Active Cooling of a Superconducting Transmon Qubit in a Hot Environment
ORAL
Abstract
Justin Peterkin1,2, Haozhi Wang2, Benjamin Remez1, Max Neiderbach1, Rohit Pant2, Mohammad Hafezi1, Christopher Richardson1,2, Alicia J. Kollár1, and B. S. Palmer1,2
1University of Maryland, College Park, Maryland 20742, USA
2Laboratory for Physical Sciences, College Park, Maryland 20740, USA
The use of dissipation and the pumping of different discrete states in quantum superconducting systems has led to the formation of interesting quantum states that would otherwise be difficult to create. Here, we discuss the use of dissipation engineering for the intent of initialization of a transmon qubit at elevated operating temperatures above 300mK. To actively cool a standard transmon qubit, with a transition frequency of less than 8 GHz, we couple it to a high-frequency cavity (>20 GHz) with a large decay rate. By exciting the excess thermal population of the transmon from its second excited state to the cooling cavity’s first excited state, the qubit’s excess population is removed, and the system is started in the ground state with a larger fidelity. We will present initial measurements and ground state fidelities for this active cooling scheme.
1University of Maryland, College Park, Maryland 20742, USA
2Laboratory for Physical Sciences, College Park, Maryland 20740, USA
The use of dissipation and the pumping of different discrete states in quantum superconducting systems has led to the formation of interesting quantum states that would otherwise be difficult to create. Here, we discuss the use of dissipation engineering for the intent of initialization of a transmon qubit at elevated operating temperatures above 300mK. To actively cool a standard transmon qubit, with a transition frequency of less than 8 GHz, we couple it to a high-frequency cavity (>20 GHz) with a large decay rate. By exciting the excess thermal population of the transmon from its second excited state to the cooling cavity’s first excited state, the qubit’s excess population is removed, and the system is started in the ground state with a larger fidelity. We will present initial measurements and ground state fidelities for this active cooling scheme.
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Presenters
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Justin M Peterkin
- University of Maryland College Park