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interpretations of quantum mechanics
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{{Quantum mechanics|cTopic=Interpretations}}An interpretation of quantum mechanics is an attempt to explain how the mathematical theory of quantum mechanics "corresponds" to reality. Although quantum mechanics has held up to rigorous and extremely precise tests in an extraordinarily broad range of experiments (not one prediction from quantum mechanics is found to be contradicted by experiments), there exist a number of contending schools of thought over their interpretation. These views on interpretation differ on such fundamental questions as whether quantum mechanics is deterministic or random, which elements of quantum mechanics can be considered "real", and what is the nature of measurement, among other matters.Despite nearly a century of debate and experiment, no consensus has been reached amongst physicists and philosophers of physics concerning which interpretation best "represents" reality.Murray Gell-Mann - Quantum Mechanics Interpretations - Feynman Sum over Histories - EPR Bertlemann'weblink P Feynman: Quantum Mechanical View of Reality 1 (Part 1weblink Schlosshauer, Maximilian, Kofler, Johannes, Zeilinger, Anton, 2013-08-01, A snapshot of foundational attitudes toward quantum mechanics, Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics, 44, 3, 222–230, 10.1016/j.shpsb.2013.04.004, 1355-2198, 1301.1069,

History

{{multiple image| header = Influential figures in the interpretation of quantum mechanics| header_align = center| header_background = #CCCCFF|align=right|direction=horizontal|image1=Erwin Schrodinger2.jpg! Interpre­tation! Year pub­lished! Author(s)! Determin­istic?! Ontologically real wave­function?! Unique history?! Hidden variables?! Collapsing wave­functions?! Observer role?! Local dynamics?! Counter­factually definite?! Extant universal wave­function?| Quantum logic|1936|Garrett Birkhoff| Time-symmetric theories|1955|Satosi Watanabe| {{yes}}| {{no}}| {{yes}}| {{yes}}| {{no}}| {{no}}| {{no}weblink| {{no}}| {{yes}}| Many-worlds interpretation|1957|Hugh Everett| {{yes}}| {{yes}}| {{no}}| {{no}}| {{no}}| {{no}}| {{yes}}| {{no}}| {{yes}}| Stochastic interpretation|1966|Edward Nelson| {{no}}| {{no}}| {{yes}}| Many-minds interpretation|1970|H. Dieter Zeh| {{yes}}| {{yes}}| {{no}}| {{no}}| {{no}}| Consistent histories|1984|Robert B. Griffiths| {{no}}| {{no}}| {{no}}| {{no}}| {{no}}| {{no}}| {{yes}}| {{no}}| {{yes}}| Transactional interpretation|1986|John G. Cramer| {{yes}}| {{yes}}| {{yes}}| {{no}}| QBism|2010| Christopher Fuchs, Ruediger Schack| {{no}}
Erwin Schrödinger>Schrödinger|width1=150|image2=Max Born.jpgMax Born>Born|width2=147|image3=Niels Bohr.jpgNiels Bohr>Bohr|width3=135}}The definition of quantum theorists' terms, such as wave functions and matrix mechanics, progressed through many stages. For instance, Erwin Schrödinger originally viewed the electron's wave function as its charge density smeared across space, whereas Max Born reinterpreted the absolute square value of the wave function as the electron's probability density distributed across space.The views of several early pioneers of quantum mechanics, such as Niels Bohr and Werner Heisenberg, are often grouped together as the "Copenhagen interpretation", though physicists and historians of physics have argued that this terminology obscures differences between the views so designated.BOOK, Jammer, Max, Max Jammer, Philosophy of Quantum Mechanics: The interpretations of quantum mechanics in historical perspective, 1974, Wiley-Interscience, JOURNAL, Camilleri, Kristian, 2009-02-01, Constructing the Myth of the Copenhagen Interpretation,weblink Perspectives on Science, 17, 1, 26–57, 1530-9274, 10.1162/posc.2009.17.1.26, While Copenhagen-type ideas were never universally embraced, challenges to a perceived Copenhagen orthodoxy gained increasing attention in the 1950s with the pilot-wave interpretation of David Bohm and the many-worlds interpretation of Hugh Everett III.Vaidman, L. (2002, March 24). Many-Worlds Interpretation of Quantum Mechanics. Retrieved March 19, 2010, from Stanford Encyclopedia of Philosophy:weblink Frank J. Tipler, The Physics of Immortality: Modern Cosmology, God, and the Resurrection of the Dead,weblink 1994, Anchor Books, 978-0-385-46799-5, Moreover, the strictly formalist position, shunning interpretation, has been challenged by proposals for falsifiable experiments that might one day distinguish among interpretations, as by measuring an AI consciousnessQuantum theory as a universal physical theory, by David Deutsch, International Journal of Theoretical Physics, Vol 24 #1 (1985) or via quantum computing.Three connections between Everett's interpretation and experiment Quantum Concepts of Space and Time, by David Deutsch, Oxford University Press (1986){{Primary source inline|date=July 2019|reason=We shouldn't just cite Deutsch for Deutsch's ideas; the community seems as divided about what QC implies for foundations as it is for anything else involving foundations}}The physicist N. David Mermin once quipped, "New interpretations appear every year. None ever disappear."JOURNAL, Mermin, N. David, 2012-07-01, Commentary: Quantum mechanics: Fixing the shifty split, Physics Today, 65, 7, 8–10, 10.1063/PT.3.1618, 0031-9228, 2012PhT....65g...8M, As a rough guide to development of the mainstream view during the 1990s to 2000s, consider the "snapshot" of opinions collected in a poll by Schlosshauer et al. at the "Quantum Physics and the Nature of Reality" conference of July 2011.JOURNAL, 1301.1069
, A Snapshot of Foundational Attitudes Toward Quantum Mechanics
, Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics
, 44
, 3
, 222–230
, 2013-01-06
, Schlosshauer
, Maximilian
, Kofler
, Johannes
, Zeilinger
, Anton
, Anton Zeilinger
, 10.1016/j.shpsb.2013.04.004
, 2013SHPMP..44..222S
,
The authors reference a similarly informal poll carried out by Max Tegmark at the "Fundamental Problems in Quantum Theory" conference in August 1997. The main conclusion of the authors is that "the Copenhagen interpretation still reigns supreme", receiving the most votes in their poll (42%), besides the rise to mainstream notability of the many-worlds interpretations:
"The Copenhagen interpretation still reigns supreme here, especially if we lump it together with intellectual offsprings such as information-based interpretations and the Quantum Bayesian interpretation. In Tegmark's poll, the Everett interpretation received 17% of the vote, which is similar to the number of votes (18%) in our poll."

Nature

More or less, all interpretations of quantum mechanics share two qualities:
  1. They interpret a formalism—a set of equations and principles to generate predictions via input of initial conditions
  2. They interpret a phenomenology—a set of observations, including those obtained by empirical research and those obtained informally, such as humans' experience of an unequivocal world
Two qualities vary among interpretations:
  1. Ontology—claims about what things, such as categories and entities, exist in the world
  2. Epistemology—claims about the possibility, scope, and means toward relevant knowledge of the world
In philosophy of science, the distinction of knowledge versus reality is termed epistemic versus ontic. A general law is a regularity of outcomes (epistemic), whereas a causal mechanism may regulate the outcomes (ontic). A phenomenon can receive interpretation either ontic or epistemic. For instance, indeterminism may be attributed to limitations of human observation and perception (epistemic), or may be explained as a real existing maybe encoded in the universe (ontic). Confusing the epistemic with the ontic, like if one were to presume that a general law actually "governs" outcomes—and that the statement of a regularity has the role of a causal mechanism—is a category mistake.In a broad sense, scientific theory can be viewed as offering scientific realism—approximately true description or explanation of the natural world—or might be perceived with antirealism. A realist stance seeks the epistemic and the ontic, whereas an antirealist stance seeks epistemic but not the ontic. In the 20th century's first half, antirealism was mainly logical positivism, which sought to exclude unobservable aspects of reality from scientific theory.{{anchor|shutup}}Since the 1950s, antirealism is more modest, usually instrumentalism, permitting talk of unobservable aspects, but ultimately discarding the very question of realism and posing scientific theory as a tool to help humans make predictions, not to attain metaphysical understanding of the world. The instrumentalist view is carried by the famous quote of David Mermin, "Shut up and calculate", often misattributed to Richard Feynman.For a discussion of the provenance of the phrase "shut up and calculate", see JOURNAL, 10.1063/1.1768652, Could Feynman have said this?, Physics Today, 57, 5, 10–11, 2004, Mermin, N. David, 2004PhT....57e..10M, Other approaches to resolve conceptual problems introduce new mathematical formalism, and so propose alternative theories with their interpretations. An example is Bohmian mechanics, whose empirical equivalence with the three standard formalisms—Schrödinger's wave mechanics, Heisenberg's matrix mechanics, and Feynman's path integral formalism—has been demonstrated.

Challenges

  1. Abstract, mathematical nature of quantum field theories: the mathematical structure of quantum mechanics is mathematically abstract without clear interpretation of its quantities.
  2. Existence of apparently indeterministic and irreversible processes: in classical field theory, a physical property at a given location in the field is readily derived. In most mathematical formulations of quantum mechanics, measurement is given a special role in the theory, as it is the sole process that can cause a nonunitary, irreversible evolution of the state.
  3. Role of the observer in determining outcomes: the Copenhagen Interpretation implies that the wavefunction is a calculational tool, and represents reality only immediately after a measurement, perhaps performed by an observer; Everettian interpretations grant that all the possibilities can be real, and that the process of measurement-type interactions cause an effective branching process.Guido Bacciagaluppi, "The role of decoherence in quantum mechanics", The Stanford Encyclopedia of Philosophy (Winter 2012), Edward N Zalta, ed.
  4. Classically unexpected correlations between remote objects: entangled quantum systems, as illustrated in the EPR paradox, obey statistics that seem to violate principles of local causality.La nouvelle cuisine, by John S Bell, last article of Speakable and Unspeakable in Quantum Mechanics, second edition.
  5. Complementarity of proffered descriptions: complementarity holds that no set of classical physical concepts can simultaneously refer to all properties of a quantum system. For instance, wave description A and particulate description B can each describe quantum system S, but not simultaneously. This implies the composition of physical properties of S does not obey the rules of classical propositional logic when using propositional connectives (see "Quantum logic"). Like contextuality, the "origin of complementarity lies in the non-commutativity of operators" that describe quantum objects (Omnès 1999).
  6. Rapidly rising intricacy, far exceeding humans' present calculational capacity, as a system's size increases: since the state space of a quantum system is exponential in the number of subsystems, it is difficult to derive classical approximations.
  7. Contextual behaviour of systems locally: Quantum contextuality demonstrates that classical intuitions in which properties of a system hold definite values, independent of the manner of their measurement, fails even for local systems. Also, physical principles such as Leibniz's Principle of the identity of indiscernibles no longer apply in the quantum domain, signalling that most classical intuitions may be incorrect about the quantum world.

Summaries

Classification adopted by Einstein

An interpretation (i.e. a semantic explanation of the formal mathematics of quantum mechanics) can be characterized by its treatment of certain matters addressed by Einstein, such as: To explain these properties, we need to be more explicit about the kind of picture an interpretation provides. To that end we will regard an interpretation as a correspondence between the elements of the mathematical formalism M and the elements of an interpreting structure I, where:
  • The mathematical formalism M consists of the Hilbert space machinery of ket-vectors, self-adjoint operators acting on the space of ket-vectors, unitary time dependence of the ket-vectors, and measurement operations. In this context a measurement operation is a transformation which turns a ket-vector into a probability distribution (for a formalization of this concept see quantum operations).
  • The interpreting structure I includes states, transitions between states, measurement operations, and possibly information about spatial extension of these elements. A measurement operation refers to an operation which returns a value and might result in a system state change. Spatial information would be exhibited by states represented as functions on configuration space. The transitions may be non-deterministic or probabilistic or there may be infinitely many states.
The crucial aspect of an interpretation is identifying which, if any, of the elements of I are regarded as physically real.The current usage of realism and completeness originated in the 1935 paper in which Einstein and others proposed the EPR paradox.JOURNAL, Einstein, A., Podolsky, B., Rosen, N., 1935, Can quantum-mechanical description of physical reality be considered complete?,weblink Phys. Rev., 47, 10, 777–780, 10.1103/physrev.47.777, 1935PhRv...47..777E, In that paper the authors proposed the concepts element of reality and the completeness of a physical theory. They characterised element of reality as a quantity whose value can be predicted with certainty before measuring or otherwise disturbing it, and defined a complete physical theory as one in which every element of physical reality is accounted for by the theory. In a semantic view of interpretation, an interpretation is complete if every element of the interpreting structure is present in the mathematics. Realism is also a property of each of the elements of the maths; an element is real if it corresponds to something in the interpreting structure. For example, in some interpretations of quantum mechanics (such as the many-worlds interpretation) the ket vector associated to the system state is said to correspond to an element of physical reality, while in other interpretations it is not.Determinism is a property characterizing state changes due to the passage of time, namely that the state at a future instant is a function of the state in the present (see time evolution). It may not always be clear whether a particular interpretation is deterministic or not, as there may not be a clear choice of a time parameter. Moreover, a given theory may have two interpretations, one of which is deterministic and the other not.Local realism has two aspects:
  • The value returned by a measurement corresponds to the value of some function in the state space. In other words, that value is an element of reality;
  • The effects of measurement have a propagation speed not exceeding some universal limit (e.g. the speed of light). In order for this to make sense, measurement operations in the interpreting structure must be localized.
A precise formulation of local realism in terms of a local hidden-variable theory was proposed by John Bell.Bell's theorem, combined with experimental testing, restricts the kinds of properties a quantum theory can have, the primary implication being that quantum mechanics cannot satisfy both the principle of locality and counterfactual definiteness.Regardless of Einstein's concerns about interpretation issues, Dirac and other quantum notables embraced the technical advances of the new theory while devoting little or no attention to interpretational aspects.

Copenhagen interpretation

The Copenhagen interpretation is the "standard" interpretation of quantum mechanics formulated by Niels Bohr and Werner Heisenberg while collaborating in Copenhagen around 1927. Bohr and Heisenberg extended the probabilistic interpretation of the wavefunction proposed originally by Max Born. The Copenhagen interpretation rejects questions like "where was the particle before I measured its position?" as meaningless. The measurement process randomly picks out exactly one of the many possibilities allowed for by the state's wave function in a manner consistent with the well-defined probabilities that are assigned to each possible state. According to the interpretation, the interaction of an observer or apparatus that is external to the quantum system is the cause of wave function collapse, thus according to Paul Davies, "reality is in the observations, not in the electron"weblink In general, after a measurement (click of a Geiger counter or a trajectory in a spark or bubble chamber) it ceases to be relevant unless subsequent experimental observations can be performed.

Many worlds

The many-worlds interpretation is an interpretation of quantum mechanics in which a universal wavefunction obeys the same deterministic, reversible laws at all times; in particular there is no (indeterministic and irreversible) wavefunction collapse associated with measurement. The phenomena associated with measurement are claimed to be explained by decoherence, which occurs when states interact with the environment producing entanglement, repeatedly "splitting" the universe into mutually unobservable alternate histories—effectively distinct universes within a greater multiverse.

Consistent histories

The consistent histories interpretation generalizes the conventional Copenhagen interpretation and attempts to provide a natural interpretation of quantum cosmology. The theory is based on a consistency criterion that allows the history of a system to be described so that the probabilities for each history obey the additive rules of classical probability. It is claimed to be consistent with the Schrödinger equation.According to this interpretation, the purpose of a quantum-mechanical theory is to predict the relative probabilities of various alternative histories (for example, of a particle).

Ensemble interpretation

The ensemble interpretation, also called the statistical interpretation, can be viewed as a minimalist interpretation. That is, it claims to make the fewest assumptions associated with the standard mathematics. It takes the statistical interpretation of Born to the fullest extent. The interpretation states that the wave function does not apply to an individual system{{spaced ndash}}for example, a single particle{{spaced ndash}}but is an abstract statistical quantity that only applies to an ensemble (a vast multitude) of similarly prepared systems or particles. Probably the most notable supporter of such an interpretation was Einstein:The most prominent current advocate of the ensemble interpretation is Leslie E. Ballentine, professor at Simon Fraser University, author of the graduate level text book Quantum Mechanics, A Modern Development. An experiment illustrating the ensemble interpretation is provided in Akira Tonomura's Video clip 1.WEB,weblink
, An experiment illustrating the ensemble interpretation
, Hitachi.com
,
, 2011-01-24, It is evident from this double-slit experiment with an ensemble of individual electrons that, since the quantum mechanical wave function (absolutely squared) describes the completed interference pattern, it must describe an ensemble.

De Broglie–Bohm theory

The de Broglie–Bohm theory of quantum mechanics (also known as the pilot wave theory) is a theory by Louis de Broglie and extended later by David Bohm to include measurements. Particles, which always have positions, are guided by the wavefunction. The wavefunction evolves according to the Schrödinger wave equation, and the wavefunction never collapses. The theory takes place in a single space-time, is non-local, and is deterministic. The simultaneous determination of a particle's position and velocity is subject to the usual uncertainty principle constraint. The theory is considered to be a hidden-variable theory, and by embracing non-locality it satisfies Bell's inequality. The measurement problem is resolved, since the particles have definite positions at all times.JOURNAL, Maudlin, T., 1995, Why Bohm's Theory Solves the Measurement Problem, Philosophy of Science, 62, 3, 479–483, 10.1086/289879, Collapse is explained as (wikt:phenomenology|phenomenological).ARXIV, Durr, D., Zanghi, N., Goldstein, S., quant-ph/9511016, Bohmian Mechanics as the Foundation of Quantum Mechanics , Nov 14, 1995, Also published in BOOK, J.T. Cushing, Arthur Fine, S. Goldstein, Bohmian Mechanics and Quantum Theory: An Appraisal,weblink 17 April 2013, Springer Science & Business Media, 978-94-015-8715-0, 21–43,

Relational quantum mechanics

The essential idea behind relational quantum mechanics, following the precedent of special relativity, is that different observers may give different accounts of the same series of events: for example, to one observer at a given point in time, a system may be in a single, "collapsed" eigenstate, while to another observer at the same time, it may be in a superposition of two or more states. Consequently, if quantum mechanics is to be a complete theory, relational quantum mechanics argues that the notion of "state" describes not the observed system itself, but the relationship, or correlation, between the system and its observer(s). The state vector of conventional quantum mechanics becomes a description of the correlation of some degrees of freedom in the observer, with respect to the observed system. However, it is held by relational quantum mechanics that this applies to all physical objects, whether or not they are conscious or macroscopic. Any "measurement event" is seen simply as an ordinary physical interaction, an establishment of the sort of correlation discussed above. Thus the physical content of the theory has to do not with objects themselves, but the relations between them.WEB,weblink
, Relational Quantum Mechanics (Stanford Encyclopedia of Philosophy)
, Plato.stanford.edu
,
, 2011-01-24, For more information, see JOURNAL, 10.1007/BF02302261, Carlo Rovelli, 1996, Relational Quantum Mechanics, International Journal of Theoretical Physics, 35, 8, 1637–1678, quant-ph/9609002, 1996IJTP...35.1637R, Carlo Rovelli,
An independent relational approach to quantum mechanics was developed in analogy with David Bohm's elucidation of special relativity,David Bohm, The Special Theory of Relativity, Benjamin, New York, 1965 in which a detection event is regarded as establishing a relationship between the quantized field and the detector. The inherent ambiguity associated with applying Heisenberg's uncertainty principle is subsequently avoided.See relational approach to wave-particle duality. For a full account see JOURNAL, 10.4006/1.3029255,weblink Quantum Optics as a Relativistic Theory of Light, Physics Essays, 9, 3, 447, 1996, Zheng, Qianbing, Kobayashi, Takayoshi, 1996PhyEs...9..447Z, Also, see Annual Report, Department of Physics, School of Science, University of Tokyo (1992) 240.

Transactional interpretation

The transactional interpretation of quantum mechanics (TIQM) by John G. Cramer is an interpretation of quantum mechanics inspired by the Wheeler–Feynman absorber theory.WEB
,weblink
, Quantum Nocality – Cramer
, Npl.washington.edu
, 2011-01-24
, dead
,weblink" title="web.archive.org/web/20101229074514weblink">weblink
, 2010-12-29
, It describes the collapse of the wave function as resulting from a time-symmetric transaction between a possibility wave from the source to the receiver (the wave function) and a possibility wave from the receiver to source (the complex conjugate of the wave function). This interpretation of quantum mechanics is unique in that it not only views the wave function as a real entity, but the complex conjugate of the wave function, which appears in the Born rule for calculating the expected value for an observable, as also real.

Stochastic mechanics

An entirely classical derivation and interpretation of Schrödinger's wave equation by analogy with Brownian motion was suggested by Princeton University professor Edward Nelson in 1966.JOURNAL, Nelson, E, 1966, Derivation of the Schrödinger Equation from Newtonian Mechanics, Phys. Rev., 150, 4, 1079–1085, 10.1103/physrev.150.1079, 1966PhRv..150.1079N, Similar considerations had previously been published, for example by R. Fürth (1933), I. Fényes (1952), and Walter Weizel (1953), and are referenced in Nelson's paper. More recent work on the stochastic interpretation has been done by M. Pavon.JOURNAL, Pavon, M., 2000, Stochastic mechanics and the Feynman integral, J. Math. Phys., 41, 9, 6060–6078, 10.1063/1.1286880, quant-ph/0007015, 2000JMP....41.6060P, An alternative stochastic interpretationJOURNAL, Roumen Tsekov, Bohmian Mechanics versus Madelung Quantum Hydrodynamics, 2012, 112–119, Ann. Univ. Sofia, Fac. Phys., 0904.0723, 2012AUSFP..SE..112T, SE, 10.13140/RG.2.1.3663.8245,weblink was developed by Roumen Tsekov.

Objective collapse theories

Objective collapse theories differ from the Copenhagen interpretation by regarding both the wave function and the process of collapse as ontologically objective (meaning these exist and occur independent of the observer). In objective theories, collapse occurs either randomly ("spontaneous localization") or when some physical threshold is reached, with observers having no special role. Thus, objective-collapse theories are realistic, indeterministic, no-hidden-variables theories. Standard quantum mechanics does not specify any mechanism of collapse; QM would need to be extended if objective collapse is correct. The requirement for an extension to QM means that objective collapse is more of a theory than an interpretation. Examples include

, Frigg, R. GRW theory
, PDF
,
, 2011-01-24,


,weblink
, Review of Penrose's Shadows of the Mind
, Thymos.com
, 1999
, 2011-01-24
,weblink" title="web.archive.org/web/20010209001439weblink">weblink
, 2001-02-09
, dead
,
  • the deterministic variant of an objective collapse theoryArthur Jabs: A conjecture concerning determinism, reduction, and measurement in quantum mechanics, Quantum Studies: Mathematics and Foundations, vol. 3, issue 4, p. 279-292 (2016), DOI 10.1007/s40509-016-0077-7, (arXiv:1204.0614)

Consciousness causes collapse (von Neumann–Wigner interpretation)

In his treatise The Mathematical Foundations of Quantum Mechanics, John von Neumann deeply analyzed the so-called measurement problem. He concluded that the entire physical universe could be made subject to the Schrödinger equation (the universal wave function). He also described how measurement could cause a collapse of the wave function.von Neumann, John. (1932/1955). Mathematical Foundations of Quantum Mechanics. Princeton: Princeton University Press. Translated by Robert T. Beyer. This point of view was prominently expanded on by Eugene Wigner, who argued that human experimenter consciousness (or maybe even dog consciousness) was critical for the collapse, but he later abandoned this interpretation.[Michael Esfeld, (1999), "Essay Review: Wigner's View of Physical Reality", published in Studies in History and Philosophy of Modern Physics, 30B, pp. 145–154, Elsevier Science Ltd.]ARXIV, quant-ph/9501014, Zvi Schreiber, The Nine Lives of Schrödinger's Cat, 1995, Variations of the consciousness causes collapse interpretation include:
Subjective reduction research
This principle, that consciousness causes the collapse, is the point of intersection between quantum mechanics and the mind/body problem; and researchers are working to detect conscious events correlated with physical events that, according to quantum theory, should involve a wave function collapse; but, thus far, results are inconclusive.Dick J. Bierman and Stephen Whitmarsh. (2006). Consciousness and Quantum Physics: Empirical Research on the Subjective Reduction of the State Vector. in Jack A. Tuszynski (Ed). The Emerging Physics of Consciousness. p. 27-48.JOURNAL, Nunn, C. M. H., etal, 1994, Collapse of a Quantum Field may Affect Brain Function. ', Journal of Consciousness Studies, 1, 1, 127–139,
Participatory anthropic principle (PAP)
John Archibald Wheeler's participatory anthropic principle says that consciousness plays some role in bringing the universe into existence.WEB,weblink
, - The anthropic universe
, 2006-02-18
, Abc.net.au
, 2011-01-24,
Other physicists have elaborated their own variations of the consciousness causes collapse interpretation; including:
  • Henry P. Stapp (Mindful Universe: Quantum Mechanics and the Participating Observer)
  • Bruce Rosenblum and Fred Kuttner (Quantum Enigma: Physics Encounters Consciousness)
  • Amit Goswami (The Self-Aware Universe)

Many minds

The many-minds interpretation of quantum mechanics extends the many-worlds interpretation by proposing that the distinction between worlds should be made at the level of the mind of an individual observer.

Quantum logic

Quantum logic can be regarded as a kind of propositional logic suitable for understanding the apparent anomalies regarding quantum measurement, most notably those concerning composition of measurement operations of complementary variables. This research area and its name originated in the 1936 paper by Garrett Birkhoff and John von Neumann, who attempted to reconcile some of the apparent inconsistencies of classical boolean logic with the facts related to measurement and observation in quantum mechanics.

Quantum information theories

Quantum informational approachesNEWS
,weblink
, In the beginning was the bit
, New Scientist
, 2001-02-17
, 2013-01-25, have attracted growing support.NEWS
,weblink
, Quantum physics has been rankling scientists for decades
, Boulder Daily Camera
, Kate Becker
, 2013-01-25
, 2013-01-25, They subdivide into two kindsInformation, Immaterialism, Instrumentalism: Old and New in Quantum Information. Christopher G. Timpson
  • Information ontologies, such as J. A. Wheeler's "it from bit". These approaches have been described as a revival of immaterialismTimpson, Op. Cit.: "Let us call the thought that information might be the basic category from which all else flows informational immaterialism."
  • Interpretations where quantum mechanics is said to describe an observer's knowledge of the world, rather than the world itself. This approach has some similarity with Bohr's thinking."Physics concerns what we can say about nature". (Niels Bohr, quoted in Petersen, A. (1963). The philosophy of Niels Bohr. Bulletin of the Atomic Scientists, 19(7):8–14.) Collapse (also known as reduction) is often interpreted as an observer acquiring information from a measurement, rather than as an objective event. These approaches have been appraised as similar to instrumentalism.
The state is not an objective property of an individual system but is that information, obtained from a knowledge of how a system was prepared, which can be used for making predictions about future measurements....A quantum mechanical state being a summary of the observer's information about an individual physical system changes both by dynamical laws, and whenever the observer acquires new information about the system through the process of measurement. The existence of two laws for the evolution of the state vector...becomes problematical only if it is believed that the state vector is an objective property of the system...The "reduction of the wavepacket" does take place in the consciousness of the observer, not because of any unique physical process which takes place there, but only because the state is a construct of the observer and not an objective property of the physical systemJOURNAL, Hartle, J. B., 1968, Quantum mechanics of individual systems, Am. J. Phys., 36, 8, 704–712, 10.1119/1.1975096, 1968AmJPh..36..704H,

Modal interpretations of quantum theory

Modal interpretations of quantum mechanics were first conceived of in 1972 by B. van Fraassen, in his paper "A formal approach to the philosophy of science." However, this term now is used to describe a larger set of models that grew out of this approach. The Stanford Encyclopedia of Philosophy describes several versions:WEB,weblink
, Modal Interpretations of Quantum Mechanics
, Stanford Encyclopedia of Philosophy
, Science.uva.nl
,
, 2011-01-24,
  • The Copenhagen variant
  • Kochen-Dieks-Healey Interpretations
  • Motivating Early Modal Interpretations, based on the work of R. Clifton, M. Dickson and J. Bub.

Time-symmetric theories

Several theories have been proposed which modify the equations of quantum mechanics to be symmetric with respect to time reversal.JOURNAL, Watanabe, Satosi, 1955, Symmetry of physical laws. Part III. Prediction and retrodiction, Reviews of Modern Physics, 27, 2, 179–186, 10.1103/revmodphys.27.179, 1955RvMP...27..179W, 10945/47584, JOURNAL, Aharonov, Y., etal, 1964, Time Symmetry in the Quantum Process of Measurement, Phys. Rev., 134, 6B, B1410–1416, 10.1103/physrev.134.b1410, 1964PhRv..134.1410A, Aharonov, Y. and Vaidman, L. "On the Two-State Vector Reformulation of Quantum Mechanics." Physica Scripta, Volume T76, pp. 85-92 (1998).JOURNAL, Wharton, K. B., 2007, Time-Symmetric Quantum Mechanics, Foundations of Physics, 37, 1, 159–168, 10.1007/s10701-006-9089-1, 2007FoPh...37..159W, JOURNAL, Wharton, K. B., 2010, A Novel Interpretation of the Klein–Gordon Equation, Foundations of Physics, 40, 3, 313–332, 10.1007/s10701-009-9398-2, 2010FoPh...40..313W, 0706.4075, JOURNAL, Heaney, M. B., 2013, A Symmetrical Interpretation of the Klein–Gordon Equation, Foundations of Physics, 43, 6, 733–746, 10.1007/s10701-013-9713-9, 1211.4645, 2013FoPh...43..733H, (E.g. see Wheeler-Feynman time-symmetric theory). This creates retrocausality: events in the future can affect ones in the past, exactly as events in the past can affect ones in the future. In these theories, a single measurement cannot fully determine the state of a system (making them a type of hidden-variables theory), but given two measurements performed at different times, it is possible to calculate the exact state of the system at all intermediate times. The collapse of the wavefunction is therefore not a physical change to the system, just a change in our knowledge of it due to the second measurement. Similarly, they explain entanglement as not being a true physical state but just an illusion created by ignoring retrocausality. The point where two particles appear to "become entangled" is simply a point where each particle is being influenced by events that occur to the other particle in the future.Not all advocates of time-symmetric causality favour modifying the unitary dynamics of standard quantum mechanics. Thus a leading exponent of the two-state vector formalism, Lev Vaidman, highlights how well the two-state vector formalism dovetails with Hugh Everett's many-worlds interpretation.Yakir Aharonov, Lev Vaidman: The Two-State Vector Formalism of Quantum Mechanics: an Updated Review. In: Juan Gonzalo Muga, Rafael Sala Mayato, Íñigo Egusquiza (eds.): Time in Quantum Mechanics, Volume 1, Lecture Notes in Physics 734, pp. 399–447, 2nd ed., Springer, 2008, {{ISBN|978-3-540-73472-7}}, {{doi|10.1007/978-3-540-73473-4_13}}, {{arXiv|quant-ph/0105101}}, p. 443

Branching space-time theories

BST theories resemble the many worlds interpretation; however, "the main difference is that the BST interpretation takes the branching of history to be a feature of the topology of the set of events with their causal relationships... rather than a consequence of the separate evolution of different components of a state vector." In MWI, it is the wave functions that branches, whereas in BST, the space-time topology itself branches.BST has applications to Bell's theorem, quantum computation and quantum gravity. It also has some resemblance to hidden-variable theories and the ensemble interpretation: particles in BST have multiple well defined trajectories at the microscopic level. These can only be treated stochastically at a coarse grained level, in line with the ensemble interpretation.Sharlow, Mark; "What Branching Spacetime might do for Physics" p.2

Other interpretations

As well as the mainstream interpretations discussed above, a number of other interpretations have been proposed which have not made a significant scientific impact for whatever reason. These range from proposals by mainstream physicists to the more occult ideas of quantum mysticism.

Comparison

The most common interpretations are summarized in the table below. The values shown in the cells of the table are not without controversy, for the precise meanings of some of the concepts involved are unclear and, in fact, are themselves at the center of the controversy surrounding the given interpretation. For another table comparing interpretations of quantum theory, see reference.BOOK, What is quantum information?, Olimpia, Lombardi, 1979-, Fortin, Sebastian, Federico, Holik, Cristian, López, 2017, 9781107142114, 138–144, 965759965, 1509.04711, 10.1017/9781316494233.009, Interpretations of Quantum Theory: A Map of Madness, No experimental evidence exists that distinguishes among these interpretations. To that extent, the physical theory stands, and is consistent with itself and with reality; difficulties arise only when one attempts to "interpret" the theory. Nevertheless, designing experiments which would test the various interpretations is the subject of active research.Most of these interpretations have variants. For example, it is difficult to get a precise definition of the Copenhagen interpretation as it was developed and argued about by many people.{| class="wikitable sortable" style="text-align:center;"
Ensemble Interpretation>Ensemble interpretation|1926|Max BornAgnostic}}| {{no}}| {{yes}}Agnostic}}| {{no}}| {{no}}| {{no}}| {{no}}| {{no}}
Copenhagen interpretation of quantum mechanics>Copenhagen interpretation|1927|Niels Bohr, Werner Heisenberg| {{no}}note1|1}}| {{yes}}| {{no}}note2|2}}Causal}}| {{yes}}| {{no}}| {{no}}
De Broglie–Bohm theory>de Broglie– Bohm theory|1927- 1952|Louis de Broglie, David Bohm| {{yes}}note3|3}}note4|4}}| {{yes}}Phenomeno­logical}}| {{no}}| {{no}}| {{yes}}| {{yes}}
Agnostic}}Agnostic}}note5|5}}| {{no}}| {{no}}Interpre­tational{{ref6}}}}Agnostic}}| {{no}}| {{no}}
Von Neumann–Wigner interpretation>Consciousness causes collapse|1961- 1993|Eugene Wigner,Henry Stapp| {{no}}| {{yes}}| {{yes}}| {{no}}| {{yes}}Causal}}| {{no}}| {{no}}| {{yes}}
note14|14}}| {{no}}| {{no}}| {{no}}note14|14}}| {{no}}
Interpre­tational{{ref7}}}}| {{yes}}Ill-posed}}| {{yes}}
note8|8}}| {{no}}note12|12}}| {{yes}}| {{no}}
Objective collapse theory>Objective collapse theories|1986- 1989Ghirardi–Rimini–Weber theory>Ghirardi–Rimini–Weber, Penrose interpretation| {{no}}| {{yes}}| {{yes}}| {{no}}| {{yes}}| {{no}}| {{no}}| {{no}}| {{no}}
Relational quantum mechanics>Relational interpretation|1994|Carlo Rovelli| {{no}weblink| {{no}}Agnostic{{ref9}}}}| {{no}}note10|10}}Intrinsic{{ref11}}}}LAST2=ROVELLIDATE=2007-03-01JOURNAL=FOUNDATIONS OF PHYSICSVOLUME=37PAGES=427–445ISSN=0015-9018BIBCODE=2007FOPH...37..427S, | {{no}}| {{no}}
note16|16}}Agnostic{{ref17}}}}| {{no}}note18|18}}Intrinsic{{ref19}}}}| {{yes}}| {{no}}| {{no}}
  • {{note label|note1|1}} According to Bohr, the concept of a physical state independent of the conditions of its experimental observation does not have a well-defined meaning. According to Heisenberg the wavefunction represents a probability, but not an objective reality itself in space and time.
  • {{note label|note2|2}} According to the Copenhagen interpretation, the wavefunction collapses when a measurement is performed.
  • {{note label|note3|3}} Both particle AND guiding wavefunction are real.
  • {{note label|note4|4}} Unique particle history, but multiple wave histories.
  • {{note label|note5|5}} But quantum logic is more limited in applicability than Coherent Histories.
  • {{note label|note6|6}} Quantum mechanics is regarded as a way of predicting observations, or a theory of measurement.
  • {{note label|note7|7}} Observers separate the universal wavefunction into orthogonal sets of experiences.
  • {{note label|note8|8}} In the TI the collapse of the state vector is interpreted as the completion of the transaction between emitter and absorber.
  • {{note label|note9|9}} Comparing histories between systems in this interpretation has no well-defined meaning.
  • {{note label|note10|10}} Any physical interaction is treated as a collapse event relative to the systems involved, not just macroscopic or conscious observers.
  • {{note label|note11|11}} The state of the system is observer-dependent, i.e., the state is specific to the reference frame of the observer.
  • {{note label|note12|12}} The transactional interpretation is explicitly non-local.
  • {{note label|note13|13}} The assumption of intrinsic periodicity is an element of non-locality consistent with relativity as the periodicity varies in a causal way.
  • {{note label|note14|14}} In the stochastic interpretation is not possible to define velocities for particles, i.e. the paths are not smooth. Moreover, to know the motion of the particles at any moment, you have to know what the Markov process is. However, once we know the exactly initial conditions and the Markov process, the theory is in fact a realistic interpretation of quantum mechanics.
  • {{note label|note16|16}} A wavefunction merely encodes an agent’s expectations for future experiences. It is no more real than a probability distribution is in subjective Bayesianism.
  • {{note label|note17|17}} Quantum theory is a tool any agent may use to help manage their expectations. The past comes into play only insofar as an agent’s individual experiences and temperament influence their priors.
  • {{note label|note18|18}} Although QBism would eschew this terminology. A change in the wavefunction that an agent ascribes to a system as a result of having an experience represents a change in his or her beliefs about further experiences they may have. See Doxastic logic.
  • {{note label|note19|19}} Observers, or more properly, participants, are as essential to the formalism as the systems they interact with.

The silent approach

Although interpretational opinions are openly and widely discussed today, that was not always the case. A notable exponent of a tendency of silence was Paul Dirac who once wrote: "The interpretation of quantum mechanics has been dealt with by many authors, and I do not want to discuss it here. I want to deal with more fundamental things."P. A. M. Dirac, The inadequacies of quantum field theory, in Paul Adrien Maurice Dirac, B. N. Kursunoglu and E. P. Wigner, Eds. (Cambridge University, Cambridge, 1987) p. 194 This position is not uncommon among practitioners of quantum mechanics.BOOK, Quantum Optics for Engineers, CRC, New York, 2014, 978-1439888537, F. J. Duarte, Others, like Nico van Kampen and Willis Lamb, have openly criticized non-orthodox interpretations of quantum mechanics.van Kampen, N. G. (2008). "The scandal of quantum mechanics". Am. J. Phys. 76: 989.Lamb, W. E. (2001). "Super classical quantum mechanics: the best interpretation of nonrelativistic quantum mechanics." Am. J. Phys. 69: 413-421.

See also

{{div col|colwidth=22em}} {{div col end}}

References

{{Reflist}}

Sources

  • JOURNAL, Bub, J., Clifton, R., 1996, A uniqueness theorem for interpretations of quantum mechanics, Studies in History and Philosophy of Modern Physics, 27B, 181–219,
  • Rudolf Carnap, 1939, "The interpretation of physics", in Foundations of Logic and Mathematics of the International Encyclopedia of Unified Science. University of Chicago Press.
  • Dickson, M., 1994, "Wavefunction tails in the modal interpretation" in Hull, D., Forbes, M., and Burian, R., eds., Proceedings of the PSA 1" 366–76. East Lansing, Michigan: Philosophy of Science Association.
  • --------, and Clifton, R., 1998, "Lorentz-invariance in modal interpretations" in Dieks, D. and Vermaas, P., eds., The Modal Interpretation of Quantum Mechanics. Dordrecht: Kluwer Academic Publishers: 9–48.
  • Fuchs, Christopher, 2002, "Quantum Mechanics as Quantum Information (and only a little more)." {{arxiv|quant-ph/0205039}}
  • -------- and A. Peres, 2000, "Quantum theory needs no ‘interpretation’", Physics Today.
  • Herbert, N., 1985. Quantum Reality: Beyond the New Physics. New York: Doubleday. {{ISBN|0-385-23569-0}}.
  • Hey, Anthony, and Walters, P., 2003. The New Quantum Universe, 2nd ed. Cambridge Univ. Press. {{ISBN|0-521-56457-3}}.
  • JOURNAL, Jackiw, Roman, Roman Jackiw, Kleppner, D., 2000, One Hundred Years of Quantum Physics, 10.1126/science.289.5481.893, 17839156, Science (journal), Science, 289, 5481, 893–898, quant-ph/0008092,
  • Max Jammer, 1966. The Conceptual Development of Quantum Mechanics. McGraw-Hill.
  • --------, 1974. The Philosophy of Quantum Mechanics. Wiley & Sons.
  • Al-Khalili, 2003. Quantum: A Guide for the Perplexed. London: Weidenfeld & Nicolson.
  • de Muynck, W. M., 2002. Foundations of quantum mechanics, an empiricist approach. Dordrecht: Kluwer Academic Publishers. {{ISBN|1-4020-0932-1}}.
  • Roland Omnès, 1999. Understanding Quantum Mechanics. Princeton Univ. Press.
  • Karl Popper, 1963. Conjectures and Refutations. London: Routledge and Kegan Paul. The chapter "Three views Concerning Human Knowledge" addresses, among other things, instrumentalism in the physical sciences.
  • Hans Reichenbach, 1944. Philosophic Foundations of Quantum Mechanics. Univ. of California Press.
  • JOURNAL, Tegmark, Max, Max Tegmark, Wheeler, J. A., 2001, 100 Years of Quantum Mysteries, Scientific American, 284, 2, 68–75, 10.1038/scientificamerican0201-68, 2001SciAm.284b..68T,
  • Bas van Fraassen, 1972, "A formal approach to the philosophy of science", in R. Colodny, ed., Paradigms and Paradoxes: The Philosophical Challenge of the Quantum Domain. Univ. of Pittsburgh Press: 303-66.
  • John A. Wheeler and Wojciech Hubert Zurek (eds), Quantum Theory and Measurement, Princeton: Princeton University Press, {{ISBN|0-691-08316-9}}, LoC QC174.125.Q38 1983.

Further reading

Almost all authors below are professional physicists.
  • David Z Albert, 1992. Quantum Mechanics and Experience. Harvard Univ. Press. {{ISBN|0-674-74112-9}}.
  • John S. Bell, 1987. Speakable and Unspeakable in Quantum Mechanics. Cambridge Univ. Press, {{ISBN|0-521-36869-3}}. The 2004 edition ({{ISBN|0-521-52338-9}}) includes two additional papers and an introduction by Alain Aspect.
  • Dmitrii Ivanovich Blokhintsev, 1968. The Philosophy of Quantum Mechanics. D. Reidel Publishing Company. {{ISBN|90-277-0105-9}}.
  • David Bohm, 1980. Wholeness and the Implicate Order. London: Routledge. {{ISBN|0-7100-0971-2}}.
  • ARXIV, Adan Cabello, 15 November 2004, Bibliographic guide to the foundations of quantum mechanics and quantum information, quant-ph/0012089,
  • David Deutsch, 1997. The Fabric of Reality. London: Allen Lane. {{ISBN|0-14-027541-X}}; {{ISBN|0-7139-9061-9}}. Argues forcefully against instrumentalism. For general readers.
  • BOOK, Quantum Optics for Engineers, CRC, New York, 2014, 978-1439888537, F. J. Duarte, Provides a pragmatic perspective on interpretations. For general readers.
  • Bernard d'Espagnat, 1976. Conceptual Foundation of Quantum Mechanics, 2nd ed. Addison Wesley. {{ISBN|0-8133-4087-X}}.
  • Bernard d'Espagnat, 1983. In Search of Reality. Springer. {{ISBN|0-387-11399-1}}.
  • Bernard d'Espagnat, 2003. Veiled Reality: An Analysis of Quantum Mechanical Concepts. Westview Press.
  • Bernard d'Espagnat, 2006. On Physics and Philosophy. Princeton Univ. Press.
  • Arthur Fine, 1986. The Shaky Game: Einstein Realism and the Quantum Theory. Science and its Conceptual Foundations. Univ. of Chicago Press. {{ISBN|0-226-24948-4}}.
  • Ghirardi, Giancarlo, 2004. Sneaking a Look at God's Cards. Princeton Univ. Press.
  • Gregg Jaeger (2009) Entanglement, Information, and the Interpretation of Quantum Mechanics. Springer. {{ISBN|978-3-540-92127-1}}.
  • N. David Mermin (1990) Boojums all the way through. Cambridge Univ. Press. {{ISBN|0-521-38880-5}}.
  • Roland Omnès, 1994. The Interpretation of Quantum Mechanics. Princeton Univ. Press. {{ISBN|0-691-03669-1}}.
  • Roland Omnès, 1999. Understanding Quantum Mechanics. Princeton Univ. Press.
  • Roland Omnès, 1999. Quantum Philosophy: Understanding and Interpreting Contemporary Science. Princeton Univ. Press.
  • Roger Penrose, 1989. The Emperor's New Mind. Oxford Univ. Press. {{ISBN|0-19-851973-7}}. Especially chpt. 6.
  • Roger Penrose, 1994. Shadows of the Mind. Oxford Univ. Press. {{ISBN|0-19-853978-9}}.
  • Roger Penrose, 2004. The Road to Reality. New York: Alfred A. Knopf. Argues that quantum theory is incomplete.
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