Dissipative preparation and stabilization of many-body quantum states in a superconducting qutrit array

  1. Yunzhao Wang,
  2. Kyrylo Snizhko,
  3. Alessandro Romito,
  4. Yuval Gefen,
  5. and Kater Murch
We present and analyze a protocol for driven-dissipatively preparing and stabilizing a quantum manybody entangled state with symmetry-protected topological order. Specifically, we consider
the experimental platform consisting of superconducting transmon circuits and linear microwave resonators. We perform theoretical modeling of this platform via pulse-level simulations based on physical features of real devices. In our protocol, transmon qutrits are mapped onto spin-1 systems. The qutrits‘ sharing of nearest-neighbor dispersive coupling to a dissipative microwave resonator enables elimination of state population in the Stotal = 2 subspace for each adjacent pair, and thus, the stabilization of the manybody system into the Affleck, Kennedy, Lieb and Tasaki (AKLT) state. We also analyze the performance of our protocol as the system size scales up to four qutrits, in terms of its fidelity as well as the stabilization time. Our work shows the capacity of driven-dissipative superconducting cQED systems to host robust and self-corrected quantum manybody states that are topologically non-trivial.

Observing a Topological Transition in Weak-Measurement-Induced Geometric Phases

  1. Yunzhao Wang,
  2. Kyrylo Snizhko,
  3. Alessandro Romito,
  4. Yuval Gefen,
  5. and Kater Murch
Measurement plays a quintessential role in the control of quantum systems. Beyond initialization and readout which pertain to projective measurements, weak measurements in particular,
through their back-action on the system, may enable various levels of coherent control. The latter ranges from observing quantum trajectories to state dragging and steering. Furthermore, just like the adiabatic evolution of quantum states that is known to induce the Berry phase, sequential weak measurements may lead to path-dependent geometric phases. Here we measure the geometric phases induced by sequences of weak measurements and demonstrate a topological transition in the geometric phase controlled by measurement strength. This connection between weak measurement induced quantum dynamics and topological transitions reveals subtle topological features in measurement-based manipulation of quantum systems. Our protocol could be implemented for classes of operations (e.g. braiding) which are topological in nature. Furthermore, our results open new horizons for measurement-enabled quantum control of many-body topological states.

Measurement of geometric dephasing using a superconducting qubit

  1. S. Berger,
  2. M. Pechal,
  3. P. Kurpiers,
  4. A.A. Abdumalikov,
  5. C. Eichler,
  6. J. A. Mlynek,
  7. A. Shnirman,
  8. Yuval Gefen,
  9. A. Wallraff,
  10. and S. Filipp
A quantum system interacting with its environment is subject to dephasing which ultimately destroys the information it holds. Using a superconducting qubit, we experimentally show that
this dephasing has both dynamic and geometric origins. It is found that geometric dephasing, which is present even in the adiabatic limit and when no geometric phase is acquired, can either reduce or restore coherence depending on the orientation of the path the qubit traces out in its projective Hilbert space. It accompanies the evolution of any system in Hilbert space subjected to noise.