Tag: Materials Science

Modeling the Zero-Phonon Line of Strained SnV Centers in Diamond; Including Reflections on Computational Cost and Accuracy.

Authors: Danny E.P. Vanpoucke
Journal: Diam. Relat. Mater. 165, 113669 (2026)
doi: 10.1016/j.diamond.2026.113669  (SI: 10.1016/j.diamond.2026.113735)
IF(2024): 5.1
export: bibtex
pdf: <DiamRelatMater> <DRM-corrigendum: SI> <ArXiv (main+SI)>

 

Modeling SnV color centers under strain.
Graphical Abstract:  The SnV color center is modelled using first principle calculations to predict the zero-phonon-lines in diamond under hydrostatic strain.

Abstract

Among the group-IV vacancy color centers in diamond, the SnV holds promise for photonics based quantum applications. In this work, the Tin-Vacancy (SnV) zero-phonon line (ZPL) and its pressure coefficient are calculated using first principles approaches. The predicted absolute ZPL position is shown to be strongly influenced by the method and supercell size used. The results are therefore extrapolated to the dilute limit allowing for direct comparison with experiments. The importance of identifying the color-center related Kohn–Sham states is highlighted, as well as the shifting of these states due to electron excitations as well as supercell size and k-point position. In contrast to the absolute ZPL positions, the relative position of the SnV0 ZPL is consistently redshifted about 43 nm compared to the SnV ZPL. In addition, the pressure coefficient is shown to be very robust over different methods, always resulting in a value of about 1.4 nm/GPa, for both SnV0 and SnV. Finally, the computational accuracy and cost are put into perspective.

Permanent link to this article: https://dannyvanpoucke.be/2026-paper_snvcolorcenter/

Special Issue: (R)Evolutions in the Integration of Artificial Intelligence and Machine Learning in Carbon-Based Materials Research

In light of the ever growing interest in AI and ML within the context of materials research, I’m guest editing a special issue together with Konstantin Klyukin from Auburn University. More information can be found on the flyer below.

(And yes the robot and diamond are AI generated, though it took some effort to get it to have the right number or arms, hold a diamond and look sideways at the same time. 😉

 

 

Permanent link to this article: https://dannyvanpoucke.be/special-issue-revolutions-in-the-integration-of-artificial-intelligence-and-machine-learning-in-carbon-based-materials-research/

MSc Materiomics defences & new QuATOMs members

MSc Thesis presentation of Brent Motmans and Eleonora Thomas (master materiomics students 2025). Both presenting applications of ML in materials research.

MSc Thesis presentation of Brent Motmans and Eleonora Thomas (master materiomics students 2025). Both presenting applications of ML in materials research: Machine Learning particle sizes using small lab-scale datasets (Brent) and development of Machine Learned Interatomic Potentials for the modelling of (the dynamics of) H-based defects in diamond.

Today we had the MSc presentations of the master Materiomics. The culmination of two year of hard study and intens research activities resulting in a final master thesis paper. This year the QuATOMs group hosted two MSc students: Brent Motmans and Eleonora Thomas. Brent Motmans performed his research in a collaboration between the QuATOMs and DESINe groups, and investigated the application of small data machine learning for the prediction of the particle size of Cu nanoparticles. His study shows that even with a dataset of less than 20 samples a reasonable 6 feature model can be created. As in previous research, he found that standard hyperparameter tuning fails, but human intervention can resolve this issue. Eleonora Thomas on the other hand introduced Machine Learned Interatomic Potentials (MLIPs) into the group. By investigating different in literature available MLIPs, she pinpointed strengths and weaknesses of the different models, as well as the technical needs for persuing such research further in our group. As collatoral, she was able to generate a model for H diffusion in diamond, with an MAE for the total energy of <10meV/atom, competing with models like google deep-mind’s GNoME.

While working on their MSc thesis, Brent and Eleonora also applied for fellowship funding for a PhD position, and we are happy to announce both Brent and Eleonora won their grant, and will be starting in the QuATOMs group as new PhD students comming academic year. Eleonora Thomas will be working on the modelling of Lignin solvation, while Brent will work in a collaboration with  the HyMAD group on the modeling of hybrid perovskites.

Permanent link to this article: https://dannyvanpoucke.be/msc-materiomics-defences-new-quatoms-members/

Cover Nature Reviews Physics

Authors: Emanuele Bosoni, Louis Beal, Marnik Bercx, Peter Blaha, Stefan Blügel, Jens Bröder, Martin Callsen, Stefaan Cottenier, Augustin Degomme, Vladimir Dikan, Kristjan Eimre, Espen Flage-Larsen, Marco Fornari, Alberto Garcia, Luigi Genovese, Matteo Giantomassi, Sebastiaan P. Huber, Henning Janssen, Georg Kastlunger, Matthias Krack, Georg Kresse, Thomas D. Kühne, Kurt Lejaeghere, Georg K. H. Madsen, Martijn Marsman, Nicola Marzari, Gregor Michalicek, Hossein Mirhosseini, Tiziano M. A. Müller, Guido Petretto, Chris J. Pickard, Samuel Poncé, Gian-Marco Rignanese, Oleg Rubel, Thomas Ruh, Michael Sluydts, Danny E.P. Vanpoucke, Sudarshan Vijay, Michael Wolloch, Daniel Wortmann, Aliaksandr V. Yakutovich, Jusong Yu, Austin Zadoks, Bonan Zhu, and Giovanni Pizzi
Journal: Nature Reviews Physics 6(1), (2024)
doi: web only
IF(2021): 36.273
export: NA
pdf: <NatRevPhys>

Abstract

The cover of this issue shows an artistic representation of the equations of state of the periodic table elements, calculated using two all-electron codes in each of the 10 crystal structure configurations shown on the table. The cover image is based on the Perspective Article How to verify the precision of density-functional-theory implementations via reproducible and universal workflows by E. Bosoni et al., https://doi.org/10.1038/s42254-023-00655-3.  (The related paper can be found here.)

Cover Nature Reviews Physics: Accuracy of DFT modeling in solids

 

Permanent link to this article: https://dannyvanpoucke.be/paper2024_accuracycover-en/

Materiomics Chronicles: week 2

After the more gentle introductions last week during the first lectures at UHasselt, this week we dove into the deep end.

For the students of the second bachelor chemistry  the course introduction to quantum chemistry dove into the postulates of quantum chemistry. They learned about the wave-function and operators, had their first contact with the mystics notation of quantum chemistry: the bra-ket notation. For the third bachelor chemistry, the course quantum and computational chemistry was centered around perturbation theory. In addition to the theory, we applied the method to the simple system of the infinite square potential.

The electron density in the primitive diamond unit cell.

In the master materiomics the course fundamentals of materials modeling was kicked into high gear, not only did the students learn the theory behind quantum mechanical modelling, they also had their fist experience on the supercomputers of the VSC. So in addition to the road from the standard Schrödinger equation to the Hohenberg-Kohn-Sham equations of DFT, they also traveled their first steps along the road from their somewhat familiar windows OS to the bash command-line environment of the HPC unix system.

Finally, as the course introduction into quantum chemistry is part of the preparatory program of the master materiomics, I started creating the narrated versions of those lectures as well (2h worth recording, corresponding to 4h of live lectures). As the available time is limited, we are going for single shot recordings which makes things exciting in that department as well.

At the end of this week, we have added another 7h of live lectures and 2h of video lectures, putting our semester total at 19h of lectures. Upwards and onward to week 3.

Permanent link to this article: https://dannyvanpoucke.be/materiomics-chronicles-week-2/

Materiomics Chronicles: week 1

The first week of the academic year at UHasselt has come to an end, while colleagues at UGent and KULeuven are still preparing for the start of their academic year next week. Good luck to all of you.

This week started full throttle for me, with classes for each of my six courses. After introductions in classes with new students (for me) in the second bachelor chemistry and first master materiomics, and a general overview in the different courses, we quickly dove into the subject at hand.

The second bachelor students (introduction to quantum chemistry) got a soft introduction into (some of) the historical events leading up to the birth of quantum mechanics such as the black body radiation, the atomic model and the nature of light. They encountered the duck-rabbit of particle-wave duality and awakened their basic math skills with the standing wave problem. For the third bachelor students, the course on quantum and computational chemistry started with a quick recap of the course introduction to quantum mechanics, making sure they are all again up to speed with concepts like braket-notation and commutator relations.

For the master materiomics it was also a busy week. We kicked of the 1st Ma course Fundamentals of materials modeling, which starts of calm and easy with a general picture of the role of computational research as third research paradigm. We discussed in which fields computational research can be found (flabbergasting students with an example in Theology: a collaboration between Sylvia Wenmackers & Helen De Cruz),  approximation vs idealization, examples of materials research at different scales, etc. As a homework assignment the students were introduced into the world of algorithms through the lecture of Hannah Fry (Should computers run the world). For the  2nd Ma, the courses on Density Functional Theory and Machine learning and artificial intelligence in modern materials science both started. The lecture of the former focused on the nuclear wave function and how we (don’t) deal with it in DFT, but still succeed in optimizing structures. During the lecture on AI we dove into the topics of regularization and learning curves, and extended on different types of ensemble models.

At the end of week 1, this brings me to a total of 12h of lectures. Upwards and onward to week 2.

Permanent link to this article: https://dannyvanpoucke.be/materiomics-chronicles-week-1/

Practical Machine-Learning for the Materials Scientist

Scilight graphic

Individual model realizations may not perform that well, but the average model realization always performs very well.

Machine-Learning  is up and trending. You can’t open a paper, magazine or website without someone trying to convince you their new AI-improved app/service will radically change your life. It will make the production of your company more efficient and cheaper, make costumers flock to your shop and possibly cure cancer on the side. Also in science, a lot of impressive claims are being made. General promises entail that it makes the research of interest faster, better, more efficient,… There is, however, a bit of fine print which is never explicitly mentioned: you need a LOT of data. This data is used to teach your Machine-Learning algorithm whatever it is intended to learn.

In some cases, you can get lucky, and this data is already available while in other, you still need to create it yourself. In case of computational materials science this often means performing millions upon millions of calculations to create a data set on which to train the Machine-Learning algorithm.[1] The resulting Machine-Learning model may be a thousand times faster in direct comparison, but only if you ignore the compute-time deficit you start from.

In materials science, this is not only a problem for those performing first principles modeling, but also for experimental researchers. When designing a new material, you generally do not have the resources to generate thousands or millions of samples while varying the parameters involved. Quite often you are happy if you can create even a few dozen samples. So, can this research still benefit from Machine-Learning if only very small data sets are available?

In my recent work on materials design using Machine-Learning combined with small data sets, I discuss the limitations of small data sets in the context of Machine-Learning and present a natural approach for obtaining the best possible model.[2] [3]

The Good, the Bad and the Average.

(a) Simplified representation of modeling small data sets. (b) Data set size dependence of the distribution of model coefficients. (c) Evolution of model-coefficients with data set size. (d) correlation between model coefficient value and model quality.

In Machine-Learning a data set is generally split in two parts. One part to train the model, and a second part to test the quality of the model. One of the underlying assumptions to this approach is that each subset of the data set provides an accurate representation of the “true” data/model. As a result, taking a different subset to train your data should give rise to “the same model” (ignoring small numerical fluctuations). Although this is generally true for large (and huge) data sets, for  small data sets this is seldomly the case (cf. figure (a) on the side). There, the individual data points considered will have a significant impact on the final model, and different subsets give rise to very different models. Luckily the coefficients of these models still present a peaked distribution. (cf. figure (b)).

On the down side, however, if one isn’t careful in preprocessing the data set correctly, these distributions will not converge upon increasing the data set size, giving rise to erratic model behaviour.[2]

Not only the model coefficients give rise to a distribution, the same is true for the model quality. Using the same data set, but making a different split between training and test data can give rise to large differences in  quality for the model instances. Interestingly, the model quality presents a strong correlation with the model coefficients, with the best quality model instances being closer to the “true” model instance. This gives rise to a simple approach: just take many train-test splittings, and select the best model. There are quite some problems with such an approach, which are discussed in the manuscript [2]. The most important one being the fact that the quality measure on a very small data set is very volatile itself. Another is the question of how many such splittings should be considered? Should it be an exhaustive search, or are any 10 random splits good enough (obviously not)? These problems are alleviated by the nice observation that “the average” model shows not the average quality or the average model coefficients, but instead it presents the quality of the best model (as well as the best model coefficients). (cf. figure (c) and (d))

This behaviour is caused by the fact that the best model instances have model coefficients which are also the average of the coefficient distributions. This observation hold for simple and complex model classes making it widely applicable. Furthermore, for model classes for which it is possible to define a single average model instance, it gives access to a very efficient predictive model as it only requires to store model coefficients for a single instance, and predictions only require a single evaluation. For models where this is not the case one can still make use of an ensemble average to benefit from the superior model quality, but at a higher computational cost. 

References and footnotes

[1] For example, take “ANI-1: an extensible neural network potential with DFT accuracy at force field computational cost“, one of the most downloaded papers of the journal of Chemical Science. The data set the authors generated to train their neural network required them to optimize 58.000 molecules using DFT calculations. Furthermore, for these molecules a total of about 17.200.000 single-point energies were calculated (again at the DFT level). I leave it to the reader to estimate the amount of calculation time this requires.

[2] “Small Data Materials Design with Machine Learning: When the Average Model Knows Best“, Danny E. P. Vanpoucke, Onno S. J. van Knippenberg, Ko Hermans, Katrien V. Bernaerts, and Siamak Mehrkanoon, J. Appl. Phys. 128, 054901  (2020)

[3] “When the average model knows best“, Savannah Mandel, AIP SciLight 7 August (2020)

Permanent link to this article: https://dannyvanpoucke.be/practical-machine-learning/

Universiteit Van Vlaanderen: Will we be able to design new materials using our smartphone in the future?

Yesterday, I had the pleasure of giving a lecture for the Universiteit van Vlaanderen, a science communication platform where Flemish academics are asked to answer “a question related to their research“. This question is aimed to be highly clickable and very much simplified. The lecture on the other hand is aimed at a general lay public.

I build my lecture around the topic of materials simulations at the atomic scale. This task ended up being rather challenging, as my computational research has very little direct overlap with the everyday life of the average person. I deal with supercomputers (which these days tend to be bench-marked in terms of smartphone power) and the quantum mechanical simulation of materials at the atomic scale, two other topics which may ring a bell…but only as abstract topics people may have heard of.

Therefor, I crafted a story taking people on a fast ride down the rabbit hole of my work. Starting from the almost divine power of the computational materials scientist over his theoretical sample, over the reality of nano-scale materials in our day-to-day lives, past the relative size of atoms and through the game nature of simulations and the salvation of computational research by grace of Moore’s Law…to the conclusion that in 25 years, we may be designing the next generation of CPU materials on our smartphone instead of a TIER-1 supercomputer. …did I say we went down the rabbit hole?

The television experience itself was very exhilarating for me. Although my actual lecture took only 15 minutes, the entire event took almost a full day. Starting with preparations and a trial run in the afternoon (for me and my 4 colleagues) followed by make-up (to make me look pretty on television 🙂 … or just to reduce my reflectance). In the evening we had a group diner meeting the people who would be in charge of the technical aspects and entertainment of the public. And then it was 19h30. Tensions started to grow. The public entered the studio, and the show was ready to start. Before each lecture, there was a short interview to test sound and light, and introduce us to the public. As the middle presenter, I had the comfortable position not to be the first, so I could get an idea of how things went for my colleagues, and not to be the last, which can really be destructive on your nerves.

At 21h00, I was up…

and down the rabbit hole we went. 

 

 

Full periodic table, with all elements presented with their relative size (if known)

Full periodic table, with all elements presented with their relative size (if known) created for the Universiteit van Vlaanderen lecture.

 

Permanent link to this article: https://dannyvanpoucke.be/universiteit-van-vlaanderen-en/

Newsflash: Materials of the Future

This summer, I had the pleasure of being interviewed by Kim Verhaeghe, a journalist of the EOS magazine, on the topic of “materials of the future“. Materials which are currently being investigated in the lab and which in the near or distant future may have an enormous impact on our lives. While brushing up on my materials (since materials with length scales of importance beyond 1 nm are generally outside my world of accessibility), I discovered that to cover this field you would need at least an entire book just to list the “materials of the future”. Many materials deserve to be called materials of the future, because of their potential. Also depending on your background other materials may get your primary attention.

In the resulting article, Kim Verhaeghe succeeded in presenting a nice selection, and I am very happy I could contribute to the story. Introducing “the computational materials scientist” making use of supercomputers such as BrENIAC, but also new materials such as Metal-Organic Frameworks (MOF) and shedding some light on “old” materials such as diamond, graphene and carbon nanotubes.

Permanent link to this article: https://dannyvanpoucke.be/newsflash-materials-of-the-future/

Linker Functionalization in MIL-47(V)-R Metal–Organic Frameworks: Understanding the Electronic Structure

Authors: Danny E. P. Vanpoucke
Journal: J. Phys. Chem. C 121(14), 8014-8022 (2017)
doi: 10.1021/acs.jpcc.7b01491
IF(2017): 4.484
export: bibtex
pdf: <J.Phys.Chem.C>
Graphical Abstract: Evolution of the electronic band structure of MIL-47(V) upon OH-functionalization of the BDC linker.
Graphical Abstract: Evolution of the electronic band structure of MIL-47(V) upon OH-functionalization of the BDC linker. The π-orbital of the BDC linker splits upon functionalisation, and the split-off π-band moves up into the band gap, effectively reducing the latter.

Abstract

Metal–organic frameworks (MOFs) have gained much interest due to their intrinsic tunable nature. In this work, we study how linker functionalization modifies the electronic structure of the host MOF, more specifically, the MIL-47(V)-R (R = −F, −Cl, −Br, −OH, −CH3, −CF3, and −OCH3). It is shown that the presence of a functional group leads to a splitting of the π orbital on the linker. Moreover, the upward shift of the split-off π-band correlates well with the electron-withdrawing/donating nature of the functional groups. For halide functional groups the presence of lone-pair back-donation is corroborated by calculated Hirshfeld-I charges. In the case of the ferromagnetic configuration of the host MIL-47(V+IV) material a half-metal to insulator transition is noted for the −Br, −OCH3, and −OH functional groups, while for the antiferromagnetic configuration only the hydroxy group results in an effective reduction of the band gap.

Permanent link to this article: https://dannyvanpoucke.be/mof-mil47-linkerfunct-en/