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Ty Volkoff, University of California, Berkeley

Two measures of macroscopicity for quantum superpositions in countably infinite dimensional Hilbert space will be introduced: one depending on the optimal distinguishability of the components of the superposition under measurements of subsets of particles and another based on the ratio of the quantum Fisher information of the superposition to that of its components.

Ben Baragiola, University of New Mexico

Traveling wave packets of light prepared with a definite number of photons, known as multimode Fock states, are well-suited for the role of "flying qubits" to relay information in a quantum computing device. In both the optical and microwave domain, propagating single-photon fields are routinely produced and manipulated, with ongoing progress toward higher photon numbers.

Monday, April 20, 2015 2:30 pm - 3:30 pm EDT (GMT -04:00)

Jerry Chow: Taking Superconducting Qubits to the Next Generation

Jerry Chow, IBM T.J. Watson Research Center, USA

Fault tolerant quantum computing is possible by employing quantum error correction techniques. In this talk I will describe an implementation of a true quantum code using 4 lithographically defined superconducting qubits in a square lattice capable of measuring both types of possible quantum errors occurring on a single qubit. The experiment requires highly coherent qubits, high quality quantum operations implementing the detecting circuit, and a high quality independent qubit measurement set-up.

Thursday, April 30, 2015 11:00 am - 12:00 pm EDT (GMT -04:00)

Matthieu Nannini: Nanolithography using Thermal Probe AFM: principle and applications

Matthieu Nannini, McGill University

While IBM Zurich's millipede project of data storage did not
have the success anticipated it would, a new technology for nano
lithography was born. Since 2009, IBM Zurich has been refining their

Thursday, April 30, 2015 4:00 pm - 5:00 pm EDT (GMT -04:00)

Quantum Frontiers Distinguished Lecture: Sajeev John

Sajeev John, University of Toronto

Photonic band gap materials: semiconductors of light

Join us for the next Quantum Frontiers Distinguished Lecture Series when Dr. Sajeev John will talk about light-trapping crystals.

Friday, May 1, 2015 12:00 pm - 1:00 pm EDT (GMT -04:00)

Tim J. Bartley: Mesoscopic quantum optics

Tim J. Bartley, National Institute of Standards and Technology, Boulder

Fundamental to quantum optics is the study of the distribution of photons in modes of an electromagnetic field. Until now, direct photon number measurements on nonclassical states occupying a single mode have been limited to the few-photon regime (typically no more than 5). I will present results from direct measurements of nonclassical states containing up to 50 (fifty) photons, at telecom wavelengths and with total raw efficiencies well above 60%.

Monday, May 4, 2015 2:30 pm - 3:30 pm EDT (GMT -04:00)

Daniel Terno: Wave, particles and quantum control

Daniel Terno, Macquarie University

The debate on wave vs particle nature of light goes back to the days of Huygens and Newton. When used to model properties of quantum system these concepts lose their objective meaning and simply become the two aspects of wave-particle duality. Duality played a central role in Bohr—Einstein debates and prompted Bohr to formulate the complementarity principle. Complementarity leaves open the possibility that by adapting to the specific experimental sit-up a quantum system always behaves definitely either as a particle or as a wave.

Michele Piscitelli, Royal Holloway University

The focus of this talk will be a general introduction to Nuclear Magnetic Resonance (NMR) detection schemes that are based on the use of Superconducting Quantum Interference Devices (SQUIDs) as highly sensitive magnetometers. I will begin by providing an overview of the relevant concepts and principles behind SQUID-detected NMR. In the main part of my talk I will be presenting our experimental results and achievements in the field of ultralow field SQUID NMR spectroscopy and Magnetic Resonance Imaging (MRI).