Problem Solving: There’s No Place Like the Laser Lab The first optical maser demonstrated was the ruby laser (Theodor Mann, 1960). The optical gain medium is a “quasi-three-state” system. The system is called “quasi” because there are actually FOUR states total… but the two uppermost states both quickly decay into the intermediate/metastable state via mechanical losses of energy (aka. vibrations).
a. Excitations into the two upper states occur for 400nm and 550nm light. The lasing wavelength is centered around 694.3nm. Use this information to explain ruby’s red color.
b. Setting the ground state as a reference of 0eV, draw an energy diagram for the ruby gain medium… draw the levels, label and calculate the energies, … and add in arrows that indicate pumping processes, transitions via vibrational losses and the lasing transition. For the upper three states, also indicate the energy spread of the state (qualitatively… by considering the lifetime of the state).
c. The first ruby lasers were pulsed, and had a coherence length of 1.27cm in air. Assuming coherence over an entire pulse… what is the time duration of the pulse (aka the “pulse width”)?
d. Calculate the bandwidth of this laser, using the simple model relating bandwidth and coherence length that we developed in class.
e. These pulsed lasers were used by the dermatological industry… including the removal of tattoos. If each pulse contains 1.5 mJ of energy, how many photons are in a pulse?
I read the comments but this is all that I know.
Problem Solving: There’s No Place Like the Laser Lab The first optical maser demonstrated was the...