Step 1: Write down the general form of the time-dependent Schrodinger equation.
\[
i\hbar \frac{\partial \Psi(\mathbf{r}, t)}{\partial t} = \left[ -\frac{\hbar^2}{2m}\nabla^2 + V(\mathbf{r}, t) \right] \Psi(\mathbf{r}, t)
\]
where \(\Psi\) is the wave function.
Step 2: Analyze the properties of the equation.
- **Linearity:** The equation is linear because the wave function \(\Psi\) and its derivatives appear only to the first power. There are no terms like \(\Psi^2\) or \(\Psi \frac{\partial \Psi}{\partial t}\). This means that if \(\Psi_1\) and \(\Psi_2\) are solutions, then any linear combination \(c_1\Psi_1 + c_2\Psi_2\) is also a solution. This is the principle of superposition.
- **Order in time:** The equation contains a first derivative with respect to time, \(\frac{\partial}{\partial t}\). It is first-order in time.
- **Order in space:** The equation contains the Laplacian operator, \(\nabla^2 = \frac{\partial^2}{\partial x^2} + \frac{\partial^2}{\partial y^2} + \frac{\partial^2}{\partial z^2}\), which involves second derivatives with respect to spatial coordinates. It is second-order in space.
Step 3: Evaluate the given options.
1. non-linear differential equation: Incorrect.
2. linear differential equation: Correct.
3. second order equation in time: Incorrect. It is first-order in time.
4. first order equation in space: Incorrect. It is second-order in space.