论文标题
原子二进制全息图在有限距离处:分辨率,对比度和通量
Atom binary holography at a finite distance: Resolution, contrast and flux
论文作者
论文摘要
在经典的二进制全息图中,位于无穷大的目标模式是通过通过二进制掩模的孔衍射,其孔具有相同大小的孔,该孔位于矩形网格的特定位置。最近提出了菲涅耳二元原子全息图作为用亚稳定原子束实现纳米分辨率掩模的光刻的一种手段。实际上,将有制造限制的限制:二进制面膜将具有最小孔的大小,网格〜(螺距)中的孔之间的最小距离,最大尺寸,目标模式平面将始终距面罩有限距离。在本文中,我们表明,在实践中,对于给定的波长,掩码和目标图案大小,掩码和目标模式平面(屏幕平面)之间的距离将有一个跨越的值,从而导致无鉴定模式。可以证明,这种洞察力如何导致在实验局限性中产生更高的对比度和纳米分辨率的更好分辨模式。由于通量是影响纳米光刻制造的模式质量的主要因素之一,因此我们获得了``绘制通量''的表达式(有助于产生目标模式的通量,该目标模式由磁通量归一化,这是由入射到掩模结构性部分的磁通量标准化的)。从数值上讲,我们发现其比率大约像$ x^{ - 2} $相比,其中$ x $是跨越距离的掩模屏幕距离。我们提出的方法可以与可以建模为标量波的任何光束一起使用,包括声波和其他物质波束,例如氦离子或电子。
In classical binary holography, a target pattern located at infinity is generated by the diffraction of a plane wave passing through a binary mask with holes of the same size, placed at specific positions of a rectangular grid. Fresnel binary atom holography was recently proposed as a means for achieving nanometer-resolution mask-based lithography with metastable atom beams. In practice, there will be fabrication imposed limits: the binary mask will have a minimum hole size, a minimum distance between the holes in the grid~(pitch), a maximum size, and the target pattern plane will always have a finite distance from the mask. In this paper, we show that, in praxis, for a given wavelength, mask, and target pattern sizes, there will be a cross-over value for the distance between the mask and the target pattern plane (the screen plane) which results in aliasing-free patterns. It is demonstrated how this insight can lead to the generation of better-resolved patterns of higher contrast and nanometer resolution can be achieved within experimental limitations. Since flux is one of the main factors influencing the quality of patterns fabricated by nano-lithography, we obtain an expression for the ``patterning flux'' (the flux that contributes to producing the target pattern, normalized by the flux that is incident onto the structured portion of the mask). Numerically we find that its ratio scales approximately like $x^{-2}$ where $x$ is the mask-screen distance over the cross-over distance. The method that we propose can be used with any beam that can be modeled as a scalar wave, including acoustic waves and other matter-wave beams such as helium ions or electrons.