Prove that the kinetic energy operator is a Hermitian Operator

preview_player
Показать описание
Quantum Chemistry Lecture 1:

What is Quantum Mechanics? Why classical mechanics failed? Applications of Quantum Mechanics

Quantum Chemistry Lecture 2:

Difference between Quantum Mechanics and Classical Mechanics

Quantum Chemistry Lecture 3:

Heisenberg Uncertainty Principle

Quantum Chemistry Lecture 4:

De Broglie Hypothesis | Wave and Particle nature of matter

Quantum Chemistry Lecture 5:

Applications and Significance of Schrodinger Wave Equation

Quantum Chemistry Lecture 6:

What is wave Function? What does it tell us? Born interpretation of wave Function | Probability of finding a particle

Quantum Chemistry Lecture 7:

Eigen Functions and Eigen values along with Examples

Quantum Chemistry Lecture 8:

What is *Normalization* of wave function? *Why* the wave function should be normalized? *Significance* of Normalization

*Numerical Problems* on Normalization of wave function

Quantum Chemistry Lecture 9:

*Orthogonality* of wave function and *orthonormal* wave function with *Numerical Problems*

Quantum Chemistry Lecture 10:

What are operators in Quantum Mechanics and How to use them?

Quantum Chemistry Lecture 11:

Algebra of Operators in Quantum Mechanics | Properties | Addition subtraction and Multiplication

Quantum Chemistry Lecture 12:

Commutative and Non Commutative Operators with solved Problems

Quantum Chemistry Lecture 13:

Rules for writing an operator

Quantum Chemistry Lecture 14:

Hermitian Operator in Quantum Mechanics

Quantum Chemistry Lecture 15:

Properties of Hermitian Operator

Quantum Chemistry Lecture 16:

Second Property:

*Eigen Functions of Hermitian Operator corresponding to different Eigen Values are orthogonal*

Quantum Chemistry Lecture 17:

Prove that the operator for linear momentum is Hermitian

Quantum Chemistry Lecture 18:

Prove that the kinetic Energy operator is Hermitian Operator

Quantum Chemistry Lecture 19:

if two operators are Hermitian then their product is also Hermitian if they commute

Quantum Chemistry Lecture 20:

Postulates of Quantum Mechanics

Quantum Chemistry Lecture 21:

Time independent Schrodinger wave equation

Quantum Chemistry Lecture 22:

Steady state schrodinger wave equation

Quantum Chemistry Lecture 23:

Conclusion of particle in one dimensional box:

Quantum Chemistry Lecture 24:

Conclusion of particle in one dimensional box

Рекомендации по теме
Комментарии
Автор

In 11:12, why you put phi from the d(phi)/dx from the previous integral and after that you put d^2(psi*)/dx^2? Can you make a large explanation, pls?

juansalesdura
Автор

thank you! excellent explanation very detailed.

Szszsecr
Автор

Hello
How to write thr condition of hermitian operator in dirac notation ?

mohibmohib
Автор

why does the complex conjugate of Psi become zero at x=inf and -inf? 6:57
I thought we are allowed to plug in those values for x, as they often come up in related integrals

jc_bgnls
Автор

8:28
What would dv be equal to here?
Could you please explain how you got v=(d\psi*)/(dx) ?
Thank you.

BBonBon