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Rabi flopping : ウィキペディア英語版
Rabi cycle

In physics, the Rabi cycle (or Rabi flop) is the cyclic behaviour of a two-state quantum system in the presence of an oscillatory driving field. A great variety of physical processes belonging to the areas of quantum computing, condensed matter, atomic and molecular physics, and nuclear and particle physics can be conveniently studied in terms of two-level quantum mechanical systems, and exhibit Rabi flopping when coupled to an oscillatory driving field. The effect is important in quantum optics, magnetic resonance and quantum computing, and is named after Isidor Isaac Rabi.
A two-state system has two possible states, and if they are not degenerate (i.e. equal energy), the system can become "excited" when it absorbs a quantum of energy. When an atom (or some other two-level system) is illuminated by a coherent beam of photons, it will cyclically absorb photons and re-emit them by stimulated emission. One such cycle is called a Rabi cycle and the inverse of its duration the Rabi frequency of the photon beam. The effect can be modeled using the Jaynes-Cummings model and the Bloch vector formalism.
== Mathematical treatment==
A detailed mathematical description of the effect can be found on the page for the Rabi problem. For example, for a two-state atom (an atom in which an electron can either be in the excited or ground state) in an electromagnetic field with frequency tuned to the excitation energy, the probability of finding the atom in the excited state is found from the Bloch equations to be:
: |c_b(t)|^2 \propto \sin^2 (\omega t/2) ,
where \omega is the Rabi frequency.
More generally, one can consider a system where the two levels under consideration are not energy eigenstates. Therefore, if the system is initialized in one of these levels, time evolution will make the population of each of the levels oscillate with some characteristic frequency, whose angular frequency〔(Encyclopedia of Laser Physics and Technology - Rabi oscillations, Rabi frequency, stimulated emission )〕 is also known as the Rabi frequency. The state of a two-state quantum system can be represented as vectors of a two-dimensional complex Hilbert space, which means every state vector \vert\psi\rangle is represented by two complex coordinates.
: |\psi\rangle = \begin c_1 \\ c_2\end = c_1\begin 1 \\ 0\end + c_2\begin 0 \\ 1\end ; where c_1 and c_2 are the coordinates.
If the vectors are normalized, c_1 and c_2 are related by ^2+^2 = 1. The basis vectors will be represented as |1\rangle = \begin 1 \\ 0\end and |2\rangle = \begin 0 \\ 1\end
All observable physical quantities associated with this systems are 2 \times 2 Hermitian matrices, which means the Hamiltonian of the system is also a similar matrix.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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