Closure Property of Eigenfunctions
Closure Property of Eigenfunctions
A complete set of discrete eigenfunctions obeys the orthonormalization conditions . Complementary to these is the set of closure relations (x)()=δ(x-). For real eigenfunctions, the complex conjugate can be dropped. The finite sums (x)() for up to 100 are evaluated in this Demonstration. Four systems are considered: (1) infinite square-well potential with and eigenfunctions (x)=sin(nπx), , ; (2) linear harmonic oscillator with and (x)=n!(x), , ; (3) linear rigid rotor for fixed , , (x)=(x), , ; (4) hydrogen-like radial function with , (r), , .
∫(x)(x)dx=
*
ψ
m
ψ
n
δ
mn
∞
∑
n=0
*
ψ
n
ψ
n
x
0
x
0
N
∑
n=0
*
ψ
n
ψ
n
x
0
N
ℏ=m=a=1
ψ
n
0≤x≤1
n=1,2,3,…
ℏ=μ=ω=1
ψ
n
1
n
2
π
-/2
2
x
e
H
n
-∞<x<∞
n=0,1,2,…
ℏ=ℐ=1
Θ
ℓ
(2ℓ+1)(ℓ-)!
2(ℓ+)!
P
ℓ
-1≤x=cosθ≤1
ℓ=,+1,+2,…
ℏ=μ=e=1
R
nℓ
0≤r<∞
n=ℓ+1,ℓ+2,ℓ+3,…
For the first three cases, the sum approaches an oscillatory representation of the delta function . However, the hydrogenic functions represent only the discrete bound states. They do not constitute a complete set of eigenfunctions without including the continuum. The sums usually exhibit erratic behavior but sometimes do show a peaking, particularly for larger values of .
δ(x-)
x
0
Z
Details
Details
The closure relation can be derived by considering the expansion of an arbitrary function obeying the same analytic and boundary conditions as the eigenfunctions (x). If the set of eigenfunctions is complete, one can write , with expansion coefficients determined from =∫()f()d. Substituting the last relation into the expansion, we find , with the summation equivalent to the delta function .
f(x)
ψ
n
f(x)=(x)
∑
n
c
n
ψ
n
c
n
*
ψ
n
x
0
x
0
x
0
f(x)=∫()f()()d=∫f()()(x)d
∑
n
*
ψ
n
x
0
x
0
ψ
n
x
0
x
0
x
0
∑
n
*
ψ
n
x
0
ψ
n
x
0
δ(x-)
x
0
Reference: Any graduate-level text on quantum mechanics.
External Links
External Links
Permanent Citation
Permanent Citation
S. M. Blinder
"Closure Property of Eigenfunctions"
http://demonstrations.wolfram.com/ClosurePropertyOfEigenfunctions/
Wolfram Demonstrations Project
Published: March 7, 2011