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1. An electron in an infinite potential well (width A) is in a superposition state given by the 1 wavefunction: π(π₯) = [π1 (π₯) + π2 (π₯)]. Here π1 (π₯) is the ground state (lowest β2 energy state) and π2 (π₯) is the 1st excited state or next highest energy level of the infinite potential well. a. Find the probability density function|Ξ¨(π₯, π‘)|2 . Remember Ξ¨(π₯, π‘) = π(π₯)π(π‘) b. Find the average position (expectation value) of the particle β©π₯(π‘)βͺ 2. In class we learned about the uncertainty in position and momentum of a particle. Here we will determine the uncertainty (Ξπ₯Ξπ) for a particle confined in an infinite potential well. V(x) = 0 inside the well (for 0 < x < A) and V(x) = infinity everywhere else. First determine the expectation valueβ©π₯π βͺ. Recall that for a general operator T, the expectation π΄ value is given by β©πβͺ = β«0 ππβ (π₯)πππ (π₯)ππ₯. Next calculate the expectation values β©π₯π2 βͺ, β©ππ βͺ, πππ β©ππ2 βͺ . Remember the quantum operator for momentum p is given as π = π βπβ ππ₯, and the subscripts n indicate the quantized state of the particle (i.e. first energy eigenstate is E1). Keep your answers in the most general form. Now calculate Ξπ₯π = 1 1 (β©π₯π2 βͺ β β©π₯π βͺ2 ) β2 and likewise calculate Ξππ = (β©ππ2 βͺ β β©ππ βͺ2 ) β2. Finally calculate the uncertainty (Ξπ₯Ξπ). What can you say about the uncertainty of the particle in higher states (as n increases from 1 to 2 β¦β¦.)? β13.6 3. The energy levels for the Hydrogen atom is given as πΈπ = π2 in eV and n is an integer 1,2,3β¦..etc. Using this expression draw an energy level diagram for the Hydrogen atom. Derive an expression for the energy (in eV) and wavelength (nm) of light emitted from transitions between energy levels. What are the three longest wavelengths (in nm) for transitions terminating at n = 2? 4. Problem 2.25 5. Problem 2.26 6. Problem 2.27 7. Problem 2.29 8. Problem 2.33 9. Problem 2.43