An operator $\hat{O}$ is Hermitian if it is equal to its Hermitian conjugate (adjoint), denoted by $\hat{O}^\dagger$. Mathematically, the condition is:
$ \hat{O}^\dagger = \hat{O} $
We are given the operator $\hat{O} = c\hat{A} - d\hat{A}^\dagger$. To find when $\hat{O}$ is Hermitian, we first calculate its adjoint $\hat{O}^\dagger$. Using the properties of adjoints, specifically $( \alpha \hat{X} )^\dagger = \alpha^* \hat{X}^\dagger$ and $(\hat{X} - \hat{Y})^\dagger = \hat{X}^\dagger - \hat{Y}^\dagger$, where $\alpha^*$ is the complex conjugate of $\alpha$, we get:
$ \hat{O}^\dagger = (c\hat{A} - d\hat{A}^\dagger)^\dagger $
$ \hat{O}^\dagger = (c\hat{A})^\dagger - (d\hat{A}^\dagger)^\dagger $
$ \hat{O}^\dagger = c^* (\hat{A})^\dagger - d^* (\hat{A}^\dagger)^\dagger $
Since $(\hat{A}^\dagger)^\dagger = \hat{A}$, the expression simplifies to:
$ \hat{O}^\dagger = c^* \hat{A}^\dagger - d^* \hat{A} $
For $\hat{O}$ to be Hermitian, we must equate $\hat{O}$ and $\hat{O}^\dagger$:
$ c\hat{A} - d\hat{A}^\dagger = c^* \hat{A}^\dagger - d^* \hat{A} $
Rearranging the terms to group $\hat{A}$ and $\hat{A}^\dagger$:
$ (c + d^*) \hat{A} = (c^* + d) \hat{A}^\dagger $
Assuming $\hat{A}$ and $\hat{A}^\dagger$ are linearly independent (which is true since $\hat{A}$ is not Hermitian), the coefficients must satisfy:
$ c + d^* = 0 \quad \text{and} \quad c^* + d = 0 $
These two conditions are equivalent to:
$ c = -d^* \quad \text{and} \quad d = -c^* $
Let's check the given options using the conditions $c = -d^*$ and $d = -c^*$. The correct answer is Option A.
Only Option A satisfies both conditions required for the operator $(c\hat{A} - d\hat{A}^\dagger)$ to be Hermitian when $\hat{A}$ is not Hermitian.
The wavefunction of a particle in one dimension is given by
$\psi(x) = \begin{cases} M, & -a < x < a \\ 0, & \text{otherwise.} \end{cases}$
Here $M$ and $a$ are positive constants. If $\phi(p)$ is the corresponding momentum space wavefunction, which one of the following plots best represents $|\phi(p)|^2$ ?