Chapter 4: Atomic Spectra Flashcards
Give an example of an atomic two-level system.
The 1s and 2p energy levels in the H atom form a two-level system. If narrow bandwidth laser radiation is used to excite a H atom from the ground 1s state n = 2, the selection rules for electric dipole transitions restrict the excitation to the 2p state. After it is excited this state has only one possible decay pathway. It will decay by spontaneous emission to the 1s state.
What effect does stimulated emission have on a two-level system prepared in the excited state?
Stimulated emission de-excites a two-level system prepared in the excited state back to the ground state. This will result in the emission of a photon that propagates in the same direction, has the same frequency, and is in phase with the photon that stimulated the system to emit.
In a two-level system how does the Einstein A-coefficient relate to the lifetime of the excited state?
In a two-level system the lifetime of the excited state is τ2 = 1/A12.
Give an expression for the lifetime of the 4p state in the H atom in terms of the relevant Einstein A coefficients.
What is meant by the expression metastable state? Give examples of metastable states in the H atom, and in the He atom.
What is a population inversion and why is it required for the operation of a laser?
An ensemble of two-level systems exhibits a population inversion when the fraction in the excited state is greater than the fraction in the ground state. For the operation of a laser stimulated emission in the lasing medium must be more likely to occur than spontaneous emission. To ensure that stimulated emission dominates, more of the quantum systems that make up the medium must be in the upper (excited) state associated with the lasing transition than in lower (ground) state. This situation represents a population inversion.
Why can a population inversion not be generated in a two-level system?
- If population is intially at level 1, absorption most likely to occur.
- Population is then transferred yo upper (excited) level, meaning population of excited level will increase until both lv1 and lv2 are equal.
- From here, the likelihood of absorption and stimulated emission are both equal.
Why is it difficult to construct a laser that operates directly in the X-ray region of the electromagnetic spectrum?
For the operation of a laser the rate of stimulated emission must exceed the rate of spontaneous emission from the excited state. Since the rate of spontaneous emission, the Einstein A-coefficient, depends on the cube of the transition frequency, νif , it is difficult to ensure that stimulated emission dominates for very high transition frequencies, i.e., at short wavelengths in the X-ray region of the electromagnetic spectrum.
Is the bandwidth of a nanosecond pulsed laser typically larger or smaller than that of a femtosecond pulsed laser?
What is the momentum associated with a photon with a frequency of 5.63 × 1014 Hz?
Photon momentum pλ = h/λ = hν/c. Therefore the momentum associated with a photon of 5.63 × 1014 Hz is 1.2 × 10−27 kg m s−1 .
Explain Absorption
This involves the system, initially level 1, absorbing a photon and being excited to level 2. The rate of absorption is directly proportional to the no. of atoms in level 1 and the energy density of the electromagentic field.
Explain stimulated emission
A photon stimulates the system, initially at level 2, to decay to level 1 with the emission of another photon.
The photon emitted has the same frequency, is incoherent with (electromagnetic field is oscillating in phase with, and propgating) the photon that stimulated it.
Explain spontaneous emission
Rate of emission is directly proportional to he number of atoms in level 2.
Einstein coefficients
A=Einstein A coefficient for spontaneous emission
B=Einstein B coefficient for stimulated emission
Effects of finite excited state lifetimes
Transistions to states with long life times have narrow spectral width therefore when atom spontaneously decays, cannot be precisely measured, but frequency will be precise.
And vice versa