SciPost Submission Page
Bridging nano-optics and condensed matter formalisms in a unified description of inelastic scattering of relativistic electron beams
by Hugo Lourenço-Martins, Axel Lubk, Mathieu Kociak
- Published as SciPost Phys. 10, 031 (2021)
|As Contributors:||Hugo Lourenço-Martins · Axel Lubk|
|Arxiv Link:||https://arxiv.org/abs/2007.02773v3 (pdf)|
|Date submitted:||2020-11-24 15:06|
|Submitted by:||Lourenço-Martins, Hugo|
|Submitted to:||SciPost Physics|
In the last decades, the blossoming of experimental breakthroughs in the domain of electron energy loss spectroscopy (EELS) has triggered a variety of theoretical developments. Those have to deal with completely different situations, from atomically resolved phonon mapping to electron circular dichroism passing by surface plasmon mapping. All of them rely on very different physical approximations and have not yet been reconciled, despite early attempts to do so. As an effort in that direction, we report on the development of a scalar relativistic quantum electrodynamic (QED) approach of the inelastic scattering of fast electrons. This theory can be adapted to describe all modern EELS experiments, and under the relevant approximations, can be reduced to any of the last EELS theories. In that aim, we present in this paper the state of the art and the basics of scalar relativistic QED relevant to the electron inelastic scattering. We then give a clear relation between the two once antagonist descriptions of the EELS, the retarded green Dyadic, usually applied to describe photonic excitations and the quasi-static mixed dynamic form factor (MDFF), more adapted to describe core electronic excitations of material. We then use this theory to establish two important EELS-related equations. The first one relates the spatially resolved EELS to the imaginary part of the photon propagator and the incoming and outgoing electron beam wavefunction, synthesizing the most common theories developed for analyzing spatially resolved EELS experiments. The second one shows that the evolution of the electron beam density matrix is proportional to the mutual coherence tensor, proving that quite universally, the electromagnetic correlations in the target are imprinted in the coherence properties of the probing electron beam.
Published as SciPost Phys. 10, 031 (2021)
Author comments upon resubmission
We thank the referee for his thorough reading of the manuscript and for his very positive comments. We have considered all the points raised in the review. In details:
- p1: "The overlap of the electron beam with the sample e.g ...". It is not clear what is meant with 'overlap' here. I think it refers to aloof experiments vs. bulk? Otherwise both suface and bulk effects play a role and seem to be independent on the overlap of the beam with the sample?
We thank the referee for raising this ambiguity. We indeed refer to the distinction between aloof and penetrating trajectories. To clarify this point, we replaced this sentence by: “The spatial overlap of the electron beam with the sample, e.g., the importance of bulk versus surface effects.”
- fig1: an ending bracket is missing in the description of the illumination system
We thank the referee for having carefully checked the formatting of the figures. Nonetheless, we did not find the above-mentioned typo.
- p2: the magic angle is defined as the angle at which electrons are most likely deflected. This is confusing to me, but may be right. I would define the magic angle as the collection angle at which there is no dependence of the recorded spectrum on the orientation of an anisotropic sample.
The referee is right, and we have therefore modified our definition according to his suggestion. The new text reads: “For example, it has been demonstrated that the so-called magic angle, at which the dependence of the core-loss electron scattering on the orientation of an anisotropic sample is canceled, strongly depends on the retarded character of the electron to target interaction, which had been considered as negligible in core-loss investigations before.”
- p2: "X or optical ...", I would write "X-ray or optical photon"
- p2: "in a STEM has yet been provided, which includes...", I would write "in a STEM has been provided, which implies..."
- p3: "the later to the retarded case,...", I think this needs to be "latter". I suggest to search for the word "later" and replace with "latter" wherever appropriate as this occurs several times in the manuscript.
Points 4, 5 and 6 have been addressed and modified as the reviewer suggested.
- ref 18: check the spelling of Hebert (accents)
After checking, it appears that the spelling used in this manuscript is correct.
- fig2: the 'grey' part of the figure is not easy to distinguish
The figure has been enlarged and the gray adjusted to remedy that problem.
- p5: "The zz indices hind at", I think this needs to be "hint"
This typo has been correct.
- p7: "The are therefore not sufficient to model such experiments". I would argue that even for 'simple' EELS experiments, the partial coherence of the outgoing electron wave does make an important difference as even going to diffraction space will make such coherence visible in the recorded intensities. In this sense, I would argue that we always need to keep the formalism developed in this manuscript in mind, even for the seemingly simpler setups.
We have taken the remark of the referee into account and modified the text accordingly: “They are therefore not sufficient to generally model EELS experiments in the TEM and represent certain limiting cases where the above effects may be neglected”.
- p7: "In other words, non-zero out of diagonal terms entail electron interferences in the image plane". Well, this depends on which plane you are looking at and in which plane the density matrix was given. E.g. if the image plane would be in r-space, the intensity would only depend on the diagonal (assuming no lens effects etc.).
The referee is correct. We changed the pertaining phrase to: “In other words, non-zero off-diagonal terms entail electron interferences in the particular plane considered (which is defined by $z$ coordinate along the optical axis).”
- p7: "Upon comparision"...should be "comparison"
- p9: "Thanks to the Schwarz's inequality...", no need for the "'s"
- p9: "For the sake of clearness", could be "for the sake of clarity"
Points 12, 13 and 14 have been addressed and modified as the reviewer suggested.
p11: Around e.q. 54, the temperature is assumed zero. I wonder if the equations are linear whether the effect of the ignored temperature can later be added as an additive effect on top of the beam driven effect described here? Finite temperature effects can be included in the linear response theory through the use of e.g. Matsubara Green functions. Thus, such effects can be added to our theory a posteriori through a simple re-definition of the propagators (e.g. the MDFF).
p15: "at it generalize the Kubo approach...", should be "generalises"
- p15: after caption on concluding remarks "one usually calculate the Green dyadic" should be "calculates"
- p16: after eq. 105 "This term no encompass elastic...", should be "encompasses"
- p18: after eq. 119 "for a set of Gaussian random variable", should be "variables"
- p18: above eq. 123 "simulataneous" should be "simultaneous"
- p22: after caption VII, "We will therefore make furthers approximations", should be "further"
- p23: after eq. 169: "one respectively obtain equations (10)...", should be "obtains"
Points 16 to 22 have been addressed and modified as the reviewer suggested.
Submission & Refereeing History
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Reports on this Submission
Anonymous Report 2 on 2020-12-9 Invited Report
- Cite as: Anonymous, Report on arXiv:2007.02773v3, delivered 2020-12-09, doi: 10.21468/SciPost.Report.2272
1. conceptual clarity,
2. manuscript complete and self-contained
3. presents unified theory for EELS
4. connects directly to experimental method
The authors present a unified theoretical description of inelastic electron scattering as relevant for modern day electron energy electron loss experiments in transmission electron microscopes. The manuscript is of exceptional conceptual and methodological clarity. The theoretical treatment and methods are of direct relevance to experimentalists in the field.