Schrödinger's cat explained

In quantum mechanics, Schrödinger's cat is a thought experiment concerning quantum superposition. In the thought experiment, a hypothetical cat may be considered simultaneously both alive and dead, while it is unobserved in a closed box, as a result of its fate being linked to a random subatomic event that may or may not occur. This experiment viewed this way is described as a paradox. This thought experiment was devised by physicist Erwin Schrödinger in 1935[1] in a discussion with Albert Einstein[2] to illustrate what Schrödinger saw as the problems of the Copenhagen interpretation of quantum mechanics.

In Schrödinger's original formulation, a cat, a flask of poison, and a radioactive source are placed in a sealed box. If an internal radiation monitor (e.g. a Geiger counter) detects radioactivity (i.e. a single atom decaying), the flask is shattered, releasing the poison, which kills the cat. The Copenhagen interpretation implies that, after a while, the cat is simultaneously alive and dead. Yet, when one looks in the box, one sees the cat either alive or dead, not both alive and dead. This poses the question of when exactly quantum superposition ends and reality resolves into one possibility or the other.

Although originally a critique on the Copenhagen interpretation, Schrödinger's seemingly paradoxical thought experiment became part of the foundation of quantum mechanics. The scenario is often featured in theoretical discussions of the interpretations of quantum mechanics, particularly in situations involving the measurement problem. As a result, Schrödinger's cat has had enduring appeal in popular culture. The experiment is not intended to be actually performed on a cat, but rather as an easily understandable illustration of the behavior of atoms. Experiments at the atomic scale have been carried out, showing that very small objects may exist as superpositions; but superposing an object as large as a cat would pose considerable technical difficulties.

Fundamentally, the Schrödinger's cat experiment asks how long quantum superpositions last and when (or whether) they collapse. Different interpretations of the mathematics of quantum mechanics have been proposed that give different explanations for this process, but Schrödinger's cat remains an unsolved problem in physics.

Origin and motivation

Schrödinger intended his thought experiment as a discussion of the EPR article—named after its authors Einstein, Podolsky, and Rosen—in 1935.[3] [4] The EPR article highlighted the counterintuitive nature of quantum superpositions, in which a quantum system for two particles does not separate even when the particles are detected far from their last point of contact. The EPR paper concludes with a claim that this lack of separability meant that quantum mechanics as a theory of reality was incomplete.

Schrödinger and Einstein exchanged letters about Einstein's EPR article, in the course of which Einstein pointed out that the state of an unstable keg of gunpowder will, after a while, contain a superposition of both exploded and unexploded states.

To further illustrate, Schrödinger described how one could, in principle, create a superposition in a large-scale system by making it dependent on a quantum particle that was in a superposition. He proposed a scenario with a cat in a closed steel chamber, wherein the cat's life or death depended on the state of a radioactive atom, whether it had decayed and emitted radiation or not. According to Schrödinger, the Copenhagen interpretation implies that the cat remains both alive and dead until the state has been observed. Schrödinger did not wish to promote the idea of dead-and-live cats as a serious possibility; on the contrary, he intended the example to illustrate the absurdity of the existing view of quantum mechanics, and thus he was employing reductio ad absurdum.

Since Schrödinger's time, various interpretations of the mathematics of quantum mechanics have been advanced by physicists, some of which regard the "alive and dead" cat superposition as quite real, others do not.[5] [6] Intended as a critique of the Copenhagen interpretation (the prevailing orthodoxy in 1935), the Schrödinger's cat thought experiment remains a touchstone for modern interpretations of quantum mechanics and can be used to illustrate and compare their strengths and weaknesses.[7]

Thought experiment

Schrödinger wrote:[8]

Schrödinger developed his famous thought experiment in correspondence with Einstein. He suggested this 'quite ridiculous case' to illustrate his conclusion that the wave function cannot represent reality.[9] The wave function description of the complete cat system implies that the reality of the cat mixes the living and dead cat.[9] Einstein was impressed by the ability of the thought experiment to highlight these issues. In a letter to Schrödinger dated 1950, he wrote:[9] Note that the charge of gunpowder is not mentioned in Schrödinger's setup, which uses a Geiger counter as an amplifier and hydrocyanic poison instead of gunpowder. The gunpowder had been mentioned in Einstein's original suggestion to Schrödinger 15 years before, and Einstein carried it forward to the present discussion.

Analysis

In modern terms Schrodinger's hypothetical cat experiment describes the measurement problem: quantum theory describes the cat system as a combination of two possible outcomes but only one outcome is ever observed.[10] [11] The experiment poses the question, "when does a quantum system stop existing as a superposition of states and become one or the other?" (More technically, when does the actual quantum state stop being a non-trivial linear combination of states, each of which resembles different classical states, and instead begin to have a unique classical description?) Standard microscopic quantum mechanics describes multiple possible outcomes of experiments but only one outcome is observed. The thought experiment illustrates this apparent paradox. Our intuition says that the cat cannot be in more than one state simultaneously—yet the quantum mechanical description of the thought experiment requires such a condition.

Interpretations

Since Schrödinger's time, other interpretations of quantum mechanics have been proposed that give different answers to the questions posed by Schrödinger's cat of how long superpositions last and when (or whether) they collapse.

Copenhagen interpretation

See main article: Copenhagen interpretation.

A commonly held interpretation of quantum mechanics is the Copenhagen interpretation.[12] In the Copenhagen interpretation, a system stops being a superposition of states and becomes either one or the other when an observation takes place. This thought experiment makes apparent the fact that the nature of measurement, or observation, is not well-defined in this interpretation, which simply provides no explanation for the nature of the cat while the box is closed. The wavefunction description of the system consists of a superposition of the states "decayed nucleus/dead cat" and "undecayed nucleus/living cat". Only when the box is opened and observed can we make a statement about the cat.[9]

Von Neumann interpretation

See main article: Von Neumann–Wigner interpretation. In 1932, John von Neumann described in his book Mathematical Foundations a pattern where the radioactive source is observed by a device, which itself is observed by another device and so on. It makes no difference in the predictions of quantum theory where along this chain of causal effects the superposition collapses.[13] This potentially infinite chain could be broken if the last device is replaced by a conscious observer. This solved the problem because it was claimed that an individual's consciousness cannot be multiple.[14] Neumann asserted that a conscious observer is necessary for a collapse to one or the other (e.g., either a live cat or a dead cat) of the terms on the right-hand side of a wave function. This interpretation was later adopted by Eugene Wigner, who then rejected the interpretation in a thought experiment known as Wigner's friend.[15]

Wigner supposed that a friend opened the box and observed the cat without telling anyone. From Wigner's conscious perspective, the friend is now part of the wave function and has seen a live cat and seen a dead cat. To a third person's conscious perspective, Wigner himself becomes part of the wave function once Wigner learns the outcome from the friend. This could be extended indefinitely.[15]

A resolution of the paradox is that the triggering of the Geiger counter counts as a measurement of the state of the radioactive substance. Because a measurement has already occurred deciding the state of the cat, the subsequent observation by a human records only what has already occurred.[16] Analysis of an actual experiment by Roger Carpenter and A. J. Anderson found that measurement alone (for example by a Geiger counter) is sufficient to collapse a quantum wave function before any human knows of the result.[17] The apparatus indicates one of two colors depending on the outcome. The human observer sees which color is indicated, but they don't consciously know which outcome the color represents. A second human, the one who set up the apparatus, is told of the color and becomes conscious of the outcome, and the box is opened to check if the outcome matches.[13] However, it is disputed whether merely observing the color counts as a conscious observation of the outcome.[18]

Bohr's interpretation

One of the main scientists associated with the Copenhagen interpretation, Niels Bohr, offered an interpretation that is independent of a subjective observer-induced collapse of the wave function, or of measurement; instead, an "irreversible" or effectively irreversible process causes the decay of quantum coherence, which imparts the classical behavior of "observation" or "measurement".[19] [20] [21] [22] Thus, Schrödinger's cat would be either dead or alive long before the box is observed.[23]

Many-worlds interpretation

See main article: Many-worlds interpretation.

In 1957, Hugh Everett formulated the many-worlds interpretation of quantum mechanics, which does not single out observation as a special process. In the many-worlds interpretation, both alive and dead states of the cat persist after the box is opened, but are decoherent from each other. In other words, when the box is opened, the observer and the possibly-dead cat split into an observer looking at a box with a dead cat and an observer looking at a box with a live cat. But since the dead and alive states are decoherent, there is no communication or interaction between them.

When opening the box, the observer becomes entangled with the cat, so "observer states" corresponding to the cat's being alive and dead are formed; each observer state is entangled, or linked, with the cat so that the observation of the cat's state and the cat's state correspond with each other. Quantum decoherence ensures that the different outcomes have no interaction with each other. Decoherence is generally considered to prevent simultaneous observation of multiple states.[24] [25]

A variant of the Schrödinger's cat experiment, known as the quantum suicide machine, has been proposed by cosmologist Max Tegmark. It examines the Schrödinger's cat experiment from the point of view of the cat, and argues that by using this approach, one may be able to distinguish between the Copenhagen interpretation and many-worlds.

Ensemble interpretation

The ensemble interpretation states that superpositions are nothing but subensembles of a larger statistical ensemble. The state vector would not apply to individual cat experiments, but only to the statistics of many similarly prepared cat experiments. Proponents of this interpretation state that this makes the Schrödinger's cat paradox a trivial matter, or a non-issue.

This interpretation serves to discard the idea that a single physical system in quantum mechanics has a mathematical description that corresponds to it in any way.[26]

Relational interpretation

See main article: Relational quantum mechanics. The relational interpretation makes no fundamental distinction between the human experimenter, the cat, and the apparatus or between animate and inanimate systems; all are quantum systems governed by the same rules of wavefunction evolution, and all may be considered "observers". But the relational interpretation allows that different observers can give different accounts of the same series of events, depending on the information they have about the system.[27] The cat can be considered an observer of the apparatus; meanwhile, the experimenter can be considered another observer of the system in the box (the cat plus the apparatus). Before the box is opened, the cat, by nature of its being alive or dead, has information about the state of the apparatus (the atom has either decayed or not decayed); but the experimenter does not have information about the state of the box contents. In this way, the two observers simultaneously have different accounts of the situation: To the cat, the wavefunction of the apparatus has appeared to "collapse"; to the experimenter, the contents of the box appear to be in superposition. Not until the box is opened, and both observers have the same information about what happened, do both system states appear to "collapse" into the same definite result, a cat that is either alive or dead.

Transactional interpretation

In the transactional interpretation the apparatus emits an advanced wave backward in time, which combined with the wave that the source emits forward in time, forms a standing wave. The waves are seen as physically real, and the apparatus is considered an "observer". In the transactional interpretation, the collapse of the wavefunction is "atemporal" and occurs along the whole transaction between the source and the apparatus. The cat is never in superposition. Rather the cat is only in one state at any particular time, regardless of when the human experimenter looks in the box. The transactional interpretation resolves this quantum paradox.[28]

Objective collapse theories

According to objective collapse theories, superpositions are destroyed spontaneously (irrespective of external observation) when some objective physical threshold (of time, mass, temperature, irreversibility, etc.) is reached. Thus, the cat would be expected to have settled into a definite state long before the box is opened. This could loosely be phrased as "the cat observes itself" or "the environment observes the cat".

Objective collapse theories require a modification of standard quantum mechanics to allow superpositions to be destroyed by the process of time evolution.[29] These theories could ideally be tested by creating mesoscopic superposition states in the experiment. For instance, energy cat states has been proposed as a precise detector of the quantum gravity related energy decoherence models.[30]

Applications and tests

The experiment as described is a purely theoretical one, and the machine proposed is not known to have been constructed. However, successful experiments involving similar principles, e.g. superpositions of relatively large (by the standards of quantum physics) objects have been performed.[31] These experiments do not show that a cat-sized object can be superposed, but the known upper limit on "cat states" has been pushed upwards by them. In many cases the state is short-lived, even when cooled to near absolute zero.

In quantum computing the phrase "cat state" sometimes refers to the GHZ state, wherein several qubits are in an equal superposition of all being 0 and all being 1; e.g.,

|\psi\rangle=

1
\sqrt{2
} \bigg(| 00\ldots0 \rangle + |11\ldots1 \rangle \bigg).

According to at least one proposal, it may be possible to determine the state of the cat before observing it.[38] [39]

Extensions

In August 2020, physicists presented studies involving interpretations of quantum mechanics that are related to the Schrödinger's cat and Wigner's friend paradoxes, resulting in conclusions that challenge seemingly established assumptions about reality.[40] [41] [42]

See also

Further reading

External links

Notes and References

  1. Erwin Schrödinger . Erwin. Schrödinger . Die gegenwärtige Situation in der Quantenmechanik (The Present Situation in Quantum Mechanics) . . 10.1007/BF01491891 . 23 . 48 . 807–812 . Man kann auch ganz burleske Fälle konstruieren. Eine Katze wird in eine Stahlkammer gesperrt, zusammen mit folgender Höllenmaschine (die man gegen den direkten Zugriff der Katze sichern muß): in einem Geigerschen Zählrohr befindet sich eine winzige Menge radioaktiver Substanz, so wenig, daß im Laufe einer Stunde vielleicht eines von den Atomen zerfällt, ebenso wahrscheinlich aber auch keines; geschieht es, so spricht das Zählrohr an und betätigt über ein Relais ein Hämmerchen, das ein Kölbchen mit Blausäure zertrümmert. Hat man dieses ganze System eine Stunde lang sich selbst überlassen, so wird man sich sagen, daß die Katze noch lebt, wenn inzwischen kein Atom zerfallen ist. Der erste Atomzerfall würde sie vergiftet haben. Die Psi-Funktion des ganzen Systems würde das so zum Ausdruck bringen, daß in ihr die lebende und die tote Katze (s.v.v.) [sit venia verbo] zu gleichen Teilen gemischt oder verschmiert sind. Das Typische an solchen Fällen ist, daß eine ursprünglich auf den Atombereich beschränkte Unbestimmtheit sich in grobsinnliche Unbestimmtheit umsetzt, die sich dann durch direkte Beobachtung entscheiden läßt. Das hindert uns, in so naiver Weise ein „verwaschenes Modell“ als Abbild der Wirklichkeit gelten zu lassen. An sich enthielte es nichts Unklares oder Widerspruchsvolles. Es ist ein Unterschied zwischen einer verwackelten oder unscharf eingestellten Photographie und einer Aufnahme von Wolken und Nebelschwaden.. 1935NW.....23..807S . November 1935. 206795705.
  2. Web site: Fine . Arthur . The Einstein-Podolsky-Rosen Argument in Quantum Theory . Stanford Encyclopedia of Philosophy . 11 June 2020.
  3. http://prola.aps.org/abstract/PR/v47/i10/p777_1 Can Quantum-Mechanical Description of Physical Reality Be Considered Complete?
  4. Encyclopedia: Fine . Arthur . The Einstein-Podolsky-Rosen Argument in Quantum Theory . Stanford Encyclopedia of Philosophy . Stanford University . 2017 . 11 April 2021.
  5. Book: Polkinghorne . J. C. . The Quantum World . . 1985 . 67 . 0691023883 . live . https://web.archive.org/web/20150519001623/https://books.google.com/books?id=lp4JPYnLrtEC&pg=PA67&dq=%22schrodinger's+cat%22+%22alive+dead . 2015-05-19 .
  6. Book: Tetlow . Philip . Understanding Information and Computation: From Einstein to Web Science . Gower Publishing, Ltd. . 2012 . 321 . 978-1409440406 . live . https://web.archive.org/web/20150519001741/https://books.google.com/books?id=Rk7O3EG0Xn4C&pg=PA321&dq=%22alive+and+dead%22 . 2015-05-19 .
  7. Lazarou . Dimitris . Interpretation of quantum theory - An overview . 2007 . quant-ph . 0712.3466 .
  8. Trimmer. John D.. The Present Situation in Quantum Mechanics: A Translation of Schrödinger's "Cat Paradox" Paper. Proceedings of the American Philosophical Society. 1980. 124. 5. 323–338. 986572. The English translation here is based on the German original, not on the inaccurate version in this source's translation of the entire article:Schrödinger: "The Present Situation in Quantum Mechanics." 5. Are the Variables Really Blurred?
  9. Book: Baggott, J. E. . The quantum story: a history in 40 moments . 2013 . Oxford Univ. Press . 978-0-19-965597-7 . Impression: 3 . Oxford.
  10. Peres . Asher . January 1988 . Schrödinger's immortal cat . Foundations of Physics . en . 18 . 1 . 57–76 . 10.1007/BF01882873 . 0015-9018.
  11. Schlosshauer . Maximilian . 2005-02-23 . Decoherence, the measurement problem, and interpretations of quantum mechanics . Reviews of Modern Physics . 76 . 4 . 1267–1305 . 10.1103/RevModPhys.76.1267. quant-ph/0312059 .
  12. Book: Wimmel, Hermann. Quantum physics & observed reality: a critical interpretation of quantum mechanics. 9 May 2011. 1992. World Scientific. 978-981-02-1010-6. 2. live. https://web.archive.org/web/20130520185205/http://books.google.com/books?id=-4sJ_fgyZJEC&pg=PA2. 20 May 2013.
  13. Book: Hobson . Art . Tales of the Quantum: Understanding Physics' Most Fundamental Theory . 2017 . Oxford University Press . New York, NY . 9780190679637 . 200–202 . April 8, 2022.
  14. Book: Omnès . Roland . Understanding Quantum Mechanics . 1999 . Princeton University Press . Princeton, New Jersey . 0-691-00435-8 . 60–62 . April 8, 2022.
  15. Book: Levin . Frank S. . Surfing the Quantum World . 2017 . Oxford University Press . New York, NY . 978-0-19-880827-5 . 229–232 . April 8, 2022.
  16. Book: Puri . Ravinder R. . Non-Relativistic Quantum Mechanics . 2017 . Cambridge University Press . Cambridge, United Kingdom . 978-1-107-16436-9 . 146 . April 8, 2022.
  17. The death of Schrödinger's cat and of consciousness-based wave-function collapse . . 2006 . Carpenter RHS, Anderson AJ . 31 . 1 . 45–52. 2010-09-10 . https://web.archive.org/web/20061130173850/http://www.ensmp.fr/aflb/AFLB-311/aflb311m387.pdf . 2006-11-30.
  18. How to Back up or Refute Quantum Theories of Consciousness . Mind and Matter . 2016 . Okón E, Sebastián MA . 14 . 1 . 25–49.
  19. Against 'measurement' . . Physics World . 3 . 8 . 1990 . 33–41 . 10.1088/2058-7058/3/8/26.
  20. Book: . May 16, 1947 . 1985 . Niels Bohr: Collected Works . 6 . Foundations of Quantum Physics I (1926-1932) . Jørgen Kalckar . 451–454 .
  21. Book: To fathom space and time . 121 . Stig Stenholm . Quantum Optics, Experimental Gravitation, and Measurement Theory. Pierre Meystre . Pierre Meystre . Plenum Press . 1983 . The role of irreversibility in the theory of measurement has been emphasized by many. Only this way can a permanent record be obtained. The fact that separate pointer positions must be of the asymptotic nature usually associated with irreversibility has been utilized in the measurement theory of Daneri, Loinger and Prosperi (1962). It has been accepted as a formal representation of Bohr's ideas by Rosenfeld (1966)..
  22. Classical motion of meter variables in the quantum theory of measurement . Fritz Haake . April 1, 1993 . . 10.1103/PhysRevA.47.2506 . 47 . 4 . 2506–2517 . 9909217 . 1993PhRvA..47.2506H .
  23. Encyclopedia: Copenhagen Interpretation of Quantum Mechanics . 2010-09-19 . Faye . J . 2008-01-24 . . The Metaphysics Research Lab Center for the Study of Language and Information, Stanford University.
  24. Zurek . Wojciech H. . Wojciech H. Zurek . 2003 . Decoherence, einselection, and the quantum origins of the classical . quant-ph/0105127 . Reviews of Modern Physics . 75 . 3. 715 . 10.1103/revmodphys.75.715. 2003RvMP...75..715Z . 14759237 .
  25. [Wojciech H. Zurek]
  26. Smolin. Lee. October 2012. A real ensemble interpretation of quantum mechanics. Foundations of Physics. 42. 10. 1239–1261. 10.1007/s10701-012-9666-4. 0015-9018. 1104.2822. 2012FoPh...42.1239S. 118505566.
  27. Rovelli. Carlo. Carlo Rovelli. Relational Quantum Mechanics. International Journal of Theoretical Physics. 35. 1637–1678. 1996. quant-ph/9609002 . 10.1007/BF02302261. 1996IJTP...35.1637R. 8 . 16325959.
  28. Book: Cramer, John G.. The transactional interpretation of quantum mechanics. Reviews of Modern Physics. July 1986. 58. 647–685.
  29. Okon. Elias. Sudarsky. Daniel. 2014-02-01. Benefits of Objective Collapse Models for Cosmology and Quantum Gravity. Foundations of Physics. en. 44. 2. 114–143. 10.1007/s10701-014-9772-6. 1572-9516. 1309.1730. 2014FoPh...44..114O. 67831520.
  30. Khazali. Mohammadsadegh. Lau. Hon Wai. Humeniuk. Adam. Simon. Christoph. 2016-08-11. Large energy superpositions via Rydberg dressing. Physical Review A. 94. 2. 023408. 10.1103/physreva.94.023408. 2469-9926. 1509.01303. 2016PhRvA..94b3408K. 118364289.
  31. Web site: What is the world's biggest Schrodinger cat?. stackexchange.com. live. https://web.archive.org/web/20120108000629/http://physics.stackexchange.com/questions/3309/what-is-the-worlds-biggest-schrodinger-cat. 2012-01-08.
  32. Web site: Schrödinger's Cat Now Made Of Light. 27 August 2014. www.science20.com. live. https://web.archive.org/web/20120318091956/http://www.science20.com/news_articles/schr%C3%B6dingers_cat_now_made_light. 18 March 2012.
  33. C. . Monroe . D. M. . Meekhof . B. E. . King . D. J. . Wineland . A "Schrödinger's cat" Superposition State of an Atom . Science . 272 . 5265 . 1996-05-24 . 1131–1136 . 10.1126/science.272.5265.1131. 8662445 . 1996Sci...272.1131M . 2311821 .
  34. Web site: Physics World: Schrödinger's cat comes into view. 5 July 2000.
  35. http://www.scientificamerican.com/article.cfm?id=quantum-microphone Scientific American : Macro-Weirdness: "Quantum Microphone" Puts Naked-Eye Object in 2 Places at Once: A new device tests the limits of Schrödinger's cat
  36. O. . Romero-Isart . M. L. . Juan . R. . Quidant . J. I. . Cirac . Toward Quantum Superposition of Living Organisms . New Journal of Physics . 2010 . 12 . 3 . 033015 . 10.1088/1367-2630/12/3/033015 . 0909.1469 . 2010NJPh...12c3015R. 59151724 .
  37. Web site: Could 'Schrödinger's bacterium' be placed in a quantum superposition?. physicsworld.com. live. https://web.archive.org/web/20160730174613/http://physicsworld.com/cws/article/news/2015/sep/21/could-schrodingers-bacterium-be-placed-in-a-quantum-superposition. 2016-07-30.
  38. News: Najjar . Dana . Physicists Can Finally Peek at Schrödinger's Cat Without Killing It Forever . 7 November 2019 . . 7 November 2019 .
  39. Patekar . Kartik . Hofmann . Holger F. . The role of system–meter entanglement in controlling the resolution and decoherence of quantum measurements . . 21 . 10 . 103006 . 10.1088/1367-2630/ab4451. 1905.09978 . 2019 . 2019NJPh...21j3006P . free .
  40. News: Merali . Zeeya . This Twist on Schrödinger's Cat Paradox Has Major Implications for Quantum Theory - A laboratory demonstration of the classic "Wigner's friend" thought experiment could overturn cherished assumptions about reality . 17 August 2020 . . 17 August 2020 .
  41. News: Musser . George . Quantum paradox points to shaky foundations of reality . 17 August 2020 . . 17 August 2020 .
  42. Bong, Kok-Wei . et al. . A strong no-go theorem on the Wigner's friend paradox . 17 August 2020 . . 27 . 12 . 1199–1205 . 10.1038/s41567-020-0990-x . 1907.05607 . 2020NatPh..16.1199B . free .