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UID:news714@physik.unibas.ch
DTSTAMP;TZID=Europe/Zurich:20230621T115907
DTSTART;TZID=Europe/Zurich:20230623T131500
SUMMARY:Next-Generation Qubits in Superconducting Circuits
DESCRIPTION:Abstract:\\r\\nOver the past decade\, qubits encoded in superco
 nducting circuits have emerged as a leading platform for quantum informati
 on processing\, resulting in a rapidly expanding and thriving research fie
 ld. However\, present-day superconducting quantum processors are still hig
 hly susceptible to the effects of environmental noise\, which degrades the
 ir computational performance and limits applications. As a result\, develo
 ping next-generation superconducting qubits with improved protection is a 
 major research focus to accelerate the path to a fault-tolerant quantum co
 mputer.   In this talk\, I will introduce our approach for protecting qua
 ntum information in superconducting circuits\, which relies on quantum mat
 erial Josephson junction realized in superconductor-semiconductor hybrid s
 tructures [1\,2]. First\, I will describe how such hybrid quantum material
 s when placed in contact with superconductors can give rise to an exotic c
 harge-4e supercurrent and discuss approaches for experimentally detecting 
 this coherent transport of “pairs of Cooper-pairs“ [3]. Second\, I wil
 l present resulting insights in how the charge-4e supercurrent can be empl
 oyed to create a protected “0-Pi“ superconducting qubit in arrays of J
 osephson junctions and discuss how the Josephson junction arrays can be th
 eoretically modeled with effective spin models. Finally\, I will compare t
 he “0-Pi“ protected superconducting qubits to an alternative approach 
 based on topological wavefunctions\, the Majorana zero modes [4\,5]\, and 
 discuss how quantum material Josephson junctions can provide a new avenue 
 for quantum simulation.   [1] C. Schrade\, C. M. Marcus\, A. Gyenis\, PRX
  Quantum 3\, 030303 (2022) [2] A. Maiani\, M. Kjaergaard\, C. Schrade\, PR
 X Quantum 3\, 030329 (2022) [3] R. S. Souto\, M. Leijnse\, C. Schrade\, Ph
 ys. Rev. Lett. 129 267702 (2022) [4] C. Schrade and L. Fu\, Phys. Rev. Let
 t 129\, 227002 (2022) [5] C. Schrade and L. Fu\, Phys. Rev. Lett. 121\, 26
 7002 (2018)
X-ALT-DESC:<h2><span><span>Abstract:</span></span></h2>\n<p>Over the past d
 ecade\, qubits encoded in superconducting circuits have emerged as a leadi
 ng platform for quantum information processing\, resulting in a rapidly ex
 panding and thriving research field. However\, present-day superconducting
  quantum processors are still highly susceptible to the effects of environ
 mental noise\, which degrades their computational performance and limits a
 pplications. As a result\, developing next-generation superconducting qubi
 ts with improved protection is a major research focus to accelerate the pa
 th to a fault-tolerant quantum computer.&nbsp\;<br /> <br /> In this talk\
 , I will introduce our approach for protecting quantum information in supe
 rconducting circuits\, which relies on quantum material Josephson junction
  realized in superconductor-semiconductor hybrid structures [1\,2]. First\
 , I will describe how such hybrid quantum materials when placed in contact
  with superconductors can give rise to an exotic charge-4e supercurrent an
 d discuss approaches for experimentally detecting this coherent transport 
 of “pairs of Cooper-pairs“ [3]. Second\, I will present resulting insi
 ghts in how the charge-4e supercurrent can be employed to create a protect
 ed “0-Pi“ superconducting qubit in arrays of Josephson junctions and d
 iscuss how the Josephson junction arrays can be theoretically modeled with
  effective spin models. Finally\, I will compare the “0-Pi“ protected 
 superconducting qubits to an alternative approach based on topological wav
 efunctions\, the Majorana zero modes [4\,5]\, and discuss how quantum mate
 rial Josephson junctions can provide a new avenue for quantum simulation.&
 nbsp\;<br /> <br /> [1] C. Schrade\, C. M. Marcus\, A. Gyenis\, PRX Quantu
 m 3\, 030303 (2022)<br /> [2] A. Maiani\, M. Kjaergaard\, C. Schrade\, PRX
  Quantum 3\, 030329 (2022)<br /> [3] R. S. Souto\, M. Leijnse\, C. Schrade
 \, Phys. Rev. Lett. 129 267702 (2022)<br /> [4] C. Schrade and L. Fu\, Phy
 s. Rev. Lett 129\, 227002 (2022)<br /> [5] C. Schrade and L. Fu\, Phys. Re
 v. Lett. 121\, 267002 (2018)</p>
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