Step 1: Understanding the Physical Concept
In a p-type semiconductor, the acceptor level lies just above the valence band. When light shines on the material, photons can excite electrons from the valence band into the acceptor level, effectively leaving behind holes (which are positive charge carriers in semiconductors). To do this, the photon must have **at least** the energy equal to the gap between the valence band and the acceptor level.
Step 2: Given Data
From the question:
The energy required to excite an electron (and hence create a hole) is \( E = 6 \, \text{eV} \).
The constant\(hc = 1242 \, {eV·nm}\)This is the product of Planck's constant and the speed of light, converted to units that make calculating wavelength straightforward when energy is in eV and wavelength is in nm.
Step 3: Formula Used
We use the energy-wavelength relation of photons: \[ E = \frac{hc}{\lambda} \] Solving for wavelength \( \lambda \), we get: \[ \lambda = \frac{hc}{E} \]
Step 4: Substituting the Values
Now substitute the given values into the formula:
Step 5: Interpreting the Result
The calculated wavelength of 207 nm represents the maximum wavelength of light that still has enough energy to create a hole in the p-type semiconductor. Any wavelength longer than this (i.e., lower energy) won't have enough energy to excite the electron and thus cannot generate a hole.
Step 6: Final Answer
\[ \boxed{\lambda = 207 \, \text{nm}} \] Therefore, the correct answer is: Option 3: 207 nm.
Step 1: Understanding the Physical Concept
In a p-type semiconductor, the acceptor level lies just above the valence band. When light shines on the material, photons can excite electrons from the valence band into the acceptor level, effectively leaving behind holes (which are positive charge carriers in semiconductors). To do this, the photon must have **at least** the energy equal to the gap between the valence band and the acceptor level.
Step 2: Given Data
From the question:
The energy required to excite an electron (and hence create a hole) is \( E = 6 \, \text{eV} \).
The constant\(hc = 1242 \, {eV·nm}\)This is the product of Planck's constant and the speed of light, converted to units that make calculating wavelength straightforward when energy is in eV and wavelength is in nm.
Step 3: Formula Used
We use the energy-wavelength relation of photons: \[ E = \frac{hc}{\lambda} \] Solving for wavelength \( \lambda \), we get: \[ \lambda = \frac{hc}{E} \]
Step 4: Substituting the Values
Now substitute the given values into the formula:
Step 5: Interpreting the Result
The calculated wavelength of 207 nm represents the maximum wavelength of light that still has enough energy to create a hole in the p-type semiconductor. Any wavelength longer than this (i.e., lower energy) won't have enough energy to excite the electron and thus cannot generate a hole.
Step 6: Final Answer
\[ \boxed{\lambda = 207 \, \text{nm}} \] Therefore, the correct answer is: Option 3: 207 nm.
The stopping potential (\(V_0\)) versus frequency (\(\nu\)) of a graph for the photoelectric effect in a metal is given. From the graph, the Planck's constant (\(h\)) is:

In the diagram shown below, both the strings AB and CD are made of the same material and have the same cross-section. The pulleys are light and frictionless. If the speed of the wave in string AB is \( v_1 \) and in CD is \( v_2 \), then the ratio \( \frac{v_1}{v_2} \) is:
