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Quantum Mechanics: Deviation, Time-Independent Equation, and Energy Bands, Slides of Computer Science

Various topics in quantum mechanics, including standard deviation in position and momentum, the time-independent schrodinger equation, and the energy bands formation in a periodic potential. It also discusses the properties of stationary states, the infinite square well, and the harmonic oscillator. Additionally, it touches upon the delta-function potential and free particle.

Typology: Slides

2012/2013

Uploaded on 03/21/2013

dharmendrae
dharmendrae 🇮🇳

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Schrödinger Equation
1. Wave Equation
2. Time Independent Schrodinger Equation
3. Transfer Matrix Approach and the
PCPBT Tool
4. Periodic Potentials and the Periodic
Potentials Tool
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Download Quantum Mechanics: Deviation, Time-Independent Equation, and Energy Bands and more Slides Computer Science in PDF only on Docsity!

Schrödinger Equation

1. Wave Equation

2. Time Independent Schrodinger Equation

3. Transfer Matrix Approach and the

PCPBT Tool

4. Periodic Potentials and the Periodic

Potentials Tool

Statistical interpretation

Born’s statistical interpretation : { probability of finding the particle between x and ( x + dx ) at time t }

Probability

is probability density

 x t dx

  ^

2 The probability of infinite interval : ( , ) Docsity.com

Operator and expectation value (average / mean)

expectation value of position x :

expectation value of momentum :

x  x x t dx  x dx

 

  (^)      ( , )^2 *

operator x represent position;

operator represent momentum in x -direction. ■ all physics quantities can be written in terms of position and momentum

Heisenberg uncertainty principle

(proof ref. chap 3)

standard deviation the variance of distribution, where individual physics quantity

2 2

2 2

2 2

2 2 2

2

( 2 )

( ) ( )

j j

j j j j

j j j j

j j j

 

  

  

    

2. The Time Independent

Schrodinger Equation

2.1 Stationary state

Assume V is independent of t , use separation of variables

Deduce from equation (2.1) , then

time-independent Schrödinger equation

thus equation (2.2)

(iii) Linear combination of separable solution

2.2 Infinite square well( one dimensional box)

and boundary conditions:

normalize

■ first three states and probability density of infinite square well

solve equation (2.3) by use ladder operator

rewrite equation (2.3) by ladder operator :

compare equation(2.3)

similarly

discussion (i)

and

(iii) there must exist a min state with

and from

and

so the ladder of stationary states can illustrate :