Research News

Thu, 03/09/2017 | Strong Coupling Cavity QED with Gate-Defined Double Quantum Dots Enabled by a High Impedance Resonator

The efficient transfer of energy across different quantum systems - an essential ingredient to quantum-information-processing protocols - requires that the coupling between these systems is stronger than the decay rate of either one. Here we report experiments in which we have reached this so-called strong-coupling regime in a hybrid system consisting of a gate-defined double quantum dot and a superconducting resonator. These results underline the potential of circuit-QED experiments with semiconductor nano-structures both for quantum information processing and for fundamental studies of light–matter interactions.

Tue, 11/29/2016 | Gamble for Science

On November 30, 2016 one of the largest quantum physics experiments will take place. The "BIG Bell Test" is a worldwide "citizen science" project, coordinated by the Institute of Photonic Sciences, which intends to carry out a set of simultaneous quantum physics experiments in eleven different labs around the world, including the Quantum Device Lab. To be successful at least 30'000 people are supposed to generate random sequences of "zeros" and "ones" by playing a video game. 

Fri, 06/03/2016 | Superconducting Switch for Fast On-Chip Routing of Quantum Microwave Fields

For a quantum computer, switching a signal carried by single microwave photons is desirable in scaling up superconducting circuitry. In this work, we design and build such a switch, integrate it on a chip with a single-photon source, and prove that it works with nonclassical microwave input. Our device offers negligible heating, relatively large bandwidth, low nonlinearity, and single-pole double-throw switching in mere nanoseconds. It is well suited for applications where signal routing must be controlled by real-time feedback, as in multiplexing qubit control and readout, or distributing entanglement in quantum networks.

Mon, 05/16/2016 | Measurement of a vacuum-induced geometric phase

Can you roll a basketball on the floor so that the ball comes back to the same position, but the orientation of its pattern has changed? Yes, you can, and after a few tries you will find out that the final orientation of the pattern is determined by the path traced by the ball on the floor. Quantum systems behave pretty much the same way: when subjected to a slowly varying external field, they acquire a phase that depends on the path they trace in their Hilbert space, that is, a geometric phase. In this work we have studied what happens when the external field is itself a quantum system, namely, a harmonic oscillator which can be populated with any number of photons. Instead of varying the state of the field, we prepare the field in a given state and slowly vary its coupling to the system. What we find is that a geometric phase is acquired even when the field is in the vacuum state, a result that has no semiclassical explanation but is correctly predicted by a full quantum theory. Our ability to control this phase opens new possibilities for the coherent manipulation of hybrid atom-cavity systems, with direct implications for quantum information processing. The results are published in Science Advances.

Wed, 12/16/2015 | Exploring Interacting Quantum Many-Body Systems by Experimentally Creating Continuous Matrix Product States in Superconducting Circuits

By employing a fully controlled cavity quantum electrodynamic system made of superconducting circuits, we experimentally create matrix product states, a class of states that has proven to be extremely powerful as a variational ansatz for numerical simulations. We create 1000 such quantum states and efficiently probe their correlation properties to determine an approximation to the ground state of a model describing a gas of interacting quantum particles. Having physical access to the simulated ground-state wave functions enables us to also probe higher-order correlation functions beyond measuring the ground-state energy. The experimental data are in good agreement with the exact solution over a wide range of interaction strengths of the model.