Singlet-Triplet and Exchange-Only Flopping-Mode Spin Qubits

Semiconductor-based spin qubits embedded into a superconducting microwave cavity constitute a fast-progressing and promising platform for realizing fast and fault-tolerant qubit control with long-range two-qubit coupling. The flopping-mode spin qubit consists of a single electron in a double quantum dot; it combines a charge qubit with a spin qubit. With its strong and tunable cavity coupling, the flopping-mode qubit is proven to be well suited for low-power qubit control and cavity-mediated long-range quantum gates. The singlet-triplet (ST) and exchange-only (EO) qubits are multielectron realizations that go without broadband control and are protected from some types of noise, but are challenging to couple to each other and to microwave cavities. We combine the flopping-mode concept with the ST and EO qubits and propose two new flopping-mode qubits that consist of three (four) quantum dots, occupied by two (three) electrons near the <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mo stretchy="false">(</a:mo><a:mn>1</a:mn><a:mo>,</a:mo><a:mn>0</a:mn><a:mo>,</a:mo><a:mn>1</a:mn><a:mo stretchy="false">)</a:mo><a:mo stretchy="false">↔</a:mo><a:mo stretchy="false">(</a:mo><a:mn>0</a:mn><a:mo>,</a:mo><a:mn>1</a:mn><a:mo>,</a:mo><a:mn>1</a:mn><a:mo stretchy="false">)</a:mo><a:mspace width="0.2em"/><a:mo stretchy="false">[</a:mo><a:mo stretchy="false">(</a:mo><a:mn>1</a:mn><a:mo>,</a:mo><a:mn>0</a:mn><a:mo>,</a:mo><a:mn>1</a:mn><a:mo>,</a:mo><a:mn>1</a:mn><a:mo stretchy="false">)</a:mo><a:mo stretchy="false">↔</a:mo><a:mo stretchy="false">(</a:mo><a:mn>0</a:mn><a:mo>,</a:mo><a:mn>1</a:mn><a:mo>,</a:mo><a:mn>1</a:mn><a:mo>,</a:mo><a:mn>1</a:mn><a:mo stretchy="false">)</a:mo><a:mo stretchy="false">]</a:mo></a:math> charge transition. The two-electron system augments the <p:math xmlns:p="http://www.w3.org/1998/Math/MathML" display="inline"><p:msub><p:mi>ST</p:mi><p:mn>0</p:mn></p:msub></p:math> spin qubit with a charge qubit that interacts transversally and longitudinally with a cavity. Both couplings are highly tunable, and the longitudinal coupling distinguishes the flopping-mode ST qubit from the regular flopping-mode qubit. The longitudinal coupling allows for nondissipative universal control similar to superconducting transmon qubits. The EO flopping-mode qubit comprises four dots occupied by three electrons and opens a new possibility to perform two-qubit gates for EO qubits that are challenging to perform directly with the exchange coupling. We use input-output theory to provide means of extracting the coupling strengths from cavity transmission data.