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.
- 2.
\(\hbar \) is abbreviated to \(\hbar = \frac{1}{2},1\) and \(2\) depending on papers, which sometimes leads to confusion.
- 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.
References
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Collett, M.J., Gardiner, C.W.: Squeezing of intracavity and traveling-wave light fields produced in parametric amplification. Phys. Rev. A 30, 1386 (1984)
Gardiner, C.W., Collett, M.J.: Input and output in damped quantum systems: Quantum stochastic differential equations and the master equation. Phys. Rev. A 31, 3761 (1985)
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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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DOI: https://doi.org/10.1007/978-4-431-55019-8_2
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