Schondiger wave equation, Schemes and Mind Maps of Physics

The Schrodinger equation and wave-function, which are fundamental concepts in quantum mechanics. It discusses the normalization of wave-function, superposition principle, and probability interpretation. The document also provides specific examples of wave-functions for a photon, harmonic motion, and free particle. The Schrodinger equation is derived and explained in detail. suitable for students studying quantum mechanics or related fields.

Typology: Schemes and Mind Maps

2015/2016

Available from 10/25/2022

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bg1
|
2
dx=1
3. Normalization
Ψ= Ψ
1
+Ψ
2
4. Superposition principle
5 Continuous and single valued
1. All measurable information about the particle is available.
6 It can be computed by solving the Schrodinger Equation
2. Although is a complex, is real and it gives probability
Ψ
|Ψ|
2
pf3
pf4
pf5
pf8
pf9

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2

3. Normalization dx = 1 Ψ= Ψ 1 + Ψ 4. Superposition principle 2 **5 Continuous and single valued

  1. All measurable information about the particle is available. 6 It can be computed by solving the Schrodinger Equation
  2. Although** (^) Ψ is a complex, (^) |Ψ| is real and it gives probability 2

∫|Ψ^ (^ x^ ,^ t )|

2 dx = 1 Conservation of Probability (normalization) Schrodinger Equation Wave-function^ (complex) Probability interpretation: P ( x ) dx =|Ψ ( x , t )| 2 dx What is Schrodinger equation? Atom Harmonic motion Free particle Specific Examples

H =

P

2 2 m

  • U ( x )=

2 2 m

2x 2

  • U ( x )

i ℏ

∂ Ψ ( x , t ) ∂ t

2 2 m

2 Ψ ( x , t ) ∂ x 2

  • U ( x ) Ψ ( x , t )

i ℏ

∂ Ψ ( x , t ) ∂ t = H Ψ ( x , t ) Schrodinger Equation

For a photon, wavefunction is of the wave form Ψ ( x ,t ) = A e i ( kx − ω t ) k =

But and wavelength:^ λ^ =^

h p Ψ ( x ,t ) = A e i ( px − ω t ) Therefore, k =

h p = p

[ we can also use the form (^) Ψ ( x ,t ) = A sin ( kx − ω t )]

Schrodinger Equation

i ℏ

∂ Ψ ( x , t ) ∂ t

2 2 m

2 Ψ ( x , t ) ∂ x 2

  • U ( x ) Ψ ( x , t )

i ℏ

∂ Ψ ( x , t ) ∂ t = H Ψ ( x , t )

H = −

2 2 m

2x 2

  • U ( x ) or

Time independent Schrodinger Equation i ℏ ∂ Ψ ( x , t ) ∂ t = − ℏ 2 2 m2 Ψ ( x , t ) ∂ x 2

  • U ( x ) Ψ ( x , t ) Let us assume the following solution: Ψ ( x ,t ) = ψ ( x ) ϕ ( t ) i ℏ ϕ ( t ) ∂ ϕ ( t ) ∂ t = 1

ψ ( x ) [^

− ℏ 2 2 m2 ψ( x ) ∂ x 2

  • U ( x ) ψ ( x )

]

= E