2004
DOI: 10.1017/cbo9780511616754
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Introduction to Quantum Optics

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Cited by 39 publications
(22 citation statements)
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“…Our implementation relies on a photonic walker implemented by an attenuated coherent laser pulse with its polarisation representing the internal (coin) degree of freedom. In this way, our system makes use of the equivalence of coherent light and a single quantum particle when propagating in a linear optical network [70]. Figure 3 shows the physical implementation of the quantum walk setup: Our time-multiplexing architecture relies on translating the external (position) degree of freedom of the walker into the time domain by splitting the pulses up spatially, routing them through fibres of different length and subsequently merging the two paths again.…”
Section: Experimental Implementation 31 Time-multiplexing Setupmentioning
confidence: 99%
“…Our implementation relies on a photonic walker implemented by an attenuated coherent laser pulse with its polarisation representing the internal (coin) degree of freedom. In this way, our system makes use of the equivalence of coherent light and a single quantum particle when propagating in a linear optical network [70]. Figure 3 shows the physical implementation of the quantum walk setup: Our time-multiplexing architecture relies on translating the external (position) degree of freedom of the walker into the time domain by splitting the pulses up spatially, routing them through fibres of different length and subsequently merging the two paths again.…”
Section: Experimental Implementation 31 Time-multiplexing Setupmentioning
confidence: 99%
“…The absolute phase constants are physical in the sense that physical situations exist where they can be determined. For example, when two independent weak quasimonochromatic laser beams (photon wave functions) are superposed [18], [19]. In the superpositions the absolute phases become relative phases and determine the positions of the interference fringes.…”
Section: The Absolute Phase Constantsmentioning
confidence: 99%
“…Note that for Lindblad-type master equations (28), the previous definition extends to the Lindblad operators L i ∈ B(H), see Eq. (29), which also commute with the unitary operator U . We stress that this is the case termed strong symmetry in the language of Refs.…”
Section: Symmetry and Degenerate Steady Statesmentioning
confidence: 99%