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In quantum mechanics, **bra–ket notation,** or **Dirac notation**, is ubiquitous. The notation uses the angle brackets, "" and "", and a vertical bar "", to construct "bras" /brɑː/ and "kets" /kɛt/ .

- Introduction
- Vector spaces
- Vectors vs kets
- Bra-ket notation
- Inner product and bra-ket identification on Hilbert space
- Non-normalizable states and non-Hilbert spaces
- Usage in quantum mechanics
- Spinless position–space wave function
- Overlap of states
- Changing basis for a spin-½ particle
- Pitfalls and ambiguous uses
- Separation of inner product and vectors
- Reuse of symbols
- Hermitian conjugate of kets
- Operations inside bras and kets
- Linear operators
- Linear operators acting on kets
- Linear operators acting on bras
- Outer products
- Hermitian conjugate operator
- Properties
- Linearity
- Associativity
- Hermitian conjugation
- Composite bras and kets
- The unit operator
- Notation used by mathematicians
- See also
- Notes
- References
- External links

A **ket** looks like "". Mathematically it denotes a vector, , in an abstract (complex) vector space , and physically it represents a state of some quantum system.

A **bra** looks like "", and mathematically it denotes a linear form , i.e. a linear map that maps each vector in to a number in the complex plane . Letting the linear functional act on a vector is written as .

Assume on exists an inner product with antilinear first argument, which makes a Hilbert space. Then with this inner product each vector can be identified with a corresponding linear form, by placing the vector in the anti-linear first slot of the inner product: . The correspondence between these notations is then . The linear form is a covector to , and the set of all covectors form a subspace of the dual vector space , to the initial vector space . The purpose of this linear form can now be understood in terms of making projections on the state , to find how linearly dependent two states are, etc.

For the vector space , kets can be identified with column vectors, and bras with row vectors. Combinations of bras, kets, and operators are interpreted using matrix multiplication. If has the standard hermitian inner product , under this identification, the identification of kets and bras and vice versa provided by the inner product is taking the Hermitian conjugate (denoted ).

It is common to suppress the vector or linear form from the bra–ket notation and only use a label inside the typography for the bra or ket. For example, the spin operator on a two dimensional space of spinors, has eigenvalues ½ with eigenspinors . In bra-ket notation one typically denotes this as , and . Just as above, kets and bras with the same label are interpreted as kets and bras corresponding to each other using the inner product. In particular when also identified with row and column vectors, kets and bras with the same label are identified with Hermitian conjugate column and row vectors.

Bra–ket notation was effectively established in 1939 by Paul Dirac ^{ [1] }^{ [2] } and is thus also known as the Dirac notation. (Still, the bra-ket notation has a precursor in Hermann Grassmann's use of the notation for his inner products nearly 100 years earlier.^{ [3] }^{ [4] })

Bra–ket notation is a notation for linear algebra and linear operators on complex vector spaces together with their dual space both in the finite-dimensional and infinite-dimensional case. It is specifically designed to ease the types of calculations that frequently come up in quantum mechanics. Its use in quantum mechanics is quite widespread. Many phenomena that are explained using quantum mechanics are explained using bra–ket notation.

In mathematics, the term "vector" is used for an element of any vector space. In physics, however, the term "vector" is much more specific: "vector" refers almost exclusively to quantities like displacement or velocity, which have components that relate directly to the three dimensions of space, or relativistically, to the four of space time. Such vectors are typically denoted with over arrows (), boldface () or indices ().

In quantum mechanics, a quantum state is typically represented as an element of a complex Hilbert space, for example, the infinite-dimensional vector space of all possible wavefunctions (square integrable functions mapping each point of 3D space to a complex number) or some more abstract Hilbert space constructed more algebraically. Since the term "vector" is already used for something else (see previous paragraph), and physicists tend to prefer conventional notation to stating what space something is an element of, it is common and useful to denote an element of an abstract complex vector spaces as a ket using vertical bars and angular brackets and refer to them as "kets" rather than as vectors and pronounced "ket-" or "ket-A" for |*A*⟩.

Symbols, letters, numbers, or even words—whatever serves as a convenient label—can be used as the label inside a ket, with the making clear that the label indicates a vector in vector space. In other words, the symbol "|*A*⟩" has a specific and universal mathematical meaning, while just the "*A*" by itself does not. For example, |1⟩ + |2⟩ is not necessarily equal to |3⟩. Nevertheless, for convenience, there is usually some logical scheme behind the labels inside kets, such as the common practice of labeling energy eigenkets in quantum mechanics through a listing of their quantum numbers. At its simplest, the label inside the ket is the eigenvalue of a physical operator, such as , , , etc.

Since kets are just vectors in a Hermitian vector space they can be manipulated using the usual rules of linear algebra, for example:

Note how the last line above involves infinitely many different kets, one for each real number *x*.

Since the ket is an element of a vector space, a **bra** is an element of its dual space, i.e. a bra is a linear functional which is a linear map from the vector space to the complex numbers. Thus, it is useful to think of kets and bras as being elements of different vector spaces (see below however) with both being different useful concepts.

A bra and a ket (i.e. a functional and a vector), can be combined to an operator of rank one with outer product

The bra-ket notation is particularly useful in Hilbert spaces which have an inner product ^{ [5] } that allows Hermitian conjugation and identifying a vector with a linear functional, i.e. a ket with a bra, and vice versa (see Riesz representation theorem). The inner product on Hilbert space (with the first argument anti linear as preferred by physicists) is fully equivalent to an (anti linear) identification between the space of kets and that of bras in the bra ket notation: for a vector ket define a functional (i.e. bra) by

In the simple case where we consider the vector space , a ket can be identified with a column vector, and a bra as a row vector. If moreover we use the standard Hermitian inner product on , the bra corresponding to a ket, in particular a bra ⟨*m*| and a ket |*m*⟩ with the same label are conjugate transpose. Moreover, conventions are set up in such a way that writing bras, kets, and linear operators next to each other simply imply matrix multiplication.^{ [6] } In particular the outer product of a column and a row vector ket and bra can be identified with matrix multiplication (column vector times row vector equals matrix).

For a finite-dimensional vector space, using a fixed orthonormal basis, the inner product can be written as a matrix multiplication of a row vector with a column vector:

Based on this, the bras and kets can be defined as:

and then it is understood that a bra next to a ket implies matrix multiplication.

The conjugate transpose (also called *Hermitian conjugate*) of a bra is the corresponding ket and vice versa:

because if one starts with the bra

then performs a complex conjugation, and then a matrix transpose, one ends up with the ket

Writing elements of a finite dimensional (or mutatis mutandis, countably infinite) vector space as a column vector of numbers requires picking a basis. Picking a basis is not always helpful because quantum mechanics calculations involve frequently switching between different bases (e.g. position basis, momentum basis, energy eigenbasis), and one can write something like "|*m*⟩" without committing to any particular basis. In situations involving two different important basis vectors, the basis vectors can be taken in the notation explicitly and here will be referred simply as "|*−*⟩" and "|*+*⟩".

Bra–ket notation can be used even if the vector space is not a Hilbert space.

In quantum mechanics, it is common practice to write down kets which have infinite norm, i.e. non-normalizable wavefunctions. Examples include states whose wavefunctions are Dirac delta functions or infinite plane waves. These do not, technically, belong to the Hilbert space itself. However, the definition of "Hilbert space" can be broadened to accommodate these states (see the Gelfand–Naimark–Segal construction or rigged Hilbert spaces). The bra–ket notation continues to work in an analogous way in this broader context.

Banach spaces are a different generalization of Hilbert spaces. In a Banach space B, the vectors may be notated by kets and the continuous linear functionals by bras. Over any vector space without topology, we may also notate the vectors by kets and the linear functionals by bras. In these more general contexts, the bracket does not have the meaning of an inner product, because the Riesz representation theorem does not apply.

The mathematical structure of quantum mechanics is based in large part on linear algebra:

- Wave functions and other quantum states can be represented as vectors in a complex Hilbert space. (The exact structure of this Hilbert space depends on the situation.) In bra–ket notation, for example, an electron might be in the "state" |
*ψ*⟩. (Technically, the quantum states are*rays*of vectors in the Hilbert space, as*c*|*ψ*⟩ corresponds to the same state for any nonzero complex number*c*.) - Quantum superpositions can be described as vector sums of the constituent states. For example, an electron in the state |1⟩ +
*i*|2⟩ is in a quantum superposition of the states |1⟩ and |2⟩. - Measurements are associated with linear operators (called observables) on the Hilbert space of quantum states.
- Dynamics are also described by linear operators on the Hilbert space. For example, in the Schrödinger picture, there is a linear time evolution operator
*U*with the property that if an electron is in state |*ψ*⟩ right now, at a later time it will be in the state*U*|*ψ*⟩, the same*U*for every possible |*ψ*⟩. - Wave function normalization is scaling a wave function so that its norm is 1.

Since virtually every calculation in quantum mechanics involves vectors and linear operators, it can involve, and often does involve, bra–ket notation. A few examples follow:

The Hilbert space of a spin-0 point particle is spanned by a "position basis" { |**r**⟩ }, where the label **r** extends over the set of all points in position space. This label is the eigenvalue of the position operator acting on such a basis state, . Since there are an uncountably infinite number of vector components in the basis, this is an uncountably infinite-dimensional Hilbert space. The dimensions of the Hilbert space (usually infinite) and position space (usually 1, 2 or 3) are not to be conflated.

Starting from any ket |Ψ⟩ in this Hilbert space, one may *define* a complex scalar function of **r**, known as a wavefunction,

On the left-hand side, Ψ(**r**) is a function mapping any point in space to a complex number; on the right-hand side, |Ψ⟩ = ∫ d^{3}**r** Ψ(**r**) |**r**⟩ is a ket consisting of a superposition of kets with relative coefficients specified by that function.

It is then customary to define linear operators acting on wavefunctions in terms of linear operators acting on kets, by

For instance, the momentum operator has the following coordinate representation,

One occasionally even encounters an expression such as

though this is something of an abuse of notation. The differential operator must be understood to be an abstract operator, acting on kets, that has the effect of differentiating wavefunctions once the expression is projected onto the position basis, even though, in the momentum basis, this operator amounts to a mere multiplication operator (by *iħ***p**). That is, to say,

or

In quantum mechanics the expression ⟨*φ*|*ψ*⟩ is typically interpreted as the probability amplitude for the state *ψ* to collapse into the state *φ*. Mathematically, this means the coefficient for the projection of *ψ* onto *φ*. It is also described as the projection of state *ψ* onto state *φ*.

A stationary spin-½ particle has a two-dimensional Hilbert space. One orthonormal basis is:

where |↑_{z}⟩ is the state with a definite value of the spin operator *S _{z}* equal to +½ and |↓

Since these are a basis, *any* quantum state of the particle can be expressed as a linear combination (i.e., quantum superposition) of these two states:

where *a _{ψ}* and

A *different* basis for the same Hilbert space is:

defined in terms of *S _{x}* rather than

Again, *any* state of the particle can be expressed as a linear combination of these two:

In vector form, you might write

depending on which basis you are using. In other words, the "coordinates" of a vector depend on the basis used.

There is a mathematical relationship between , , and ; see change of basis.

There are some conventions and uses of notation that may be confusing or ambiguous for the non-initiated or early student.

A cause for confusion is that the notation does not separate the inner-product operation from the notation for a (bra) vector. If a (dual space) bra-vector is constructed as a linear combination of other bra-vectors (for instance when expressing it in some basis) the notation creates some ambiguity and hides mathematical details. We can compare bra-ket notation to using bold for vectors, such as , and for the inner product. Consider the following dual space bra-vector in the basis :

It has to be determined by convention if the complex numbers are inside or outside of the inner product, and each convention gives different results.

It is common to use the same symbol for *labels* and *constants*. For example, , where the symbol is used simultaneously as the *name of the operator*, its *eigenvector* and the associated *eigenvalue*. Sometimes the *hat* is also dropped for operators, and one can see notation such as ^{ [7] }

It is common to see the usage , where the dagger () corresponds to the Hermitian conjugate. This is however not correct in a technical sense, since the ket, , represents a vector in a complex Hilbert-space , and the bra, , is a linear functional on vectors in . In other words, is just a vector, while is the combination of a vector and an inner product.

This is done for a fast notation of scaling vectors. For instance, if the vector is scaled by , it may be denoted . This can be ambiguous since is simply a label for a state, and not a mathematical object on which operations can be performed. This usage is more common when denoting vectors as tensor products, where part of the labels are moved **outside** the designed slot, e.g. .

A linear operator is a map that inputs a ket and outputs a ket. (In order to be called "linear", it is required to have certain properties.) In other words, if is a linear operator and is a ket-vector, then is another ket-vector.

In an -dimensional Hilbert space, we can impose a basis on the space and represent in terms of its coordinates as a column vector. Using the same basis for , it is represented by an complex matrix. The ket-vector can now be computed by matrix multiplication.

Linear operators are ubiquitous in the theory of quantum mechanics. For example, observable physical quantities are represented by self-adjoint operators, such as energy or momentum, whereas transformative processes are represented by unitary linear operators such as rotation or the progression of time.

Operators can also be viewed as acting on bras *from the right hand side*. Specifically, if * A* is a linear operator and ⟨

(in other words, a function composition). This expression is commonly written as (cf. energy inner product)

In an *N*-dimensional Hilbert space, ⟨*φ*| can be written as a 1 × *N* row vector, and * A* (as in the previous section) is an

If the same state vector appears on both bra and ket side,

then this expression gives the expectation value, or mean or average value, of the observable represented by operator * A* for the physical system in the state |

A convenient way to define linear operators on a Hilbert space H is given by the outer product: if ⟨*ϕ*| is a bra and |*ψ*⟩ is a ket, the outer product

denotes the rank-one operator with the rule

- .

For a finite-dimensional vector space, the outer product can be understood as simple matrix multiplication:

The outer product is an *N* × *N* matrix, as expected for a linear operator.

One of the uses of the outer product is to construct projection operators. Given a ket |*ψ*⟩ of norm 1, the orthogonal projection onto the subspace spanned by |*ψ*⟩ is

This is an idempotent in the algebra of observables that acts on the Hilbert space.

Just as kets and bras can be transformed into each other (making |*ψ*⟩ into ⟨*ψ*|), the element from the dual space corresponding to *A*|*ψ*⟩ is ⟨*ψ*|*A*^{†}, where *A*^{†} denotes the Hermitian conjugate (or adjoint) of the operator *A*. In other words,

If *A* is expressed as an *N* × *N* matrix, then *A*^{†} is its conjugate transpose.

Self-adjoint operators, where *A* = *A*^{†}, play an important role in quantum mechanics; for example, an observable is always described by a self-adjoint operator. If A is a self-adjoint operator, then ⟨*ψ*|*A*|*ψ*⟩ is always a real number (not complex). This implies that expectation values of observables are real.

Bra–ket notation was designed to facilitate the formal manipulation of linear-algebraic expressions. Some of the properties that allow this manipulation are listed herein. In what follows, *c*_{1} and *c*_{2} denote arbitrary complex numbers, *c** denotes the complex conjugate of *c*, *A* and *B* denote arbitrary linear operators, and these properties are to hold for any choice of bras and kets.

- Since bras are linear functionals,

- By the definition of addition and scalar multiplication of linear functionals in the dual space,
^{ [8] }

Given any expression involving complex numbers, bras, kets, inner products, outer products, and/or linear operators (but not addition), written in bra–ket notation, the parenthetical groupings do not matter (i.e., the associative property holds). For example:

and so forth. The expressions on the right (with no parentheses whatsoever) are allowed to be written unambiguously *because* of the equalities on the left. Note that the associative property does *not* hold for expressions that include nonlinear operators, such as the antilinear time reversal operator in physics.

Bra–ket notation makes it particularly easy to compute the Hermitian conjugate (also called *dagger*, and denoted †) of expressions. The formal rules are:

- The Hermitian conjugate of a bra is the corresponding ket, and vice versa.
- The Hermitian conjugate of a complex number is its complex conjugate.
- The Hermitian conjugate of the Hermitian conjugate of anything (linear operators, bras, kets, numbers) is itself—i.e.,

- Given any combination of complex numbers, bras, kets, inner products, outer products, and/or linear operators, written in bra–ket notation, its Hermitian conjugate can be computed by reversing the order of the components, and taking the Hermitian conjugate of each.

These rules are sufficient to formally write the Hermitian conjugate of any such expression; some examples are as follows:

- Kets:

- Inner products:

- Note that ⟨
*φ*|*ψ*⟩ is a scalar, so the Hermitian conjugate is just the complex conjugate, i.e.

- Matrix elements:

- Outer products:

Two Hilbert spaces *V* and *W* may form a third space *V* ⊗ *W* by a tensor product. In quantum mechanics, this is used for describing composite systems. If a system is composed of two subsystems described in *V* and *W* respectively, then the Hilbert space of the entire system is the tensor product of the two spaces. (The exception to this is if the subsystems are actually identical particles. In that case, the situation is a little more complicated.)

If |*ψ*⟩ is a ket in *V* and |*φ*⟩ is a ket in *W*, the direct product of the two kets is a ket in *V* ⊗ *W*. This is written in various notations:

See quantum entanglement and the EPR paradox for applications of this product.

Consider a complete orthonormal system (* basis *),

for a Hilbert space *H*, with respect to the norm from an inner product ⟨·,·⟩.

From basic functional analysis, it is known that any ket can also be written as

with ⟨·|·⟩ the inner product on the Hilbert space.

From the commutativity of kets with (complex) scalars, it follows that

must be the *identity operator*, which sends each vector to itself.

This, then, can be inserted in any expression without affecting its value; for example

where, in the last line, the Einstein summation convention has been used to avoid clutter.

In quantum mechanics, it often occurs that little or no information about the inner product ⟨*ψ*|*φ*⟩ of two arbitrary (state) kets is present, while it is still possible to say something about the expansion coefficients ⟨*ψ*|*e _{i}*⟩ = ⟨

For more information, see Resolution of the identity,

- 1 = ∫ d
*x*|*x*⟩⟨*x*| = ∫ d*p*|*p*⟩⟨*p*|, where - |
*p*⟩ = ∫ d*x**e*^{ixp/ħ}|*x*⟩/√2*πħ*.

Since ⟨*x*′|*x*⟩ = *δ*(*x* − *x*′), plane waves follow,

- ⟨
*x*|*p*⟩ =*e*^{ixp/ħ}/√2*πħ*.

In his book (1958), Ch. III.20, Dirac defines the *standard ket* which, up to a normalization, is the translationally invariant momentum eigenstate in the momentum representation, i.e., . Consequently, the corresponding wavefunction is a constant, , and

- , as well as .

Typically, when all matrix elements of an operator such as

are available, this resolution serves to reconstitute the full operator,

The object physicists are considering when using bra–ket notation is a Hilbert space (a complete inner product space).

Let H be a Hilbert space and *h* ∈ H a vector in H. What physicists would denote by |*h*⟩ is the vector itself. That is,

- .

Let H* be the dual space of H. This is the space of linear functionals on H. The isomorphism Φ : H → H* is defined by Φ(*h*) = *φ _{h}*, where for every

- ,

where IP(·,·), (·,·), ⟨·,·⟩ and ⟨·|·⟩ are different notations for expressing an inner product between two elements in a Hilbert space (or for the first three, in any inner product space). Notational confusion arises when identifying *φ _{h}* and

One ignores the parentheses and removes the double bars. Some properties of this notation are convenient since we are dealing with linear operators and composition acts like a ring multiplication.

Moreover, mathematicians usually write the dual entity not at the first place, as the physicists do, but at the second one, and they usually use not an asterisk but an overline (which the physicists reserve for averages and the Dirac spinor adjoint) to denote complex conjugate numbers; i.e., for scalar products mathematicians usually write

whereas physicists would write for the same quantity

- ↑ Dirac 1939
- ↑ Shankar 1994 , Chapter 1
- ↑ Grassmann 1862
- ↑ Lecture 2 | Quantum Entanglements, Part 1 (Stanford), Leonard Susskind on complex numbers, complex conjugate, bra, ket. 2006-10-02.
- ↑ Lecture 2 | Quantum Entanglements, Part 1 (Stanford), Leonard Susskind on inner product, 2006-10-02.
- ↑ Gidney, Craig (2017). Bra–Ket Notation Trivializes Matrix Multiplication
- ↑ Sakurai, Jun John (21 September 2017).
*Modern Quantum Mechanics*(2nd ed.). Cambridge University Press. ISBN 978-1-108-42241-3. - ↑ Lecture notes by Robert Littlejohn, eqns 12 and 13

In quantum mechanics, the **Hamiltonian** of a system is an operator corresponding to the total energy of that system, including both kinetic energy and potential energy. Its spectrum, the system's *energy spectrum* or its set of *energy eigenvalues*, is the set of possible outcomes obtainable from a measurement of the system's total energy. Due to its close relation to the energy spectrum and time-evolution of a system, it is of fundamental importance in most formulations of quantum theory.

**Riesz representation theorem**, sometimes called **Riesz–Fréchet representation theorem**, named after Frigyes Riesz and Maurice René Fréchet, establishes an important connection between a Hilbert space and its continuous dual space. If the underlying field is the real numbers, the two are isometrically isomorphic; if the underlying field is the complex numbers, the two are isometrically anti-isomorphic. The (anti-) isomorphism is a particular natural one as will be described next; a natural isomorphism.

The **Schrödinger equation** is a linear partial differential equation that governs the wave function of a quantum-mechanical system. It is a key result in quantum mechanics, and its discovery was a significant landmark in the development of the subject. The equation is named after Erwin Schrödinger, who postulated the equation in 1925, and published it in 1926, forming the basis for the work that resulted in his Nobel Prize in Physics in 1933.

A **wave function** in quantum physics is a mathematical description of the quantum state of an isolated quantum system. The wave function is a complex-valued probability amplitude, and the probabilities for the possible results of measurements made on the system can be derived from it. The most common symbols for a wave function are the Greek letters *ψ* and Ψ.

**Quantum decoherence** is the loss of quantum coherence. In quantum mechanics, particles such as electrons are described by a wave function, a mathematical representation of the quantum state of a system; a probabilistic interpretation of the wave function is used to explain various quantum effects. As long as there exists a definite phase relation between different states, the system is said to be coherent. A definite phase relationship is necessary to perform quantum computing on quantum information encoded in quantum states. Coherence is preserved under the laws of quantum physics.

In mathematics, a **self-adjoint operator** on a finite-dimensional complex vector space *V* with inner product is a linear map *A* that is its own adjoint: for all vectors v and w. If *V* is finite-dimensional with a given orthonormal basis, this is equivalent to the condition that the matrix of *A* is a Hermitian matrix, i.e., equal to its conjugate transpose *A*^{∗}. By the finite-dimensional spectral theorem, *V* has an orthonormal basis such that the matrix of *A* relative to this basis is a diagonal matrix with entries in the real numbers. In this article, we consider generalizations of this concept to operators on Hilbert spaces of arbitrary dimension.

The **Fock space** is an algebraic construction used in quantum mechanics to construct the quantum states space of a variable or unknown number of identical particles from a single particle Hilbert space H. It is named after V. A. Fock who first introduced it in his 1932 paper "Konfigurationsraum und zweite Quantelung".

In physics, an **operator** is a function over a space of physical states onto another space of physical states. The simplest example of the utility of operators is the study of symmetry. Because of this, they are very useful tools in classical mechanics. Operators are even more important in quantum mechanics, where they form an intrinsic part of the formulation of the theory.

In mathematics, **spectral theory** is an inclusive term for theories extending the eigenvector and eigenvalue theory of a single square matrix to a much broader theory of the structure of operators in a variety of mathematical spaces. It is a result of studies of linear algebra and the solutions of systems of linear equations and their generalizations. The theory is connected to that of analytic functions because the spectral properties of an operator are related to analytic functions of the spectral parameter.

In physics, the **S-matrix** or **scattering matrix** relates the initial state and the final state of a physical system undergoing a scattering process. It is used in quantum mechanics, scattering theory and quantum field theory (QFT).

In quantum mechanics and computing, the **Bloch sphere** is a geometrical representation of the pure state space of a two-level quantum mechanical system (qubit), named after the physicist Felix Bloch.

In quantum mechanics, a **two-state system** is a quantum system that can exist in any quantum superposition of two independent quantum states. The Hilbert space describing such a system is two-dimensional. Therefore, a complete basis spanning the space will consist of two independent states. Any two-state system can also be seen as a qubit.

The **Ehrenfest theorem**, named after Paul Ehrenfest, an Austrian theoretical physicist at Leiden University, relates the time derivative of the expectation values of the position and momentum operators *x* and *p* to the expectation value of the force on a massive particle moving in a scalar potential ,

In mathematics, and in particular functional analysis, the **tensor product of Hilbert spaces** is a way to extend the tensor product construction so that the result of taking a tensor product of two Hilbert spaces is another Hilbert space. Roughly speaking, the tensor product is the metric space completion of the ordinary tensor product. This is an example of a topological tensor product. The tensor product allows Hilbert spaces to be collected into a symmetric monoidal category.

**Sinusoidal plane-wave solutions** are particular solutions to the electromagnetic wave equation.

**Photon polarization** is the quantum mechanical description of the classical polarized sinusoidal plane electromagnetic wave. An individual photon can be described as having right or left circular polarization, or a superposition of the two. Equivalently, a photon can be described as having horizontal or vertical linear polarization, or a superposition of the two.

The **theoretical and experimental justification for the Schrödinger equation** motivates the discovery of the Schrödinger equation, the equation that describes the dynamics of nonrelativistic particles. The motivation uses photons, which are relativistic particles with dynamics described by Maxwell's equations, as an analogue for all types of particles.

In quantum physics, a **quantum state** is a mathematical entity that provides a probability distribution for the outcomes of each possible measurement on a system. Knowledge of the quantum state together with the rules for the system's evolution in time exhausts all that can be predicted about the system's behavior. A mixture of quantum states is again a quantum state. Quantum states that cannot be written as a mixture of other states are called **pure quantum states**, while all other states are called **mixed quantum states**. A pure quantum state can be represented by a ray in a Hilbert space over the complex numbers, while mixed states are represented by density matrices, which are positive semidefinite operators that act on Hilbert spaces.

This is a glossary for the terminology often encountered in undergraduate quantum mechanics courses.

In pure and applied mathematics, quantum mechanics and computer graphics, a **tensor operator** generalizes the notion of operators which are scalars and vectors. A special class of these are **spherical tensor operators** which apply the notion of the spherical basis and spherical harmonics. The spherical basis closely relates to the description of angular momentum in quantum mechanics and spherical harmonic functions. The coordinate-free generalization of a tensor operator is known as a **representation operator**.

- Dirac, P. A. M. (1939). "A new notation for quantum mechanics".
*Mathematical Proceedings of the Cambridge Philosophical Society*.**35**(3): 416–418. Bibcode:1939PCPS...35..416D. doi:10.1017/S0305004100021162.. Also see his standard text,*The Principles of Quantum Mechanics*, IV edition, Clarendon Press (1958), ISBN 978-0198520115 - Grassmann, H. (1862).
*Extension Theory*. History of Mathematics Sources. 2000 translation by Lloyd C. Kannenberg. American Mathematical Society, London Mathematical Society. - Cajori, Florian (1929).
*A History Of Mathematical Notations Volume II*. Open Court Publishing. p. 134. ISBN 978-0-486-67766-8. - Shankar, R. (1994).
*Principles of Quantum Mechanics*(2nd ed.). ISBN 0-306-44790-8. - Feynman, Richard P.; Leighton, Robert B.; Sands, Matthew (1965).
*The Feynman Lectures on Physics*.**III**. Reading, MA: Addison-Wesley. ISBN 0-201-02118-8.

- Richard Fitzpatrick, "Quantum Mechanics: A graduate level course", The University of Texas at Austin. Includes:
- 1. Ket space
- 2. Bra space
- 3. Operators
- 4. The outer product
- 5. Eigenvalues and eigenvectors

- Robert Littlejohn, Lecture notes on "The Mathematical Formalism of Quantum mechanics", including bra-ket notation. University of California, Berkeley.
- Gieres, F. (2000). "Mathematical surprises and Dirac's formalism in quantum mechanics".
*Rep. Prog. Phys*.**63**(12): 1893–1931. arXiv: quant-ph/9907069 . Bibcode:2000RPPh...63.1893G. doi:10.1088/0034-4885/63/12/201. S2CID 10854218.

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