Quantum Mechanics (8hrs) · Engineering Physics

Wave function and its characteristics

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Wave function and its characteristics

1. What the Wave Function Is

Wave function ψ(r,t)ψ(r,t) (complex) is the state description in quantum mechanics: it encodes everything knowable about a particle. Born's interpretation (1926):

∣ψ(r,t)∣2=probabilitydensity(probabilityperunitvolumetofindparticlenearratt)|ψ(r,t)|² = probability density (probability per unit volume to find particle near r at t)

so ∫V∣ψ∣2dV∫_{V} |ψ|² dV = probability to find particle in VV. ψψ itself has no direct physical meaning; only ∣ψ∣2 |ψ|² does.

2. Normalization and Probability

Total probability must be 1:

∫allspace∣ψ(r,t)∣2dV=1(normalized)∫_{all space} |ψ(r,t)|² dV =1 (normalized)

If ψψ not normalized, normalize:

ψnorm=ψ/√(∫∣ψ∣2dV)ψ_{norm}= ψ/√(∫|ψ|² dV)
  • Expectation value:
⟨A⟩=∫ψ∗A^ψdV⟨A⟩ = ∫ ψ* \hat{A} ψ dV

where A^\hat{A} is operator (e.g., xx, p=−iħ∇p=-iħ∇).

  • ψψ must be single-valued (one value per point).

3. Characteristics / Conditions for a Physically Acceptable ψψ

Condition Why
Finite everywhere (not ±∞) probability cannot be infinite
Single-valued one probability per point
Continuous (ψψ itself) else dψ/dxdψ/dx ambiguous
Continuous derivative dψ/dxdψ/dx (except where VV→∞) ensures pp expectation finite; at infinite wall, derivative may jump but ψψ continuous and zero
Square-integrable / normalizable ∫∣ψ∣2finite∫|ψ|² finite so can normalize to 1

These are boundary conditions that quantize energy (particle in box).

4. Superposition

If ψ1,ψ2ψ_1, ψ_2 are allowed states, then

ψ=c1ψ1+c2ψ2ψ = c_1 ψ_1 + c_2 ψ_2

is also allowed (linear Schrödinger equation) — leading to interference.

5. Worked Examples

(a) ψ = A e^{-x²/2a²} (Gaussian) normalizable: |A|² ∫ e^{-x²/a²}dx =|A|² a√π=1 ⇒ A= (a√π)^{-1/2} ✓

(b) ψ = A sin(nπx/L) for 0<x<L, zero outside: continuous at  x=0,L? ψ=0 at edges ⇒ continuous ✓

(c) ψ = x (not square-integrable over all space ⇒ not physical for free particle, but okay on finite box with normalization)

(d) Need to check: ψ = e^{ikx} not normalizable over infinite space but okay as plane wave (delta normalization) for free particle.

(e) Probability to find particle between a and b: P= ∫_{a}^{b} |ψ|² dx

6. Exam Points

  • State Born interpretation ∣ψ∣2 |ψ|² as probability density — 3-5 marks, very frequent.
  • Normalization ∫∣ψ∣2=1∫|ψ|²=1 — 3 marks, frequent.
  • List characteristics (finite, single-valued, continuous, normalizable) — 5 marks, very frequent.
  • Distinguish ψψ vs ∣ψ∣2|ψ|² — 3 marks.
  • Compute normalization constant AA for given ψψ — 5-7 marks, very frequent.
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