arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 2007.15798cond-mat.mtrl-sciphysics.chem-phquant-ph
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中性Tb(II)(Cp $^{\rm{iPr5}}$)$_2$单分子磁体的电调谐超精细光谱

Electrically tuned hyperfine spectrum in neutral Tb(II)(Cp$^{\rm{iPr5}}$)$_2$ single-molecule magnet

Robert L. Smith, Aleksander L. Wysocki, Kyungwha Park

摘要:

具有长自旋相干时间的分子自旋量子比特以及对这种量子比特的非侵入性操作方法具有很高的需求。结果表明,分子电子和核自旋能级都可以作为量子比特。在具有掺杂剂的固态系统中,当掺杂剂的核处的电子自旋密度高时,电场被示出有效地改变核自旋量子比特能级之间的间距。受这种固态系统的启发,我们提出具有不寻常的Ln $^{2+}$电子构型的二价镧系元素(Ln)配合物在Ln核自旋和电子自由度之间具有强的相互作用,这使得相互作用具有电调谐。作为一个例子,我们用完全活性空间自洽场方法研究了中性Tb(II)(Cp $^{\rm{iPr5}}$)$_2$单分子磁体(SMM)中$^{159}$ Tb核的电子结构和超精细相互作用.计算结果表明,低能态由$4f^8(6s,5d_{z^2})^1$、4 $f^8$(5 $d_{x^2-y^2}$)$^1$和$4f^8(5d_{xy})^1$构型产生.我们计算的超精细相互作用参数和电子核光谱在我们的多组态方法。我们发现,超精细相互作用是约一个数量级大于Tb(III)的Pc $_2$ SMMs。这是由于Tb原子核自旋与原子核上电子自旋密度之间存在着强烈的费米接触相互作用,而这种相互作用是由占据$(6s,5d)$轨道引起的。我们还发现费米接触项对电场的响应导致电子-核能级分离的电调谐。这种超精细斯塔克效应可能对量子计算中分子核自旋的应用很有用。

英文摘要:

Molecular spin qubits with long spin coherence time as well as non-invasive operation methods on such qubits are in high demand. It was shown that both molecular electronic and nuclear spin levels can be used as qubits. In solid state systems with dopants, an electric field was shown to effectively change the spacing between the nuclear spin qubit levels when the electron spin density is high at the nucleus of the dopant. Inspired by such solid-state systems, we propose that divalent lanthanide (Ln) complexes with an unusual electronic configuration of Ln$^{2+}$ have a strong interaction between the Ln nuclear spin and the electronic degrees of freedom, which renders electrical tuning of the interaction. As an example, we study electronic structure and hyperfine interaction of the $^{159}$Tb nucleus in a neutral Tb(II)(Cp$^{\rm{iPr5}}$)$_2$ single-molecule magnet (SMM) using the complete active space self-consistent field method with spin-orbit interaction included within the restricted active space state interaction. Our calculations show that the low-energy states arise from $4f^8(6s,5d_{z^2})^1$, 4$f^8$(5$d_{x^2-y^2}$)$^1$, and $4f^8(5d_{xy})^1$ configurations. We compute the hyperfine interaction parameters and the electronic-nuclear spectrum within our multiconfigurational approach. We find that the hyperfine interaction is about one order of magnitude greater than that for Tb(III)Pc$_2$ SMMs. This stems from the strong Fermi contact interaction between the Tb nuclear spin and the electron spin density at the nucleus that originates from the occupation of the $(6s,5d)$ orbitals. We also uncover that the response of the Fermi contact term to electric field results in electrical tuning of the electronic-nuclear level separations. This hyperfine Stark effect may be useful for applications of molecular nuclear spins for quantum computing.

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