# Creation and annihilation operators

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**Creation and annihilation operators** are mathematical operators that have widespread applications in quantum mechanics, notably in the study of quantum harmonic oscillators and many-particle systems.^{[1]} An annihilation operator lowers the number of particles in a given state by one. A creation operator increases the number of particles in a given state by one, and it is the adjoint of the annihilation operator. In many subfields of physics and chemistry, the use of these operators instead of wavefunctions is known as second quantization.

Creation and annihilation operators can act on states of various types of particles. For example, in quantum chemistry and many-body theory the creation and annihilation operators often act on electron states. They can also refer specifically to the ladder operators for the quantum harmonic oscillator. In the latter case, the raising operator is interpreted as a creation operator, adding a quantum of energy to the oscillator system (similarly for the lowering operator). They can be used to represent phonons.

The mathematics for the creation and annihilation operators for bosons is the same as for the ladder operators of the quantum harmonic oscillator.^{[2]} For example, the commutator of the creation and annihilation operators that are associated with the same boson state equals one, while all other commutators vanish. However, for fermions the mathematics is different, involving anticommutators instead of commutators.^{[3]}

## Contents

## Ladder operators for quantum harmonic oscillator

In the context of the quantum harmonic oscillator, we reinterpret the ladder operators as creation and annihilation operators, adding or subtracting fixed quanta of energy to the oscillator system. Creation/annihilation operators are different for bosons (integer spin) and fermions (half-integer spin). This is because their wavefunctions have different symmetry properties.

First consider the simpler bosonic case of the phonons of the quantum harmonic oscillator.

Start with the Schrödinger equation for the one-dimensional time independent quantum harmonic oscillator

Make a coordinate substitution to nondimensionalize the differential equation

and the Schrödinger equation for the oscillator becomes

Note that the quantity is the same energy as that found for light quanta and that the parenthesis in the Hamiltonian can be written as

The last two terms can be simplified by considering their effect on an arbitrary differentiable function f(q),

which implies,

Therefore

and the Schrödinger equation for the oscillator becomes, with substitution of the above and rearrangement of the factor of 1/2,

If we define

- as the "creation operator" or the "raising operator" and
- as the "annihilation operator" or the "lowering operator"

then the Schrödinger equation for the oscillator becomes

This is *significantly* simpler than the original form. Further simplifications of this equation enables one to derive all the properties listed above thus far.

Letting , where "p" is the nondimensionalized momentum operator then we have

and

Note that these imply that

The operators and may be contrasted with normal operators. A normal operator has a representation where are self-adjoint and commute, i.e. . By contrast, has the representation where are self-adjoint but . As a consequence, and have a common set of eigenfunctions (and are simultaneously diagonalizable), whereas p and q famously don't and aren't.

Thus, although in the present case one is dealing with non-normal operators, by the commutation relations given above, the Hamiltonian operator can be expressed as

And the and operators have the following commutation relations with the Hamiltonian^{[4]}

These relations can be used to find the energy eigenstates of the quantum harmonic oscillator. Assuming that is an eigenstate of the Hamiltonian . Using these commutation relations it can be shown that^{[4]}

This shows that and are also eigenstates of the Hamiltonian with eigenvalues and . This identifies the operators and as lowering and rising operators between the eigenstates. Energy difference between two eigenstates is .

The ground state can be found by assuming that the lowering operator possesses a nontrivial kernel, with . Using the formula above for the Hamiltonian, one obtains

so is an eigenfunction of the Hamiltonian. This gives the ground state energy . This allows to identify the energy eigenvalue of any eigenstate as^{[4]}

Furthermore it can be shown that the first-mentioned operator, the **number operator** plays a most-important role in applications, while the second one, can simply be replaced by So one simply gets

### Applications

The ground state of the quantum harmonic oscillator can be found by imposing the condition that

Written out as a differential equation, the wavefunction satisfies

which has the solution

The normalization constant *C* can be found to be from , using the Gaussian integral.

### Matrix representation

The matrix counterparts of the creation and annihilation operators obtained from the quantum harmonic oscillator model are

Substituting backwards, the laddering operators are recovered. They can be obtained via the relationships and . The wavefunctions are those of the quantum harmonic oscillator, and are sometimes called the "number basis".

### Generalized creation and annihilation operators

The operators derived above are actually a specific instance of a more generalized class of creation and annihilation operators. The more abstract form of the operators satisfy the properties below.

Let *H* be the one-particle Hilbert space. To get the bosonic CCR algebra, look at the algebra generated by *a*(*f*)Template:What for any *f* in *H*. The operatorTemplate:What *a*(*f*) is called an annihilation operator and the map *a*(.) is antilinear. Its adjoint is *a*^{†}(*f*) which is linear in *H*.

For a boson,

where we are using bra–ket notation.

For a fermion, the anticommutators are

A CAR algebra.

Physically speaking, *a*(*f*) removes (i.e. annihilates) a particle in the state | *f* whereas *a*^{†}(*f*) creates a particle in the state | *f* .

The free field vacuum state is the state with no particles. In other words,

where | 0 is the vacuum state.

If | *f* is normalized so that *f* | *f* = 1, then *a*^{†}(*f*) *a*(*f*) gives the number of particles in the state | *f* .

### Creation and annihilation operators for reaction-diffusion equations

The annihilation and creation operator description has also been useful to analyze classical reaction diffusion equations, such as the situation when a gas of molecules *A* diffuse and interact on contact, forming an inert product: *A* + *A* → ∅ . To see how this kind of reaction can be described by the annihilation and creation operator formalism, consider particles at a site on a 1-d lattice. Each particle moves to the right or left with a certain probability, and each pair of particles at the same site annihilates each other with a certain other probability.

The probability that one particle leaves the site during the short time period is proportional to , let us say a probability to hop left and to hop right. All particles will stay put with a probability . (Since is so short, the probability that two or more will leave during is very small and will be ignored.)

We can now describe the occupation of particles on the lattice as a `ket' of the form | *..., n _{-1}, n_{0}, n_{1}, ...* . It represents the juxtaposition (or conjunction, or tensor product) of the number states ..., |

*n*, |

_{-1}*n*, |

_{0}*n*, ... located at the individual sites of the lattice. A slight modificationTemplate:What of the annihilation and creation operators is needed so that

_{1}and

for all *n≥0*. This modification preserves the commutation relation

Now let *a _{i}=a π_{i}*, where

*π*selects the

_{i}*i*

^{th}component of ψ. That is,

*a*makes a copy of the state |

_{i}*n*in an abstract place and then applies

_{i}*a*to it. Then

*a*, where

_{i}^{†}=ι_{i}a^{†}*ι*inserts an abstract state at the

_{i}*i*

^{th}site. Thus, for example, the net effect of

*a*is to move an eigenstate from the

_{i-1}^{†}a_{i}*i*

^{th}to the (

*i-1*)

^{th}site while multiplying with the appropriate eigenvalue.

This allows us to write the pure diffusive behaviour of the particles as

where the sum is over *i*.

The reaction term can be deduced by noting that particles can interact in different ways, so that the probability that a pair annihilates is and the probability that no pair annihilates is leaving us with a term

yielding

Other kinds of interactions can be included in a similar manner.

This kind of notation allows the use of quantum field theoretic techniques to be used in the analysis of reaction diffusion systems.

## Creation and annihilation operators in quantum field theories

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In quantum field theories and many-body problems one works with creation and annihilation operators of quantum states, and . These operators change the eigenvalues of the number operator,

by one, in analogy to the harmonic oscillator. The indices (such as ) represent quantum numbers that label the single-particle states of the system; hence, they are not necessarily single numbers. For example, a tuple of quantum numbers is used to label states in the hydrogen atom.

The commutation relations of creation and annihilation operators in a multiple-boson system are,

where is the commutator and is the Kronecker delta.

For fermions, the commutator is replaced by the anticommutator ,

Therefore, exchanging disjoint (i.e. ) operators in a product of creation of annihilation operators will reverse the sign in fermion systems, but not in boson systems.

## See also

- Bogoliubov transformations - arises in the theory of quantum optics.
- Optical Phase Space
- Fock space
- Canonical commutation relations

## References

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## Footnotes

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