Philosophers
Mortimer Adler Rogers Albritton Alexander of Aphrodisias Samuel Alexander William Alston Anaximander G.E.M.Anscombe Anselm Louise Antony Thomas Aquinas Aristotle David Armstrong Harald Atmanspacher Robert Audi Augustine J.L.Austin A.J.Ayer Alexander Bain Mark Balaguer Jeffrey Barrett William Barrett William Belsham Henri Bergson George Berkeley Isaiah Berlin Richard J. Bernstein Bernard Berofsky Robert Bishop Max Black Susanne Bobzien Emil du BoisReymond Hilary Bok Laurence BonJour George Boole Émile Boutroux Daniel Boyd F.H.Bradley C.D.Broad Michael Burke Lawrence Cahoone C.A.Campbell Joseph Keim Campbell Rudolf Carnap Carneades Nancy Cartwright Gregg Caruso Ernst Cassirer David Chalmers Roderick Chisholm Chrysippus Cicero Tom Clark Randolph Clarke Samuel Clarke Anthony Collins Antonella Corradini Diodorus Cronus Jonathan Dancy Donald Davidson Mario De Caro Democritus Daniel Dennett Jacques Derrida René Descartes Richard Double Fred Dretske John Dupré John Earman Laura Waddell Ekstrom Epictetus Epicurus Austin Farrer Herbert Feigl Arthur Fine John Martin Fischer Frederic Fitch Owen Flanagan Luciano Floridi Philippa Foot Alfred Fouilleé Harry Frankfurt Richard L. Franklin Bas van Fraassen Michael Frede Gottlob Frege Peter Geach Edmund Gettier Carl Ginet Alvin Goldman Gorgias Nicholas St. John Green H.Paul Grice Ian Hacking Ishtiyaque Haji Stuart Hampshire W.F.R.Hardie Sam Harris William Hasker R.M.Hare Georg W.F. Hegel Martin Heidegger Heraclitus R.E.Hobart Thomas Hobbes David Hodgson Shadsworth Hodgson Baron d'Holbach Ted Honderich Pamela Huby David Hume Ferenc Huoranszki Frank Jackson William James Lord Kames Robert Kane Immanuel Kant Tomis Kapitan Walter Kaufmann Jaegwon Kim William King Hilary Kornblith Christine Korsgaard Saul Kripke Thomas Kuhn Andrea Lavazza Christoph Lehner Keith Lehrer Gottfried Leibniz Jules Lequyer Leucippus Michael Levin Joseph Levine George Henry Lewes C.I.Lewis David Lewis Peter Lipton C. Lloyd Morgan John Locke Michael Lockwood Arthur O. Lovejoy E. Jonathan Lowe John R. Lucas Lucretius Alasdair MacIntyre Ruth Barcan Marcus Tim Maudlin James Martineau Nicholas Maxwell Storrs McCall Hugh McCann Colin McGinn Michael McKenna Brian McLaughlin John McTaggart Paul E. Meehl Uwe Meixner Alfred Mele Trenton Merricks John Stuart Mill Dickinson Miller G.E.Moore Thomas Nagel Otto Neurath Friedrich Nietzsche John Norton P.H.NowellSmith Robert Nozick William of Ockham Timothy O'Connor Parmenides David F. Pears Charles Sanders Peirce Derk Pereboom Steven Pinker Plato Karl Popper Porphyry Huw Price H.A.Prichard Protagoras Hilary Putnam Willard van Orman Quine Frank Ramsey Ayn Rand Michael Rea Thomas Reid Charles Renouvier Nicholas Rescher C.W.Rietdijk Richard Rorty Josiah Royce Bertrand Russell Paul Russell Gilbert Ryle JeanPaul Sartre Kenneth Sayre T.M.Scanlon Moritz Schlick Arthur Schopenhauer John Searle Wilfrid Sellars Alan Sidelle Ted Sider Henry Sidgwick Walter SinnottArmstrong J.J.C.Smart Saul Smilansky Michael Smith Baruch Spinoza L. Susan Stebbing Isabelle Stengers George F. Stout Galen Strawson Peter Strawson Eleonore Stump Francisco Suárez Richard Taylor Kevin Timpe Mark Twain Peter Unger Peter van Inwagen Manuel Vargas John Venn Kadri Vihvelin Voltaire G.H. von Wright David Foster Wallace R. Jay Wallace W.G.Ward Ted Warfield Roy Weatherford C.F. von Weizsäcker William Whewell Alfred North Whitehead David Widerker David Wiggins Bernard Williams Timothy Williamson Ludwig Wittgenstein Susan Wolf Scientists David Albert Michael Arbib Walter Baade Bernard Baars Jeffrey Bada Leslie Ballentine Marcello Barbieri Gregory Bateson Horace Barlow John S. Bell Mara Beller Charles Bennett Ludwig von Bertalanffy Susan Blackmore Margaret Boden David Bohm Niels Bohr Ludwig Boltzmann Emile Borel Max Born Satyendra Nath Bose Walther Bothe Jean Bricmont Hans Briegel Leon Brillouin Stephen Brush Henry Thomas Buckle S. H. Burbury Melvin Calvin Donald Campbell Sadi Carnot Anthony Cashmore Eric Chaisson Gregory Chaitin JeanPierre Changeux Rudolf Clausius Arthur Holly Compton John Conway Jerry Coyne John Cramer Francis Crick E. P. Culverwell Antonio Damasio Olivier Darrigol Charles Darwin Richard Dawkins Terrence Deacon Lüder Deecke Richard Dedekind Louis de Broglie Stanislas Dehaene Max Delbrück Abraham de Moivre Bernard d'Espagnat Paul Dirac Hans Driesch John Eccles Arthur Stanley Eddington Gerald Edelman Paul Ehrenfest Manfred Eigen Albert Einstein George F. R. Ellis Hugh Everett, III Franz Exner Richard Feynman R. A. Fisher David Foster Joseph Fourier Philipp Frank Steven Frautschi Edward Fredkin Benjamin GalOr Howard Gardner Lila Gatlin Michael Gazzaniga Nicholas GeorgescuRoegen GianCarlo Ghirardi J. Willard Gibbs James J. Gibson Nicolas Gisin Paul Glimcher Thomas Gold A. O. Gomes Brian Goodwin Joshua Greene Dirk ter Haar Jacques Hadamard Mark Hadley Patrick Haggard J. B. S. Haldane Stuart Hameroff Augustin Hamon Sam Harris Ralph Hartley Hyman Hartman Jeff Hawkins JohnDylan Haynes Donald Hebb Martin Heisenberg Werner Heisenberg John Herschel Basil Hiley Art Hobson Jesper Hoffmeyer Don Howard John H. Jackson William Stanley Jevons Roman Jakobson E. T. Jaynes Pascual Jordan Eric Kandel Ruth E. Kastner Stuart Kauffman Martin J. Klein William R. Klemm Christof Koch Simon Kochen Hans Kornhuber Stephen Kosslyn Daniel Koshland Ladislav Kovàč Leopold Kronecker Rolf Landauer Alfred Landé PierreSimon Laplace Karl Lashley David Layzer Joseph LeDoux Gerald Lettvin Gilbert Lewis Benjamin Libet David Lindley Seth Lloyd Hendrik Lorentz Werner Loewenstein Josef Loschmidt Ernst Mach Donald MacKay Henry Margenau Owen Maroney David Marr Humberto Maturana James Clerk Maxwell Ernst Mayr John McCarthy Warren McCulloch N. David Mermin George Miller Stanley Miller Ulrich Mohrhoff Jacques Monod Vernon Mountcastle Emmy Noether Donald Norman Alexander Oparin Abraham Pais Howard Pattee Wolfgang Pauli Massimo Pauri Wilder Penfield Roger Penrose Steven Pinker Colin Pittendrigh Walter Pitts Max Planck Susan Pockett Henri Poincaré Daniel Pollen Ilya Prigogine Hans Primas Zenon Pylyshyn Henry Quastler Adolphe Quételet Pasco Rakic Nicolas Rashevsky Lord Rayleigh Frederick Reif Jürgen Renn Giacomo Rizzolati A.A. Roback Emil Roduner Juan Roederer Jerome Rothstein David Ruelle David Rumelhart Robert Sapolsky Tilman Sauer Ferdinand de Saussure Jürgen Schmidhuber Erwin Schrödinger Aaron Schurger Sebastian Seung Thomas Sebeok Franco Selleri Claude Shannon Charles Sherrington David Shiang Abner Shimony Herbert Simon Dean Keith Simonton Edmund Sinnott B. F. Skinner Lee Smolin Ray Solomonoff Roger Sperry John Stachel Henry Stapp Tom Stonier Antoine Suarez Leo Szilard Max Tegmark Teilhard de Chardin Libb Thims William Thomson (Kelvin) Richard Tolman Giulio Tononi Peter Tse Alan Turing Francisco Varela Vlatko Vedral Mikhail Volkenstein Heinz von Foerster Richard von Mises John von Neumann Jakob von Uexküll C. S. Unnikrishnan C. H. Waddington John B. Watson Daniel Wegner Steven Weinberg Paul A. Weiss Herman Weyl John Wheeler Wilhelm Wien Norbert Wiener Eugene Wigner E. O. Wilson Günther Witzany Stephen Wolfram H. Dieter Zeh Semir Zeki Ernst Zermelo Wojciech Zurek Konrad Zuse Fritz Zwicky Presentations Biosemiotics Free Will Mental Causation James Symposium 
CAN QUANTUMMECHANICAL DESCRIPTION OF PHYSICAL REALITY BE CONSIDERED COMPLETE?
Albert Einstein, Boris Podolsky, and Nathan Rosen In a complete theory there is an element corresponding to each element of reality. A sufficient condition for the reality of a physical quantity is the possibility of predicting it with certainty, without disturbing the system. In quantum mechanics in the case of two physical quantities described by noncommuting operators, the knowledge of one precludes the knowledge of the other. Then either (1) the description of reality given by the wave function in quantum mechanics is not complete or (2) these two quantities cannot have simultaneous reality. Consideration of the problem of making predictions concerning a system on the basis of measurements made on another system that had previously interacted with it leads to the result that if (1) is false then (2) is also false. One is thus led to conclude that the description of reality as given by a wave function is not complete.
1.
Any serious consideration of a physical theory must take into account the distinction between the objective reality, which is independent of any theory, and the physical concepts with which the theory operates. These concepts are intended to correspond with the objective reality, and by means of these concepts we picture this reality to ourselves. In attempting to judge the success of a physical theory, we may ask ourselves two questions: (1) "Is the theory correct?" and (2) "Is the description given by the theory complete?" It is only in the case in which positive answers may be given to both of these questions, that the concepts of the theory may be said to be satisfactory. The correctness of the theory is judged by the degree of agreement between the conclusions of the theory and human experience. This experience, which alone enables us to make inferences about reality, in physics takes the form of experiment and measurement. It is the second question that we wish to consider here, as applied to quantum mechanics. Whatever the meaning assigned to the term complete, the following requirement for a complete theory seems to be a necessary one: every element of the physical reality must have a counterpart in the physical theory. We shall call this the condition of completeness. The second question is thus easily answered, as soon as we are able to decide what are the elements of the physical reality. The elements of the physical reality cannot be determined by a priori philosophical considerations, but must be found by an appeal to results of experiments and measurements. A comprehensive definition of reality is, however, unnecessary for our purpose.
In quantum mechanics, expectation values can generally only be specified probabilistically, with confirmation provided statistically.
We shall be satisfied
with the following criterion, which we regard as
reasonable. If, without in any way disturbing a
system, we can predict with certainty {i.e., with
probability equal to unity) the value of a physical
quantity, then there exists an element of physical
reality corresponding to this physical quantity. It
seems to us that this criterion, while far from
exhausting all possible ways of recognizing a
physical reality, at least provides us with one
such way, whenever the conditions set down in
it occur. Regarded not as a necessary, but
merely as a sufficient, condition of reality, this
criterion is in agreement with classical as well as
quantummechanical ideas of reality.
For Einstein, a statistical theory is incomplete To illustrate the ideas involved let us consider the quantummechanical description of the behavior of a particle having a single degree of freedom. The fundamental concept of the theory is the concept of state, which is supposed to be completely characterized by the wave function ψ, which is a function of the variables chosen to describe the particle's behavior. Corresponding to each physically observable quantity A there is an operator, which may be designated by the same letter. If ψ is an eigenfunction of the operator A, that is, if
ψ' ≡ Aψ = aψ, (1)
where a is a number, then the physical quantity A has with certainty the value α whenever the particle is in the state given by ψ. In accordance with our criterion of reality, for a particle in the state given by ψ for which Eq. (1) holds, there is an element of physical reality corresponding to the physical quantity A. Let, for example,
ψ = e^{(2πi/h) p0x}, (2)
where h is Planck's constant, p_{0} is some constant number, and x the independent variable. Since the operator corresponding to the momentum of the particle is
p = ( h/2πi ) δ / δx = p_{0}x, (3)
we obtain
ψ' = pψ = ( h/2πi ) δψ / δx, (4)
Thus, in the state given by Eq. (2), the momentum has certainly the value p_{0}. It thus has meaning to say that the momentum of the particle in the state given by Eq. (2) is real. On the other hand if Eq. (1) does not hold, we can no longer speak of the physical quantity A having a particular value. This is the case, for example, with the coordinate of the particle. The operator corresponding to it, say q, is the operator of multiplication by the independent variable. Thus,
qψ = qψ ≠ aψ, (5)
In accordance with quantum mechanics we can only say that the relative probability that a measurement of the coordinate will give a result lying between a and b is
P(a,b) = ∫_{a}^{b} ψ*ψdx = b  a, (6)
Since this probability is independent of a, but depends only upon the difference b — a, we see that all values of the coordinate are equally probable. A definite value of the coordinate, for a particle in the state given by Eq. (2), is thus not predictable, but may be obtained only by a direct measurement. Such a measurement however disturbs the particle and thus alters its state. After the coordinate is determined, the particle will no longer be in the state given by Eq. (2). The usual conclusion from this in quantum mechanics is that when the momentum of a particle is known, its coordinate has no physical reality. More generally, it is shown in quantum mechanics that, if the operators corresponding to two physical quantities, say A and B, do not commute, that is, if AB ≠ BA, then the precise knowledge of one of them precludes such a knowledge of the other. Furthermore, any attempt to determine the latter experimentally will alter the state of the system in such a way as to destroy the knowledge of the first. From this follows that either (1) the quantummechanical description of reality given by the wave function is not complete or (2) when the operators corresponding to two physical quantities do not commute the two quantities cannot have simultaneous reality. For if both of them had simultaneous reality — and thus definite values — these values would enter into the complete description, according to the condition of completeness. If then the wave function provided such a complete description of reality, it would contain these values; these would then be predictable. This not being the case, we are left with the alternatives stated. In quantum mechanics it is usually assumed that the wave function does contain a complete description of the physical reality of the system in the state to which it corresponds. At first sight this assumption is entirely reasonable, for the information obtainable from a wave function seems to correspond exactly to what can be measured without altering the state of the system. We shall show, however, that this assumption, together with the criterion of reality given above, leads to a contradiction.
2.
For this purpose let us suppose that we have two systems, I and II, which we permit to inter act from the time t = 0 to t = T, after which time we suppose that there is no longer any interaction between the two parts. We suppose further that the states of the two systems before t = 0 were known. We can then calculate with the help of Schrödinger's equation the state of the combined system I + II at any subsequent time; in particular, for any t > T. Let us designate the corresponding wave function by Ψ. We cannot, however, calculate the state in which either one of the two systems is left after the interaction. This, according to quantum mechanics, can be done only with the help of further measurements,, by a process known as the reduction of the wave packet. Let us consider the essentials of this process.
Let a_{1}, a_{2}, a_{3},... be the eigenvalues of some
physical quantity A pertaining to system I and
Ψ (x_{1} , x_{2}) = Σ _{n=1}^{ ∞} ψ_{n} (x_{2} ) u_{n} (x_{1}), (7)
where x_{2} stands for the variables used to describe the second system. Here ψ_{n} (x_{2}) are to be regarded merely as the coefficients of the expansion of Ψ into a series of orthogonal functions u_{n} (x_{1}). Suppose now that the quantity A is measured and it is found that it has the value a_{k}. It is then concluded that after the measurement the first system is left in the state given by the wave function u_{k} (x_{1}), and that the second system is left in the state given by the wave function ψ_{k} (x_{2}). This is the process of reduction of the wave packet; the wave packet given by the infinite series (7) is reduced to a single term ψ_{k} (x_{2}) u_{k} (x_{1}) The set of functions u_{n} (x_{1}) is determined by the choice of the physical quantity A. If, instead of this, we had chosen another quantity, say B, having the eigenvalues b_{1}, b_{2}, b_{3},...and eigen functions v_{1} (x_{1}), v_{2} (x_{1}), v_{3} (x_{1}), ... we should have obtained, instead of Eq. (7), the expansion
Ψ (x_{1} , x_{2}) = Σ _{s=1}^{ ∞} φ_{s} (x_{2} ) v_{s} (x_{1}), (8)
where φ_{s}'s are the new coefficients. If now the quantity B is measured and is found to have the value b_{r}, we conclude that after the measurement the first system is left in the state given by v_{r} (x_{1}) and the second system is left in the state given by φ_{s} (x_{2} ). We see therefore that, as a consequence of two different measurements performed upon the first system, the second system may be left in states with two different wave functions.
Here is the error in most discussions of EPR. At the time of the measurement, a coherent twoparticle wave function ψ_{12} describes both particles. Measurement that locates one particle simultaneously determines the properties of the second particle (in the preferred frame in which the particles source is at rest).
On the other
hand, since at the time of measurement the two
systems no longer interact, no real change can
take place in the second system in consequence
of anything that may be done to the first system.
This is, of course, merely a statement of what is
meant by the absence of an interaction between
the two systems. Thus, it is possible to assign two
different wave functions (in our example ψ_{k} and
φ_{r} to the same reality (the second system after
the interaction with the first).
Only then does ψ_{12} → ψ_{1} ψ_{2} Now, it may happen that the two wave functions, ψ_{k} and φ_{r}, are eigenfunctions of two noncommuting operators corresponding to some physical quantities P and Q, respectively. That this may actually be the case can best be shown by an example. Let us suppose that the two systems are two particles, and that
Ψ (x_{1} , x_{2}) = ∫ _{∞}^{ +∞} e ^{ ( 2πi / h ) ( x1  x2 + x0 ) p} dp, (9)
where x_{0} is some constant. Let A be the momentum of the first particle; then, as we have seen in Eq. (4), its eigenfunctions will be
u_{p}( x_{1} ) = e ^{ ( 2πi / h ) p x1} , (10)
corresponding to the eigenvalue p. Since we have here the case of a continuous spectrum, Eq. (7) will now be written
Ψ (x_{1} , x_{2}) = ∫ _{∞}^{ +∞} ψ_{p} (x_{2} ) u_{p} (x_{1}) dp, (11)
where
ψ_{p} (x_{2} ) = e ^{ ( 2πi / h ) ( x2  x0 ) p } ,
(12)
(12) This ψ_{p} however is the eigenfunction of the operator
P = (h / 2 π i) δ/ δx_{2},
(13)
corresponding to the eigenvalue — p of the momentum of the second particle. On the other hand, if B is the coordinate of the first particle, it has for eigenfunctions
v ( x_{1} ) = δ ( x_{1}  x )
(14)
corresponding to the eigenvalue x, where δ ( x_{1}  x ) is the wellknown Dirac deltafunction. Eq. (8) in this case becomes
Ψ (x_{1} , x_{2}) = ∫ _{∞}^{ +∞} φ _{x} (x_{2} ) v_{x} (x_{1}) dx, (15)
where
φ_{x} ( x_{2} ) = ∫ _{∞}^{ +∞} e ^{ ( 2πi / h ) ( x2  x0 ) p } d p
= h δ ( x  x_{2} + x_{0} ) (16)
This φ_{x}, however, is the eigenfunction of the operator
Q = x_{2}, (17)
corresponding to the eigenvalue x + x_{0} of the coordinate of the second particle. Since
P Q  Q P = h / 2πi, (18)
we have shown that it is in general possible for ψ_{k} and φ_{r} to be eigenfunctions of two noncommuting operators, corresponding to physical quantities. Returning now to the general case contemplated in Eqs. (7) and (8), we assume that ψ_{k} and φ_{r} are indeed eigenfunctions of some noncommuting operators P and Q, corresponding to the eigenvalues p_{k} and q_{r}, respectively. Thus, by measuring either A or B we are in a position to predict with certainty, and without in any way disturbing the second system, either the value of the quantity P (that is p_{k}) or the value of the quantity Q (that is q_{r}). In accordance with our criterion of reality, in the first case we must consider the quantity P as being an element of reality, in the second case the quantity Q is an element of reality. But, as we have seen, both wave functions ψ_{k} and φ_{r} belong to the same reality. Previously we proved that either (1) the quantummechanical description of reality given by the wave function is not complete or (2) when the operators corresponding to two physical quantities do not commute the two quantities cannot have simultaneous reality. Starting then with the assumption that the wave function does give a complete description of the physical reality, we arrived at the conclusion that two physical quantities, with noncommuting operators, can have simultaneous reality. Thus the negation of (1) leads to the negation of the only other alternative (2). We are thus forced to conclude that the quantummechanical description of physical reality given by wave functions is not complete. One could object to this conclusion on the grounds that our criterion of reality is not sufficiently restrictive. Indeed, one would not arrive at our conclusion if one insisted that two or more physical quantities can be regarded as simultaneous elements of reality only when they can be simultaneously measured or predicted. On this point of view, since either one or the other, but not both simultaneously, of the quantities P and Q can be predicted, they are not simultaneously real. This makes the reality of P and Q depend upon the process of measurement carried out on the first system, which does not disturb the second system in any way. No reasonable definition of reality could be expected to permit this. While we have thus shown that the wave function does not provide a complete description of the physical reality, we left open the question of whether or not such a description exists. We believe, however, that such a theory is possible. For a modern analysis of this paradox, see EPR. For Teachers
For Scholars
