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Question

Consider an operator $\hat{A}$ which is not Hermitian. Find the possible values of $c$ and $d$ such that the operator $(c\hat{A} - d\hat{A}^\dagger)$ is Hermitian.

The correct answer is
$c = i \text{ and } d = i$

Hermitian Operator Condition Derivation

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} $

Operator Adjoint Calculation

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} $

Condition for Hermiticity

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^* $

Testing the Options

Let's check the given options using the conditions $c = -d^*$ and $d = -c^*$. The correct answer is Option A.

  • Option A: $c = i, d = i$
    • Check $c = -d^*$: $i = -(i)^* = -(-i) = i$. (True)
    • Check $d = -c^*$: $i = -(i)^* = -(-i) = i$. (True)
    Both conditions hold.
  • Option B: $c = 1, d = 1$
    • Check $c = -d^*$: $1 = -(1)^* = -1$. (False)
  • Option C: $c = -1, d = i$
    • Check $c = -d^*$: $-1 = -(i)^* = -(-i) = i$. (False)
  • Option D: $c = i, d = -i$
    • Check $c = -d^*$: $i = -(-i)^* = -(i) = -i$. (False)

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.

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Important Questions from Operators Commutators Heisenberg Picture

  1. Which of the following operators is/are self-adjoint?
  2. Consider operators $\hat{A}$, $\hat{B}$, and $\hat{C}$ for three observables of a quantum system satisfying $[\hat{A}, \hat{B}] = 0$, $[\hat{B}, \hat{C}] = 0$, and $[\hat{A}, \hat{C}] \neq 0$, with uncertainties $\Delta A, \Delta B, \Delta C$, respectively. From the options given below, which is/are implied by the commutation relations among $\hat{A}, \hat{B}$, and $\hat{C}$?
  3. Let $|m\rangle$ and $|n\rangle$ denote the energy eigenstates of a one-dimensional simple harmonic oscillator. The position and momentum operators are $\hat{X}$ and $\hat{P}$, respectively. The matrix element $\langle m|\hat{P}\hat{X}|n\rangle$ is non-zero when
  4. 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 $|\phi(p)|^2$ ?

  5. If $H$ is the Hamiltonian for a free particle with mass $m$, the commutator $[x, [x, H]]$ is
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