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里德伯-基态分子由一个里德伯原子和一个基态原子组成, 束缚机制是里德伯电子与基态原子的低能电子散射相互作用. 理论上, 通过低能电子散射Fermi赝势模型, 数值计算了铯(36D5/2+6S1/2)里德伯-基态分子的绝热势能曲线, 提取了里德伯分子的束缚能和平衡核间距等光谱参数. 实验上, 利用双光子光缔合技术成功制备了散射三重态(TΣ, Triplet)和散射单重态-三重态混合(S,TΣ, Mixed)形成的里德伯-基态分子, 获得了里德伯分子的光缔合光谱, 测量的势阱深度与理论计算结果相吻合. 另外, 以散射三重态为例, 分析了里德伯分子的光缔合光谱在外加电场中的展宽现象, 获得其平均永久电偶极矩
$|\bar{d}|$ 为(12.10 ± 1.65) Debye ((4.76 ± 0.65) ea0), 与理论计算结果保持一致. 该研究为实验上制备D态里德伯-基态分子提供了可行的实验方案, 对理解里德伯分子的光谱特性具有重要意义.-
关键词:
- 超冷里德伯-基态分子 /
- 光缔合光谱 /
- 绝热势能曲线 /
- 电偶极矩
Ultra-cold long-range Rydberg molecules, consisting of a Rydberg atom and a ground-state atom or another Rydberg atom or ion, have attracted considerable attention due to their exaggerated properties, such as huge size, long chemical bond, large polarization and electric dipole moment, abundant vibrational states and exotic adiabatic potentials. The binding mechanism of Rydberg molecules is a low-energy scattering interaction between the Rydberg electron and the ground state atom for ground-Rydberg molecules or long-range multipole interaction for Rydberg-atom macrodimers and Rydberg-ion molecules, in contrast to covalent bonds, ionic bonds of normal and van der Waals interaction. Owing to its huge size, the dynamic evolution becomes slow compared with normal diatomic molecules and the ultra-long chemical bonds allow being imaged directly by high resolution imaging technology, which makes it convenient to observe the molecular dynamics process chemical reaction process in real time. The investigation of Rydberg molecules will be significant for understanding the mechanism of molecular collision and quantum chemical reaction. In this work, we study the ultra-cold Rydberg-ground state molecules theoretically and experimentally. Theoretically, we calculate the adiabatic potential energy curve of cesium (36D5/2+ 6S1/2) Rydberg molecule based on the Fermi model of low energy electron scattering by numerically solving the Hamiltonian of Rydberg molecules. And also, we obtain its characteristic parameters, such as the potential depth, binding energy and equilibrium nuclear distance of Rydberg molecule. Experimentally, the Rydberg-ground molecules are investigated by a photoassociation spectroscopy, where two laser pulses are used to achieve a two-photon transition, and their spectra are obtained by ion detection technology. We successfully observe the Rydberg-ground state molecular spectra that correspond to a scattering triplet and a scattering single-triplet mixture (S,TΣ). The measured binding energy of Rydberg-ground state molecules is in good agreement with the theoretical result. In addition, taking the Rydberg-ground state molecules formed by scattering triplet (TΣ) for example, we demonstrate the spectrum broadening of Rydberg molecules in a weak electric field, from which we obtain the permanent electric dipole moments $|\bar{d}|$ of polar Rydberg-ground state molecules about (12.10$ \pm $ 1.65) Debye ((4.76$ \pm $ 0.65) ea0). The results are consistent with the theoretical calculations. Our study provides a feasible scheme for the experimental preparation of D-type Rydberg-ground molecules, which is of great significance in studying the binding mechanism and the spectral characteristics of polar Rydberg molecules.-
Keywords:
- ultra-cold Rydberg-ground molecule /
- photoassociation spectrum /
- adiabatic potential energy curve /
- permanent electric dipole moment
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图 1 里德伯-基态分子模型. 以里德伯离子核为中心, 基态原子位于轴矢量
$\boldsymbol{R}$ 的位置, 里德伯电子距离核的距离为r.$ {\widehat{S}}_{1} $ 为里德伯电子自旋,$ {\widehat{S}}_{2} $ 和$ {\widehat{I}}_{2} $ 分别对应基态原子的电子自旋和核自旋Fig. 1. Model of a Rydberg-ground molecule. The Rydberg core is located in the center, the ground atom is located at the position of the axial vector
$\boldsymbol{R}$ , and the distance between the Rydberg electron and the core is$ r $ .$ {\widehat{S}}_{1} $ is the spin of Rydberg electron, and$ {\widehat{S}}_{2} $ and$ {\widehat{I}}_{2} $ are the spin of the electron and nuclear of the ground atom.
图 2 数值计算的铯(36D5/2+6S1/2)分子的势能曲线, 彩色的波包为最外层势阱中基态
$ \upsilon =0 $ 的振动波函数Fig. 2. Calculated adiabatic potentials for cesium Rydberg-ground molecule of (36D5/2+6S1/2). The color filled wave packet is the vibration wave function of the outermost potential for
$ \upsilon =0 $ .
图 3 (a) 双光子激发能级示意图; (b) 两束激发光反向传播作用于MOT&ODT中心; 里德堡原子和分子由脉冲电场电离后到达MCP, 由boxcar采集和计算机记录; (c) 实验时序图; 关断MOT&ODT光之后, 同时打开两束激发光, 之后由斜坡脉冲电离电场电离里德伯原子和分子, 直流电场用于电偶极矩的研究
Fig. 3. (a) Schematic diagram of two photon excitation. (b) Schematic diagram of experimental set up. Two excitation lasers overlap in the center of MOT&ODT. Rydberg atoms and molecules ionized by a pulsed electric field arriving at MCP, which is collected with boxcar and recorded by computer. (c) Experimental sequence diagram. After turning off the MOT&ODT, two excitation lasers are turned on at the same time, and the Rydberg atoms and molecules were ionized by a ramp pulse ionization electric field. The direct current electric field is used to study the electric dipole moment.
图 4 铯(36D5/2+6S1/2)里德伯-基态分子的双光子光缔合光谱. 红色三角形标记的峰为振动基态
$ \upsilon =0 $ 的里德堡分子信号. 蓝色的短线标记了理论计算的束缚势阱. 插图为阴影区域的放大Fig. 4. Two-color photoassociation spectra of Cs (36D5/2+6S1/2) Rydberg-ground molecule. The short blue line marks the theoretically calculated bound potential well. Red triangles denote the Rydberg-molecular signal for
$ \upsilon =0 $ . Inset is an enlargement of the shaded area.
图 5 电场为
$ 0.09 $ (a)和$0.37\;\rm{V}/\rm{c}\rm{m}$ (b)时, 三重态相互作用形成的里德伯-基态分子的光缔合光谱. 红色实线为理论拟合的分子电偶极矩Fig. 5. Photoassociation spectra of Rydberg ground molecules formed by triplet interaction when the electric field is
$ 0.09 $ (a) and$0.37\;\rm{V}/\rm{c}\rm{m}$ (b). Red solid line are the theoretical fitting of molecular electric dipole moment. -
[1] Omont A 1977 J. de Phys. 38 1343
Google Scholar
[2] Greene C H, Dickinson A S, Sadeghpour H R 2000 Phys. Rev. Lett. 85 2458
Google Scholar
[3] Khuskivadze A A, Chibisov M I, Fabrikant I I 2002 Phys. Rev. A 66 042709
Google Scholar
[4] Chibisov M I, Khuskivadze A A, Fabrikant I I 2002 J. Phys. B 35 L193
Google Scholar
[5] Hamilton E L, Greene C H, Sadeghpour H R 2002 J. Phys. B 35 L199
Google Scholar
[6] Lesanovsky I, Schmelcher P, Sadeghpour H R 2006 J. Phys. B 39 L69
Google Scholar
[7] Bendkowsky V, Bjoern B, Nipper J, Shaffer J P, Robert L, Pfau T 2009 Nature 458 1005
Google Scholar
[8] Bellos M A, Carollo R, Banerjee J, Eyler E E, Gould P L 2013 Phys. Rev. Lett. 111 053001
Google Scholar
[9] Anderson D A, Miller S A, Raithel G 2014 Phys. Rev. Lett. 112 163201
Google Scholar
[10] Krupp A T, Gaj A, Balewski J B, Ilzhöfer P, Hofferberth S, Löw R, Pfau T, Kurz M, Schmelcher P 2014 Phys. Rev. Lett. 112 143008
Google Scholar
[11] Maclennan J L, Chen Y J, Raithel G 2019 Phys. Rev. A 99 033407
Google Scholar
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Google Scholar
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Google Scholar
[14] Sassmannshausen H, Merkt F, Deiglmayr J 2015 Phys. Rev. Lett. 114 133201
Google Scholar
[15] Fey C, Hummel F, Schmelcher P 2019 Phys. Rev. A 99 022506
Google Scholar
[16] Bai S, Han X, Bai J, Jiao Y, Wang H, Zhao J, Jia S 2020 J. Chem. Phys. 152 084302
Google Scholar
[17] Bai S, Han X, Bai J, Jiao Y, Zhao J, Jia S, Raithel G 2020 Phys. Rev. Res. 2 033525
Google Scholar
[18] Overstreet K R, Schwettmann A, Tallant J, Booth D, Shaffer J P 2009 Nat. Phys 5 581
Google Scholar
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Google Scholar
[20] Duspayev A, Han X, Viray M A, Ma L, Zhao J, Raithel G 2021 Phys. Rev. Res. 3 023114
Google Scholar
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Google Scholar
[22] Zuber N, Anasuri V S V, Berngruber M, Zou Y Q, Meinert F, Löw R, Pfau T 2022 Nature 605 453
Google Scholar
[23] Li W, Pohl T, Rost J M, Rittenhouse S T, Sadeghpour H R, Nipper J, Butscher B, Balewski J B, Bendkowsky V, Löw R 2011 Science 334 1110
Google Scholar
[24] Niederprüm T, Thomas O, Eichert T, Lippe C, Pérez-Ríos J, Greene C H, Ott H 2016 Nat. Commun. 7 12820
Google Scholar
[25] Weimer H, Müller M, Lesanovsky I, Zoller P, Büchler H 2010 Nat. Phys. 6 382
Google Scholar
[26] Lukin M D, Fleischhauer M, Côté R, Duan L M, Jaksch D, Cirac J I, Zoller P 2001 Phys. Rev. Lett. 87 037901
Google Scholar
[27] Alizadeh E, Orlando T M, Sanche L 2015 Annu. Rev. Phys. Chem. 66 379
Google Scholar
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