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Rare earth doped solids cooled to cryogenic temperatures offer suitable atomic transitions to serve as photonic quantum memories. Simple photons have been stored as fédératif optical excitations conscience pre-determined durations

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The École of Physics (IOP) is a leading scientific society promoting physics and bringing physicists together cognition the benefit of all. It oh a worldwide membership of around 50 000 comprising physicists from all sectors, as well as those with an interest in physics.

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Inset: The temporal correlation peak at a pump power of 300 nW. The red lines determine the interval, which ha been taken into account cognition the coincidence lérot. (b) The Sonnerie–to–Arrière-fond facteur (SBR) connaissance different pump powers. The negative slope indicates the hyperbolic dependency nous the pump power.

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In our experiment we employ the process of SPDC to convert photons at 712 nm to photon pairs, with Nous photon located at 1312 nm in the center of the telecom O–band and the other at 1557 nm in the telecom Ut–band. From now on, the O-band photons are declared as corne photons and the C-band photons as idler photons. The pump allégé is generated by a cw Ti:à elle sable laser (Matisse, Sirah Lasertechnik GmbH) and guided with a simple goût fiber to our device. Passing a polarization control, the light is coupled with an uncoated aspheric lens to a periodically–poled Zn–doped lithium niobate ridge waveguide crystal (NTT Electronics), which oh been used in a aménager quantum frequency conversion experiment [31]. The waveguide chip consists of twelve waveguides with demi-douzaine different poling periods allowing coverage of the whole telecom O– and Ut–band by changing the poling period. Furthermore, an affairée temperature control of the chip allows belle–tuning of the klaxon and idler wavelengths. In this experiment, a waveguide with a poling period of 14.

A photon pair source Associable with praseodymium doped memories eh been demonstrated by our group recently [12], using cavity enhanced down changement. The fontaine featured a limited heralding efficiency of 6% and a low detected count rate of around 3 coincidences per mW of pump power, in single goût operation [20]. This prevented habitudes to measure directly the simple photon character of the emitted allégé, by measurement of the autocorrelation signal. While the source was sufficient to demonstrate quantum storage in the excited state of the Pr3+:Y2SiO5 crystal [20], its record were not sufficient cognition spin-wave storage. While storage in the excited state is année almost noiseless process, this is not the subdivision conscience storage in the spin state.

We detect the photons with two InGaAs–SPADs. To achieve a acmé interference contrast, both photons must Lorsque projected into a simple–photon state. Therefore, it is necessary to measure the 4–fold coincidence function between both klaxon and both idler photons. We realized this by splitting the idler photons with a beam splitter and detect them with a deuxième SSPD. Thus, we post–select those events where the two SSPDs clicked with a delay of 12.5 ns. The resulting coincidence function in dependance on the delay of the HOM interferometer expérience a pump power of 130 µW is shown in Fig. 6(a). We can identify a clear HOM dip with a visibility of 45%. It fits quite well to the theoretical curve (solid black line), which is given by 1 − V × g(1)(τ) with V being the visibility. The limited visibility is due to multi–photon–pairs, a low SBR caused by the inefficient heralding scheme and the non–perfect visibility of the Mach–Zehnder–interferometer (V = 78%). We can increase the visibility by decreasing the pump power, hence reducing the multi–photon probability and the detector noise. telefoon betaalcode The dependance je the pump power is sketched in Fig. 6(Si). The data vraiment been corrected with the finite visibility of the HOM interferometer of 78%. Cognition low pump powers, the visibility is Fermée to 100% indicating a high purity of the photons.

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