Two-level system
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In quantum mechanics, a two-level system is a system in which there are two physical states of different energy. That is, if we take the time-independent Hamiltonian to be [H], then we say that the two levels are [\psi_a] and [\psi_b] with corresponding energy eigenvalues [E_a] and [E_b], which may or may not be different. These states are always taken to be orthonormal, i.e. [\left\langle\psi_a|\psi_b\right\rangle=\delta_.] If the system is initialized in the state [\Psi(t=0)=c_a\left.|\psi_a\right\rangle+c_b\left.|\psi_b\right\rangle] then after evolving for some time [t] under the Hamiltonian [H], the state will be [\Psi(t) = c_a e^}\left|\psi_a\right\rangle+c_b e^}\left|\psi_b\right\rangle]
The set of all states in a two-level system is known as a Bloch sphere. Two-level systems are particularly important to the field of quantum computing as they can be used to implement qubits.
See also
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