Properties of Hermitian operator
All the observable quantity in quantum mechanics are associated with corresponding operators. The expectation value of the quantity is always real sign value is called Hermitian operator. And here we discussed about the properties of Hermitian operator.
Summary
All the observable quantity in quantum mechanics are associated with corresponding operators. The expectation value of the quantity is always real sign value is called Hermitian operator. And here we discussed about the properties of Hermitian operator.
Things to Remember
Properties of Hermitian operator.
(1) Sum of any two like Hermitian is also Hermitian.
2) Eigen value of a Hermitian operator is always real.
3. the product of two Hermitian operator is Hermitian only if they commute.
i.e. If ˆA and ˆB are any two Hermitian operators then their product ˆAˆB is Hermitian only if [ˆA,ˆB] =0.
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Properties of Hermitian operator
Properties of Hermitian operators:
(1) Sum of any two like Hermitian is also Hermitian.
Let ˆA and ˆB be any two like Hermitian operators.
Sum of two operators, ˆC=ˆA+ˆB
We have to show that ˆC is also Hermitian
⇒ Let ψ(x) be a valid wave function.
Now,
∫∞−∞ψ∗(ˆAψ)dx=∫∞−∞(ˆAψ)∗ψdx⋯(1)
[ˆA] is Hermition.
and
∫∞−∞ψ∗(ˆBψ)dx=∫∞−∞(ˆBψ)∗ψdx⋯(2)
[ˆB] is Hermitian
Adding (1) and (2), we get,
∫∞−∞ψ∗(ˆAψ)dx+∫∞−∞ψ∗(ˆBψ)dx=∫∞−∞(ˆAψ)∗ψdx+∫∞−∞(ˆBψ)∗ψdx
or,∫∞−∞ψ∗[ˆAψ+ˆBψ]dx=∫∞−∞[(ˆAψ)∗+(ˆBψ)∗]ψdx
or,∫∞−∞[(ˆA+ˆB)ψ]dx=∫∞−∞[(ˆAψ+ˆBψ)∗]ψdx
or,∫∞−∞ψ∗(ˆcψ)dx=∫∞−∞[(ˆcψ)]∗ψdx⋯(3)
Where, ˆc=ˆA+ˆB is Hermitian.
(2) Eigen value of a Hermitian operator is always real:
⇒
Let λ be the eigen value of a Hermitian operator ˆA ove wave function ψ(x).
The eigen value equation of \(\hat A\0 is
ˆAψ(x)=λψ(x)⋯(1)
We have to show that λ is real i.e. λ∗=λ.
Taking complex conjugate of equation (1)
[ˆAψ(x)]∗=[λψ(x)]∗
or,[ˆAψ(x)]∗=λ∗ψ∗(x)⋯(2)
Multiplying equation (2) by ψ(x) from right and integrating
∫∞−∞[ˆAψ(x)]∗ψ(x)dx=λ∗∫∞−∞ψ∗(x)ψ(x)dx⋯(3)
Since, ˆA is Hermitian.
∫∞−∞ψ∗(x)[ˆAψ(x)]dx=∫∞−∞[ˆAψ(x)]∗ψ(x)dx⋯(4)
Using (4) in (3), we get,
or,∫∞−∞ψ∗(x)[ˆAψ(x)]dx=λ∗∫∞−∞ψ∗(x)ψ(x)dx
Using equation (1)
or,∫∞−∞ψ∗(x)[λψ(x)]dx=λ∗∫∞−∞ψ∗(x)ψ(x)dx
or,λ∫∞−∞ψ∗(x)ψ(x)dx=λ∗∫∞−∞ψ∗(x)ψ(x)dx
or,(λ−λ∗)∫∞−∞ψ∗(x)ψ(x)dx=0
Since, ∫∞−∞ψ∗(x)ψ(x)dx≠0
λ−λ∗=0
∴λ=λ∗
Hence, eigen value of a Hermitian operator is always real.
3. the product of two Hermitian operator is Hermitian only if they commute.
i.e. If ˆA and ˆB are any two Hermitian operators then their product ˆAˆB is Hermitian only if [ˆA,ˆB] =0.
⇒ Proof:
As ˆA is Hermitian:
∫∞−∞(ˆAψ)∗ψdx=∫∞−∞ψ∗(ˆAψ)dx⋯(1)
As ˆB is Hermitian:
∫∞−∞(ˆBψ)∗ψdx=∫∞−∞ψ∗(ˆBψ)dx⋯(2)
The product of ˆA and ˆB is ˆAˆB.
Now, ∫∞−∞[ˆAˆBψ]∗ψdx=∫∞−∞[ˆA(ˆBψ)∗ψdx
=∫∞−∞[ˆBψ]∗[ˆAψ]dx
∴ˆA is Hermitian.
=∫∞−∞ψ∗[ˆB(ˆAψ)]dx
∴ˆB is alos Hermitian.
=∫∞−∞ψ∗[ˆBˆAψ]dx
or,∫∞−∞[ˆAˆBψ]∗ψdx=∫∞−∞ψ∗[ˆAˆBψ]dxonlyifˆAˆB=ˆBˆA
→[ˆA,ˆB]=0
Hence product of the two Hermitian operator is Hermitian only if they commute.
Reference:
- Mathews, P.M and K Venkatesan. A Text Book of Quantum Mechanics. New Delhi: Tata McGraw Hill Publishing Co. Ltd, 1997.
- Merzbacher, E. Quantum Mechanics . New York: John Wiley, 1969.
- Prakash, S and S Salauja. Quantum Mechanics. Kedar Nath Ram Nath Publishing Co, 2002.
- Singh, S.P, M.K and K Singh. Quantum Mechanics. Chand & Company Ltd., 2002.
Lesson
Operator formalism in Quantum mechanics
Subject
Physics
Grade
Bachelor of Science
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