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The quantum-mechanical "
Schrödinger's cat"
paradox according to the Many-Worlds interpretation. In this
interpretation, every quantum event is a branch point; the cat is both
alive and dead, even before the box is opened, but the "alive" and
"dead" cats are in different branches of the universe, both of which are
equally real, but which do not interact with each other.
The many-worlds interpretation (MWI) is an interpretation of quantum mechanics that asserts that the universal wavefunction is objectively real, and that there is no wavefunction collapse. This implies that all possible outcomes of quantum measurements are physically realized in some "world" or universe. In contrast to some other interpretations, such as the Copenhagen interpretation, the evolution of reality as a whole in MWI is rigidly deterministic. Many-worlds is also called the relative state formulation or the Everett interpretation, after physicist Hugh Everett, who first proposed it in 1957. Bryce DeWitt popularized the formulation and named it many-worlds in the 1960s and 1970s.
In many-worlds, the subjective appearance of wavefunction collapse is explained by the mechanism of quantum decoherence. Decoherence approaches to interpreting quantum theory have been widely explored and developed since the 1970s,
and have become quite popular. MWI is now considered a mainstream
interpretation along with the other decoherence interpretations, collapse theories (including the Copenhagen interpretation), and hidden variable theories such as Bohmian mechanics.
The many-worlds interpretation implies that there are very many universes, perhaps infinitely many. It is one of many multiverse hypotheses in physics and philosophy. MWI views time as a many-branched tree, wherein every possible quantum outcome is realised. This is intended to resolve some paradoxes of quantum theory, such as the EPR paradox and Schrödinger's cat, since every possible outcome of a quantum event exists in its own universe.
History
In 1952 Erwin Schrödinger
gave a lecture in Dublin in which at one point he jocularly warned his
audience that what he was about to say might "seem lunatic". He went on
to assert that while what the equation
that won him a Nobel prize seems to be describing is several different
histories, they are "not alternatives but all really happen
simultaneously". This is the earliest known reference to many-worlds.
MWI originated in Everett's Princeton Ph.D. thesis "The Theory of the Universal Wavefunction", developed under his thesis advisor John Archibald Wheeler,
a shorter summary of which was published in 1957 under the title
"Relative State Formulation of Quantum Mechanics" (Wheeler contributed
the title "relative state"; Everett originally called his approach the "Correlation Interpretation", where "correlation" refers to quantum entanglement). The phrase "many-worlds" is due to Bryce DeWitt, who was responsible for the wider popularisation of Everett's theory, which was largely ignored for a decade after publication.
Overview of the interpretation
The
key idea of the many-worlds interpretation is that unitary quantum
mechanics describes the whole universe. In particular, it describes a
measurement as a unitary transformation, without using a collapse postulate, and describes observers as ordinary quantum-mechanical systems.
This stands in sharp contrast to the Copenhagen interpretation, on
which a measurement is a "primitive" concept, not describable by quantum
mechanics, the universe is divided into a quantum and a classical
domain, and the collapse postulate is central. MWI's main conclusion is that the universe (or multiverse in this context) is composed of a quantum superposition of an infinite or undefinable amount or number of increasingly divergent, non-communicating parallel universes or quantum worlds.
The many-worlds interpretation makes essential use of decoherence to explain the measurement process and the emergence of a quasi-classical world. Wojciech H. Zurek,
one of decoherence theory's pioneers, stated: "Under scrutiny of the
environment, only pointer states remain unchanged. Other states decohere
into mixtures of stable pointer states that can persist, and, in this
sense, exist: They are einselected." Żurek emphasizes that his work does not depend on a particular interpretation.
The many-worlds interpretation shares many similarities with the decoherent histories interpretation, which also uses decoherence to explain the process of measurement or wavefunction collapse.MWI treats the other histories or worlds as real since it regards the universal wavefunction as the "basic physical entity" or "the fundamental entity, obeying at all times a deterministic wave equation". Decoherent histories, on the other hand, needs only one of the histories (or worlds) to be real.
Several authors, including Wheeler, Everett and Deutsch, call many-worlds a theory, rather than just an interpretation.
Everett argued that it was the "only completely coherent approach to
explaining both the contents of quantum mechanics and the appearance of
the world."
Deutsch dismissed the idea that many-worlds is an "interpretation",
saying that to call it that "is like talking about dinosaurs as an
'interpretation' of fossil records."
Formulation
In Everett's formulation, a measuring apparatus M and an object system S
form a composite system, each of which prior to measurement exists in
well-defined (but time-dependent) states. Measurement is regarded as
causing M and S to interact. After S interacts with M,
it is no longer possible to describe either system by an independent
state. According to Everett, the only meaningful descriptions of each
system are relative states: for example the relative state of S given the state of M or the relative state of M given the state of S. In DeWitt's formulation, the state of S
after a sequence of measurements is given by a quantum superposition of
states, each one corresponding to an alternative measurement history of
S.
Schematic illustration of splitting as a result of a repeated measurement.
For example, consider the smallest possible truly quantum system S,
as shown in the illustration. This describes for instance, the
spin-state of an electron. Considering a specific axis (say the z-axis)
the north pole represents spin "up" and the south pole, spin "down".
The superposition states of the system are described by a sphere called
the Bloch sphere. To perform a measurement on S, it is made to interact with another similar system M.
After the interaction, the combined system can be regarded as a quantum
superposition of two "alternative histories" of the original system S,
one in which "up" was observed and the other in which "down" was
observed. Each subsequent binary measurement (that is interaction with a
system M) causes a similar split in the history tree. Thus after
three measurements, the system can be regarded as a quantum
superposition of 8 = 2 × 2 × 2 copies of the original system S.
Relative state
In his 1957 doctoral dissertation, Everett proposed that rather than
modeling an isolated quantum system subject to external observation, one
could mathematically model an object as well as its observers as purely
physical systems within the mathematical framework developed by Paul Dirac, John von Neumann and others, discarding altogether the ad hoc mechanism of wave function collapse.
Since Everett's original work, a number of similar formalisms
have appeared in the literature. One is the relative state formulation.
It makes two assumptions: first, the wavefunction is not simply a
description of the object's state, but is entirely equivalent to the
object—a claim it has in common with some other interpretations. Second,
observation or measurement has no special laws or mechanics, unlike in
the Copenhagen interpretation,
which considers the wavefunction collapse a special kind of event that
occurs as a result of observation. Instead, measurement in the relative
state formulation is the consequence of a configuration change in an
observer's memory described by the same basic wave physics as the object
being modeled.
The many-worlds interpretation is DeWitt's popularisation of
Everett, who had referred to the combined observer–object system as
split by an observation, each split corresponding to the different or
multiple possible outcomes of an observation. These splits generate a
tree, as shown in the graphic above. Subsequently, DeWitt introduced the
term "world" to describe a complete measurement history of an observer,
which corresponds roughly to a single branch of that tree.
Under the many-worlds interpretation, the Schrödinger equation,
or relativistic analog, holds all the time everywhere. An observation
or measurement is modeled by applying the wave equation to the entire
system comprising the observer and the object. One consequence is
that every observation can be thought of as causing the combined
observer–object's wavefunction to change into a quantum superposition of
two or more non-interacting branches, or split into many "worlds".
Since many observation-like events have happened and are constantly
happening, there are an enormous and growing number of simultaneously
existing states.
If a system is composed of two or more subsystems, the system's
state will be a superposition of products of the subsystems' states.
Each product of subsystem states in the overall superposition evolves
over time independently of other products. Once the subsystems interact,
their states have become correlated or entangled and can no longer be considered independent. In Everett's terminology each subsystem state was now correlated with its relative state, since each subsystem must now be considered relative to the other subsystems with which it has interacted.
Properties
MWI removes the observer-dependent role in the quantum measurement process by replacing wavefunction collapse with quantum decoherence.
Since the observer's role lies at the heart of most if not all "quantum
paradoxes," this automatically resolves a number of problems, such as Schrödinger's cat thought experiment, the EPR paradox, von Neumann's "boundary problem", and even wave-particle duality.
Since the Copenhagen interpretation requires the existence of a
classical domain beyond the one described by quantum mechanics, it has
been criticized as inadequate for the study of cosmology. MWI was developed with the explicit goal of allowing quantum mechanics to be applied to the universe as a whole, making quantum cosmology possible.
MWI is a realist, deterministic, and local theory. It achieves this by removing wavefunction collapse, which is indeterministic and non-local, from the deterministic and local equations of quantum theory.
MWI (like other, broader multiverse theories) provides a context for the anthropic principle, which may provide an explanation for the fine-tuned universe.
MWI depends crucially on the linearity of quantum mechanics. If the final theory of everything is non-linear with respect to wavefunctions, then many-worlds is invalid.. While quantum gravity or string theory may be non-linear in this respect, there is no evidence of this as yet.
Interpreting wavefunction collapse
As with the other interpretations of quantum mechanics, the
many-worlds interpretation is motivated by behavior that can be
illustrated by the double-slit experiment. When particles of light
(or anything else) pass through the double slit, a calculation assuming
wavelike behavior of light can be used to identify where the particles
are likely to be observed. Yet when the particles are observed in this
experiment, they appear as particles (i.e., at definite places) and not
as non-localized waves.
Some versions of the Copenhagen interpretation of quantum mechanics proposed a process of "collapse"
in which an indeterminate quantum system would probabilistically
collapse down onto, or select, just one determinate outcome to "explain"
this phenomenon of observation. Wavefunction collapse was widely
regarded as artificial and ad hoc,
so an alternative interpretation in which the behavior of measurement
could be understood from more fundamental physical principles was
considered desirable.
Everett's Ph.D. work provided such an interpretation. He argued
that for a composite system—such as a subject (the "observer" or
measuring apparatus) observing an object (the "observed" system, such as
a particle)—the claim that either the observer or the observed has a
well-defined state is meaningless; in modern parlance, the observer and
the observed have become entangled: we can only specify the state of one
relative to the other, i.e., the state of the observer and the observed are correlated after
the observation is made. This led Everett to derive from the unitary,
deterministic dynamics alone (i.e., without assuming wavefunction
collapse) the notion of a relativity of states.
Everett noticed that the unitary, deterministic dynamics alone entailed that after an observation is made each element of the quantum superposition
of the combined subject–object wavefunction contains two "relative
states": a "collapsed" object state and an associated observer who has
observed the same collapsed outcome; what the observer sees and the
state of the object have become correlated by the act of measurement or
observation. The subsequent evolution of each pair of relative
subject–object states proceeds with complete indifference as to the
presence or absence of the other elements, as if wavefunction
collapse has occurred, which has the consequence that later observations
are always consistent with the earlier observations. Thus the appearance
of the object's wavefunction's collapse has emerged from the unitary,
deterministic theory itself. (This answered Einstein's early criticism
of quantum theory, that the theory should define what is observed, not
for the observables to define the theory.)
Since the wavefunction merely appears to have collapsed then, Everett
reasoned, there was no need to actually assume that it had collapsed.
And so, invoking Occam's razor, he removed the postulate of wavefunction collapse from the theory.
Testability
In 1985, David Deutsch proposed a variant of the Wigner's friend thought experiment as a test of many-worlds versus the Copenhagen interpretation.
It consists of an experimenter (Wigner's friend) making a measurement
on a quantum system in an isolated laboratory, and another experimenter
(Wigner) who would make a measurement on the first one. According to the
many-worlds theory, the first experimenter would end up in a
macroscopic superposition of seeing one result of the measurement in one
branch, and another result in another branch. The second experimenter
could then interfere these two branches in order to test whether it is
in fact in a macroscopic superposition or has collapsed into a single
branch, as predicted by the Copenhagen interpretation. Since then
Lockwood (1989), Vaidman and others have made similar proposals.
These proposals require placing macroscopic objects in a coherent
superposition and interfering them, a task now beyond experimental
capability.
Probability and the Born rule
Since
the many-worlds interpretation's inception, physicists have been
puzzled about the role of probability in it. As put by Wallace, there
are two facets to the question: the incoherence problem, which asks why we should assign probabilities at all to outcomes that are certain to occur in some worlds, and the quantitative problem, which asks why the probabilities should be given by the Born rule.
Everett tried to answer these questions in the paper that
introduced many-worlds. To address the incoherence problem, he argued
that an observer who makes a sequence of measurements on a quantum
system will in general have an apparently random sequence of results in
their memory, which justifies the use of probabilities to describe the
measurement process.
To address the quantitative problem, Everett proposed a derivation of
the Born rule based on the properties that a measure on the branches of
the wavefunction should have. His derivation has been criticized as relying on unmotivated assumptions.
Since then several other derivations of the Born rule in the
many-worlds framework have been proposed. There is no consensus on
whether this has been successful.
Frequentism
DeWitt and Graham and Farhi et al., among others, have proposed derivations of the Born rule based on a frequentist
interpretation of probability. They try to show that in the limit of
infinitely many measurements no worlds would have relative frequencies
that didn't match the probabilities given by the Born rule, but these
derivations have been shown to be mathematically incorrect.
Decision theory
A decision-theoretic derivation of the Born rule was produced by David Deutsch (1999) and refined by Wallace (2002–2009) and Saunders (2004).
They consider an agent who takes part in a quantum gamble: the agent
makes a measurement on a quantum system, branches as a consequence, and
each of the agent's future selves receives a reward that depends on the
measurement result. The agent uses decision theory to evaluate the price
they would pay to take part in such a gamble, and concludes that the
price is given by the utility of the rewards weighted according to the
Born rule. Some reviews have been positive, although these arguments
remain highly controversial; some theoretical physicists have taken them
as supporting the case for parallel universes. For example, a New Scientist story on a 2007 conference about Everettian interpretations
quoted physicist Andy Albrecht as saying, "This work will go down as
one of the most important developments in the history of science." In contrast, the philosopher Huw Price, also attending the conference, found the Deutsch–Wallace–Saunders approach fundamentally flawed.
Symmetries and invariance
Żurek (2005)
has produced a derivation of the Born rule based on the symmetries of
entangled states; Schlosshauer and Fine argue that Żurek's derivation is
not rigorous, as it does not define what probability is and has several
unstated assumptions about how it should behave.
Charles Sebens and Sean M. Carroll, building on work by Lev Vaidman, proposed a similar approach based on self-locating uncertainty.
In this approach, decoherence creates multiple identical copies of
observers, who can assign credences to being on different branches using
the Born rule. The Sebens–Carroll approach has been criticized by Adrian Kent, and Vaidman himself does not find it satisfactory.
The preferred basis problem
As
originally formulated by Everett and DeWitt, the many-worlds
interpretation had a privileged role for measurements: they determined
which basis
of a quantum system would give rise to the eponymous worlds. Without
this the theory was ambiguous, as a quantum state can equally well be
described (e.g.) as having a well-defined position or as being a
superposition of two delocalised states. The assumption that the
preferred basis to use is the one from a measurement of position results
in worlds having objects in well-defined positions, instead of worlds
with delocalised objects (which would be grossly incompatible with
experiment). This special role for measurements is problematic for the
theory, as it contradicts Everett and DeWitt's goal of having a
reductionist theory and undermines their criticism of the ill-defined
measurement postulate of the Copenhagen interpretation. This is known today as the preferred basis problem.
The preferred basis problem has been solved, according to Saunders and Wallace, among others, by incorporating decoherence in the many-worlds theory.
In this approach, the preferred basis does not have to be postulated,
but rather is identified as the basis stable under environmental
decoherence. In this way measurements no longer play a special role;
rather, any interaction that causes decoherence causes the world to
split. Since decoherence is never complete, there will always remain
some infinitesimal overlap between two worlds, making it arbitrary
whether a pair of worlds has split or not.
Wallace argues that this is not problematic: it only shows that worlds
are not a part of the fundamental ontology, but rather of the emergent ontology, where these approximate, effective descriptions are routine in the physical sciences.
Since in this approach the worlds are derived, it follows that they
must be present in any other interpretation of quantum mechanics that
does not have a collapse mechanism, such as Bohmian mechanics.
This approach to deriving the preferred basis has been criticized
as creating a circularity with derivations of probability in the
many-worlds interpretation, as decoherence theory depends on
probability, and probability depends on the ontology derived from
decoherence.
Wallace contends that decoherence theory depends not on probability but
only on the notion that one is allowed to do approximations in physics.
Reception
MWI's
initial reception was overwhelmingly negative, with the notable
exception of DeWitt. Wheeler made considerable efforts to formulate the
theory in a way that would be palatable to Bohr, visited Copenhagen in
1956 to discuss it with him, and convinced Everett to visit as well,
which happened in 1959. Nevertheless, Bohr and his collaborators
completely rejected the theory. Everett left academia in 1956, never to return, and Wheeler eventually disavowed the theory.
One of MWI's strongest advocates is David Deutsch. According to Deutsch, the single photon interference pattern observed in the double slit experiment
can be explained by interference of photons in multiple universes.
Viewed this way, the single photon interference experiment is
indistinguishable from the multiple photon interference experiment. In a
more practical vein, in one of the earliest papers on quantum
computing, he suggested that parallelism that results from MWI could lead to "a
method by which certain probabilistic tasks can be performed faster by a
universal quantum computer than by any classical restriction of it". Deutsch has also proposed that MWI will be testable (at least against "naive" Copenhagenism) when reversible computers become conscious via the reversible observation of spin.
Asher Peres was an outspoken critic of MWI. A section of his 1993 textbook had the title Everett's interpretation and other bizarre theories.
Peres argued that the various many-worlds interpretations merely shift
the arbitrariness or vagueness of the collapse postulate to the question
of when "worlds" can be regarded as separate, and that no objective
criterion for that separation can actually be formulated.
Some consider MWI unfalsifiable and hence unscientific because the multiple parallel universes are non-communicating, in the sense that no information can be passed between them. Others claim MWI is directly testable.
Victor J. Stenger remarked that Murray Gell-Mann's published work explicitly rejects the existence of simultaneous parallel universes. Collaborating with James Hartle, Gell-Mann had been, before his death, working toward the development a more "palatable" post-Everett quantum mechanics.
Stenger thought it fair to say that most physicists dismiss the
many-worlds interpretation as too extreme, while noting it "has merit in
finding a place for the observer inside the system being analyzed and
doing away with the troublesome notion of wave function collapse".
Philosophers of science James Ladyman and Don Ross state that the
MWI could be true, but that they do not embrace it. They note that no
quantum theory is yet empirically adequate for describing all of
reality, given its lack of unification with general relativity, and so they do not see a reason to regard any interpretation of quantum mechanics as the final word in metaphysics.
They also suggest that the multiple branches may be an artifact of
incomplete descriptions and of using quantum mechanics to represent the
states of macroscopic objects. They argue that macroscopic objects are
significantly different from microscopic objects in not being isolated
from the environment, and that using quantum formalism to describe them
lacks explanatory and descriptive power and accuracy.
Polls
A poll of 72 "leading quantum cosmologists and other quantum field theorists" conducted before 1991 by L. David Raub showed 58% agreement with "Yes, I think MWI is true".
Max Tegmark
reports the result of a "highly unscientific" poll taken at a 1997
quantum mechanics workshop. According to Tegmark, "The many worlds
interpretation (MWI) scored second, comfortably ahead of the consistent histories and Bohm interpretations."
In response to Sean M. Carroll's statement "As crazy as it sounds, most working physicists buy into the many-worlds theory", Michael Nielsen
counters: "at a quantum computing conference at Cambridge in 1998, a
many-worlder surveyed the audience of approximately 200 people...
Many-worlds did just fine, garnering support on a level comparable to,
but somewhat below, Copenhagen and decoherence." But Nielsen notes that
it seemed most attendees found it to be a waste of time: Peres "got a
huge and sustained round of applause…when he got up at the end of the
polling and asked 'And who here believes the laws of physics are decided
by a democratic vote?'"
A 2005 poll of fewer than 40 students and researchers taken after
a course on the Interpretation of Quantum Mechanics at the Institute
for Quantum Computing University of Waterloo found "Many Worlds (and
decoherence)" to be the least favored.
A 2011 poll of 33 participants at an Austrian conference found 6
endorsed MWI, 8 "Information-based/information-theoretical", and 14
Copenhagen; the authors remark that MWI received a similar percentage of votes as in Tegmark's 1997 poll.
Debate whether the other worlds are real
Everett believed in the literal reality of the other quantum worlds. His son reported that he "never wavered in his belief over his many-worlds theory".
According to Martin Gardner, the "other" worlds of MWI have two different interpretations: real or unreal; he claimed that Stephen Hawking and Steven Weinberg both favour the unreal interpretation.
Gardner also claimed that most physicists favour the unreal
interpretation, whereas the "realist" view is supported only by MWI
experts such as Deutsch and DeWitt. Hawking has said that "according to
Feynman's idea", all other histories are as "equally real" as our own, and Gardner reports Hawking saying that MWI is "trivially true".
In a 1983 interview, Hawking also said he regarded MWI as
"self-evidently correct" but was dismissive of questions about the
interpretation of quantum mechanics, saying, "When I hear of Schrödinger's cat, I reach for my gun."
In the same interview, he also said, "But, look: All that one does,
really, is to calculate conditional probabilities—in other words, the
probability of A happening, given B. I think that that's all the many
worlds interpretation is. Some people overlay it with a lot of mysticism
about the wave function splitting into different parts. But all that
you're calculating is conditional probabilities." Elsewhere Hawking contrasted his attitude towards the "reality" of physical theories with that of his colleague Roger Penrose, saying, "He's a Platonist and I'm a positivist.
He's worried that Schrödinger's cat is in a quantum state, where it is
half alive and half dead. He feels that can't correspond to reality. But
that doesn't bother me. I don't demand that a theory correspond to
reality because I don't know what it is. Reality is not a quality you
can test with litmus paper. All I'm concerned with is that the theory
should predict the results of measurements. Quantum theory does this
very successfully."
For his own part, Penrose agrees with Hawking that QM applied to the
universe implies MW, but he believes the lack of a successful theory of quantum gravity negates the claimed universality of conventional QM.
Speculative implications
Quantum suicide thought experiment
Quantum suicide is a thought experiment in quantum mechanics and the philosophy of physics. Purportedly, it can distinguish between the Copenhagen interpretation of quantum mechanics and the many-worlds interpretation by means of a variation of the Schrödinger's cat thought experiment, from the cat's point of view. Quantum immortality refers to the subjective experience of surviving quantum suicide.
Most experts believe that the experiment would not work in the
real world, because the world with the surviving experimenter has a
lower "measure" than the world prior to the experiment, making it less
likely that the experimenter will go on to experience their survival.
Absurdly improbable timelines
DeWitt
has stated that "[Everett, Wheeler and Graham] do not in the end
exclude any element of the superposition. All the worlds are there, even
those in which everything goes wrong and all the statistical laws break
down."
Max Tegmark has affirmed that absurd or highly unlikely events
are inevitable but rare under the MWI. To quote Tegmark, "Things
inconsistent with the laws of physics will never happen—everything else
will... it's important to keep track of the statistics, since even if
everything conceivable happens somewhere, really freak events happen
only exponentially rarely."
Ladyman and Ross state that, in general, many of the unrealized
possibilities that are discussed in other scientific fields will not
have counterparts in other branches, because they are in fact
incompatible with the universal wavefunction.