Abstract
In quantum theory, all physical fields are described on a fundamental level by the principle of quantum theory. In the Heisenberg picture, the quantum states of systems are represented by vector in a Hilbert space. A convenient basis in this space is the Fock representation. The normalized basis ket vector |>, can be constructed from the vector |0>, called vacuum. Observable will not always have a definite value and one, in general, can only predict probabilities for the outcome of measurements.
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