Special Physics Seminar
Cavity quantum electrodynamics with quantum transport
Mircea Trif
Institute for Interdisciplinary Information Sciences
Tsinghua University
The field of cavity quantum electrodynamics (cQED) with quantum conductors
has become an extremely active field of research. The milestone year was
2004, when superconducting qubits have been integrated within a microwave
cavity in order to reach, for the very first time in the condensed matter
context, the strong coupling regime between photons and matter. Since then,
many other systems have been successfully coupled to microwave cavities, such
as quantum wires, carbon nanotubes, quantum dots, etc. Such hybrid systems
offer platforms for new kinds of physics, as one can engineer and manipulate
the electromagnetic environment at will.
The versatility of the cQED method relies on the fact that it allows to 1)
monitor in a noninvasive fashion the electronic states in quantum conductors,
both in equilibrium and non-equilibrium situations, 2) to affect and manipulate
the electronic transport, 3) to establish long-range correlations between
remote quantum conductors and, finally, 4) it opens the pathway to create
non-classical states of light by means of electronic transport. In this talk,
I will discuss some of these aspects for various types of quantum conductors out
of equilibrium. I will focus on tunnel junctions, magnetic tunnel junctions,
quantum dots and Josephson junctions, respectively. I will show that one
can reveal properties that are invisible in electronic transport (via the
conductance), in particular in out-of-equilibrium situations pertaining to
a large voltage bias applied over the quantum conductor. For the case of
voltage biased Josephson junction, I will show that the emitted radiation
is non-classical in the sense that the photonic correlators violate some
Cauchy-Schwarz inequalities. I will confront the theory with some recent
experimental studies where such violations have been measured.
Tuesday, February 6th 2018, 11:00
Ernest Rutherford Physics Building, R.E. Bell Conference Room (room 103)
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