ERC starting grant – QD-CQED A quantum dot in a cavity: A solid state platform for quantum operations

The QD-CQED project aims at implementing elementary quantum operations using semiconductor quantum dots inserted in optical microcavities. photon or entangled photon pairs will be developed and used to demonstrate quantum teleportation and entanglement swapping. With an additional carrier inside the quantum dot, our objective is also to demonstrate spin-photon entanglement and head toward the remote entanglement of two spins. (2011-2016)

A new ultrabright source of entangled photon pairs.

Nature_lett 

 

 

Ultrabright source of entangled photon pairs

Adrien Dousse, Jan Suffczyński, Alexios Beveratos, Olivier Krebs, Aristide Lemaître, Isabelle Sagnes, Jacqueline Bloch, Paul Voisin & Pascale Senellart
Nature 466, 217–220 doi:10.1038/nature09148

 

At the very heart of applications such as quantum cryptography, computation and teleportation lies a fascinating phenomenon known as “entanglement”. Two photons are entangled if the properties of one depend on those of the other, whatever the distance separating them. A new source of entangled photons twenty times brighter than all existing systems has been developed by a team from the Laboratoire de Photonique et de Nano-structures (LPN) of CNRS. This novel device is capable of considerably boosting the rate of quantum communications and constitutes a key component in future quantum logic processes. These results are published in the journal Nature on the 8 July 2010.

Take a photon in Paris and another in Tokyo: if they are “entangled”, they are interdependent and measuring the properties of one makes it possible to know the properties of the other instantly, whatever the distance separating them. This mysterious property, known as “entanglement”, has far reaching application potential in information fields such as quantum cryptography, quantum computation and quantum teleportation. Normally, researchers use sources of entangled photon pairs that are easy to put in place (a laser transforming a photon into two photons of different color) but with very low brightness: less than one pulse out of 100 actually contains a pair of entangled photons, which considerably restricts the rate of any quantum communication. In addition, the size of such sources means they cannot be easily integrated into microsystems.

 

A team from the Laboratoire de Photonique et de Nano-structures (LPN) of CNRS has developed a light source of entangled photons twenty times brighter than all existing systems. The researchers have invented a novel “photonic molecule” system in which a semiconductor quantum dot(1) emits a pair of entangled photons per excitation pulse. This photonic molecule constitutes a trap for each of the photons of the pair and allows them to be collected efficiently. This new source operates at a rate of one pair of photons collected every 8 pulses (compared to less than one pair every 100 pulses so far). In the long run, the researchers should be able to reach a rate close to one pair of photons per pulse. This device could make it possible to manufacture electroluminescent diodes of entangled photon pairs, with rates close to one gigahertz (in other words around on billion hertz). Moreover, the LPN scientists have also shown that the use of this “photonic molecule” concept allows the quality of the entanglement of the emitted photon pairs to be improved.

Entangled_cartoon

© Jean-Louis Le Hir

This image represents, in the top right hand corner, the new component produced in this experiment: two pillars of micrometric size are coupled to form the “photonic molecule”.
The semiconductor quantum dot (of nanometric size) is inserted into one of the pillars (visible as the bright spot in the right hand pillar). The lower part of the image shows the radiation pattern of the entangled photons emitted by the component.

 

A deterministic Technique to Insert a Single Quantum Dot in a Cavity

To fabricate efficient devices, we need to make sure that a quantum dot is coupled to a single mode of the electromagnetic field.
We can approach such ideal situation by controlling the quantum dot spontaneous emission, through cavity quantum electrodynamics.
To do so, the quantum dot must be in both spectral and spatial resonance with the cavity mode. Yet, quantum dots usually grow with random spatial positions and a wide distribution of their spectral properties. As a result, usual nanofabrication techniques present fabrication yields in the low 10-4.

We have invented a technique which enables to fabricate as many as desired ideally coupled quantum dot-cavity devices, with a fabrication yield close to unity.
Our technique relies on a low temperature photolithography, with an in situ monitoring of the quantum dot emission.
The emission monitoring makes it possible to select the quantum dot with desired optical properties, to measure the quantum dot spatial location with 50 nm accuracy and to expose the photoresist to define a disk centered on the QD. The hole in the resist will later be used as a mask for the micropillar etching, ensuring that the quantum dot will be located at the maximum of the fundamental optical mode.

post_insitu

Dozens of micropillar microcavities with diameters ranging from 1 to 2.3 µm are fabricated. Each of them embeds a spectrally resonant quantum dot in its center. Using this technique, we have demonstrated on demand control the spontaneous emission for one or two QDs coupled to a cavity mode, with an acceleration of spontaneous emission close to 10. Increasing the quality factor of the cavity mode, we have recently demonstrated scalable implementation of strongly coupled QD cavity devices.

 

Further reading

 

“Controlled Light-Matter Coupling for a Single Quantum Dot Embedded in a Pillar Microcavity Using Far-Field Optical Lithography”, A. Dousse, L. Lanco, J. Suffczynski, E. Semenova, A. Miard, A. Lemaître, I. Sagnes, C. Roblin, J. Bloch, P. Senellart, Phys. Rev. Lett. 101, 267404 (2008)

 

“Scalable implementation of strongly coupled cavity-quantum dot devices” , A. Dousse, J. Suffczynski, R. Braive, A. Miard, A. Lemaître, I. Sagnes, L. Lanco, J. Bloch, P. Voisin, P. Senellart, Appl. Phys. Lett. 94, 121102 (2009)