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000189241 0247_ $$2doi$$a10.1016/j.ultramic.2014.11.019
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000189241 0247_ $$2ISSN$$a1879-2723
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000189241 037__ $$aFZJ-2015-02429
000189241 082__ $$a570
000189241 1001_ $$0P:(DE-HGF)0$$aChang, S$$b0$$eCorresponding Author
000189241 245__ $$aOptimising electron holography in the presence of partial coherence and instrument instabilities
000189241 260__ $$aAmsterdam$$bElsevier Science$$c2015
000189241 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1428931562_30908
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000189241 520__ $$aOff-axis electron holography provides a direct means of retrieving the phase of the wavefield in a transmission electron microscope, enabling measurement of electric and magnetic fields at length scales from microns to nanometers. To maximise the accuracy of the technique, it is important to acquire holograms using experimental conditions that optimise the phase resolution for a given spatial resolution. These conditions are determined by a number of competing parameters, especially the spatial coherence and the instrument instabilities. Here, we describe a simple, yet accurate, model for predicting the dose rate and exposure time that give the best phase resolution in a single hologram. Experimental studies were undertaken to verify the model of spatial coherence and instrument instabilities that are required for the optimisation. The model is applicable to electron holography in both standard mode and Lorentz mode, and it is relatively simple to apply.
000189241 536__ $$0G:(DE-HGF)POF3-143$$a143 - Controlling Configuration-Based Phenomena (POF3-143)$$cPOF3-143$$fPOF III$$x0
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000189241 7001_ $$0P:(DE-Juel1)159157$$aDwyer, Christian$$b1$$ufzj
000189241 7001_ $$0P:(DE-Juel1)144965$$aBoothroyd, Christopher Brian$$b2$$ufzj
000189241 7001_ $$0P:(DE-Juel1)144121$$aDunin-Borkowski, Rafal$$b3$$ufzj
000189241 773__ $$0PERI:(DE-600)1479043-9$$a10.1016/j.ultramic.2014.11.019$$gVol. 151, p. 37 - 45$$p37 - 45$$tUltramicroscopy$$v151$$x0304-3991$$y2015
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000189241 9141_ $$y2015
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