Step 1: Recall the property of Hermitian matrices.
A matrix \(A\) is Hermitian if \(A^{\dagger} = A\).
For two Hermitian matrices \(P\) and \(Q\), we have \(P^{\dagger} = P\) and \(Q^{\dagger} = Q\).
Step 2: Check \(PQ + QP\).
\[
(PQ + QP)^{\dagger} = Q^{\dagger} P^{\dagger} + P^{\dagger} Q^{\dagger} = QP + PQ = PQ + QP
\]
Thus, \(PQ + QP\) is Hermitian.
Step 3: Check \(i(PQ - QP)\).
\[
[i(PQ - QP)]^{\dagger} = -i(Q^{\dagger} P^{\dagger} - P^{\dagger} Q^{\dagger}) = i(PQ - QP)
\]
Hence, \(i(PQ - QP)\) is Hermitian.
Step 4: Check the remaining options.
- \(PQ\) is not necessarily Hermitian because \((PQ)^{\dagger} = QP\).
- \(PQ - QP\) is anti-Hermitian since \((PQ - QP)^{\dagger} = -(PQ - QP)\).
Step 5: Conclusion.
Hence, the correct statements are (A) and (B).
If the system of equations: $$ \begin{aligned} 3x + y + \beta z &= 3 \\2x + \alpha y + z &= 2 \\x + 2y + z &= 4 \end{aligned} $$ has infinitely many solutions, then the value of \( 22\beta - 9\alpha \) is:

At a particular temperature T, Planck's energy density of black body radiation in terms of frequency is \(\rho_T(\nu) = 8 \times 10^{-18} \text{ J/m}^3 \text{ Hz}^{-1}\) at \(\nu = 3 \times 10^{14}\) Hz. Then Planck's energy density \(\rho_T(\lambda)\) at the corresponding wavelength (\(\lambda\)) has the value \rule{1cm}{0.15mm} \(\times 10^2 \text{ J/m}^4\). (in integer)
[Speed of light \(c = 3 \times 10^8\) m/s]
(Note: The unit for \(\rho_T(\nu)\) in the original problem was given as J/m³, which is dimensionally incorrect for a spectral density. The correct unit J/(m³·Hz) or J·s/m³ is used here for the solution.)