Information about Wave Function Collapse
In certain interpretations of quantum mechanics, wave function collapse is one of two processes by which quantum systems apparently evolve according to the laws of quantum mechanics. It is also called collapse of the state vector or reduction of the wave packet. The reality of wave function collapse has always been debated, i.e., whether it is a fundamental physical phenomenon in its own right (which may yet emerge from a theory of everything) or just an epiphenomenon of another process, such as quantum decoherence. In recent decades the quantum decoherence view has gained popularity.
where the
s specify the different quantum "alternatives" available (technically, they form an orthonormal eigenvector basis which implies
). An observable or measurable parameter of the system is associated with each eigenbasis, with each quantum alternative having a specific value or eigenvalue,
, of the observable.
The
are the probability amplitude coefficients, which are complex numbers. For simplicity we shall assume that our wave function is normalised:
, which implies that
.
With these definitions it is easy to describe the process of collapse:
When an external agency measures the observable associated with the eigenbasis then the state of the wave function changes from
to just one of the
s with Born probability
. This is called collapse because all the other terms in the expansion of the wave function have vanished or collapsed into nothing.
If a more general measurement is made to detect if the system is in a state
then the system makes a "jump" or quantum leap from the original state
to the final state
with probability of
. Quantum leaps and wave function collapse are therefore opposite sides of the same coin.
In general, quantum systems exist in superpositions of those basis states that most closely correspond to classical descriptions, and -- when not being measured or observed, evolve according to the time dependent Schrödinger equation, relativistic quantum field theory or some form of quantum gravity or string theory, which is process (2) mentioned above. However, when the wave function collapses -- process (1) -- from an observer's perspective the state seems to "leap" or "jump" to just one of the basis states and uniquely acquire the value of the property being measured,
, that is associated with that particular basis state. After the collapse, the system begins to evolve again according to the Schrödinger equation or some equivalent wave equation.
Hence, in experiments such as the double-slit experiment each individual photon arrives at a discrete point on the screen, but as more and more photons are accumulated, they form an interference pattern overall.
The existence of the wave function collapse is required in
Note that a general description of the evolution of quantum mechanical systems is possible by using density operators and quantum operations. In this formalism (which is closely related to the C*-algebraic formalism) the collapse of the wave function corresponds to a non-unitary quantum operation.
Note also that the physical significance ascribed to the wave function varies from interpretation to interpretation, and even within an interpretation, such as the Copenhagen Interpretation. If the wave function merely encodes an observer's knowledge of the universe then the wave function collapse corresponds to the receipt of new information -- this is somewhat analogous to the situation in classical physics, except that the classical "wave function" does not necessarily obey a wave equation. If the wave function is physically real, in some sense and to some extent, then the collapse of the wave function is also seen as a real process, to the same extent. One of the paradoxes of quantum theory is that wave function seems to be more than just information (otherwise interference effects are hard to explain) and often less than real, since the collapse seems to take place faster-than-light and triggered by observers.
Outline
The state or wave function of physical system, at some time, can be expressed in Dirac or bra-ket notation as:
where the
s specify the different quantum "alternatives" available (technically, they form an orthonormal eigenvector basis which implies
). An observable or measurable parameter of the system is associated with each eigenbasis, with each quantum alternative having a specific value or eigenvalue,
, of the observable.
The
are the probability amplitude coefficients, which are complex numbers. For simplicity we shall assume that our wave function is normalised:
, which implies that
.
With these definitions it is easy to describe the process of collapse:
When an external agency measures the observable associated with the eigenbasis then the state of the wave function changes from
to just one of the
s with Born probability
. This is called collapse because all the other terms in the expansion of the wave function have vanished or collapsed into nothing.
If a more general measurement is made to detect if the system is in a state
then the system makes a "jump" or quantum leap from the original state
to the final state
with probability of
. Quantum leaps and wave function collapse are therefore opposite sides of the same coin.
History and Context
By the time John von Neumann wrote his famous treatise Mathematische Grundlagen der Quantenmechanik in 1932[1], the phenomenon of "wave function collapse" was accommodated into the mathematical formulation of quantum mechanics by postulating that there were two processes of wave function change:- The probabilistic, non-unitary, non-local, discontinuous change brought about by observation and measurement, as outlined above.
- The deterministic, unitary, continuous time evolution of an isolated system that obeys Schrödinger's equation (or nowadays some relativistic, local equivalent).
In general, quantum systems exist in superpositions of those basis states that most closely correspond to classical descriptions, and -- when not being measured or observed, evolve according to the time dependent Schrödinger equation, relativistic quantum field theory or some form of quantum gravity or string theory, which is process (2) mentioned above. However, when the wave function collapses -- process (1) -- from an observer's perspective the state seems to "leap" or "jump" to just one of the basis states and uniquely acquire the value of the property being measured,
, that is associated with that particular basis state. After the collapse, the system begins to evolve again according to the Schrödinger equation or some equivalent wave equation.
Hence, in experiments such as the double-slit experiment each individual photon arrives at a discrete point on the screen, but as more and more photons are accumulated, they form an interference pattern overall.
The existence of the wave function collapse is required in
- the Copenhagen interpretation
- the so-called transactional interpretation
- in a "spiritual interpretation" in which consciousness causes collapse.
- interpretations based on consistent histories
- the many-worlds interpretation
- the Bohm interpretation
- the Ensemble Interpretation
Note that a general description of the evolution of quantum mechanical systems is possible by using density operators and quantum operations. In this formalism (which is closely related to the C*-algebraic formalism) the collapse of the wave function corresponds to a non-unitary quantum operation.
Note also that the physical significance ascribed to the wave function varies from interpretation to interpretation, and even within an interpretation, such as the Copenhagen Interpretation. If the wave function merely encodes an observer's knowledge of the universe then the wave function collapse corresponds to the receipt of new information -- this is somewhat analogous to the situation in classical physics, except that the classical "wave function" does not necessarily obey a wave equation. If the wave function is physically real, in some sense and to some extent, then the collapse of the wave function is also seen as a real process, to the same extent. One of the paradoxes of quantum theory is that wave function seems to be more than just information (otherwise interference effects are hard to explain) and often less than real, since the collapse seems to take place faster-than-light and triggered by observers.
Notes
1. ^ "the “collapse” or “reduction” of the wave function. This was introduced by Heisenberg in his uncertainty paper [3] and later postulated by von Neumann as a dynamical process independent of the Schrodinger equation"Kiefer, C. On the interpretation of quantum theory – from Copenhagen to the present day
See also
- Arrow of time
- Interpretation of quantum mechanics
- Quantum decoherence
- Quantum interference
- Schrödinger's cat
An interpretation of quantum mechanics is a statement which attempts to explain how quantum mechanics informs our understanding of nature. Although quantum mechanics has been extensively tested in very fine experiments, some believe the fundamentals of the theory are yet to be
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quantum mechanics is the study of the relationship between energy quanta (radiation) and matter, in particular that between valence shell electrons and photons. Quantum mechanics is a fundamental branch of physics with wide applications in both experimental and theoretical physics.
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quantum mechanics is the study of the relationship between energy quanta (radiation) and matter, in particular that between valence shell electrons and photons. Quantum mechanics is a fundamental branch of physics with wide applications in both experimental and theoretical physics.
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theory of everything (ToE) is a hypothetical theory of theoretical physics that fully explains and links together all known physical phenomena. Initially, the term was used with an ironic connotation to refer to various overgeneralized theories.
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An epiphenomenon is a secondary phenomenon that occurs alongside a primary phenomenon.
Often, a causal relationship between the phenomena is implied: the epiphenomenon is a consequence of the primary phenomenon.
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Often, a causal relationship between the phenomena is implied: the epiphenomenon is a consequence of the primary phenomenon.
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Please [improve the article] or discuss this issue on the talk page. This article has been tagged since April 2007.
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Please [improve the article] or discuss this issue on the talk page. This article has been tagged since April 2007.
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A wave function is a mathematical tool that quantum mechanics uses to describe any physical system. It is a function from a space that consists of the possible states of the system into the complex numbers. The laws of quantum mechanics (i.e.
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Bra-ket notation is the standard notation for describing quantum states in the theory of quantum mechanics. It can also be used to denote abstract vectors and linear functionals in pure mathematics.
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In linear algebra, two vectors in an inner product space are orthonormal if they are orthogonal (their inner product is 0) and both of unit length (the norm of each is 1). A set of vectors which is pairwise orthonormal (any two vectors in it are orthonormal) is called an
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eigenvector of the transformation and the blue vector is not. Since the red vector was neither stretched nor compressed, its eigenvalue is 1. All vectors with the same vertical direction - i.e., parallel to this vector - are also eigenvectors, with the same eigenvalue.
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basis is a set of vectors that, in a linear combination, can represent every vector in a given vector space, and such that no element of the set can be represented as a linear combination of the others. In other words, a basis is a linearly independent spanning set.
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eigenvector of the transformation and the blue vector is not. Since the red vector was neither stretched nor compressed, its eigenvalue is 1. All vectors with the same vertical direction - i.e., parallel to this vector - are also eigenvectors, with the same eigenvalue.
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In quantum mechanics, a probability amplitude is a complex-valued function that describes an uncertain or unknown quantity. For example, each particle has a probability amplitude describing its position. This amplitude is the wave function, expressed as a function of position.
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In mathematics, a complex number is a number of the form
where a and b are real numbers, and i is the imaginary unit, with the property i ² = −1.
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where a and b are real numbers, and i is the imaginary unit, with the property i ² = −1.
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In quantum mechanics, the Born probability is a probability of an event calculated from a wavefunction or more generally from the density matrix. The probability (or its density) equals the squared modulus of the normalized complex probability amplitude :
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quantum leap or quantum jump is a change of an electron from one energy state to another within an atom. It is discontinuous; the electron jumps from one energy level to another instantaneously.
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John von Neumann
John von Neumann in the 1940s
Born November 28 1903
Budapest, Austria-Hungary
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John von Neumann in the 1940s
Born November 28 1903
Budapest, Austria-Hungary
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19th century - 20th century - 21st century
1900s 1910s 1920s - 1930s - 1940s 1950s 1960s
1929 1930 1931 - 1932 - 1933 1934 1935
Year 1932 (MCMXXXII
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1900s 1910s 1920s - 1930s - 1940s 1950s 1960s
1929 1930 1931 - 1932 - 1933 1934 1935
Year 1932 (MCMXXXII
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The mathematical formulation of quantum mechanics is the body of mathematical formalisms which permits a rigorous description of quantum mechanics. It is distinguished from mathematical formalisms for theories developed prior to the early 1900s by the use of abstract mathematical
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Probability is the likelihood that something is the case or will happen. Probability theory is used extensively in areas such as statistics, mathematics, science and philosophy to draw conclusions about the likelihood of potential events and the underlying mechanics of
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A unitary transformation is an isomorphism between two Hilbert spaces. In other words, a unitary transformation is a bijective function
where and are Hilbert spaces, such that
for all and in .
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where and are Hilbert spaces, such that
for all and in .
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principle of locality is that distant objects cannot have direct influence on one another: an object is influenced directly only by its immediate surroundings. This was stated as follows by Albert Einstein in his article "Quantum Mechanics and Reality" ("Quanten-Mechanik und
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The framework of quantum mechanics requires a careful definition of measurement, and a thorough discussion of its practical and philosophical implications.
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Measurement from a practical point of view
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Determinism is the philosophical proposition that every event, including human cognition and behavior, decision and action, is causally determined by an unbroken chain of prior occurrences.
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A unitary transformation is an isomorphism between two Hilbert spaces. In other words, a unitary transformation is a bijective function
where and are Hilbert spaces, such that
for all and in .
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where and are Hilbert spaces, such that
for all and in .
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Time evolution is the change of state brought about by the passage of time, applicable to systems with internal state (also called stateful systems). In this formulation, time is not required to be a continuous parameter, but may be discrete or even .
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Schrödinger equation, proposed by the Austrian physicist Erwin Schrödinger in 1926, describes the space- and time-dependence of quantum mechanical systems. It is of central importance in non-relativistic quantum mechanics, playing a role for microscopic particles analogous to
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principle of locality is that distant objects cannot have direct influence on one another: an object is influenced directly only by its immediate surroundings. This was stated as follows by Albert Einstein in his article "Quantum Mechanics and Reality" ("Quanten-Mechanik und
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Quantum superposition is the application of the superposition principle to quantum mechanics. The superposition principle is the addition of the amplitudes of waves from interference. In quantum mechanics it is the amplitudes of wavefunctions, or state vectors, that add.
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Schrödinger equation, proposed by the Austrian physicist Erwin Schrödinger in 1926, describes the space- and time-dependence of quantum mechanical systems. It is of central importance in non-relativistic quantum mechanics, playing a role for microscopic particles analogous to
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