TY - JOUR
T1 - Quantum process tomography of a Mølmer-Sørensen interaction
AU - Navon, Nir
AU - Akerman, Nitzan
AU - Kotler, Shlomi
AU - Glickman, Yinnon
AU - Ozeri, Roee
N1 - Israeli Science Foundation; Minerva Foundation; German-Israeli Foundation for Scientific Research; Crown Photonics Center; Wolfson Family Charitable Trust; Yeda-Sela Center for Basic ResearchThis research was supported by the Israeli Science Foundation, the Minerva Foundation, the German-Israeli Foundation for Scientific Research, the Crown Photonics Center, the Wolfson Family Charitable Trust, Yeda-Sela Center for Basic Research, David Dickstein of France, and M. Kushner Schnur of Mexico.
PY - 2014/7/28
Y1 - 2014/7/28
N2 - We present a simple tomographic protocol, for two-qubit systems, that relies on a single discriminatory transition and no direct spatially selective imaging. This scheme exploits excess micromotion in the trap to realize all operations required to prepare all input states and analyze all output states. We demonstrate a two-qubit entangling gate with a Bell state production fidelity of 0.981(6), and apply the above protocol to perform the first quantum process tomography of a Mølmer-Sørensen entangling gate. We characterize its χ-process matrix, the simplest for an entanglement gate on a separable-states basis, and observe that our dominant source of error is accurately modeled by a quantum depolarization channel.
AB - We present a simple tomographic protocol, for two-qubit systems, that relies on a single discriminatory transition and no direct spatially selective imaging. This scheme exploits excess micromotion in the trap to realize all operations required to prepare all input states and analyze all output states. We demonstrate a two-qubit entangling gate with a Bell state production fidelity of 0.981(6), and apply the above protocol to perform the first quantum process tomography of a Mølmer-Sørensen entangling gate. We characterize its χ-process matrix, the simplest for an entanglement gate on a separable-states basis, and observe that our dominant source of error is accurately modeled by a quantum depolarization channel.
UR - http://www.scopus.com/inward/record.url?scp=84905189549&partnerID=8YFLogxK
U2 - https://doi.org/10.1103/PhysRevA.90.010103
DO - https://doi.org/10.1103/PhysRevA.90.010103
M3 - مقالة
SN - 1050-2947
VL - 90
JO - Physical Review A - Atomic, Molecular, and Optical Physics
JF - Physical Review A - Atomic, Molecular, and Optical Physics
IS - 1
M1 - 010103
ER -