PART A:
The electrons in solids can be found
"in closely spaced energy levels that form a continuos distribution of energy with in a certain range."
PART B:
When an electron in the valance band in an insulator gains additional energy.
it can jump to
"an energy state in the conduction band only if it has gained an amount of energy at least equal to the band gap."
PART C:
When an electron in the highest energy band in a conductor gains additional energy, it can jump to
an adjacent energy state within the same band.
PART D:
The main difference between insulators and semiconductors is that
"In semiconductors, the energy gap between the valence and conduction
band is considerably smaller than in insulators."
PART E:
The energy arsociated with this wave length is
$$ \begin{aligned} &\Delta \mathrm{E}=\frac{h c}{\lambda}=\frac{\left(6.63 \times 10^{34} \mathrm{Js}\right)\left(3 \times 10^{6} \mathrm{~m} / \mathrm{s}\right)}{\left(1.37 \times 10^{-6} \mathrm{~m}\right)} \\ &\Rightarrow \Delta \mathrm{E}=14.518 \times 10^{30} \mathrm{~J} \end{aligned} $$
Converting this in \(\mathrm{eV}\), we have \(\Delta \mathrm{E}=\frac{14.518 \times 10^{.20}}{1.6 \times 10^{-8}}\)
\(\Rightarrow \Delta \mathrm{E}=0.907 \mathrm{eV}>\) the band gap of germanium \(=0.67 \mathrm{eV}\)
Hence the elecrons will jump from valance band to conduction band
Hence the answer is YES.
PART A: The electrons in solids can be found ____________in only certain discrete sharp energy states...
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