MIT 8.04 Quantum Physics I, Spring 2016 View the complete course: ocw.mit.edu/8-0... Instructor: Barton Zwiebach License: Creative Commons BY-NC-SA More information at ocw.mit.edu/terms More courses at ocw.mit.edu
Пікірлер: 20
@janakmedicos97354 жыл бұрын
Effective potential. Effective range. And the barrier energy and boundaries conditions.
@jimmyb9983 жыл бұрын
An unlucky choice, that m is both the mass (in terms like -h/^2/2m ) and the azimuthal quantum number (in Y_{ml});...
@janakmedicos97354 жыл бұрын
Effective potential.
@not_amanullah2 ай бұрын
Thanks ❤️🤍
@janakmedicos97354 жыл бұрын
Boundary value problems. Boundary conditions and effective range .
@ronandominick2213 жыл бұрын
I realize I'm kinda off topic but does anyone know of a good site to watch newly released series online?
@ericzion20253 жыл бұрын
@Xzavier Roman yup, been watching on flixzone for since march myself :D
@ronandominick2213 жыл бұрын
@Xzavier Roman thank you, I signed up and it seems like a nice service =) I appreciate it!
@xzavierroman39493 жыл бұрын
@Ronan Dominick glad I could help xD
@not_amanullah2 ай бұрын
This is helpful ❤️🤍
@xinzhang3017 Жыл бұрын
wow, 13k views at the end of the series
@zphuo6 жыл бұрын
@12:00, why right side of equation the Eu(r) = 0?
@fabriziotabasso16946 жыл бұрын
ZiPan Huo vi I guess that since U(r) was defined as U(r) = r Re(r) if r-->0 then U(r) also goes to zero
@prasadpawar70274 жыл бұрын
Because compared to centrifugal term RHS is puny as r--->0.
@jiaqigan63984 жыл бұрын
Imagine when r goes to zero, the effective potential goes to infinite large, then we can view it as a rigid boundary wall, which means that the wave function have to satisfy the boundary condition. Since this is a wave function in 3D and centered at r=0, then u(0) must be 0.
@wondererasl4 жыл бұрын
@5:35 How come d^3 x = r^2 dr d omega
@yyc34914 жыл бұрын
in the polar coordinate system, dV = rsinθdφ · rdθ · dr = r^2 dr sinθ dθ dφ.