At t = 0 the hydrogen atom is in the superposition state Ξ¨(πβ, 0) =1β3π100 + π΄π210 where A is a real positive constant. Find A by normalization
Given wave function is
"\\psi(r,0) = \\frac{1}{\\sqrt {3}} \\psi _{100}+ A \\psi_{210}"
According to Normalization condition,
"\\int |\\psi(r,0)|^2 dr=1"
"\\int |\\frac{1}{\\sqrt {3}} \\psi _{100}+ A \\psi_{210}|^2 dr=1"
"\\frac{1}{3}\\int |\\psi _{100}|^2 dr + A^2 \\int |\\psi _{210}|^2 dr=1"
"\\frac{1}{3}+A^2=1"
Since "\\int |\\psi _{100}|^2 dr =1 and" "\\int |\\psi _{210}|^2 dr=1"
On simplifying above equation, we get
"A=\\sqrt\\frac{2}{3}"
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