The energy density of states of an electron in a one-dimensional potential well of infinitely high walls is (the symbols have their usual meanings)
A. $$\frac{{L\sqrt m }}{{\pi \hbar \sqrt {2E} }}$$
B. $$\frac{{Lm}}{{\pi \hbar \sqrt E }}$$
C. $$\frac{{Lm}}{{\pi \hbar \sqrt {2E} }}$$
D. $$\frac{{L\sqrt m }}{{2\pi \hbar E}}$$
Answer: Option A
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