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I was fortunate to listen to your lecture at GRC 2024; it was the last lecture of the conference, if I remember correctly. After coming back, I found your channel. All the lectures are extremely useful for anyone who is in touch with solid-state chemistry. It is like a thriller series. I hope to get more content in the future.

Hi.... I have a little queation. Why the square and rectangular lattices are not identified as non premivite one? (16.20) Kindly explain.

This is really an excellent series of video! Is there any pdf that we can download so that we can refer back in the future, your slides are excellent!

Thank you very much for this awesome lecture, it was a great help. I will surely come back and rewatch certain parts in the future.

You the goat fr

I’m touching myself to this

#enjoyingmyself

Wow so cool

Great work !!

Great video, thank you so much Pat!!

VERY VALUABLE AND USEFUL PRESENTATION

Really good study video!3q

命哈哈哈哈哈哈哈

Would love to see if start a series on crystal defects in detail

Thanks for the very explicit explanation!

Thanks for the video. Really helped with the understanding of structure factors.

命。。。

Great

Thank you, finally I see more where these come from 🙏 My teaching materials just kind of skipped the geometry lol

is there a wrong about position of the a* and b* in 11:07?

Thx ❤

Thank you for the video

Dear Professor Woodward Thank you for the inspiring lectures! The example of the F atom chain is very beneficial to my understanding. I wonder whether you have some recommendation references on one-dimensional band structures like this. Thanks!

Could i have the articles

Please where this book

Best lecture Thanks sir!

Thank you sir for these highly structured and instructive lectures. Everything is perfect, especially the voice, and the way you present the lectures is fantastic and allows us to understand the phenomena studied from other angles. I'd like to ask you a question about lecture 12 in this first series of lectures (the lecture that precedes this lecture 13). I don't know whether you've forgotten to include it or whether there's just been a mistake in numbering. Thank you.

Even though English ist not my first language, I understood him better than my lecture in german(first language) so wow it’s very well explained👏👏

My Master's degree Tuitor..📝🤭..I will graduate in this school one day🇰🇪

Very well explained, a hundred thanks!

Thank you very much sir!

24:09 why (h^2+k^2+l^2)=(1/d^2)/0.0567 ? Can you please explain how we made that conclusion, please?

Dear Professor, I have a simple question: Kroneker's delta is defined based on the cubic lattice?

Super valuable for my PhD now. Thanks so much

Thank you! There is something I didn't really get a grasp on though. What exactly is K in the K/a and where do we find it's value?

very clear . thank you so much

thanks!

Excellent and clear explanation, thank you

Amazing content, made things clearer, thanks a lot

Good lecture

thank you sir

501th like

Thanks for ur explicit explanation! great help; a supplement about that calculation of corundum:physics.nist.gov/PhysRefData/XrayMassCoef/tab3.html; I believe the website had moved to this one, and you need another website to seach for the energy: physics.nist.gov/PhysRefData/XrayTrans/Html/search.html

Makes you really think about the power of a metallic spacecraft skin that could take advantage of Jahn Teller Effects in combinatorial with Hall effects.

Thanks a lot. One of the best lectures I have seen in RUclips❤

Thank you very much, Can you do one for graphite?

nice explanation! Could you please explain highest occupied valance band and lowest unoccupied conduction band?

Thank you for this wonderfully clear introduction! Greetings from Cape Town!

What is the value of 'V' ?

Can you please share the pdf if possible ?