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Abstract

In this chapter, we briefly review quantum optics. We first show quantized electromagnetic fields. The electric and magnetic field operators are represented by the photon annihilation and creation operators. We then show three characteristic single-mode quantum states: the coherent state, vacuum state and squeezed vacuum state. The squeezed state is the essential resource for one-way quantum computation. It can be experimentally generated by using optical parametric oscillators (OPOs). The quantum formalism of an OPO is provided via the quantum Langevin equation. As the last issue, we refer to homodyne measurement, which is the essential measurement technique in quantum optics.

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Notes

  1. 1.

    To be precise, a mode is defined by integrating wave vectors with a mode function which has distinctive nonzero values around a specific wave vector. Therefore, the commutation relations (Eqs. (2.22) and (2.23)) do not become delta functions.

  2. 2.

    \(\hbar \) is abbreviated to \(\hbar = \frac{1}{2},1\) and \(2\) depending on papers, which sometimes leads to confusion.

  3. 3.

    When \(r>0\), it becomes an \(x\)-squeezed state. When \(r=0\), it is the vacuum state. When \(r<0\), it becomes a \(p\)-squeezed state.

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Correspondence to Ryuji Ukai .

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Ukai, R. (2015). Quantum Optics. In: Multi-Step Multi-Input One-Way Quantum Information Processing with Spatial and Temporal Modes of Light. Springer Theses. Springer, Tokyo. https://doi.org/10.1007/978-4-431-55019-8_2

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