Determine fine-structure constant

In summary: I see, thanks. Can you give me a hint on how I...In summary, the hyperfine structure in the transition 6s $^2S_{1/2}$ - 8p $^2P_{3/2}$ in 115In (I = 9/2) was found using a narrow-band tunable laser and a collimated atomic beam. The 6 components shown have the following frequencies 31, 112, 210, 8450, 8515 and 8596 MHz.
  • #1
Philip Land
56
3

Homework Statement


The figure below shows the hyperfine structure in the transition 6s $^2S_{1/2}$ - 8p $^2P_{3/2}$ in 115In (I = 9/2). The measurement is made using a narrow-band tunable laser and a collimated atomic beam; hence the Doppler width is greatly reduced. The 6 components shown have the following frequencies 31, 112, 210, 8450, 8515 and 8596 MHz. Draw a schematic figure of the energy levels with the appropriate quantum numbers and show the allowed transitions. Determine the hyperfine constants, in MHz, for the two fine structure levels

(Image is just a blurry graph and not necessary, all data is given)

Homework Equations


$$E_{hfs}=\frac{A}{2}[F(F+1) - J(J+1)-I(I+1)] (1)$$

The Attempt at a Solution



F=|J+I|,...,|J-I|. For the dubblet P that would be F=(6,5,4,3). So I have F,J and I.

Since I don't have energydifferences (I think), I'm not sure how to put up a equationsystem to solve for (1). Are there another formula/concept I should use instead?

*Note I'm a beginner at atomic physics, brand new to these concepts so maybe I'm missing something obvious*
 
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  • #2
Hi Philip Land and welcome to PF.
:welcome:

Drawing the energy level diagram and identifying the transitions would be extremely useful as a first step. Have you done that? If "yes", please post the drawing; if "no", please do it.

On edit: Please post the graph that you think is "not necessary". Also, if you think that "all data is given", why then do you think that you "don't have the energy differences"?
 
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  • #3
kuruman said:
Hi Philip Land and welcome to PF.
:welcome:

Drawing the energy level diagram and identifying the transitions would be extremely useful as a first step. Have you done that? If "yes", please post the drawing; if "no", please do it.

On edit: Please post the graph that you think is "not necessary". Also, if you think that "all data is given", why then do you think that you "don't have the energy differences"?

Hi!

Thank you for your reply.

I did as you said and drew the energy diagram. See uploaded picture. Also a print-screen of the graph belonging to the exercise.

You are right, I do probably have the energy differences in MHz, but I'm not quite sure how to identify the transitions.

I also tried to use formula (1), with the biggest frequency, 8596MHz on the left hand side, and used $F_{max}$ as my F in the equation. But that was a bold guess and the the answer got wrong.

So now I'm pretty stuck again, I know there is the Landé interval rule stating $$Energy ratio = \frac{F_{max}}{F_{max}-1} (2)$$ but I can't see how that can help me determine A either...
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  • #4
OK, so you have the a diagram of the energy levels and the transitions. Now use your equation for Ehfs to obtain values for the energy levels in terms of A (remember the A values will be different for the 6s and 8p states, you are asked to find both). Assume a value T (unknown) for the energy difference between the unsplit S and P states. Now derive expressions for the energies of the allowed transitions. Do you observe any patterns that would help you assign the observed frequencies to particular transitions?
 
  • #5
mjc123 said:
OK, so you have the a diagram of the energy levels and the transitions. Now use your equation for Ehfs to obtain values for the energy levels in terms of A (remember the A values will be different for the 6s and 8p states, you are asked to find both). Assume a value T (unknown) for the energy difference between the unsplit S and P states. Now derive expressions for the energies of the allowed transitions. Do you observe any patterns that would help you assign the observed frequencies to particular transitions?

Hi!

Thanks for your answer.

I see. Starting with ##P_{3/2}##, I sat up 4 equations for all the F values (6,5,4,3). Then I solved for A (see attached picture).

Now I guess all I need to do is to figure out what ##E_{F=i}## for i=(6,5,4,3). I tried to use them in magnitude order, but the result got plain wrong.

Am I on the right track or am I thinking about it wrong? Because I really can't see the connection between the given frequencies and ##E_{hfs}##.

Thanks on advance.
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  • #6
The frequencies aren't directly connected to Ehfs. They are transition frequencies, so refer to the difference between two energy levels. Repeat what you've done for the 2S level, and work out the energies of the allowed transitions.
 
  • #7
mjc123 said:
The frequencies aren't directly connected to Ehfs. They are transition frequencies, so refer to the difference between two energy levels. Repeat what you've done for the 2S level, and work out the energies of the allowed transitions.
Are you suggesting that I multiply with planks constant and change unit? Or do you mean I should do something else?

I see, thanks. Can you give me a hint on how I work out these energies so I can solve for A? And do you mean I need to repeat the same doe ##^2S## before working out the energies to determine A for ##^2P##?

Thanks in advance!
 
  • #8
Philip Land said:
Are you suggesting that I multiply with planks constant and change unit?
No, use MHz as your "energy" unit, as you are given the frequencies in MHz and asked for the A values in MHz.
Philip Land said:
And do you mean I need to repeat the same doe 2S2S^2S before working out the energies to determine A for 2P2P^2P?
Yes. You need to obtain expressions for the TRANSITION energies. You can't work out A (2P) just from the expressions for the 2P energy levels, because you have no (direct) data on the relative energies of these levels. You have frequencies for the transitions between the 6s and 8p levels.
 
  • #9
mjc123 said:
No, use MHz as your "energy" unit, as you are given the frequencies in MHz and asked for the A values in MHz.

Yes. You need to obtain expressions for the TRANSITION energies. You can't work out A (2P) just from the expressions for the 2P energy levels, because you have no (direct) data on the relative energies of these levels. You have frequencies for the transitions between the 6s and 8p levels.
Thanks for your help!

I see. Sorry for being confused, this is a central part but not covered in lectures or textbook and I really want to grasp this.

I now have the expressions $$A_{^2P} = \frac{1}{4}[ \frac{E_6}{6.75} + \frac{E_5}{0.75} - \frac{E_4}{4.25} - \frac{E_3}{8.25} ] (1) $$
$$A_{^2S} = \frac{1}{2}[ \frac{E_5}{2.25} - \frac{E_4}{2.75} ] (2) $$

Is it so that the frequencies now is the energy-differences in these expressions, e.g. ##E_6 - E_5## is the given frequencies. I'm still not sure how I know what frequency correspond to what energy differences. Nor how to solve the equation system above. Do you have a lsat hint on this so it clicks?
 
  • #10
Once again, you can't solve the equation system because you don't know what the energies are. Try doing what I have suggested several times. Get expressions for the energies in terms of the A constants (rather than the other way round). To simplify, let us give the lowest energy level (E4 of 2S) a value of 0. What is the energy of E5(2S)? Let us give the lowest 2P level (E3) a value of T (I suggested a different definition for T above, but run with this, it's simpler). What are the energies of the other 2P levels?
Now work out expressions for the energies of the allowed transitions between levels. You have drawn these transitions in post #3.
Then look for patterns in the transitions that may help you assign them. Look at the differences between the transition energies. For example, as the transitions 6→5, 5→5 and 4→5 all terminate on the same lower state, the differences between them should be the same as the differences between the 6, 5 and 4 levels of 2P. Does this help you find A(2P)?
Hint: A(2S) and A(2P) may be very different!
 
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Related to Determine fine-structure constant

1. What is the fine-structure constant?

The fine-structure constant, also known as the Sommerfeld constant, is a dimensionless physical constant that characterizes the strength of the electromagnetic interaction between elementary particles. It is denoted by the symbol α and has a value of approximately 1/137.

2. How is the fine-structure constant determined?

The fine-structure constant is determined through experimental measurements and theoretical calculations. One method involves measuring the ratio of the strengths of two different atomic transitions, known as the Rydberg constant. Another method involves using quantum electrodynamics (QED) to calculate the value of α based on fundamental physical constants.

3. What is the significance of the fine-structure constant?

The fine-structure constant is a fundamental constant that plays a crucial role in describing the behavior of atoms, molecules, and subatomic particles. It is also related to other important physical constants such as the speed of light, Planck's constant, and the elementary charge. Its precise value has implications for the structure and behavior of matter at the microscopic level.

4. Has the value of the fine-structure constant changed over time?

The fine-structure constant is believed to be a constant of nature, meaning that its value does not change over time or in different locations in the universe. However, there have been some controversial claims of slight variations in its value based on different experimental results. Further research is needed to confirm these claims.

5. What are some applications of the fine-structure constant?

The fine-structure constant has various applications in physics, chemistry, and engineering. It is used in the design of electronic devices, such as transistors and computer chips. It also plays a role in the understanding of atomic and molecular structures and in the development of quantum technologies. Additionally, the precise value of α is important for testing the validity of theoretical models and theories in physics.

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