arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 2312.06332quant-phphysics.atom-phphysics.optics
收藏

弱磁场中核自旋量子比特的保相干冷却

Coherence-preserving cooling of nuclear spin qubits in a weak magnetic field

Xiao-Feng Shi

AI总结:

提出弱磁场下⁸⁷Sr核自旋量子比特的保相干边带冷却理论,利用依赖m_J的AC Stark频移抑制超精细导致的核自旋混合,并支持由两个最低Zeeman子态定义量子比特。

摘要:

二价中性原子的核自旋存储器可在强磁场中实现保自旋的分辨边带冷却[Phys. Rev. Lett. 99, 123001 (2007)]。我们提出了一种在弱磁场中冷却⁸⁷Sr核自旋量子比特的理论。该理论依赖于将5s5p ¹P₁激光激发至邻近态,从而产生相对于超精细相互作用较大的、依赖于m_J的AC Stark频移。这有效抑制了由超精细相互作用引起的核自旋混合。通过由AC Stark频移的¹P₁态淬灭的钟态进行边带冷却,可使原子在保持核自旋的情况下自发辐射回到基态。该理论不仅兼容低磁场,还适用于核自旋量子比特由两个最低Zeeman子态定义的情形。

英文摘要:

Nuclear spin memories of divalent neutral atoms can allow spin-preserving resolved-sideband cooling in a strong magnetic field [Phys. Rev. Lett. 99, 123001 (2007)]. We present a theory for cooling $^{87}$Sr nuclear-spin qubits in a weak magnetic field. The theory depends on laser excitation of $5s5p~^1P_1$ to a nearby state which results in $m_J$-dependent AC Stark shifts large compared to the hyperfine interaction. This effectively suppresses the nuclear-spin mixing due to the hyperfine interaction. Sideband cooling via the clock state quenched by the AC Stark-shifted $^1P_1$ state leads to nuclear-spin-preserving spontaneous emission back to the ground state. More than being compatible with low magnetic fields, the theory is applicable when the nuclear spin qubits are defined by the two lowest Zeeman substates.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

↑