Deriving The Feynman Path Integral Part 2

preview_player
Показать описание
Today I finish the derivation of the Feynman path integral for quantum mechanics.

Like my hat? Get it at:

Derivation Part 1:

Baker Cambell Hausdorff derivation:

BCH properties and Justifying Neglected Terms:

Info on probability measures:

An axiomatic approach to the euclidian path integral:

Other nice discussions on the measure:

Рекомендации по теме
Комментарии
Автор

Me: *just finished freshmen year of high school*
Me:*watches video*
Me: Why is he writing in minecraft enchantment table?

bakirhusremovic
Автор

Incredible video! You will not find physics like this so well explained any where else on the internet. Phenomenal. Keep doing what your doing, please.

seandimmock
Автор

Terrific. Have read a dozen or so derivations of the path integral, but this is by far the clearest and most step-by-step.

JoseTheWrangler
Автор

I don't even study physics but here i am

danielcheung
Автор

I barely understand this & I probably misunderstand everything I *think* I halfway-understand.

This is a great video, but also very humbling to me.

Can’t wait ‘till I get all the tools for this & suddenly understand “ohhhh, so THAT meant THAT”

blurb
Автор

Thanks. Crystal clear in your derivation. Good job! I actually find it easier to understand a complex concept through vigorous math than through some sort of qualitative analogy. As physics get more advanced it becomes harder and harder to explain difficult concepts via simple analogy.

flyyufelix
Автор

i swear to god i love you, hope my gauge theory teacher were u

Aaron-zihw
Автор

0:13 “but we’re all gonna be okay” first of all, don’t lie to me Andrew

SuperPBrady
Автор

thank you for the great video! I think I spotted a small mistake at 31:40. I think there was an extra "N" being added to the numerator when you substitute delta-tau with i-delta-t. I guess you were going to substitute delta-tau with (i T / N) and then substitute in i-delta-t.

clth
Автор

Andrew: "It's like a bajillion degrees in New Mexico"
Also Andrew: *wears a flannel*

jackhudson
Автор

Ahh good shit Andrew.
I would be so down for a video on measures or actually solving the integral for the harmonic oscilator or something.

ratman
Автор

An absolute marvel of a video duo! The path integral has ALWAYS been a mystery to me quantitatively. I had no issues conceptually, but this brought it all together. Many thanks! However, as much as I hate to say it, but also stoked that I found it, there is a mistake... Around the 32 minute mark, when you're substituting delta-t for delta-tau, it's a direct substitution. There is no N in the numerator of the Gaussian measure.

dangernuke
Автор

Amazing video!!! Absolutely loved it Andrew! Great job! It would be amazing if you could do a part-3 of this talking about different measures and also how this leads us to the partition function, correlation functions etc.

varunvenkat
Автор

Hi Andrew,


I have a question regarding the factor raised to N/2 power, you say at 25:46 that it is making the integral converge, but that seems to be making it explode since you have a growth like N^N. Great work on the video!

vladkovalchuk
Автор

Very good job Andrew! I started to read path integral on Altand's QFT textbook. Didn't make sense, so I came here. Now I can read it properly this time.

dikshantdulal
Автор

I've been waiting for this for so long, 38 mins of Feynman. :)

joshuapasa
Автор

So what career can I do to avoid this completely

IonKattTMCE
Автор

Idk why I’m here. Just had my tonsil removed and this was somewhat entertaining 😄

michaelmyers
Автор

Thank you very much ! Great demonstration ; it makes me remember with happiness about my studies in physics !

clem
Автор

Damn man. Couldn't understand Path Integrals but this video saved me. This made my day, my week, my month. 🔥

mihirsingh