An atomic state of hydrogen is represented by following wave function $$\psi \left( {r,\,\theta ,\,\phi } \right) = \frac{1}{{\sqrt 2 }}{\left( {\frac{1}{{{a_0}}}} \right)^{\frac{3}{2}}}\left( {1 - \frac{r}{{2{a_0}}}} \right){e^{\frac{{ - r}}{{2{a_0}}}}}\cos \theta $$ where, a0 is a constant. The quantum numbers of the state are
A. l = 0, m = 0, n = 1
B. l = 1, m = 1, n = 2
C. l = 1, m = 0, n = 2
D. l = 2, m = 0, n = 3
Answer: Option B
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