Week 9: Not What You Want, But What You Need
Aryan R -
Introduction
Dear readers,
Here is the blog post you have all been waiting for fervently! In this upcoming blog, after overcoming the arduous trial that is VCA for Sm3Ru4Sn11Ge2, I have finally produced the band structure for it.

The Really Really Technical Explanation
Notably, the Sm3Ru4Sn13 graph is less crowded than the one above, suggesting it is a better TE material than Sm3Ru4Sn11Ge2, although both are not likely thermoelectric materials. However, what the above graph suggests is that this material is potentially a good material to explore complex quantum behavior such as non-conventional superconductivity. The f-bands from the Ru seem to be heavily overlapping with the others (the crowding of the spaghetti you see above), and if they overlap with the conduction band then they could participate in hybridization with itinerant electrons, leading to strong electronic correlations.
This type of hybridization is a hallmark of heavy fermion systems, where localized f-electron states interact with conduction electrons, giving rise to emergent phenomena such as unconventional superconductivity, quantum criticality, or non-Fermi liquid behavior.In particular, if the f-bands lie near or cross the Fermi level, even partially, they can mediate Cooper pairing mechanisms that deviate from the classical BCS theory-enabling, for instance, d-wave or even more exotic pairing symmetries. The structural complexity of the skutterudite lattice further enhances this possibility by introducing subtle symmetry-breaking distortions that can lift degeneracies and tune band interactions.
Next Week!
Since this alloy seems more promising in terms of quantum behavior, the pdos analysis next week will also focus on those aspects to determine where these materials can best be implemented. I hope to see you all excited for next week! Thank you so much for reading!

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