Atom
Pinhole Camera
The most difficult problem
in atom optics is the problem of high-resolution focusing of neutral
atoms, which is promising for the nondestructive method for probing
the surface at the atomic level, as well as for the creation of nanostructures
on the surface. Although there are many proposals for focusing of atomic
beams, this problem is experimentally unsolved. The main difficulty
is the creation of the interaction potential of the atom with the electromagnetic
field that is close to an "ideal" lens for atoms.
We developed a new approach
to the problem of focusing and construction of an image in atom optics,
which is based on a well known idea of "optical pinhole camera"
(Fig.1) . The pinhole camera in optics is a camera without a lens. Light
forming an image passes through a pin hole.
In our experiment with
the atom pinhole camera (Fig.2) the atomic beam passes through a set
of holes in a metal mask (Fig.3) and thereby forms, by analogy with
optics, a "glowing" object of a given geometry (Fig.4). The
atoms pass through the holes in the mask, propagate in vacuum along
rectilinear trajectories, similar to light rays, and are incident on
a thin film placed at a distance L from the mask with a large number
(n =107–108 /cm2) of nanoholes
(50 nm diameter). Each hole of the film is a pinhole camera for atoms,
which forms its individual image of the object on the substrate surface
placed at a distance of l behind the film. In this geometry, a set of
the images of the object, which are decreased by a factor of about m
= L / l ~ 10000 this leads to a decrease in the profile height of the
created nanostructures at a given exposition.[1]

Fig.1
Optical Pinhole Camera
|

Fig.2
Atom Pinhole Camera
|

Fig.3
The mask in the form of greak letter Lambda
|

Fig.4
One of ten million identical
nanostructures made with the mask lambda
|
Next figures (Fig.5, Fig.6) shows the
detailed image of a simple cross. As seen in the figures, the cross
consists of the nanostructures that are images of the object mask.
| 
Fig.6 Three
of the 107 images of the "cross" |

Fig.7 The
surface section (800 x 800 nm) with the image of the "cross"
object |
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