Natural broadening of lithium sub-levels

In summary, the 2p state of lithium exhibits two fine structure components due to spin-orbit interaction, with wavelengths of 670.960nm and 670.975nm. At 700K, the comparison between Doppler and natural broadening shows that the lifetime of the 2p state is 27ns and the relative change in wavelength, Δλ/λ, is much smaller than 1. The uncertainty principle can be used to calculate the natural broadening, with a value of approximately 50m. However, converting ΔE to Δλ leads to a significantly larger value, highlighting the importance of using relative values.
  • #1
gboff21
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0

Homework Statement


In the 2p state of lithium, two fine structure components are formed due to spin-orbit interaction. They produce wavelengths of 670.960nm and 670.975nm. Compare Doppler and natural broadening at 700K. The lifetime of the 2p state is 27ns and [itex]\frac{\Delta \lambda}{\lambda} ~= \frac{\Delta \nu}{\nu} [/itex] at [itex]\frac{\Delta \nu}{\nu} << 1[/itex]

Homework Equations



Given Doppler broadening: [itex]\Delta \nu = \frac{2 \nu_{0}}{c}\sqrt{\frac{2KT}{M}*ln(2)}[/itex]

The Attempt at a Solution


My Natural broadening derivation:
uncertainty principle: [itex]\Delta E \tau = \hbar[/itex] (tau is lifetime)
so [itex]\Delta \lambda = 2 \pi c \tau[/itex] (which comes out as ~50m)
This is clearly wrong since the doppler broadening comes out as in the order of 10^-12.

Any clues?
 
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  • #2
How did you get ##\Delta \lambda## based on ##\Delta E##? That relation depends on the wavelength itself.
It is easier to convert ##\Delta E## to ##\Delta \nu##.
 
  • #3
E=hc/λ
and either way (nu or lambda) the answer is stupidly large
 
  • #4
E=hc/λ, but not ΔE=hc/Δλ!
$$E+\Delta E=\frac{hc}{\lambda+\Delta \lambda} \approx \frac{hc}{\lambda}(1-\frac{\Delta \lambda}{\lambda})$$
Simplified:
$$\Delta E=-\Delta \lambda \frac{hc}{\lambda^2}$$

It is easier to use relative values everywhere:
$$\frac{\Delta E}{E}=\frac{\Delta \nu}{\nu}=-\frac{\Delta \lambda}{\lambda}$$
 
  • #5
Now it's so obvious!
Thanks a lot mfb!
 

Related to Natural broadening of lithium sub-levels

1. What is natural broadening of lithium sub-levels?

Natural broadening of lithium sub-levels refers to the phenomenon in which the energy levels of lithium atoms are not perfectly defined, but instead have a certain range of values. This is due to the uncertainty principle in quantum mechanics, which states that the position and energy of a particle cannot be known simultaneously with 100% accuracy.

2. How does natural broadening occur in lithium sub-levels?

Natural broadening occurs in lithium sub-levels due to the finite lifetimes of excited states. When an electron in a lithium atom is excited to a higher energy level, it can spontaneously emit a photon and return to its ground state. However, the exact timing of this emission is uncertain, leading to a broadening of the energy levels.

3. What is the significance of natural broadening of lithium sub-levels?

The natural broadening of lithium sub-levels has significant implications for spectroscopy and the study of atomic and molecular structure. By analyzing the broadening of spectral lines, scientists can gain insights into the energy levels and interactions of particles within a system.

4. Can natural broadening be controlled or eliminated?

No, natural broadening cannot be controlled or eliminated as it is a fundamental property of quantum mechanics. However, it can be reduced by using techniques such as Doppler broadening, in which the thermal motion of atoms smears out the energy levels, resulting in a narrower spectral line.

5. How is natural broadening of lithium sub-levels different from other types of broadening?

Natural broadening is different from other types of broadening, such as collisional broadening or pressure broadening, which occur due to external factors such as collisions with other particles. Natural broadening, on the other hand, is an inherent property of particles and is not influenced by external factors.

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