Angular momentum addition
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- Опубліковано 1 лис 2024
- The process of adding angular momentum in quantum mechanics is a rich topic, one that we can only briefly touch on, but it is an important topic that you should be aware of. Here there be Clebsch-Gordan coefficients. (This lecture is part of a series for a course based on Griffiths' Introduction to Quantum Mechanics. The Full playlist is at www.youtube.com...)
Two weeks short of being 7 years old, this video is still among the best on UA-cam to explain the horrific "Addition of Angular Momenta" paragraph in Griffiths. Brilliant.
It's 11 years old now
Adding angular momentum is one of the most difficult things I have come across in physics so far. I hate how hard it is.
@eh6794 I think I got a 2:1 in it which would be in the 60-70% range. In the UK that's considered good. Good luck with your finals!
Thank you for explaining this in a way that finally makes sense. One of the best videos ever.
Finally!, as a mathematician that is trying it's way into physics I can finally use my knowledge on freaking representation theory from my tesis hahah sorry it is just that it was really hard for me to understand those topics when I was developing my tesis but now I can use it, actually I stopped the video several times bc I was connecting the dots already and when he said exactly what I was thinking I was so happy. Haha well have fun in life and wish me luck on my master in physics bc I am going to need it :3
Brant Carlson you da MVP, I wouldn't understand any of this without watching and rewatching your videos. Thanks for sticking through with completing this lecture set!
Brant, thank you for saving my semester!
Thanks to you, I've spared 2 hours trying to study it from the books, alone. Your explanation is very clear ! Merci !
This is the greatest video on this topic I have ever seen
you're a good guy, Brant, I appreciate it a lot.
Bro how did u explain this so well, still unsure about some things but i think i understand a lot more than before the video
Class has started to go over this, This helps so much! Thank you !
What is the reason to use the lowering operator here? As far as I can tell, it does not provide any further information, since we already know the S_z Momenta. We also know the possible spin combinations. I'm confused....
What if the two particle interact with each other and the coupling constant is a non zero quantity (J). How will the J be incorporated in the addition of angular momentum?
thank you very much you just helped me a lot !
with CG coefficients i don't understand because my teachers writes when s1=1 and s2=1/2 ...... |3/2 -1/2> = sqrt (2/3) |1 0> |1/2 -1/2> + sqrt(1/3) |1 -1> |1/2 1/2>
Thank you this really helped!
Perfekt. Danke !
Thank you very much indeed.
... and they are bloody complicated, I got scared after hearing this, and when I understood, I got that complicated is an understatement :(
briliant
Can you explain me how you got the state at 7:30 ?
ua-cam.com/video/xeYysQWLXqE/v-deo.html - Check this video to understand how the fourth state is derived from orthogonality argument.
At 4:35 where is the factor of h-bar?
Very often angular momenta are given in units of h-bar -- otherwise h's would be abound.
Better than Griffiths
Thank you! now i think i understand it!
You are the best :)
Thank you
omg, very helpful :3
Thanks