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Not to be confused with Wave equation.

A **wave function** (or **wavefunction**) in quantum mechanics describes the quantum state of a system of one or more particles, and contains all the information about the system considered in isolation. Quantities associated with measurements, such as the average momentum of a particle, are derived from the wave function by mathematical operations that describe its interaction with observational devices. Thus it is a central entity in quantum mechanics. The most common symbols for a wave function are the Greek letters *ψ* or Ψ (lower-case and capital psi). The Schrödinger equation determines how the wave function evolves over time, that is, the wave function is the solution of the Schrödinger equation. The wave function behaves qualitatively like other waves, such as water waves or waves on a string, because the Schrödinger equation is mathematically a type of wave equation. This explains the name "wave function", and gives rise to wave–particle duality. The wave of the wave function, however, is not a wave in physical space; it is a wave in an abstract mathematical "space", and in this respect it differs fundamentally from water waves or waves on a string.^{[1]}^{[2]}^{[3]}^{[4]}^{[5]}^{[6]}^{[7]}

The wave function may be represented as a complex vector-valued function over its domain, but for a given system such a representation is not unique. It may be taken to be a function of time and all position coordinates of the particles, that is, the wave function is in *position space*. A wave function may similarly be considered over *momentum space*; a function instead of time and the momenta of all the particles. In general, the wave function of a system is a function of continuous and discrete variables characterizing the system's degrees of freedom, and there is *one* wave function for the entire system, not a separate wave function for each particle in the system. Some particles, like electrons and photons, have nonzero spin, and the wave function must include this fundamental property as an intrinsic degree of freedom. In general, for a particle with *half-integer* spin the wave function is a spinor, for a particle with *integer* spin the wave function is a tensor. Particles with spin zero are called scalar particles, those with spin 1 vector particles, and more generally for higher integer spin, tensor particles. No *elementary* particle with spin ^{3}⁄_{2} or higher is known, except for the hypothesized spin 2 graviton.

In the Copenhagen interpretation, an interpretation of quantum mechanics, the squared modulus of the wave function, |*ψ*|^{2}, is a real number interpreted as the probability density of measuring a particle as being at a given place at a given time. Since the wave function is complex valued, only its relative phase and relative magnitude can be measured. Its value does not in isolation tell anything about the magnitudes or directions of measurable observables; one has to apply quantum operators to the wave function *ψ* and find the eigenvalues which correspond to sets of possible results of measurement.

The unit of measurement for *ψ* depends on the system. For one particle in three dimensions, its units are [length]^{−3/2}. These units are required so that an integral of |*ψ*|^{2} over a region of three-dimensional space is a dimensionless probability (the probability that the particle is measured as being in that region). For different numbers of particles and/or dimensions, the units vary and can be found by dimensional analysis.^{[8]}

- 1 Historical background
- 2 Wave functions and function spaces
- 3 Definition (one spinless particle in 1d)
- 4 Definitions (other cases)
- 5 Inner product
- 6 Units of the wave function
- 7 Distinguishable and identical particles
- 8 Wave functions as elements of an abstract vector space
- 9 Position representations
- 10 Ontology
- 11 Examples
- 12 See also
- 13 Remarks
- 14 References
- 15 Further reading
- 16 External links

Quantum mechanics |
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In the 1920s and 1930s, quantum mechanics was developed using calculus and linear algebra. Those who used the techniques of calculus included Louis de Broglie, Erwin Schrödinger, and others, developing "wave mechanics". Those who applied the methods of linear algebra included Werner Heisenberg, Max Born, and others, developing "matrix mechanics". Schrödinger subsequently showed that the two approaches were equivalent.^{[9]}

In 1905 Planck postulated the proportionality between the frequency of a photon and its energy, in the Planck-Einstein relation, *E* = *hf*. In 1925, De Broglie published the corresponding relation between momentum and wavelength, *λ* = *h*/*p*, now called the De Broglie relation. These equations represent wave–particle duality. In 1926, Schrödinger published the famous wave equation now named after him, indeed the Schrödinger equation, based on classical energy conservation using quantum operators and the de Broglie relations such that the solutions of the equation are the wave functions for the quantum system. Later Pauli invented the Pauli equation that adds a description of electron's spin and magnetic dipole. However, *no one*, even Schrödinger or De Broglie, was clear on *how to interpret it*.^{[10]} Around 1924–27, Max Born, Heisenberg, Bohr and others provided the perspective of *probability amplitude*.^{[11]} This is the *Copenhagen interpretation* of quantum mechanics. There are many other interpretations of quantum mechanics, but this relates calculations of quantum mechanics directly to probabilistic experimental observations.

In 1927, Hartree and Fock made the first step in an attempt to solve the *N*-body wave function, and developed the *self-consistency cycle*: an iterative algorithm to approximate the solution. Now it is also known as the Hartree–Fock method.^{[12]} The Slater determinant and permanent (of a matrix) was part of the method, provided by John C. Slater.

Schrödinger did encounter an equation for the wave function that satisfied relativistic energy conservation *before* he published the non-relativistic one, but discarded it as it predicted negative probabilities and negative energies. In 1927, Klein, Gordon and Fock also found it, but incorporated the electromagnetic interaction and proved that it was Lorentz invariant. De Broglie also arrived at the same equation in 1928. This relativistic wave equation is now most commonly known as the Klein–Gordon equation.^{[13]}

In 1927, Pauli phenomenologically found a non-relativistic equation to describe spin-1/2 particles in electromagnetic fields, now called the Pauli equation. Pauli found the wave function was not described by a single complex function of space and time, but needed two complex numbers, which respectively correspond to the spin +1/2 and −1/2 states of the fermion. Soon after in 1928, Dirac found an equation from the first successful unification of special relativity and quantum mechanics applied to the electron, now called the Dirac equation. In this, the wave function is a *spinor* represented by four complex-valued components:^{[12]} two for the electron and two for the electron's antiparticle, the positron. In the non-relativistic limit, the Dirac wave function resembles the Pauli wavefunction for the electron. Later, other relativistic wave equations were found.

Functional analysis is commonly used to formulate the wave function with a necessary mathematical precision; usually they are quadratically integrable functions (at least locally) because it is compatible with the Hilbert space formalism mentioned below. The set on which their function space is defined is the configuration space of the system. In many situations it is a Euclidean space, that implies that wave functions are functions of several real variables. Superficially, this formalism is simple to understand for the following reasons.

- If the wave function is to change throughout space and time, one would expect the wave function to be a function of the position and time coordinates. It is solved from the Schrödinger equation (or other relativistic wave equations), a linear partial differential equation:

- Functions can easily describe wave-like motion, using periodic functions, and Fourier analysis can be readily done.
- Functions are easy to produce, visualize, and interpret, because of the pictorial nature of the graph of a function. One can plot curves, surfaces, contour lines, more generally any level sets. If the situation is in a high number of dimensions – one can analyze the function in a lower-dimensional slice to see the behavior of the function within that confined region.

For concreteness and simplicity, in this article, when coordinates are needed we use Cartesian coordinates so that **r** is short for (*x*, *y*, *z*), although spherical polar coordinates and other orthogonal coordinates are often useful to solve the Schrödinger equation for potentials with certain geometric symmetries, in which case the position and wave function is expressed in these coordinates.

One does not have to define wave functions necessarily on real spaces: appropriate function spaces can be defined wherever a measure can provide integration. Operator theory and linear algebra, as shown below, can deal with situations where the real analysis is not applicable.

The following constraints on the wave function are formulated for the calculations and physical interpretation to make sense:^{[14]}^{[15]}

- It must everywhere be a continuous function, and continuously differentiable.
- It must everywhere satisfy the relevant normalization condition, because the particle or system of particles exists somewhere with 100% certainty. For this to be so, the wave function must be square integrable.

A requirement less restrictive is that the wave function must belong to the Sobolev space *W*^{1,2}. It means that it is differentiable in the sense of distributions, and its gradient is square-integrable. This relaxation is necessary for potentials that are not functions but are distributions, such as the Dirac delta function.

If these requirements are not met, it is not possible to interpret the wave function as a probability amplitude.^{[16]}

For now, consider the simple case of a single particle, without spin, in one spatial dimension. (More general cases are discussed below).

The state of such a particle is completely described by its wave function:

where *x* is position and *t* is time. This is a complex-valued function of two real variables *x* and *t*.

If interpreted as a probability amplitude, the square modulus of the wave function is the positive real number

interpreted as the *probability density* that the particle is at *x*, rather than some other location. The star * indicates complex conjugate. If the particle's position is measured, its location is not deterministic, but is described by a probability distribution. The probability that its position *x* will be in the interval *a* ≤ *x* ≤ *b* is the integral of the density over this interval:

where *t* is the time at which the particle was measured. This leads to the **normalization condition**:

because if the particle is measured, there is 100% probability that it will be *somewhere*.

Since the Schrödinger equation is linear, if any number of wave functions Ψ_{n} for *n* = 1, 2, ... are solutions of the equation, then so is their sum, and their scalar multiples by complex numbers *a _{n}*. Taking scalar multiplication and addition together is known as a linear combination:

This is the *superposition principle*. Multiplying a wave function Ψ by any nonzero constant complex number *c* to obtain *c*Ψ does not change any information about the quantum system, because *c* cancels in the Schrödinger equation for *c*Ψ. All that happens is that any normalization constants will be rescaled.

Since linear combinations of wave functions obtain more wave functions, the set of all wave functions *W* = {Ψ(*x*, *t*)} is an infinite dimensional vector space over the field of complex numbers. To form a vector space basis *B*, we need a **maximal** set of wave functions *ψ*_{1}, *ψ*_{2}, ... in *W* which are linearly independent: *each* one of them is *not* a linear combination of the others, for example *ψ*_{1} ≠ *z*_{2}*ψ*_{2} + *z*_{3}*ψ*_{3} + ... and *ψ*_{2} ≠ *z*_{1}*ψ*_{1} + *z*_{3}*ψ*_{3} + ..., etc., for any complex numbers *z _{n}* and every function in

In this way, Ψ(*x*, *t*) can be viewed as an infinite dimensional vector, where the complex-valued coefficients *a _{n}* are the components of the vector. The choice of which wave functions to use as a basis is not unique, but if a change of basis is made, the components

The particle also has a wave function in momentum space:

where *p* is the momentum in one dimension, which can be any value from −∞ to +∞, and *t* is time.

All the previous remarks on superposition, normalization, etc. apply similarly. In particular, if the particle's momentum is measured, the result is not deterministic, but is described by a probability distribution:

and the normalization condition is:

The position-space and momentum-space wave functions are Fourier transforms of each other, therefore both contain the same information, and either one alone is sufficient to calculate any property of the particle. As elements of **abstract physical Hilbert space**, whose elements are the possible states of the system under consideration, they represent the same object, but they are not equal when viewed as square-integrable functions. (A function and its Fourier transform are not equal.) For one dimension:^{[17]}

Sometimes the wave-vector *k* is used in place of momentum *p*, since they are related by the de Broglie relation

and the equivalent space is referred to as *k*-space. Again it makes no difference which is used since *p* and *k* are equivalent – up to a constant. In practice, the position-space wave function is used much more often than the momentum-space wave function. The potential entering the Schrödinger equation determines in which basis the description is easiest. For the harmonic oscillator, *x* and *p* enter symmetrically, so there it doesn't matter which description one uses.

In the common formulations of quantum mechanics, the wave function is never a function of both the position *and* momentum of a particle at any instant, because of the Heisenberg uncertainty principle; if the position of the particle is known exactly, the momentum is not known at all, and vice versa. For a particle in 1d we can never write a wave function as Ψ(*x*, *p*, *t*). Taken together, *x* and *p* are called phase space variables. However, it is possible to construct a phase space formulation of quantum mechanics, using different mathematics and physical interpretations, in a way that does not violate the uncertainty principle.

Following are the general forms of the wave function for systems in higher dimensions and more particles, as well as including other degrees of freedom than position coordinates or momentum components.

The position-space wave function of a single particle in three spatial dimensions is similar to the case of one spatial dimension above:

where **r** is the position vector in three-dimensional space, and *t* is time. As always Ψ(**r**, *t*) is a complex number, for this case a complex-valued function of four real variables.

If there are many particles, in general there is only one wave function, not a separate wave function for each particle. The fact that *one* wave function describes *many* particles is what makes quantum entanglement and the EPR paradox possible. The position-space wave function for *N* particles is written:^{[12]}

where **r**_{i} is the position of the *i*th particle in three-dimensional space, and *t* is time. Altogether, this is a complex-valued function of 3*N* + 1 real variables.

For a particle with spin, the wave function can be written in "position–spin space" as:

where **r** is a position in three-dimensional space, *t* is time, and *s*_{z} is the spin projection quantum number along the *z* axis. (The *z* axis is an arbitrary choice; other axes can be used instead if the wave function is transformed appropriately, see below.) The *s _{z}* parameter, unlike

For spinless wave functions, Ψ* Ψ is the complex scalar needed for normalization, but for spin wave functions the Hermitian conjugate (complex conjugate of the transpose of the column vector into a row vector) is required to obtain the real number Ψ^{†} Ψ (the ordering of Ψ^{†} and Ψ does matter – see matrix multiplication).

Since the position and spin degrees of freedom of the particle are separate from one another, the wave function is a product of a purely position space wave function *ψ* and a purely spin-dependent function *ξ*:^{[18]}

The wave function for *N* particles each with spin is:

and the wave function is a product of a position space wave function *ψ* and a spin-dependent function *ξ*:^{[19]}

Concerning the general case of *N* particles with spin in 3d, if Ψ is interpreted as a probability amplitude, the probability density is:

and the probability that particle 1 is in region *R*_{1} with spin *s*_{z1} = *m*_{1} *and* particle 2 is in region *R*_{2} with spin *s*_{z2} = *m*_{2} etc. at time *t* is the integral of the probability density over these regions and spins:

The multidimensional Fourier transforms of the position or position–spin space wave functions yields momentum or momentum–spin space wave functions.

The **inner product** of two wave functions Ψ_{1} and Ψ_{2} is useful and important for a number of reasons given below. For the case of one spinless particle in 1d, it can be defined as the complex number (at time *t*)^{[nb 1]}

More generally, the formulae for the inner products are integrals over all coordinates or momenta and sums over all spin quantum numbers. That is, for one spinless particle in 3d the inner product of two wave functions can be defined as the complex number:

while for many spinless particles in 3d:

(altogether, this is *N* three-dimensional volume integrals with differential volume elements *d*^{3}**r**_{i}, also written "*dV*_{i}" or "*dx _{i} dy_{i} dz_{i}*"). For one particle with spin in 3d:

and for the general case of *N* particles with spin in 3d:

(altogether, *N* three-dimensional volume integrals followed by *N* sums over the spins).

In the Copenhagen interpretation, the modulus squared of the inner product (a complex number) gives a real number

which is interpreted as the probability of the wave function Ψ_{2} "collapsing" to the new wave function Ψ_{1} upon measurement of an observable, whose eigenvalues are the possible results of the measurement, with Ψ_{1} being an eigenvector of the resulting eigenvalue.

Although the inner product of two wave functions is a complex number, the inner product of a wave function Ψ with itself,

is *always* a positive real number. The number ||Ψ|| (not ||Ψ||^{2}) is called the **norm** of the wave function Ψ, and is not the same as the modulus |Ψ|.

A wave function is normalized if:

If Ψ is not normalized, then dividing by its norm gives the normalized function Ψ/||Ψ||.

Two wave functions Ψ_{1} and Ψ_{2} are orthogonal if their inner product is zero:

A set of wave functions Ψ_{1}, Ψ_{2}, ... are orthonormal if they are each normalized and are all orthogonal to each other:

where *m* and *n* each take values 1, 2, ..., and *δ _{mn}* is the Kronecker delta (+1 for

Returning to the superposition above:

if the basis wave functions *ψ _{n}* are orthonormal, then the coefficients have a particularly simple form:

If the basis wave functions were not orthonormal, then the coefficients would be different.

Analogous to the position case, the inner product of two wave functions Φ_{1}(*p*, *t*) and Φ_{2}(*p*, *t*) can be defined as:

and similarly for more particles in higher dimensions.

One particular solution to the time-independent Schrödinger equation is

a plane wave, which can be used in the description of a particle with momentum exactly *p*, since it is an eigenfunction of the momentum operator. These functions are not normalizable to unity (they aren't square-integrable), so they are not really elements of physical Hilbert space. The set

forms what is called the **momentum basis**. This "basis" is not a basis in the usual mathematical sense. For one thing, since the functions aren't normalizable, they are instead **normalized to a delta function**,

For another thing, though they are linearly independent, there are too many of them (they form an uncountable set) for a basis for physical Hilbert space. They can still be used to express all functions in it using Fourier transforms as described above.

Although wave functions are complex numbers, both the real and imaginary parts each have the same units (the imaginary unit *i* is a pure number without physical units). The units of *ψ* depend on the number of particles *N* the wave function describes, and the number of spatial or momentum dimensions *n* of the system.

When integrating |*ψ*|^{2} over all the coordinates, the volume element *d*^{n}**r**_{1}*d*^{n}**r**_{2}...*d*^{n}**r**_{N} has units of [length]^{Nn}. Since the normalization conditions require the integral to be the unitless number 1, |*ψ*|^{2} must have units of [length]^{−Nn}, thus the units of |*ψ*| and hence *ψ* are [length]^{−Nn/2}. Likewise, in momentum space, length is replaced by momentum, and the units are [momentum]^{−Nn/2}. These results are true for particles of any spin, since for particles with spin, the summations are over dimensionless spin quantum numbers.

Further information: Identical particles § wave function representation

In quantum mechanics there is a fundamental distinction between *identical particles* and *distinguishable* particles. For example, any two electrons are identical and fundamentally indistinguishable from each other; the laws of physics make it impossible to "stamp an identification number" on a certain electron to keep track of it.^{[20]} This translates to a requirement on the wave function for a system of *N* identical particles all of common spin *s*; the wave function of the system is either totally symmetric or totally antisymmetric in all the positions of the particles:^{[21]}

where the + sign occurs if the particles are *all bosons* (*s* = 0, 1, 2,...), and − sign if they are *all fermions* (*s* = 1/2, 3/2,...). For *N* identical particles there is no such thing as "mixed symmetry": the wave function cannot be symmetric for some of the particles and antisymmetric for others. Notice the physical interchange of particles corresponds to mathematically switching arguments in the wave function.

The antisymmetry feature of fermionic wave functions leads to the Pauli principle. Generally, bosonic and fermionic symmetry requirements are the manifestation of particle statistics and are present in other quantum state formalisms.

For *N* *distinguishable* particles (no two being identical), there is no requirement for the wave function to be either symmetric or antisymmetric.

For a collection of particles, some identical all of spin *s* with coordinates **r**_{1}, **r**_{2}, ... and others distinguishable **x**_{1}, **x**_{2}, ... (not identical with each other, and not identical to the aforementioned identical particles), the wave function is symmetric or antisymmetric in the identical particle coordinates **r**_{i} only:

Again, there is no symmetry requirement for the distinguishable particle coordinates **x**_{i}.

Main article: Quantum state

The set of all possible wave functions (at any given time) forms an abstract mathematical vector space. This vector space is infinite-dimensional, because there is no finite set of functions which can be added together in various combinations to create every possible function. Specifically, the *entire* wave function is treated as a *single* abstract vector:

where |Ψ⟩ is a "ket" (a vector) written in bra–ket notation. As always, the state vector for the system is solved from the Schrödinger equation (or other dynamical pictures of quantum mechanics):

The statement that "wave functions form an abstract vector space" means that it is possible to multiply wave functions by complex numbers and add together different wave functions in a coherent superposition. If |*ψ*⟩ and |*ϕ*⟩ are two states in the vector space, and *a* and *b* are two complex numbers, then the linear combination

(subject to normalization) is also in the same vector space. The dual vectors are denoted as "bras", ⟨Ψ|, which do not live in the same space as |Ψ⟩, but instead the dual space:

where * denotes complex conjugate.

The inner product of two wave functions |Ψ_{1}⟩ and |Ψ_{2}⟩ can be defined by

For these reasons, wave functions are elements of a Hilbert space. See the quantum state article for more explanation of the Hilbert space formalism and its consequences to quantum physics.

There are several advantages to understanding wave functions as elements of an abstract vector space:

- All the powerful tools of linear algebra can be used to manipulate and understand wave functions. For example:
- Linear algebra explains how a vector space can be given a basis, and then any vector in the vector space can be expressed in this basis. This explains the relationship between a wave function in position space and a wave function in momentum space, and suggests that there are other possibilities too.
- Bra–ket notation can be used to manipulate wave functions.

- The idea that quantum states are vectors in an abstract vector space (technically, a complex projective Hilbert space) is completely general in all aspects of quantum mechanics and quantum field theory, whereas the idea that quantum states are complex-valued "wave" functions of space is only true in certain situations.

Following is a summary of the bra–ket formalism applied to wave functions, with general discrete or continuous bases.

A Hilbert space with a discrete basis |*ε _{i}*⟩ for

Orthonormal bases are convenient to work with because the inner product of two vectors have simple expressions. A wave function |Ψ⟩ expressed in this discrete basis of the Hilbert space, and the corresponding bra in the dual space, are respectively given by:

where the complex numbers

are the components of the vector. The column vector is a useful way to list the numbers, and operations on the entire vector can be done according to matrix addition and multiplication. The entire vector |Ψ⟩ is independent of the basis, but the components depend on the basis. If a change of basis is made, the components of the vector must also change to compensate.

A Hilbert space with a continuous basis { |*ε*⟩ } is orthonormal if the inner product of all pairs of basis kets are given by the Dirac delta function:

As with the discrete bases, a symbol *ε* is used in the basis states, two common notations are |*ε*⟩ and sometimes |Ψ_{ε}⟩. A particular basis ket may be subscripted |*ε*_{0}⟩ ≡ |Ψ_{ε0}⟩ or primed |*ε*′⟩ ≡ |Ψ_{ε′}⟩, or simply given another symbol in place of *ε*.

While discrete basis vectors are summed over a discrete index, continuous basis vectors are integrated over a continuous index (a variable of a function). In what follows, all integrals are with respect to the real-valued basis variable *ε* (not complex-valued), over the required range. Usually this is just the real line or subsets of it. The state |Ψ⟩ in the continuous basis of the Hilbert space, with the corresponding bra in the dual space, are respectively given by:^{[22]}

where the components are the complex-valued functions

of a real variable *ε*.

The **completeness conditions** (also called **closure relations**) are

for discrete and continuous orthonormal bases, respectively. An orthonormal set of kets form bases if and only if they satisfy these relations.^{[22]} In each case, the equality to unity means this is an identity operator; its action on any state leaves it unchanged. Multiplying any state on the right of these gives the representation of the state |Ψ⟩ in the basis. The inner product of a first state |Ψ_{1}⟩ with a second |Ψ_{2}⟩ can also be obtained by multiplying |Ψ_{1}⟩ on the left and |Ψ_{2}⟩ on the right of the relevant completeness condition.

Physically, the nature of the inner product is dependent on the basis in use, because the basis is chosen to reflect the quantum state of the system.

If |Ψ_{1}⟩ is a state in the above basis with components *c*_{1}, *c*_{2}, ..., *c*_{n} and |Ψ_{2}⟩ is another state in the same basis with components *z*_{1}, *z*_{2}, ..., *z*_{n}, the inner product is the complex number:

If |Ψ_{1}⟩ is a state in the above continuous basis with components Ψ_{1}(*ε*′), and |Ψ_{2}⟩ is another state in the same basis with components Ψ_{2}(*ε*), the inner product is the complex number:

where the integrals are taken over all *ε* and *ε*′.

The square of the **norm (magnitude)** of the state vector |Ψ⟩ is given by the inner product of |Ψ⟩ with itself, a real number:

for the discrete and continuous bases, respectively. Each say the projection of a complex probability amplitude onto itself is real. If |Ψ⟩ is normalized, these expressions would be each separately equal to 1. If the state is not normalized, then dividing by its magnitude normalizes the state:

In the literature, the following results are often presented with normalized wavefunctions. Here, we keep the normalization factors to show where they appear if the wavefunction is not already normalized.

For the discrete basis, projecting the normalized state |Ψ_{N}⟩ onto a particular state the system may collapse to, |*ε _{q}*⟩, gives the complex number;

so the modulus squared of this gives a real number;

In the Copenhagen interpretation, this is the probability of state |*ε _{q}*⟩ occurring.

In the continuous basis, the projection of the normalized state onto some particular basis |*ε*′⟩ is a complex-valued function;

so the squared modulus is a real-valued function

In the Copenhagen interpretation, this function is the *probability density function* of measuring the observable *ε*′, so integrating this with respect to *ε*′ between *a* ≤ *ε*′ ≤ *b* gives:

the probability of finding the system with *ε*′ between *ε*′ = *a* and *ε*′ = *b*.

The physical meaning of the components of |Ψ⟩ is given by the *wave function collapse postulate*, also known as wave function collapse. If the observable(s) *ε* (momentum and/or spin, position and/or spin, etc.) corresponding to states |*ε _{i}*⟩ has distinct and definite values,

In the Schrödinger picture, the states evolve in time, so the time dependence is placed in |Ψ⟩ according to:^{[23]}

for discrete bases, or

for continuous bases. However, in the Heisenberg picture the states |Ψ⟩ are constant in time and time dependence is placed in the Heisenberg operators, so |Ψ⟩ is not written as |Ψ(*t*)⟩.

Further information: Bra-ket notation § Composite bras and kets

It is useful to introduce another operation with the physical interpretation of forming composite states from a collection of other states. This is the tensor product. Given two systems described by states |Ψ⟩ and |Φ⟩, the tensor product of the states forms the composite state denoted by |Ψ⟩⊗|Φ⟩ or simply without any operation symbol |Ψ⟩|Φ⟩, and the new system includes both of the original systems together. The tensor product state |Ψ⟩|Φ⟩ lives in a new space; the tensor product of the original Hilbert spaces. The bases spanning this space are the tensor products of the original bases. The product is not commutative in general, so |Ψ⟩|Φ⟩ ≠ |Φ⟩|Ψ⟩. If |Ψ⟩ has components *c _{i}* and |Φ⟩ has components

and the notation can be simplified by abbreviating |*A*⟩ = |Ψ⟩|Φ⟩, *A _{ij}* =

The same procedure follows for continuous bases using integration. This can also be extended to any number of states, however taking tensor products for fermions and bosons is complicated by the symmetry requirements, see identical particles for general results.

For a spinless particle in one spatial dimension (the *x*-axis or real line), the state |Ψ⟩ can be expanded in terms of a continuum of basis states; |*x*⟩, also written |Ψ_{x}⟩, corresponding to the set of all position coordinates *x*. The completeness condition for this basis is

and the orthogonality relation is

The state |Ψ⟩ is expressed by:

in which the "wave function" described as a function is a component of the complex state vector.

The inner product as stated at the beginning of this article is:

If the particle is confined to a region *R* (a subset of the *x*-axis), the integrals in the inner product and completeness condition would be integrals over *R*.

The previous example can be extended to more particles in higher dimensions, and include spin.

For one spinless particle in 3d, the basis states are |**r**⟩ and any state vector |Ψ⟩ in this space is expressed in terms of the basis vectors as |**r**⟩:

with components:

For *N* spinless particles in 3d, the basis states are |**r**_{1}, ..., **r**_{N}⟩. This is the tensor product of the one-particle position bases |**r**_{1}⟩, |**r**_{2}⟩, ..., |**r**_{N}⟩, each of which spans the separate one-particle Hilbert spaces, so |**r**_{1}, ..., **r**_{N}⟩ are the basis states for the tensor product of the one-particle Hilbert spaces (the Hilbert space for the composite many particle system). Any state vector |Ψ⟩ in this space is

with components:

For one particle with spin in 3d, the basis states are |**r**, *s*_{z}⟩, the tensor product of the position basis |**r**⟩ and spin basis |*s*_{z}⟩, which exists in a new space from the spin space and position space alone. Any state |Ψ⟩ in this space is:

with components:

For *N* particles with spin in 3d, the basis states are |**r**_{1}, ..., **r**_{N}, *s*_{z 1}, ..., *s*_{z N}⟩, the tensor product of the position basis |**r**_{1}, ..., **r**_{N}⟩ and spin basis |*s*_{z 1}, ..., *s*_{z N}⟩, which exists in a new space from the spin space and position space alone. Any state in this space is:

with components:

If the particles are restricted to regions of position space, then the integrals in the completeness relations are taken over those regions, rather than the entire coordinate space. For the general case of many particles with spin in 3d, if particle 1 is in region *R*_{1}, particle 2 is in region *R*_{2}, and so on, the state in this position–spin representation is:

The orthogonality relation for this basis is:

and the inner product of |Ψ_{1}⟩ and |Ψ_{2}⟩ is:

Momentum space wave functions are similar, using the momentum vectors of the particles as continuous bases, namely |**p**⟩, |**p**_{1}, **p**_{2}, ..., **p**_{N}⟩, etc.

Main article: Interpretations of quantum mechanics

Whether the wave function really exists, and what it represents, are major questions in the interpretation of quantum mechanics. Many famous physicists of a previous generation puzzled over this problem, such as Schrödinger, Einstein and Bohr. Some advocate formulations or variants of the Copenhagen interpretation (e.g. Bohr, Wigner and von Neumann) while others, such as Wheeler or Jaynes, take the more classical approach^{[24]} and regard the wave function as representing information in the mind of the observer, i.e. a measure of our knowledge of reality. Some, including Schrödinger, Bohm and Everett and others, argued that the wave function must have an objective, physical existence. Einstein thought that a complete description of physical reality should refer directly to physical space and time, as distinct from the wave function, which refers to an abstract mathematical space.^{[25]} For more on this topic, see Interpretations of quantum mechanics.

Main article: Free particle

A free particle in 3d with wave vector **k** and angular frequency *ω* has a wave function

Main article: Particle in a box

A particle is restricted to a 1D region between *x* = 0 and *x* = *L*; its wave function is:

To normalize the wave function we need to find the value of the arbitrary constant *A*; solved from

From Ψ, we have |Ψ|^{2} = *A*^{2}, so the integral becomes;

Solving this equation gives *A* = 1/√*L*, so the normalized wave function in the box is;

Main articles: Finite potential barrier and Quantum tunnelling

One of most prominent features of the wave mechanics is a possibility for a particle to reach a location with a prohibitive (in classical mechanics) force potential. In the one-dimensional case of particles with energy less than in the square potential

the steady-state solutions to the wave equation have the form (for some constants )

Note that these wave functions are not normalized; see scattering theory for discussion.

The standard interpretation of this is as a stream of particles being fired at the step from the left (the direction of negative *x*): setting *A*_{r} = 1 corresponds to firing particles singly; the terms containing *A*_{r} and *C*_{r} signify motion to the right, while *A*_{l} and *C*_{l} – to the left. Under this beam interpretation, put *C*_{l} = 0 since no particles are coming from the right. By applying the continuity of wave functions and their derivatives at the boundaries, it is hence possible to determine the constants above.

Some examples of wave functions for specific applications include:

- Boson
- de Broglie–Bohm theory
- Double-slit experiment
- Faraday wave
- Fermion
- Schrödinger equation
- Wave function collapse
- Wave packet

**^**The functions are here assumed to be elements of*L*^{2}, the space of square integrable functions. The elements of this space are more precisely equivalence classes of square integrable functions, two functions declared equivalent if they differ on a set of Lebesgue measure 0. This is necessary to obtain an inner product (that is, (Ψ, Ψ) = 0 ⇒ Ψ ≡ 0) as opposed to a**semi-inner product**. The integral is taken to be the Lebesque integral. This is essential in proving completeness of the space, thus yielding a complete inner product space = Hilbert space.

**^**Born, M. (1927). Physical aspects of quantum mechanics,*Nature*,**119**, 354–357.**^**Heisenberg, W. (1958).*Physics and Philosophy: the Revolution in Modern Science*, Harper & Row, New York, p. 143.**^**Heisenberg, W. (1927/1985/2009). Heisenberg is quoted by Camilleri, K. (2009), (from Bohr, N. (1985),*Collected Works*, edited by J. Kalckar, volume 6, 'Foundations of Quantum Mechanics I 1926–1932, Morth-Holland, Amsterdam, p. 140),*Heisenberg and the Interpretation of Quantum Mechanics: the Physicist as Philosopher*, Cambridge University Press, Cambridge UK, ISBN 978-0-521-88484-6, p. 71.**^**Murdoch, D. (1987).*Niels Bohr's Philosophy of Physics*, Cambridge University Press, Cambridge UK, ISBN 0-521-33320-2, p. 43.**^**de Broglie, L., (1960).*Non-linear Wave Mechanics: a Causal Interpretation*, Elsevier, Amsterdam, p. 48.**^**Landau, L.D., Lifshitz, E.M. (1958/1965).*Quantum Mechanics: Non-relativistic Theory*, translated from Russian by J.B. Sykes and J.S. Bell, second edition 1965, Pergamon Press, Oxford UK, p. 6.**^**Newton, R.G. (2002).*Quantum Physics: a Text for Graduate Students*, Springer, New York, ISBN 0-387-95473-2, pp. 19–21.**^**R.G. Lerner, G.L. Trigg (1991).*Encyclopaedia of Physics*(2nd ed.). VHC Publishers. pp. 1223–1229. ISBN 0-89573-752-3.**^**Hanle, P.A. (December 1977), "Erwin Schrodinger's Reaction to Louis de Broglie's Thesis on the Quantum Theory.",*Isis***68**(4): 606–609, doi:10.1086/351880**^**Physics for Scientists and Engineers – with Modern Physics (6th Edition), P. A. Tipler, G. Mosca, Freeman, 2008, ISBN 0-7167-8964-7**^**Sears' and Zemansky's University Physics, Young and Freedman (12th edition), Pearson Ed. & Addison-Wesley Inc., 2008, ISBN 978-0-321-50130-1- ^
^{a}^{b}^{c}Quanta: A handbook of concepts, P.W. Atkins, Oxford University Press, 1974, ISBN 0-19-855493-1 **^**Particle Physics (3rd Edition), B.R. Martin, G. Shaw, Manchester Physics Series, John Wiley & Sons, 2008, ISBN 978-0-470-03294-7**^**Quantum Physics of Atoms, Molecules, Solids, Nuclei and Particles (2nd Edition), R. Resnick, R. Eisberg, John Wiley & Sons, 1985, ISBN 978-0-471-87373-0**^**A.I.M. Rae (2008).*Quantum Mechanics***2**(5th ed.). Taylor & Francis Group. ISBN 1-5848-89705.**^**P. W. Atkins (1974).*Quanta: A Handbook of Concepts*. p. 258. ISBN 0-19-855494-X.**^**Griffiths.*Introduction to Quantum Mechanics*(1st ed.). p. 107.**^**N. Zettili.*Quantum Mechanics: Concepts and Applications*(2nd ed.). p. 300-301. ISBN 978-0-470-02679-3.**^**N. Zettili.*Quantum Mechanics: Concepts and Applications*(2nd ed.). p. 468. ISBN 978-0-470-02679-3.**^**Griffiths, p. 179 of the first edition**^**N. Zettili.*Quantum Mechanics: Concepts and Applications*(2nd ed.). p. 463. ISBN 978-0-470-02679-3.- ^
^{a}^{b}Y. Peleg, R. Pnini, E. Zaarur, E. Hecht.*Quantum Mechanics*. Schaum's Outlines (2nd ed.). pp. 64–65. ISBN 978-0-07-162358-2. **^**Y. Peleg, R. Pnini, E. Zaarur, E. Hecht (2010).*Quantum mechanics*. Schaum's outlines (2nd ed.). McGraw Hill. pp. 68–69. ISBN 978-0-07-162358-2.**^**E. T. Jaynes.*Probability Theory: The Logic of Science*, Cambridge University Press (2003),**^**Einstein, A. (1951). Reply to Criticism, in*Albert Einstein: Philosopher-Scientist*, edited by P.A. Schilpp, Open Court, La Salle IL, volume 2, pages 663–688, p. 682.

- L.D. Landau, E.M. Lifshitz (1977).
*Quantum Mechanics: Non-Relativistic Theory*. Vol. 3 (3rd ed.). Pergamon Press. ISBN 978-0-08-020940-1. - Griffiths, David J. (2004).
*Introduction to Quantum Mechanics (2nd ed.)*. Prentice Hall. ISBN 0-13-111892-7. - Yong-Ki Kim (September 2, 2000). "Practical Atomic Physics".
*National Institute of Standards and Technology*(Maryland): 1 (55 pages). Retrieved 2010-08-17. - Polkinghorne, John (2002).
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