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Opinion


and the imaging lenses, finding the sample, re-focusing, and correcting beam tilt; and (b) the change of object magnifi- cation also changes the magnification of the interference, requiring the adjustment of the voltage at the biprism and at least one of the imaging lenses. Both (a) and (b) have to be balanced iteratively, adding to the long delays when chang- ing magnification. Thus changing from an overview of the specimen area to a more detailed view rudely interrupts live phase imaging—and that is where most users lose interest in the technique. Te solution. Te solution is to separate the magnification


of the interference fringes (with respect to the camera) from the magnification of the object. An approach to this was proposed in 2001 [13]. As shown in Figure 1, adding lenses between the objective lens and the biprism allows magnification changes of the sample while the original lenses below the biprism main- tain the interference fringes with respect to the camera. Add- ing lenses to the optical train in the suggested area should not be complicated; Cs correctors are more complex, and we know how to handle them. I believe it is time for this simple modification to be


made in a well-designed holography microscope. Such a microscope could be used like any other transmission elec- tron microscope, but it would allow imaging the object simultaneously in its intensity and phase, live in real time. Then magnetic and electric fields become visible supporting investigations of p-n junctions, magnetoresistive RAM, and electric fields around toner particles. At high resolution, local crystal tilt becomes obvious on the unit-cell scale, and biological objects would show much improved contrast even under low dose conditions—to name a few applications. Thus, electron holography could truly evolve into a main- stream technology and provide in real time all the informa- tion the electron wave contains.


References [1] “Frits Zernike,” Wikipedia, Te accessed June 3, 2018.


Free Encyclopedia,


[2] D Gabor, Nature 161(4098) (1948) 777–78. [3] G Möllenstedt and H Düker, Naturwissenschaſten 42 (1955) 41.


[4] EN Leith and J Upatnieks, J Opt Soc Am 52(10) (1962) 1123–30.


[5] O Scherzer, J Appl Phys 20 (1949) 20. [6] HW Zandbergen and DV Dyck, Microsc Res Techniq 49(3) (2000) 301–23.


[7] H Rose, Optik 39 (1973–74) 416. [8] E Voelkl et al., Scanning Microscopy 11 (1997) 407–16. [9] D Cooper et al., Appl Phys Lett 91 (2007) 143501.


[10] E Voelkl and D Tang, Ultramicroscopy 110 (2010) 447–59.


[11] E Voelkl and A Ponce Microsc Microanal 24 (Suppl 1) (2018) 1462–63.


[12] E Voelkl et al., Microsc Microanal 21 (Suppl 3) (2015) 1951–52.


[13] E Voelkl et al., Electron holography microscope. US Pat- ent 6,617,580, filed December 27, 2001.


2019 January • www.microscopy-today.com


Comparison of duoplasmatron versus Hyperion (operating on Cameca NanoSIMS) shows beam current as a function of spot size.


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