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Design of a Scanning Atom Probe with Improved Mass Resolution using Post Deceleration

机译:使用后减速的改进质量分辨率设计扫描原子探针

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In a time-of-flight atom probe instrument using voltage pulses, the acceleration of the field-evaporated ions through a time-varying field leads to an uncertainty in their kinetic energy, and thus, degradation in the mass resolution [1]. Atom probes, have tended to include some energy compensation, using either a Poschenrieder lens [2] or a reflection [3] to compensate for this variation and improve mass resolution. In the scanning atom probe (SAP), originally proposed by Nishikawa et al. [4], and the local electrode atom probe described by Kelly et al.[5], the distance from specimen to counter electrode is <100μm. Mass resolution in these configurations can be improved using different methods than previously. Kelly et al. [6] have used post acceleration to improve mass resolution. This relies on a very small separation between tip and electrode which allows field evaporation at lower applied voltages - around 5 kV as opposed to the usual more 10-20 kV. By post accelerating the ions, the energy variation is reduced relative to the total energy, thus improving in the mass resolution. Cerezo et al. [8] adopted a different approach, using a design for the counter electrode in which the ions evaporated on the pulse are decelerated to the applied dc potential. The voltage used in deceleration is therefore only a small part of the total applied voltage since the pulse fraction is usually 15%-20%, and the lensing effects generated are small. The total ion energy is also kept small, such that the time resolution is not compromised.
机译:在使用电压脉冲的飞行时间原子探针仪器中,通过时变场通过野外蒸发离子的加速导致其动能的不确定性,因此质量分辨率的降解[1]。原子探针倾向于包括一些能量补偿,使用Poschenrieder透镜[2]或反射[3]来补偿这种变化并改善质量分辨率。在扫描原子探针(SAP)中,最初由Nishikawa等人提出。 [4],以及凯利等人描述的局部电极原子探针。[5],从样本到对电极的距离<100μm。可以使用与先前不同的方法改进这些配置中的质量分辨率。 Kelly等人。 [6]使用后加速度提高质量分辨率。这依赖于尖端和电极之间的非常小的分离,其允许在较低施加的电压下蒸发 - 约5kV,而不是通常的10-20 kV。通过促进离子的后,相对于总能量,能量变化降低,从而改善质量分辨率。 Cerezo等。 [8]采用不同的方法,使用用于对电极的设计,其中脉冲上蒸发的离子被减速到施加的直流电位。因此,减速的电压仅是总施加电压的一小部分,因为脉冲分数通常为15%-20%,产生的镜头效果很小。总离子能量也保持小,使得时间分辨率不会受到损害。

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