Rotating wave approximation
Encyclopedia
The rotating wave approximation is an approximation used in atom optics
and magnetic resonance
. In this approximation, terms in a Hamiltonian
which oscillate rapidly are neglected. This is a valid approximation when the applied electromagnetic radiation is near resonance with an atomic resonance, and the intensity is low. Explicitly, terms in the Hamiltonians which oscillate with frequencies are neglected, while terms which oscillate with frequencies are kept, where is the light frequency and is a transition frequency.
The name of the approximation stems from the form of the Hamiltonian in the interaction picture
, as shown below. By switching to this picture the evolution of an atom due to the corresponding atomic Hamiltonian is absorbed into the system ket
, leaving only the evolution due to the interaction of the atom with the light field to consider. It is in this picture that the rapidly-oscillating terms mentioned previously can be neglected. Since in some sense the interaction picture can be thought of as rotating with the system ket only that part of the electromagnetic wave that approximately co-rotates is kept; the counter-rotating component is discarded.
and ground states and respectively (using the Dirac bracket notation
). Let the energy difference between the states be so that is the transition frequency of the system. Then the unperturbed Hamiltonian
of the atom can be written as
Suppose the atom is placed at in an external (classical) electric field
of frequency , given by (so that the field contains both positive- and negative-frequency modes in general). Then under the dipole approximation the interaction Hamiltonian can be expressed as
where is the dipole moment operator of the atom. The total Hamiltonian for the atom-light system is therefore The atom does not have a dipole moment when it is in an energy eigenstate, so This means that defining allows the dipole operator to be written as
(with `' denoting the Hermitian conjugate). The interaction Hamiltonian can then be shown to be (see the Derivations section below)
Atom optics
Atom optics is the area of physics which deals with beams of cold, slowly moving neutral atoms, as a special case of a particle beam....
and magnetic resonance
Magnetic resonance
Magnetic resonance can mean:*Nuclear magnetic resonance*Electron spin resonance*Magnetic resonance imaging *Functional magnetic resonance imaging *Muon spin spectroscopy...
. In this approximation, terms in a Hamiltonian
Hamiltonian (quantum mechanics)
In quantum mechanics, the Hamiltonian H, also Ȟ or Ĥ, is the operator corresponding to the total energy of the system. Its spectrum is the set of possible outcomes when one measures the total energy of a system...
which oscillate rapidly are neglected. This is a valid approximation when the applied electromagnetic radiation is near resonance with an atomic resonance, and the intensity is low. Explicitly, terms in the Hamiltonians which oscillate with frequencies are neglected, while terms which oscillate with frequencies are kept, where is the light frequency and is a transition frequency.
The name of the approximation stems from the form of the Hamiltonian in the interaction picture
Interaction picture
In quantum mechanics, the Interaction picture is an intermediate between the Schrödinger picture and the Heisenberg picture. Whereas in the other two pictures either the state vector or the operators carry time dependence, in the interaction picture both carry part of the time dependence of...
, as shown below. By switching to this picture the evolution of an atom due to the corresponding atomic Hamiltonian is absorbed into the system ket
Bra-ket notation
Bra-ket notation is a standard notation for describing quantum states in the theory of quantum mechanics composed of angle brackets and vertical bars. It can also be used to denote abstract vectors and linear functionals in mathematics...
, leaving only the evolution due to the interaction of the atom with the light field to consider. It is in this picture that the rapidly-oscillating terms mentioned previously can be neglected. Since in some sense the interaction picture can be thought of as rotating with the system ket only that part of the electromagnetic wave that approximately co-rotates is kept; the counter-rotating component is discarded.
Mathematical formulation
For simplicity consider a two-level atomic system with excitedExcited state
Excitation is an elevation in energy level above an arbitrary baseline energy state. In physics there is a specific technical definition for energy level which is often associated with an atom being excited to an excited state....
and ground states and respectively (using the Dirac bracket notation
Bra-ket notation
Bra-ket notation is a standard notation for describing quantum states in the theory of quantum mechanics composed of angle brackets and vertical bars. It can also be used to denote abstract vectors and linear functionals in mathematics...
). Let the energy difference between the states be so that is the transition frequency of the system. Then the unperturbed Hamiltonian
Hamiltonian (quantum mechanics)
In quantum mechanics, the Hamiltonian H, also Ȟ or Ĥ, is the operator corresponding to the total energy of the system. Its spectrum is the set of possible outcomes when one measures the total energy of a system...
of the atom can be written as
Suppose the atom is placed at in an external (classical) electric field
Electric field
In physics, an electric field surrounds electrically charged particles and time-varying magnetic fields. The electric field depicts the force exerted on other electrically charged objects by the electrically charged particle the field is surrounding...
of frequency , given by (so that the field contains both positive- and negative-frequency modes in general). Then under the dipole approximation the interaction Hamiltonian can be expressed as
where is the dipole moment operator of the atom. The total Hamiltonian for the atom-light system is therefore The atom does not have a dipole moment when it is in an energy eigenstate, so This means that defining allows the dipole operator to be written as
(with `' denoting the Hermitian conjugate). The interaction Hamiltonian can then be shown to be (see the Derivations section below)
-
where is the Rabi frequencyRabi frequencyThe Rabi frequency is the frequency of population oscillation for a given atomic transition in a given light field. It is associated with the strength of the coupling between the light and the transition. Rabi flopping between the levels of a 2-level system illuminated with resonant light, will...
and is the counter-rotating frequency. To see why the terms are called `counter-rotating' consider a unitary transformationUnitary transformationIn mathematics, a unitary transformation may be informally defined as a transformation that respects the inner product: the inner product of two vectors before the transformation is equal to their inner product after the transformation....
to the interaction or Dirac pictureInteraction pictureIn quantum mechanics, the Interaction picture is an intermediate between the Schrödinger picture and the Heisenberg picture. Whereas in the other two pictures either the state vector or the operators carry time dependence, in the interaction picture both carry part of the time dependence of...
where the transformed Hamiltonian is given by
-
where is the detuning of the light field.
Making the approximation
This is the point at which the rotating wave approximation is made. The dipole approximation has been assumed, and for this to remain valid the electric field must be near resonanceResonanceIn physics, resonance is the tendency of a system to oscillate at a greater amplitude at some frequencies than at others. These are known as the system's resonant frequencies...
with the atomic transition. This means that and the complex exponentials multiplying and can be considered to be rapidly oscillating. Hence on any appreciable time scale the oscillations will quickly average to 0. The rotating wave approximation is thus the claim that these terms are negligible and the Hamiltonian can be written in the interaction picture as
-
Finally, in the Schrödinger pictureSchrödinger pictureIn physics, the Schrödinger picture is a formulation of quantum mechanics in which the state vectors evolve in time, but the operators are constant. This differs from the Heisenberg picture which keeps the states constant while the observables evolve in time...
the Hamiltonian is given by
-
At this point the rotating wave approximation is complete. A common first step beyond this is to remove the remaining time dependence in the Hamiltonian via another unitary transformation.
Derivations
Given the above definitions the interaction Hamiltonian is
-
as stated. The next stage is to find the Hamiltonian in the interaction picture, The unitary operator required for the transformation is
and an arbitrary state transforms to The Schrödinger equationSchrödinger equationThe Schrödinger equation was formulated in 1926 by Austrian physicist Erwin Schrödinger. Used in physics , it is an equation that describes how the quantum state of a physical system changes in time....
must still hold in this new picture, so
-
where a dot denotes the time derivativeTime derivativeA time derivative is a derivative of a function with respect to time, usually interpreted as the rate of change of the value of the function. The variable denoting time is usually written as t\,.-Notation:...
. This shows that the new Hamiltonian is given by
-
Using a Taylor series expansion of the exponential,
-
and operating on
-
Operating from the left on the second term of above yields zero by orthogonality of and , and the same results apply to the operation of the second exponential from the right. Thus, the new Hamiltonian becomes
-
The penultimate equality can be easily seen from the series expansionSeries expansionIn mathematics, a series expansion is a method for calculating a function that cannot be expressed by just elementary operators . The resulting so-called series often can be limited to a finite number of terms, thus yielding an approximation of the function...
of the exponential map and the fact that
for i and j each equal to e or g (and the Kronecker delta).
The final step is to transform the approximate Hamiltonian back to the Schrödinger picture. The first line of the previous calculation shows that
, so in the same manner as the last calculation,
-
The atomic Hamiltonian was unaffected by the approximation, so the total Hamiltonian in the Schrödinger picture under the rotating wave approximation is
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