In this work we study a family of bosonic lattice models that combine an on-site repulsion term with a nearest-neighbor pairing term, $sum_{< i,j>} a^dagger_i a^dagger_j + mathrm{H.c.}$Like the original Bose-Hubbard model, the nearest-neighbor term is responsible for the mobility of bosons and it competes with the local interaction, inducing two-mode squeezing. However, unlike a trivial hopping, the counter-rotating terms form pairing cannot be studied with a simple mean-field theory and does not present a quantum phase transition in phase space. Instead, we show that there is a cross-over from a pure insulator to long-range correlations that start up as soon as the two-mode squeezing is switched on. We also show how this model can be naturally implemented using coupled microwave resonators and superconducting qubits.
Coupled superconducting transmission line resonators have applications in
quantum information processing and fundamental quantum mechanics. A particular
example is the realization offast beam splitters, which however is hampered by
two-mode squeezer terms. Here, we experimentally study superconducting
microstrip resonators which are coupled over one third of their length. By
varying the position of this coupling region we can tune the strength of the
two-mode squeezer coupling from 2.4% to 12.9% of the resonance frequency of
5.44GHz. Nevertheless, the beam splitter coupling rate for maximally suppressed
two-mode squeezing is 810MHz, enabling the construction of a fast and pure beam
splitter.
Based on a circuit QED qubit-cavity array a source of two-mode entangled
microwave radiation is designed. Our scheme is rooted in the combination of
external driving, collective phenomenaand dissipation. On top of that the
reflexion symmetry is broken via external driving permitting the appearance of
chiral emission. Our findings go beyond the applications and are relevant for
fundamental physics, since we show how to implement quantum lattice models
exhibiting criticality driven by dissipation.
In this work we theoretically analyze a circuit QED design where propagating
quantum microwaves interact with a single artificial atom, a single Cooper pair
box. In particular, we derivea master equation in the so-called transmon
regime, including coherent drives. Inspired by recent experiments, we then
apply the master equation to describe the dynamics in both a two-level and a
three-level approximation of the atom. In the two-level case, we also discuss
how to measure photon antibunching in the reflected field and how it is
affected by finite temperature and finite detection bandwidth.
In this work we show that a tunable coupling between microwave resonators can
be engineered by means of simple Josephson junctions circuits, such as dc- and
rf-SQUIDs. We show thatby controlling the time dependence of the coupling it
is possible to switch on and off and modulate the cross-talk, boost the
interaction towards the ultrastrong regime, as well as to engineer red and blue
sideband couplings, nonlinear photon hopping and classical gauge fields. We
discuss how these dynamically tunable superconducting circuits enable key
applications in the fields of all optical quantum computing, continuous
variable quantum information and quantum simulation – all within the reach of
state of the art in circuit-QED experiments.