2019
DOI: 10.1088/1367-2630/ab4f43
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Measuring the temperature and heating rate of a single ion by imaging

Abstract: We present a technique based on high resolution imaging to measure the absolute temperature and the heating rate of a single ion trapped at the focus of a deep parabolic mirror. We collect the fluorescence light scattered by the ion during laser cooling and image it onto a camera. Accounting for the size of the point-spread function and the magnification of the imaging system, we determine the spatial extent of the ion, from which we infer the mean phonon occupation number in the trap. Repeating such measureme… Show more

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Cited by 9 publications
(4 citation statements)
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References 33 publications
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“…(55)式的积分可以被写为 [27] ⟨J 实验上已经成功构造出了离子晶体的多种构 型, 比如直线构型、之字构型 [40] 、螺旋构型 [41] 和带 拓扑结的之字构型 [42] . 实验上也实现了离子晶体 在不同构型之间的结构相变 [43] , 而且观察到温度 对离子晶体构型的影响 [44,45] . 目前对有关低维系统热传导的理论已经在实验 室中有所应用, 比如在离子阱中的协同冷却技术, 这种技术能够在只对离子晶体中的一个离子进行冷 却的情况下, 降低离子晶体中所有离子的温度 [49,50] .…”
Section: 并且满足以下条件unclassified
“…(55)式的积分可以被写为 [27] ⟨J 实验上已经成功构造出了离子晶体的多种构 型, 比如直线构型、之字构型 [40] 、螺旋构型 [41] 和带 拓扑结的之字构型 [42] . 实验上也实现了离子晶体 在不同构型之间的结构相变 [43] , 而且观察到温度 对离子晶体构型的影响 [44,45] . 目前对有关低维系统热传导的理论已经在实验 室中有所应用, 比如在离子阱中的协同冷却技术, 这种技术能够在只对离子晶体中的一个离子进行冷 却的情况下, 降低离子晶体中所有离子的温度 [49,50] .…”
Section: 并且满足以下条件unclassified
“…Thus, we can tune the temperature associated with the axial motion, typically between about 1 mK up to 200 mK. In order to relate the applied noise amplitude with temperature, we use the spatial thermometry technique [30,34]. We determine the RMS width of the ion ∆z th , see Fig.…”
Section: Experimental Implementation Of Coherent Wave Packet Excitati...mentioning
confidence: 99%
“…The spatial spread of the atom is important for experiments requiring strong interaction of the atoms with tightly focused light and needs to be small in comparison to the size of the focal spot. [ 9–11 ] This requirement is particularly stringent when focusing a dipole wave from full solid angle, where the full widths at half maximum of the point spread function are 0.4 wavelengths in the lateral direction and about 0.6 wavelengths along the optical axis, respectively. The spatial spread of the atom along direction i is given by σi=σ0,i·1+truen¯iwith σ0,i=/2mωi the spread of the atom in the ground state of an harmonic oscillator of mass m and trap frequency ωi.…”
Section: Characteristics Of the Optical Trapmentioning
confidence: 99%
“…[6,7] The maximum possible coupling is also affected by the thermal motion of the trapped ion. [5,6,9] This thermal motion results in a spatial averaging over the electric field in the tight focal spot and thus in an effective reduction of the amplitude experienced by the ion. The same effect was also observed for neutral atoms in an optical dipole trap [10,11] and counteracted by polarization gradient cooling.…”
Section: Introductionmentioning
confidence: 99%