][35][36] Bohm and Hiley considered the relativistic invariance of a quantum theory based on the notion of beables, a term coined by John Bell[37] to distinguish these variables from observables.[38] Hiley and a co-worker later extended the work further to curved spacetime.[39] Bohm and Hiley demonstrated that the non-locality of quantum theory can be understood as limit case of a purely local theory, provided the transmission of active information is allowed to be greater than the speed of light, and that this limit case yields approximations to both quantum theory and relativity.[40]

Summarizing Bohm's and his own interpretation, Hiley has explained that the quantum potential "does not give rise to a mechanical force in the Newtonian sense. Thus while the Newtonian potential drives the particle along the trajectory, the quantum potential organises the form of the trajectories in response to the experimental conditions." The quantum potential can be understood as an aspect of "some kind of self-organising process" involving a basic underlying field.[41][42] The quantum potential (or information potential) links the quantum system under investigation to the measuring apparatus, thereby giving that system a significance within the context defined by the apparatus.[43] It acts on each quantum particle individually, each particle influencing itself. Hiley cites the wording of Paul Dirac: "Each electron only interferes with itself" and adds: "Somehow the ‘quantum force’ is a ‘private’ force. It thus cannot be regarded as a distortion of some underlying sub-quantum medium as was originally suggested by de Broglie".[44] It is independent of field intensity, thus fulfilling a precondition for non-locality, and it carries information about the whole experimental arrangement in which the particle finds itself.[44]

In processes of non-signalling transmission of qubits in a system consisting of multiple particles (a process that is generally called "quantum teleportation" by physicists), active information is transferred from one particle to another, and in the Bohm model this transfer is mediated by the non-local quantum potential.[45][46]

Implicate orders, pre-space and algebraic structures

Much of Bohm and Hiley's work in the 1970s and 1980s has expanded on the notion of implicate, explicate and generative orders proposed by Bohm.[47][48] This concept is described in the books Wholeness and the Implicate Order[49] by Bohm and Science, Order, and Creativity by Bohm and F. David Peat.[50] The theoretical framework underlying this approach has been developed by the Birkbeck group over the last decennies.

In 1981, Bohm and Hiley introduced the "characteristic matrix", a non-Hermitian extension of the density matrix. The Wigner and Moyal transformation of the characteristic matrix yields a complex function, for which the dynamics can be described in terms of a (generalized) Liouville equation with the aid of a matrix operating in phase space, leading to eigenvalues that can be identified with stationary states of motion. From the characteristic matrix, they constructed a further matrix that has only non-negative eigenvalues which can thus be interpreted as a quantum "statistical matrix". Bohm and Hiley thus demonstrated a relation between the Wigner–Moyal approach and Bohm's theory of an implicate order that allows to avoid the problem of negative probabilities. They noted that this work stands in close connection with Ilya Prigogine's proposal of a Liouville space extension of quantum mechanics.[51] They extended this approach further to relativistic phase space using results of Mario Schönberg.[52] Their approach was subsequently applied by Peter R. Holland to fermions and by Alves O. Bolivar to bosons.[53][54]

As of 1980, Hiley and his co-worker Fabio A. M. Frescura expanded on the notion of an implicate order by building on the work of Fritz Sauter and Marcel Riesz who had identified spinors with left ideals of an algebra. Frescura and Hiley, in turn, described the spinor using algebraic approaches that had been developed in the 19th century by the mathematicians Grassmann, Hamilton, and Clifford.[55][56][57] In 1984, they suggested that an implicate order could be carried by an algebra, with the explicate order being contained in the various representations of this algebra.[58] Bohm and Hiley expanded on the concept that "relativistic quantum mechanics can be expressed completely through the interweaving of three basic algebras, the bosonic, the fermionic and the Clifford" and that in this manner "the whole of relativisic quantum mechanics can also be put into an implicate order" as suggested in earlier publications of David Bohm of 1973 and 1980.[59] On this basis, they expressed the twistor theory of Penrose as a Clifford algebra, thereby describing structure and forms of ordinary space as an explicit order that unfolds from an implicate order, the latter constituting a pre-space.[59] The spinor is described mathematically as an ideal in the Pauli Clifford algebra, the twistor as an ideal in the conformal Clifford algebra.[60] In a preprint that remained unpublished for many years, Bohm, P.G. Davies and Hiley presented their algebraic approach in context with the work of Arthur Stanley Eddington. With their approach based on idempotents of an algebra, they "incorporate Bohr's notion of ‘wholeness’ and d'Espagnat's concept of ‘non-separability’ in a very basic way".[61]

Quantum Cloud by Antony Gormley, influenced by an exchange of thoughts among Hiley and Gormley on algebra and pre-space.[62]

The notion of another order underlying space was not new. Along similar lines, both Gerard 't Hooft and John Archibald Wheeler, questioning whether space-time was the appropriate starting-point for describing physics, had called for a deeper structure as starting point, and Wheeler had proposed a notion of pre-space which he called pregeometry, from which spacetime geometry should emerge as a limiting case. Bohm and Hiley underline Wheeler's view, yet point out they do not build on the notion of a foam-like structure as proposed by Wheeler and by Stephen Hawking.[59] Bohm and Hiley, instead, worked together towards a representation of the implicate order in form of an appropriate algebra or other pre-space. They considered spacetime itself as part of an explicit order that is connected to pre-space as implicit order. The spacetime manifold and properties of locality and non-locality then arise from an order in such pre-space.

In the view of Bohm and Hiley, "things, such as particles, objects, and indeed subjects, are considered as semi-autonomous quasi-local features of this underlying activity".[63] These features can be considered to be independent only up to a certain level of approximation in which certain criteria are fulfilled. In this picture, the classical limit for quantum phenomena, in terms of a condition that the action function is not much greater than Planck's constant, indicates one such criterion. Bohm and Hiley used the word holomovement for the underlying activity in the various orders together.[47] This term is intended to extend beyond the movement of objects in space and beyond the notion of process, covering movement in a wide context such as for instance the "movement" of a symphony: a "a total ordering which involves the whole movement, past and anticipated, at any one moment".[63] This concept, which avowedly has similarities with the notion of organic mechanism of Alfred North Whitehead,[63] underlies Bohm and Hiley´s efforts to establish algebraic structures that relate to quantum physics and to find an ordering that describes thought processes and the mind.

They investigated non-locality of spacetime also in terms of the time dimension. In 1985, Bohm and Hiley showed that Wheeler's delayed choice experiment does not require the existence of the past to be limited to its recording in the present.[64] Hiley and R. E. Callaghan later confirmed this view, which stands in stark contrast to Wheeler's earlier statement that "the past has no existence except as it is recorded in the present",[65] by a detailed trajectory analysis for delayed choice experiments[66] and by an investigation into welcher Weg experiments.[67]

Bohm and Hiley sketched also how Bohm's model could be treated under the point of view of statistical mechanics, and their joint work on this was published in their book (1993) and a subsequent publication (1996).[68]

Hiley has pursued work on algebraic structures in quantum theory throughout his scientific career.[51][55][56][57][58][59][69][70][71][72][73][74][75][76][77][78] After Bohm's death in 1992, he published several papers on how different formulations of quantum physics, including Bohm's, can be brought in context.[75][79][80] Hiley also pursued further work on the thought experiments set out by Einstein-Podolsky-Rosen and by Lucien Hardy, in particular considering the relation to special relativity.[81][82][83][84]

In the late 1990's, Hiley expanded further on the notion he had developed with Bohm on the description of quantum phenomena in terms of processes.[85][86] Hiley and his co-worker Marco Fernandes interpret time as an aspect of process that should be represented by a mathematically appropriate description in terms of an algebra of process. For Hiley and Fernandes, time should be considered in terms of "moments" rather than extensionless points in time, in conventional terms implying an integration over time, recalling also that from the "characteristic matrix" of Bohm and Hiley[51] a positive definite probability can be obtained.[86] They model the unfolding of implicate and explicate orders and the evolution of such orders by a mathematical formalism which Hiley has termed the Clifford algebra of process.[85]

Projections into shadow manifolds

Around the same time, in 1997, Hiley's co-worker Melvin Brown[87] showed that the Bohm interpretation of quantum physics need not rely on a formulation in terms of ordinary space (-space), but can be formulated, alternatively, in terms of momentum space (-space).[88][72][89] Brown and Hiley refer to such spaces as "shadow manifolds" (adopting the term "shadow" from Michał Heller[90]). In the classical limit, the shadow spaces converge to one unique phase space.

Brown and Hiley later showed that the Schrödinger equation can be written in a purely algebraic form that is independent of any representation in a Hilbert space, and that in their algebraic formulation of quantum mechanics the equation of motion takes on the same form as for the Heisenberg equation of motion, except that the bra and ket in the bra-ket notation each stand for an element of the algebra and the Heisenberg time evolution is an inner automorphism in the algebra.[72]

Hiley has emphasized that quantum processes cannot be displayed in phase space for reason of lacking commutativity.[74] As Israel Gelfand had shown, commutative algebras allow a unique manifold to be constructed as a sub-space which is dual to the algebra; non-commutative algebras in contrast cannot be associated with a unique underlying manifold. Instead, a non-commutative algebra requires a multiplicity of shadow manifolds. These shadow manifolds can be constructed from the algebra by means of projections into subspaces; however, the projections inevitably lead to distortions, in similar manner as Mercator projections inevitably result in distortions in geographical maps.[74][76]

Relation of the de Broglie–Bohm theory to quantum phase space and Wigner–Moyal

In 2001, picking up on the "characteristic matrix" developed with Bohm in 1981[51] and the notion of a "moment" introduced with Fernandes in 1997,[86] Hiley proposed to use a moment as "an extended structure in both space and time" as a basis for a quantum dynamics, to take the place of the notion of a point particle.[74] The quasi-probability distribution can be understood as the density matrix re-expressed in terms of a mean position and momentum of a "cell" in phase space, and the Bohm interpretation arises from the dynamics of these "cells" if the particle is considered to be at the center of the cell.[91][92] Hiley later pointed out that the equations defining the Bohm approach can be taken to be implicit in certain equations of the 1949 publication by José Enrique Moyal on the phase space formulation of quantum mechanics; he emphasized that this link between the two approaches could be of relevance for constructing a quantum geometry.[7]

In 2005, building on his work with Brown, [72] Hiley showed that the construction of subspaces allows the Bohm interpretation to be understood in terms of the choice of the x-representation as shadow phase space as one particular choice among an infinite number of possible shadow phase spaces.[75] This is similar, so Hiley,[66] to the demonstration given by mathematician Maurice A. de Gosson that "the Schrödinger equation can be shown rigorously to exist in the covering groups of the symplectic group of classical physics and the quantum potential arises by projecting down onto the underlying group".[93] In Hiley's framework, the quantum potential arises as "a direct consequence of projecting the non-commutative algebraic structure onto a shadow manifold" and as a necessary feature which ensures that both energy and momentum are conserved.[75][94] Similarly, the Bohm and the Wigner approach are shown to be two different shadow phase space representations.[91]

With these results, Hiley gave evidence to the notion that the ontology of implicate and explicate orders could be understood as a process described in terms of an underlying non-commutative algebra, from which spacetime could be abstracted as one possible representation.[72] The algebraic structure is identified with an implicate order, and its shadow manifolds with the sets of explicate orders that are consistent with that implicate order.[80]

Here emerges, in Hiley's words, "a radically new way of looking at the way quantum processes enfold in time", built on the work of Bohm and Hiley in the 1980´s:[74] in this school of thought, processes of movement can be seen as automorphisms within and between inequivalent representations of the algebra. In the first case, the transformation is an inner automorphism, which is a way of expressing the enfolding and unfolding movement in terms of potentialities of the process; in the second case it is an outer automorphism, or transformation to a new Hilbert space, which is a way of expressing an actual change.

Hierarchy of Clifford algebras

Clifford algebras Cp,q and wave equations
algebra signature equation
C4,2 +, +, +, +, -, - Twistor twistor
C1,3 +, -, -, - Dirac relativistic spin-½
C3,0 +, +, + Pauli spin-½
C0,1 - Schrödinger spin-0

Starting from the notion of a process algebra as proposed by Hermann Grassmann and by Stuart Kauffman, Hiley showed how three Clifford algebras C0,1, C3,0, C1,3 form a hierarchy of Clifford algebras over the real numbers that describe the dynamics of the Schrödinger, Pauli and Dirac particles, respectively.[80] Using this approach to describe relativistic particle quantum mechanics, Hiley and R. E. Callaghan presented a complete relativistic version of the Bohm model for the Dirac particle in analogy to Bohm's approach to the non-relativistic Schrödinger equation, thereby refuting the long-standing misconception that the Bohm model could not be applied in the relativistic domain.[76][77][78][80] Hiley pointed out that the Dirac particle has a ‘quantum potential’ which is the exact relativistic generalisation of the quantum potential found originally by de Broglie and Bohm.[80] Within the same hierarchy, the twistor of Roger Penrose links to the conformal Clifford algebra C4,2 over the reals, and what Hiley calls the Bohm energy and the Bohm momentum arises directly from the standard energy-momentum tensor.[95] The technique developed by Hiley and his co-workers demonstrates

"that quantum phenomena per se can be entirely described in terms of Clifford algebras taken over the reals without the need to appeal to specific representation in terms of wave functions in a Hilbert space. This removes the necessity of using Hilbert space and all the physical imagery that goes with the use of the wave function".[78]

Hiley has worked with Maurice A. de Gosson on the relation between classical and quantum physics, presenting a mathematical derivation of the Schrödinger equation from Hamiltonian mechanics.[96] Together with mathematicians Ernst Binz and Maurice A. de Gosson, Hiley showed how "a characteristic Clifford algebra emerges from each (2n-dimensional) phase space" and discussed relations of quaternion algebra, symplectic geometry and quantum mechanics.[97]

Observed trajectories and their algebraic description

In 2011, de Gosson and Hiley showed that when in Bohm's model a continuous observation of a trajectory is performed, the observed trajectory is identical to the classical particle trajectory. This finding puts the Bohm model in connection to the well-known quantum Zeno effect.[98]

Later that year, for the first time experimental results were published which displayed the properties expected for Bohm trajectories. More specifically, photon trajectories were observed by means of weak measurements in a double-slit interferometer which displayed the qualitative features that had been predicted, ten years earlier, by Partha Ghose for Bohm trajectories.[99][100][101] The same year, Hiley showed that a description of weak processes – "weak" in the sense of weak measurements – can be included in his framework of an algebraic description of quantum processes by extending the framework to include not only (orthogonal) Clifford algebras but also the Moyal algebra, a symplectic Clifford algebra.[102]

Relations to other work

Hiley has repeatedly discussed the reasons for which the Bohm interpretation has met resistance, these reasons relating for instance to the role of the quantum potential term and to assumptions on particle trajectories.[7][67][79][103][104][105][106] He has shown how the energy-momentum-relations in the Bohm model can be obtained directly from the energy-momentum tensor of quantum field theory.[78] He has referred to this as "a remarkable discovery, so obvious that I am surprised we didn't spot it sooner", pointing out that on this basis the quantum potential constitutes the missing energy term that is required for local energy-momentum conservation.[107] Hiley has pointed out how the Bohm model and Bell's inequalities allowed a debate on the notion of non-locality in quantum physics or, in Niels Bohr's words, wholeness to surface.[108]

He has stated that his recent focus on noncommutative geometry appears to be very much in line with the work of Fred van Oystaeyen on noncommutative topology.[109]

Ignazio Licata cites Bohm and Hiley's approach as formulating "a quantum event as the expression of a deeper quantum process" that connects a description in terms of space-time with a description in non-local, quantum mechanical terms.[89] Hiley is cited, together with Whitehead, Bohr and Bohm, for the "stance of elevating processes to a privileged role in theories of physics".[110] His view of process as fundamental has been seen as similar to the approach taken by the physicist Lee Smolin. This stands quite in contrast to other approaches, in particular to the blockworld approach in which spacetime is static.[111]

Mind and matter

Hiley and Paavo Pylkkänen addressed the question of the relation between mind and matter by the hypothesis of an active information contributing to quantum potential.[112][113][114][115] Recalling notions underlying Bohm's approach, Hiley emphasises that active information "informs" in the sense of a literal meaning of the word: it "induces a change of form from within", and "this active side of the notion of information […] seems to be relevant both to material processes and to thought".[116] He emphasizes: "even though the quantum level may be analogous to the human mind only in a rather limited way, it does help to understand the interlevel relationships if there are some common features, such as the activity of information, shared by the different levels. The idea is not to reduce everything to the quantum level but rather to propose a hierarchy of levels, which makes room for a more subtle notion of determinism and chance".[112]

Referring to two fundamental notions of René Descartes, Hiley states that "if we can give up the assumption that space-time is absolutely necessary for describing physical processes, then it is possible to bring the two apparently separate domains of res extensa and res cogitans into one common domain", and he adds that "by using the notion of process and its description by an algebraic structure, we have the beginnings of a descriptive form that will enable us to understand quantum processes and will also enable us to explore the relation between mind and matter in new ways."[85]

Bohm and Hiley's work on implicate and explicate order approaches mind and matter are aspects of the same process.[63]

"Our proposal is that in the brain there is a manifest (or physical) side and a subtle (or mental) side acting at various levels. At each level, we can regard one side the manifest or material side, while the other is regarded as subtle or mental side. The material side involves electrochemical processes of various kinds, it involves neuron activity and so on. The mental side involves the subtle or virtual activities that can be actualised by active information mediating between the two sides.
These sides […] are two aspects of the same process. […] what is subtle at one level can become what is manifest at the next level and so on. In other words if we look at the mental side, this too can be divided into a relatively stable and manifest side and a yet more subtle side. Thus there is no real division between what is manifest and what is subtle and in consequence there is no real division between mind and matter".[117]

Hiley also worked with biologist Brian Goodwin on a process view of biological life, with an alternate view on Darwinism.[118] Hiley aims at finding "an algebraic description of those aspects of this implicate order where mind and matter have their origins".[119]

Publications

Books
  • F. David Peat (Editor) and Basil Hiley (Editor): Quantum Implications: Essays in Honour of David Bohm, Routledge & Kegan Paul Ltd, London & New York, 1987 (edition of 1991 ISBN 978-0-415-06960-1)
  • David Bohm, Basil Hiley: The Undivided Universe: An Ontological Interpretation of Quantum Theory, Routledge, 1993, ISBN 0-415-06588-7
Other
  • Foreword to: "The Principles of Newtonian and Quantum Mechanics – The Need for Planck's Constant, h" by Maurice A. de Gosson, Imperial College Press, World Scientific Publishing, 2001, ISBN 1-86094-274-1
  • Foreword to the 1996 edition of: "The Special Theory of Relativity" by David Bohm, Routledge, ISBN 0-203-20386-0
  • Attention: This template ({{cite doi}}) is deprecated. To cite the publication identified by doi:10.1098/rsbm.1997.0007, please use {{cite journal}} (if it was published in a bona fide academic journal, otherwise {{cite report}} with |doi=10.1098/rsbm.1997.0007 instead. (abstract)

References

  1. ^ Basil Hiley, website of Maurice A. de Gosson, 2005, accessed on 1 September 2012
  2. ^ Olival Freire, Jr.: Continuity and change: charting David Bohm's evolving ideas on quantum mechanics, In: Décio Krause, Antonio Videira (eds.): Brazilian Studies in the Philosphy and History of Science, Boston Studies in the Philosophy of Science, Springer, ISBN 978-90-481-9421-6, pp.291–300, therein p. 296–297
  3. ^ a b c Interview with Basil Hiley conducted by Olival Freire on January 11, 2008, Oral History Transcript, Niels Bohr Library & Archives, American Institute of Physics
  4. ^ B. J. Hiley and M. F. Sykes: Probability of Initial Ring Closure in the Restricted Random-Walk Model of a Macromolecule, Journal of Chemical Physics, volume 34, number 5, pp. 1531, 1961, doi:10.1063/1.1701041 (abstract)
  5. ^ B. J. Hiley, G. S. Joyce: The Ising model with long-range interactions, Proceedings of the Physical Society, volume 85, number 3, 1965, doi:10.1088/0370-1328/85/3/310 (abstract)
  6. ^ M. F. Sykes, J. W. Essam, B. R. Heap, B. J. Hiley: Lattice Constant Systems and Graph Theory, Journal of Mathematical Physics, volume 7, number 9, pp. 1557, 1966, doi:10.1063/1.1705066 (abstract)
  7. ^ a b c d e B. J. Hiley: On the Relationship Between the Wigner-Moyal and Bohm Approaches to Quantum Mechanics: A Step to a More General Theory?, Foundations of Physics, Volume 40, Number 4 ("Jeffrey Bub Festschrift"), 2009, pp. 356-367, doi:10.1007/s10701-009-9320-y (PDF)
  8. ^ CV, Mind and Matter (downloaded 17 March 2012)
  9. ^ Quote: "my own interests were very much directed towards trying to base physics on the general notion of process, an idea that attracted me to Bohm in the first place, as he had similar thoughts" in Basil Hiley's introductory note to the paper by David Bohm: On the role of hidden variables in the fundamental structure of physics, Foundations of Physics, vol. 26, no. 6, 1966, pp. 719-786, doi:10.1007/BF02058632
  10. ^ See for example the characterization of their work together by Joseph Jaworski in his book Source: The Inner Path of Knowledge Creation, Berrett-Koehler Publishers, 2012
  11. ^ Attention: This template ({{cite doi}}) is deprecated. To cite the publication identified by doi:10.1098/rsbm.1997.0007, please use {{cite journal}} (if it was published in a bona fide academic journal, otherwise {{cite report}} with |doi=10.1098/rsbm.1997.0007 instead.
  12. ^ Basil Hiley (short CV), Scientific and Medical Network
  13. ^ Paavo Pylkkänen: Foreword by the Editor, in: David Bohm and Charles Biederman, and Paavo Pylkkänen (ed.): Bohm-Biederman Correspondence, ISBN 978-0-415-16225-8, p. xiv
  14. ^ David Bohm, Basil J. Hiley, Allan E. G. Stuart: On a new mode of description in physics, International Journal of Theoretical Physics, Volume 3, Number 3, pp. 171-183, 1970, doi:10.1007/BF00671000 (abstract)
  15. ^ A. Baracca, D. J. Bohm, B. J. Hiley, A. E. G. Stuart: On some new notions concerning locality and nonlocality in the quantum theory, Il nuovo cemento B, Volume 28, Number 2, pp. 453-466, 1972, doi:10.1007/BF02726670 abstract
  16. ^ a b D. Bohm, B. J. Hiley: On the intuitive understanding of nonlocality as implied by quantum theory, Foundations of Physics, Volume 5, Number 1, 1975, pp. 93-109, doi:10.1007/BF01100319 (abstract, full text)
  17. ^ D. J. Bohm, B. J. Hiley: Nonlocality and polarization correlations of annihilation quanta, Il Nuovo Cimento B (1971-1996), vol. 35, no. 1, pp. 137-144, 1976, doi:10.1007/BF02726290 (abstract)
  18. ^ Statement on "first presented" quoted from B. J. Hiley: Nonlocality in microsystems, in: Joseph S. King, Karl H. Pribram (eds.): Scale in Conscious Experience: Is the Brain Too Important to be Left to Specialists to Study?, Psychology Press, 1995, pp. 318 ff., p. 319, which takes reference to: C. Philippidis, C. Dewdney and B. J. Hiley: Quantum interference and the quantum potential, Il Nuovo Cimento B, Volume 52, Number 1, pp. 15-28, 1979, doi:10.1007/BF02743566 (abstract)
  19. ^ C. Philippidis, C. Dewdney and B. J. Hiley: Quantum interference and the quantum potential, Il Nuovo Cimento B, Volume 52, Number 1, pp. 15-28, 1979, doi:10.1007/BF02743566 (abstract)
  20. ^ C. Dewdney, B. J. Hiley: A quantum potential description of one-dimensional time-dependent scattering from square barriers and square wells, Foundations of Physics, Volume 12, Number 1, pp. 27–48, 1982, doi:10.1007/BF00726873 (abstract)
  21. ^ Olival Freire jr.: A story without an ending: the quantum physics controversy 1950–1970, Science & Education, vol. 12, pp. 573–586, 2003, p. 576
  22. ^ D. Bohm and B. J. Hiley: On the Aharonov-Bohm effect, Il Nuovo Cimento A, Volume 52, Number 3, pp. 295-308, 1979, doi:10.1007/BF02770900 (abstract)
  23. ^ David Bohm, Basil Hiley: The de Broglie pilot wave theory and the further development and new insights arising out of it, Foundations of Physics, volume 12, number 10, 1982, Appendix: On the background of the papers on trajectories interpretation, by D. Bohm, (PDF)
  24. ^ David J. Bohm, Basil J. Hiley: Some Remarks on Sarfatti's Proposed Connection Between Quantum Phenomena and the Volitional Activity of the Observer-Participator. Psychoenergetic Systems 1: 173-179, 1976
  25. ^ David J. Bohm, Basil J. Hiley: Einstein and Non-Locality in the Quantum Theory. In Einstein: The First Hundred Years, ed. Maurice Goldsmith, Alan Mackay, and James Woudhugsen, pp. 47-61. Oxford: Pergamon Press, 1980
  26. ^ D. Bohm, B. J. Hiley: Nonlocality in quantum theory understood in terms of Einstein's nonlinear field approach, Foundations of Physics, Volume 11, Numbers 7-8, pp. 529-546, 1981, doi:10.1007/BF00726935 (abstract)
  27. ^ a b D. Bohm, B. J. Hiley: Measurement understood through the quantum potential approach, Foundations of Physics, Volume 14, Number 3, pp. 255-274, 1984, doi:10.1007/BF00730211 (abstract)
  28. ^ D. Bohm, B. J. Hiley: Unbroken Quantum Realism, from Microscopic to Macroscopic Levels, Physics Review Letters, vol. 55, no. 23, pp. 2511–2514, 1985, doi:10.1103/PhysRevLett.55.2511 (abstract)
  29. ^ See also the citation of Bohm and Hiley's article Unbroken Quantum Realism, from Microscopic to Macroscopic Levels by David Hestenes: "Bohm and Hiley, among others, have argued forcefully that the identification of bicharacteristics of the Schrödinger wave function with possible electron paths lead to sensible particle interpretations of electron interference and tunneling as well as other aspects of Schrödinger electron theory." David Hestenes: On decoupling probability from kinematics in quantum mechanics, In: P.F. Fougère (ed.): Maximum Entropy and Bayesian Methods, Kluwer Academic Publishers, 1990, pp. 161–183
  30. ^ With reference to Bohm's publication of 1952, cited from Basil J. Hiley: The role of the quantum potential. In: G. Tarozzi, Alwyn Van der Merwe: Open questions in quantum physics: invited papers on the foundations of microphysics, Springer, 1985, pages 237 ff., therein page 238
  31. ^ Interview with Basil Hiley conducted by M. Perus, downloaded February 15, 2012
  32. ^ Basil J. Hiley: The role of the quantum potential. In: G. Tarozzi, Alwyn Van der Merwe: Open questions in quantum physics: invited papers on the foundations of microphysics, Springer, 1985, pages 237 ff., therein page 239
  33. ^ P.N. Kaloyerou, Investigation of the Quantum Potential in the Relativistic Domain, PhD. Thesis, Birkbeck College, London (1985)
  34. ^ D. Bohm, B. J. Hiley, P. N. Kaloyerou: An ontological basis for the quantum theory, Physics Reports (Review section of Physics Letters), volume 144, number 6, pp. 321–375, 1987 (PDF), therein: D. Bohm, B. J. Hiley: I. Non-relativistic particle systems, pp. 321–348, and D. Bohm, B. J. Hiley, P. N. Kaloyerou: II. A causal interpretation of quantum fields, pp. 349–375
  35. ^ P.N. Kaloyerou, Phys. Rep. 244, 288 (1994).
  36. ^ P.N. Kaloyerou, in "Bohmian Mechanics and Quantum Theory: An Appraisal", eds. J.T. Cushing, A. Fine and S. Goldstein, Kluwer, Dordrecht, 155 (1996).
  37. ^ John Bell, Speakable and Unspeakable in Quantum Mechanics
  38. ^ D. Bohm, B. J. Hiley: On the relativistic invariance of a quantum theory based on beables, Foundations of Physics, Volume 21, Number 2, Part V. Invited Papers Dedicated To John Stewart Bell, pp. 243-250, 1991, doi:10.1007/BF01889535 (abstract)
  39. ^ B. J. Hiley, A. H. Aziz Muft: The ontological interpretation of quantum field theory applied in a cosmological context. In: Miguel Ferrero, Alwyn Van der Merwe (eds.): Fundamental problems in quantum physics, Fundamental theories of physics, Kluwer Academic Publishers, 1995, ISBN 0-7923-3670-4, pages 141-156
  40. ^ D. Bohm, B. J. Hiley: Non-locality and locality in the stochastic interpretation of quantum mechanics, Physics Reports, Volume 172, Issue 3, January 1989, Pages 93-122, doi:10.1016/0370-1573(89)90160-9 (abstract)
  41. ^ B. J. Hiley: Active Information and Teleportation, In: Epistemological and Experimental Perspectives on Quantum Physics, D. Greenberger et al. (eds.), pages 113-126, Kluwer, Netherlands, 1999, p. 7
  42. ^ For a "point of view that goes beyond mechanicm", see also Chapter V. of D. Bohm's book "Causality and Chance in Modern Physics, 1957, Routledge, ISBN 0-8122-1002-6
  43. ^ B. J. Hiley: Information, quantum theory and the brain. In: Gordon G. Globus (ed.), Karl H. Pribram (ed.), Giuseppe Vitiello (ed.): Brain and being: at the boundary between science, philosophy, language and arts, Advances in Consciousness Research, John Benjamins B.V., 2004, ISBN 90-272-5194-0, pp. 197-214, see p. 207 and p. 212
  44. ^ a b B. J. Hiley: Nonlocality in microsystems, in: Joseph S. King, Karl H. Pribram (eds.): Scale in Conscious Experience: Is the Brain Too Important to be Left to Specialists to Study?, Psychology Press, 1995, pp. 318 ff., see p. 326–327
  45. ^ B. J. Hiley: Active Information and Teleportation, In: Epistemological and Experimental Perspectives on Quantum Physics, D. Greenberger et al. (eds.), pages 113-126, Kluwer, Netherlands, 1999 (PDF)
  46. ^ O. Maroney, B. J. Hiley: Quantum state teleportation understood through the Bohm interpretation, Foundations of Physics, vol. 29, no. 9, pp. 1403-1415, 1999, doi:10.1023/A:1018861226606 (abstract)
  47. ^ a b David Bohm, Basil J. Hiley, Allan E. G. Stuart: On a new mode of description in physics, International Journal of Theoretical Physics, vol. 3, no. 3, 1970, pp. 171–183, doi:10.1007/BF00671000, abstract
  48. ^ David Bohm: Quantum theory as an indication of a new order in physics. B. Implicate and explicate order in physical law, Foundations of Physics, vol. 3, no. 2, 1973, pp. 139-168, doi:10.1007/BF00708436
  49. ^ David Bohm: Wholeness and the Implicate Order, 1980
  50. ^ David Bohm, F. David Peat: Science, Order, and Creativity, 1987
  51. ^ a b c d D. Bohm, B. J. Hiley: On a quantum algebraic approach to a generalized phase space, Foundations of Physics, vol. 11, no. 3–4, pp. 179–203, 1981, doi:10.1007/BF00726266, abstract/full text
  52. ^ D. Bohm, B.J. Hiley, Relativisitic phase space arising out of Dirac algebra, in Old and New Questions in Physics, Cosmology, Philosophy and Theoretical Biology, A. van der Merwe (ed.), pp. 67-76, Plenum Press, New York
  53. ^ P.R. Holland: Relativistic algebraic spinors and quantum motions in phase space, Foundations of Physics, vol 16, no. 8, 1986, pp. 701-719 doi:10.1007/BF00735377
  54. ^ A.O. Bolivar: Classical limit of bosons in phase space, Physica A: Statistical Mechanics and its Applications, vol. 315, no. 3–4, December 2002, pp. 601–615
  55. ^ a b F. A. M. Frescura, B. J. Hiley: The implicate order, algebras, and the spinor, Foundations of Physics , Volume 10, Numbers 1-2, pp. 7-31, 1980, doi:10.1007/BF00709014 (abstract)
  56. ^ a b F. A. M. Frescura and B. J. Hiley: The algebraization of quantum mechanics and the implicate order, Foundations of Physics, Volume 10, Numbers 9-10, 1980, pp. 705-722, doi:10.1007/BF00708417 (abstract)
  57. ^ a b F. A. M. Frescura, B. J. Hiley: Geometric interpretation of the Pauli spinor, American Journal of Physics, February 1981, Volume 49, Issue 2, pp. 152 (abstract)
  58. ^ a b F. A. M. Frescura, B. J. Hiley: Algebras, quantum theory and pre-space, p. 3–4 (published in Revista Brasileira de Fisica, Volume Especial, Julho 1984, Os 70 anos de Mario Schonberg, pp. 49-86)
  59. ^ a b c d D. Bohm, B. J. Hiley: Generalisation of the twistor to Clifford algebras as a basis for geometry, published in Revista Brasileira de Fisica, Volume Especial, Os 70 anos de Mario Schönberg, pp. 1-26, 1984 (PDF)
  60. ^ B. J. Hiley, F. David Peat: General Introduction: The development of Bohm's ideas from plasma to the implicate order, in: Basil . Hiley, F. David Peat (eds.): Quantum implications: essays in honour of David Bohm, Routledge, 1987, ISBN 0-415-06960-2, pp. 1–32, therein: p. 25
  61. ^ D.J. Bohm, P.G. Davies, B.J. Hiley: Algebraic Quantum Mechanics and Pregeometry, 1981, arXiv:quant-ph/0612002 (submitted 30 November 2006), and its introductory note by B. Hiley: Quantum Space‐Times: An Introduction to “Algebraic Quantum Mechanics and Pregeometry”, AIP Conference Proceedings 810, pp. 312-313, doi:10.1063/1.2158734
  62. ^ "During our discussions the physicist Basil Hiley explained his notions of pre-space—a mathematical structure existing before space-time and matter—to the sculptor Gormley. This led Gormley to make a radical change to his work with the piece Quantum Cloud that is now mounted over the river Thames." F. David Peat: Pathways of Chance, Pari Publishing, 2007, ISBN 978-88-901960-1-0, p. 127
  63. ^ a b c d Basil J. Hiley: Process and the Implicate Order: their relevance to Quantum Theory and Mind. (PDF)
  64. ^ D. J. Bohm, B. H. Hiley, C. Dewdney: A quantum potential approach to the Wheeler delayed-choice experiment, Nature (ISSN 0028-0836), vol. 315, May 23, 1985, pp. 294-297, (abstract)
  65. ^ John Wheeler, cited after Huw Price: Time's Arrow & Archimedes' Point: New Directions for the Physics of Time, Oxford University Press, 1996, ISBN 0-19-510095-6, p. 135
  66. ^ a b B. J. Hiley, R. E. Callaghan: Delayed-choice experiments and the Bohm approach, Physica Scripta, vol. 74, no. 3, pp. 336 ff., 2006, doi:10.1088/0031-8949/74/3/007 (abstract, preprint)
  67. ^ a b B. J. Hiley, R. E. Callaghan: What is Erased in the Quantum Erasure? Foundations of Physics, Volume 36, Number 12, pp. 1869-1883, 2006, doi:10.1007/s10701-006-9086-4 (abstract)
  68. ^ D. Bohm and B. J. Hiley: Statistical mechanics and the ontological interpretation, Foundations of Physics, Volume 26, Number 6, pp. 823–846, 1996, doi:10.1007/BF02058636, Part III. Invited Papers Dedicated to Max Jammer (abstract)
  69. ^ Basil J. Hiley und Allan E. G. Stuart: Phase space, fibre bundles and current algebras, International Journal of Theoretical Physics, Volume 4, Number 4, pp. 247-265, 1971, doi:10.1007/BF00674278 (abstract)
  70. ^ Basil Hiley, Nick Monk: Quantum phase space and the discrete Weyl algebra, Modern Physics Letters A (MPLA), volume 8, number 38, 1993, pp. 3625-3633, doi:10.1142/S0217732393002361 (abstract)
  71. ^ N. A. M. Monk, B. J. Hiley: A Unified Algebraic Approach to Quantum Theory, Foundations of Physics Letters, Volume 11, Number 4, 371-377, 1998, doi:10.1023/A:1022181008699 (abstract)
  72. ^ a b c d e M. R. Brown, B. J. Hiley: Schrodinger revisited: an algebraic approach, arXiv.org (submitted 4 May 2000, version of 19 July 2004, retrieved June 3, 2011) (abstract)
  73. ^ B. J. Hiley: A note on the role of idempotents in the extended Heisenberg algebra, Implications, Scientific Aspects of ANPA 22, pp. 107–121, Cambridge, 2001
  74. ^ a b c d e Basil J. Hiley: Towards a Dynamics of Moments: The Role of Algebraic Deformation and Inequivalent Vacuum States, published in: Correlations ed. K. G. Bowden, Proc. ANPA 23, 104-134, 2001 (PDF)
  75. ^ a b c d B.J. Hiley: Non-Commutative Quantum Geometry: A Reappraisal of the Bohm Approach to Quantum Theory. In: Avshalom C. Elitzur, Shahar Dolev, Nancy Kolenda (eds.): Quo Vadis Quantum Mechanics? The Frontiers Collection, 2005, pp. 299-324, doi:10.1007/3-540-26669-0_16 (abstract, preprint)
  76. ^ a b c B. J. Hiley, R. E. Callaghan: The Clifford Algebra approach to Quantum Mechanics A: The Schroedinger and Pauli Particles, arXiv.org (submitted on 17 Nov 2010 - abstract)
  77. ^ a b B. J. Hiley, R. E. Callaghan: The Clifford Algebra Approach to Quantum Mechanics B: The Dirac Particle and its relation to the Bohm Approach, arXiv:1011.4033 (submitted on 17 Nov 2010)
  78. ^ a b c d B. J. Hiley and R. E. Callaghan: Clifford Algebras and the Dirac-Bohm Quantum Hamilton-Jacobi Equation, Foundations of Physics, published online 20 May 2011, doi:10.1007/s10701-011-9558-z (abstract, 2010 preprint by B. Hiley)
  79. ^ a b Basil J. Hiley: Bohm Interpretation of Quantum Mechanics, Compendium of Quantum Physics, 2009, 43-47, doi:10.1007/978-3-540-70626-7_15 (abstract)
  80. ^ a b c d e B.J. Hiley: Process, distinction, groupoids and Clifford algebras: an alternative view of the quantum formalism, New Structures for Physics, Lecture Notes in Physics, 2011, Volume 813/2011, 705-752, doi:10.1007/978-3-642-12821-9_12 (abstract, PDF)
  81. ^ Oliver Cohen und Basil J. Hiley: Retrodiction in quantum mechanics, preferred Lorentz frames, and nonlocal measurements, Foundations of Physics, Volume 25, Number 12, pp. 1669-1698, 1995, doi:10.1007/BF02057882 (abstract)
  82. ^ O. Cohen, B. J. Hiley: Reexamining the assumption that elements of reality can be Lorentz invariant, Physics Review A, vol. 52, no. 1, pp. 76–81 (1995) doi:10.1103/PhysRevA.52.76 (abstract)
  83. ^ O. Cohen, B. J. Hiley: Elements of reality, Lorentz invariance, and the product rule, Foundations of Physics, Volume 26, Number 1, pp. 1–15, 1996, doi:10.1007/BF02058886 (abstract)
  84. ^ Basil J. Hiley: Bohm's Approach to the EPR Paradox, Compendium of Quantum Physics, 2009, pp. 55-58, doi:10.1007/978-3-540-70626-7_17 (abstract)
  85. ^ a b c Basil Hiley: Mind and matter: aspects of the implicate order described through algebra, published in: Karl H. Pribram, J. King (eds.): Learning as Self-Organization, pp. 569–586, Lawrence Erlbaum Associates, New Jersey, 1996, ISBN 978-0-8058-2586-2
  86. ^ a b c Basil J. Hiley, Marco Fernandes: Process and time, in: H. Atmanspacher, E. Ruhnau: Time, temporality, now: experiencing time and concepts of time in an interdisciplinary perspective, pp. 365–383, Springer, 1997, ISBN 978-3-540-62486-8 (preprint)
  87. ^ Melin Brown, Birkbeck College
  88. ^ M. R. Brown: The quantum potential: the breakdown of classical symplectic symmetry and the energy of localisation and dispersion, arXiv.org quant-ph/9703007 (submitted on 6 Mar 1997, version of 5 Feb 2002, verified from version 1 as retrieved on 20 October 2012)
  89. ^ a b Ignazio Licata: Emergence and computation at the edge of classical and quantum systems, in: Ignazio Licata, Ammar Sakaji (eds.): Physics of Emergence and Organization, World Scientific, 2008, pp. 1–26, ISBN 978-981-277-994-6, arXiv:0711.2973 (submitted 19 November 2007)
  90. ^ M. Heller, W. Sasin: Einstein-Podolski-Rosen Experiment from Noncommutative Quantum Gravity, arXiv:gr-qc/9806011v1 (submitted 3 June 1998). As cited M. R. Brown: The quantum potential: the breakdown of classical symplectic symmetry and the energy of localisation and dispersion, arXiv.org (submitted on 6 Mar 1997, version of 5 Feb 2002, retrieved 18 March 2012) (abstract)
  91. ^ a b B. J. Hiley: Phase space descriptions of quantum phenomena, in: A. Khrennikov (ed.): Quantum Theory: Re-consideration of Foundations–2, pp. 267-286, Växjö University Press, Sweden, 2003 (PDF)
  92. ^ B. Hiley: Moyal's characteristic function, the density matrix and von Neumann's idempotent (preprint)
  93. ^ Maurice A. de Gosson: "The Principles of Newtonian and Quantum Mechanics – The Need for Planck's Constant, h", Imperial College Press, World Scientific Publishing, 2001, ISBN 1-86094-274-1
  94. ^ B.J. Hiley: Phase space description of quantum mechanics and non-commutative geometry: Wigner–Moyal and Bohm in a wider context, In: Theo M. Nieuwenhuizen et al (eds.): Beyond the quantum, World Scientific Publishing, 2007, ISBN 978-981-277-117-9, pp. 203–211, therein p. 204 (preprint)
  95. ^ Basil J. Hiley: Clifford algebras as a vehicle for quantum mechanics without wave functions: The Bohm model of the Dirac equation, Vienna Symposium on the Foundations of Modern Physics 2009 (abstract)
  96. ^ Maurice A. de Gosson, Basil J. Hiley: Imprints of the Quantum World in Classical Mechanics, Foundations of Physics, doi:10.1007/s10701-011-9544-5 (abstract, arXiv:1001.4632 submitted 26 January 2010, version of 15 December 2010)
  97. ^ Ernst Binz, Maurice A. de Gosson, Basil J. Hiley: Clifford Algebras in Symplectic Geometry and Quantum Mechanics, arXiv:1112.2378v1 (submitted on 11 Dec 2011)
  98. ^ Maurice A. de Gosson, Basil J. Hiley: Zeno paradox for Bohmian trajectories: the unfolding of the metatron, January 3, 2011 (PDF - retrieved 7 June 2011)
  99. ^ Partha Ghose, A.S. Majumdar, S. Guhab, J. Sau: Bohmian trajectories for photons, Physics Letters A 290 (2001), pp. 205–213, 10 November 2001
  100. ^ Sacha Kocsis, Sylvain Ravets, Boris Braverman, Krister Shalm, Aephraim M. Steinberg: Observing the trajectories of a single photon using weak measurement, 19th Australian Instuturte of Physics (AIP) Congress, 2010 [1]
  101. ^ Sacha Kocsis, Boris Braverman, Sylvain Ravets, Martin J. Stevens, Richard P. Mirin, L. Krister Shalm, Aephraim M. Steinberg: Observing the Average Trajectories of Single Photons in a Two-Slit Interferometer, Science, vol. 332 no. 6034 pp.&nbsp:1170-1173, 3 June 2011, doi:10.1126/science.1202218 (abstract)
  102. ^ B. Hiley: Weak values: Approach through the Clifford and Moyal algebras, arXiv:1111.6536v1 (submitted on 28 November 2011)
  103. ^ B. J. Hiley: The conceptual structure of the Bohm interpretation in quantum mechanics. In Kalervo Vihtori Laurikainen, C. Montonen, K. Sunnarborg (eds.): Symposium on the Foundations of Modern Physics 1994: 70 years of matter waves, ISBN 2-86332-169-2, Éditions Frontières, 1994, pages 99-118
  104. ^ B. J. Hiley: ‘Welcher Weg’ experiments from the Bohm perspective, PACS: 03.65.Bz, (PDF)
  105. ^ B. J. Hiley, R.E Callaghan, O. Maroney: Quantum trajectories, real, surreal or an approximation to a deeper process? (submitted on 5 Oct 2000, version of 5 Nov 2000 - abstract, PDF)
  106. ^ B. J. Hiley: Some remarks on the evolution of Bohm's proposals for an alternative to standard quantum mechanics, January 30, 2011, downloaded February 13, 2012 (PDF)
  107. ^ B. J. Hiley: The Bohm approach re-assessed (2010 preprint), p. 6
  108. ^ Basil Hiley: Quantum reality unveiled through process and the implicate order, 20 February 2008, downloaded 5 February 2012
  109. ^ Basil J. Hiley: The Bohm approach re-assessed, p. 9
  110. ^ Bob Coecke, Raymond Lal: Causal categories: relativistically interacting processes, arXiv:1107.6019 (submitted 29 July 2011)
  111. ^ Michael Silberstein, W.M. Stuckey, Timothy McDevitt: Being, becoming and the undivided universe: A dialogue between relational blockworld and the implicate order concerning the unification of relativity and quantum theory, [2] (Submitted 10 August 2011, version of 17 October 2011)
  112. ^ a b Basil J. Hiley, Paavo Pylkkänen: Active information and cognitive science – A reply to Kieseppä, Brain, Mind and Physics, P. Pylkkänen et al (Eds.), IOS Press, 1997, ISBN 90-5199-254-8, p. 64 ff.
  113. ^ Basil J. Hiley, Paavo Pylkkänen: Naturalizing the mind in a quantum framework. In Paavo Pylkkänen and Tere Vadén (eds.): Dimensions of conscious experience, Advances in Consciousness Research, Volume 37, John Benjamins B.V., 2001, ISBN 90-272-5157, pages 119-144
  114. ^ Basil J. Hiley: From the Heisenberg picture to Bohm: a new perspective on active information and its relation to Shannon information , Proc. Conf. Quantum Theory: reconsideration of foundations, A. Khrennikov (ed.), pp. 141-162, Växjö University Press, Sweden, 2002, (PDF)
  115. ^ Basil J. Hiley, Paavo Pylkkänen: Can mind affect matter via active information, Mind & Matter vol. 3, no. 2, pp. 7–27, Imprint Academic, 2005
  116. ^ Basil Hiley: Process and the implicate order: their relevance to quantum theory and mind, p. 14 and p. 25
  117. ^ Basil Hiley: Quantum mechanics and the relationship between mind and matter, in: P. Pylkkanen, P. Pylkko und Antti Hautamaki (eds.): Brain, Mind and Physics (Frontiers in Artificial Intelligence and Applications), IOS Press, 1995, ISBN 978-90-5199-254-0, pp. 37–54, see pp. 51,52
  118. ^ David Bohm Quantum theory versus Copenhagen Interpretation, YouTube
  119. ^ Basil J. Hiley: Non-commutative geometry, the Bohm interpretation and the mind-matter relationship, CASYS 2000, Liège, Belgium, August 7–12, 2000, page 15

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