Translation operators are closely related to the momentum operator; for example, a translation operator that moves by an infinitesimal amount in the direction has a simple relationship to the -component of the momentum operator. Because of this relationship, conservation of momentum holds when the translation operators commute with the Hamiltonian, i.e. when laws of physics are translation-invariant. This is an example of Noether's theorem.
Action on position eigenkets and wavefunctionsEdit
The translation operator moves particles and fields by the amount . Therefore, if a particle is in an eigenstate of the position operator (i.e., precisely located at the position ), then after acts on it, the particle is at the position :
An alternative (and equivalent) way to describe what the translation operator determines is based on position-space wavefunctions. If a particle has a position-space wavefunction , and acts on the particle, the new position-space wavefunction is defined by
This relation is easier to remember as which can be read as: "The value of the new wavefunction at the new point equals the value of the old wavefunction at the old point".
Here is an example showing that these two descriptions are equivalent. The state corresponds to the wavefunction (where is the Dirac delta function), while the state corresponds to the wavefunction These indeed satisfy
In introductory physics, momentum is usually defined as mass times velocity. However, there is a more fundamental way to define momentum, in terms of translation operators. This is more specifically called canonical momentum, and it is usually but not always equal to mass times velocity; one counterexample is a charged particle in a magnetic field. This definition of momentum is especially important because the law of conservation of momentum applies only to canonical momentum, and is not universally valid if momentum is defined instead as mass times velocity (the so-called "kinetic momentum"), for reasons explained below.
The (canonical) momentum operator is defined as the gradient of the translation operators near the origin:
where is the reduced Planck's constant. For example, what is the result when the operator acts on a quantum state? To find the answer, translate the state by an infinitesimal amount in the -direction, and calculate the rate that the state is changing, and multiply it by . For example, if a state does not change at all when it is translated in the -direction, then its -component of momentum is 0.
More explicitly, is a vector operator (i.e. a vector consisting of three operators ), defined by:
where is the identity operator and is the unit vector in the -direction. ( are defined analogously.)
The equation above is the most general definition of . In the special case of a single particle with wavefunction , can be written in a more specific and useful form. In one dimension:
or in three dimensions,
as an operator acting on position-space wavefunctions. This is the familiar quantum-mechanical expression for , but we have derived it here from a more basic starting point.
We have now defined in terms of translation operators. It is also possible to write a translation operator as a function of . The method consists in expressing a given translation as a huge number of consecutive tiny translations, and then use the fact that infinitesimal translations can be written in terms of :
Hence, the momentum operator is referred to as the generator of translation.
A nice way to double-check that these relations are correct is to do a Taylor expansion of the translation operator acting on a position-space wavefunction. Expanding the exponential to all orders, the translation operator generates exactly the full Taylor expansion of a test function:
So every translation operator generates exactly the expected translation on a test function if the function is analytic in some domain of the complex plane.
In other words, if particles and fields are moved by the amount and then by the amount , overall they have been moved by the amount . For a mathematical proof, one can look at what these operators do to a particle in a position eigenstate:
Since the operators and have the same effect on every state in an eigenbasis, it follows that the operators are equal.
Since translation operators all commute with each other (see above), and since each component of the momentum operator is a sum of two scaled translation operators (e.g. ), it follows that translation operators all commute with the momentum operator, i.e.
The commutation with momentum operator holds true generally even if the system is not isolated where energy or momentum may not conserve.
The set of translation operators for all , with the operation of multiplication defined as the result of successive translations (i.e. function composition), satisfies all the axioms of a group:
Closure: When you do two translations consecutively, the result is a single different translation. (See "successive translations" property above.)
Existence of identity: A translation by the vector is the identity operator, i.e. the operator that has no effect on anything. It functions as the identity element of the group.
Every element has an inverse: As proven above, any translation operator is the inverse of the reverse translation .
Associativity: This is the claim that . It is true by definition, as is the case for any group based on function composition.
Therefore, the set of translation operators for all forms a group. Since there are continuously infinite number of elements, the translation group is a continuous group. Moreover, the translation operators commute among themselves, i.e. the product of two translation (a translation followed by another) does not depend on their order. Therefore, the translation group is an abelian group.
Expectation values of position and momentum in the translated stateEdit
Consider a single particle in one dimension. Unlike classical mechanics, in quantum mechanics a particle neither has a well defined position nor a well defined momentum. In the quantum formulation, the expectation values play the role of the classical variables. For example, if a particle is in a state , then the expectation value of the position is , where is the position operator.
If a translation operator acts on the state , creating a new state then the expectation value of position for is equal to the expectation value of position for plus the vector . This result is consistent with what you would expect from an operation that shifts the particle by that amount.
Proof that a translation operator changes the expectation value of position in the way you would expect:
Assume as stated above.
using the normalization condition , and the commutator result proven in a previous section.
On the other hand, when the translation operator acts on a state, the expectation value of the momentum is not changed. This can be proven in a similar way as the above, but using the fact that translation operators commute with the momentum operator. This result is again consistent with expectations: translating a particle does not change its velocity or mass, so its momentum should not change.
In quantum mechanics, the Hamiltonian represents the energy and dynamics of a system. Let be a newly translated state (the argument of is irrelevant here and is temporarily dropped for brevity). A Hamiltonian is said to be invariant if
This implies that
Thus, if the Hamiltonian is invariant under translation, the Hamiltonian commutes with the translation operator (loosely speaking, if we translate the system, then measure its energy, then translate it back, it amounts to the same thing as just measuring its energy directly).
First we consider the case where all the translation operators are symmetries of the system. As we will see, in this case conservation of momentum occurs.
For example, if is the Hamiltonian describing all particles and fields in the universe, and is the translation operator that shifts all particles and fields in the universe simultaneously by the same amount, then this is always a symmetry: describes the complete laws of physics in our universe, which are independent of location. As a consequence, conservation of momentum is universally valid.
On the other hand, perhaps and refer to just one particle. Then the translation operators are exact symmetries only if the particle is alone in a vacuum. Correspondingly, the momentum of a single particle is not usually conserved (it changes when the particle bumps into other objects), but it is conserved if the particle is alone in a vacuum.
Since the Hamiltonian commutes with the translation operator when the translation is invariant
it also commutes with the infinitesimal translation operator
But, whenever coincides with the period of the potential ,
Since the kinetic energy part of the Hamiltonian is already invariant under any arbitrary translation, being a function of , the entire Hamiltonian satisfies,
Now, the Hamiltonian commutes with translation operator, i.e. they can be simultaneously diagonalised. Therefore, the Hamiltonian is invariant under such translation (which no longer remains continuous). The translation becomes discrete with the period of the potential.
Discrete translation in periodic potential: Bloch's theoremEdit
The ions in a perfect crystal are arranged in a regular periodic array. So we are led to the problem of an electron in a potential with the periodicity of the underlying Bravais lattice
for all Bravais lattice vectors
However, perfect periodicity is an idealisation. Real solids are never absolutely pure, and in the neighbourhood of the impurity atoms the solid is not the same as elsewhere in the crystal. Moreover, the ions are not in fact stationary, but continually undergo thermal vibrations about their equilibrium positions. These destroy the perfect translational symmetry of a crystal. To deal with this type of problems the main problem is artificially divided in two parts: (a) the ideal fictitious perfect crystal, in which the potential is genuinely periodic, and (b) the effects on the properties of a hypothetical perfect crystal of all deviations from perfect periodicity, treated as small perturbations.
Although, the problem of electrons in a solid is in principle a many-electron problem, in independent electron approximation each electron is subjected to the one-electron Schrödinger equation with a periodic potential and is known as Bloch electron (in contrast to free particles, to which Bloch electrons reduce when the periodic potential is identically zero.)
For each Bravais lattice vector we define a translation operator which, when operating on any function shifts the argument by :
Since all translations form an Abelian group, the result of applying two successive translations does not depend on the order in which they are applied, i.e.
In addition, as the Hamiltonian is periodic, we have,
Hence, the for all Bravais lattice vectors and the Hamiltonian form a set of commutating operators. Therefore, the eigenstates of can be chosen to be simultaneous eigenstates of all the :
The eigenvalues of the translation operators are related because of the condition:
Therefore, it follows that,
Now let the 's be the three primitive vector for the Bravais lattice. By a suitable choice of , we can always write in the form
Suppose at two observers A and B prepare identical systems at and (fig. 1), respectively.If be the state vector of the system prepared by A, then the state vector of the system prepared by B will be given by
Both the systems look identical to the observers who prepared them. After time , the state vectors evolve into and respectively.
Using the above-mentioned commutation relation, the later may be written as,
which is just the translated version of the system prepared by A at time . Therefore, the two systems, which differed only by a translation at , differ only by the same translation at any instant of time. The time evolution of both the systems appear the same to the observers who prepared them. It can be concluded that the translational invariance of Hamiltonian implies that the same experiment repeated at two different places will give the same result (as seen by the local observers).