Transition state of electrons in molecules

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Discussion Overview

The discussion revolves around the transition states of electrons in molecules, specifically focusing on the absorption of wavelengths by naphtalene, anthracene, and tetracene when modeled as infinite quantum wells. Participants explore the implications of electron transitions between energy levels and the factors affecting continuous absorption of light.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions why molecules do not stop absorbing wavelengths corresponding to the first transition states over time, despite the availability of light.
  • Another participant suggests that if all molecules are excited, there would be no further absorption at that wavelength, but relaxation time allows some molecules to decay back to the ground state and absorb light again.
  • There is a discussion about the spacing between energy levels, with one participant asserting that the spacing is not constant for real molecules, while another clarifies that energy differences are proportional to n² for a particle in a box, leading to non-equally spaced levels.
  • One participant mentions that while absorbing light, molecules are also emitting energy and dropping down energy levels, which affects the absorption process.
  • Another point raised is that spontaneous emission leads to a finite lifetime for electrons in excited states, making it unlikely for them to continuously absorb photons to reach higher energy levels.
  • A later reply emphasizes that excited molecules rapidly fall back to the ground state through radiationless transitions, dissipating energy into molecular vibrations, which diminishes the probability of sequentially exciting electrons.

Areas of Agreement / Disagreement

Participants express differing views on the nature of energy level spacing and the mechanisms of absorption and emission. The discussion remains unresolved regarding the implications of these factors on continuous absorption and color change in the molecules.

Contextual Notes

Limitations include assumptions about the model of infinite quantum wells, the simplifications made regarding energy level spacing, and the effects of relaxation times and spontaneous emission on absorption processes.

goldenboy
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Hi !

In my class we have an exercise that I technically understand but that I can't get conceptually.

We have trois molecules (naphtalene, anthracene, tétracene). Considering each molecule as infinite quantum well of length 2L(naphtalene), 3L(anthracene) and 4L(tetracene), we would like to predict the wave length absorbed the electron of each molecules. To do so :

- We find the transition energy for each electron state : ΔE = h*(2n+1)/(8m*Lw)
- Then we find the wave lengths absorbed by each molecules for each transition with : λ = h*c/ΔΕ

So, the exercise is resolved. But my question is : when ALL the electrons at state n = 1 go to n = 2, and n = 2 go to n = 3, ... considering that light is always available, why molecules don't stop absorbing the wave length of the first transition states (consecutively, why the sample doesn't change its colour) through time. And why after a certain state, electron doesn't absorbe the wave length corresponding to it's transition (like in naphtalene, the last transition is from 4 to 5).

Thanks a lot for answers and sorry for my bad english. I hope i have been clear enough

Bye !
 
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If all molecules are excited, then indeed you would have no more absorption at that wavelength. But as you can see from the simple particle in a box model, the spacing between adjacent levels is always the same (this is not true for a real molecule, but close enough), so you will still get absorption at that wavelength. Also, you have to factor in the relaxation time. In most cases, before you can even reach a significant proportion of excited molecules, some will already decay back to the ground state and be able to absorb light again.
 
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DrClaude said:
[...] the spacing between adjacent levels is always the same (this is not true for a real molecule, but close enough), so you will still get absorption at that wavelength. [...]

Thanks for that answer !

However, i can't get that point : in which way the fact that spacing between adjacent levels is always the same influences that we still get absorption at that wavelength ? =)
 
goldenboy said:
However, i can't get that point : in which way the fact that spacing between adjacent levels is always the same influences that we still get absorption at that wavelength ? =)
Because the wavelength of the light must correspond to the energy difference. If the energy difference is constant, then the same wavelength is involved in all n → n+1 transitions, whatever n.
 
I think you're perhaps misreading the OP. The energy difference is proportional to 2n-1 because the energy is proportional to n2 for a particle in a box. So the levels are not equally spaced.
 
mjc123 said:
I think you're perhaps misreading the OP. The energy difference is proportional to 2n-1 because the energy is proportional to n2 for a particle in a box. So the levels are not equally spaced.
Don't know why I was thinking of the harmonic oscillator instead of the particle in a box o:)

Sorry for the confusion.
 
I would say that at the same time as absorbing they are also emitting and dropping down energy levels.
 
goldenboy said:
So, the exercise is resolved. But my question is : when ALL the electrons at state n = 1 go to n = 2, and n = 2 go to n = 3, ... considering that light is always available, why molecules don't stop absorbing the wave length of the first transition states (consecutively, why the sample doesn't change its colour) through time. And why after a certain state, electron doesn't absorbe the wave length corresponding to it's transition (like in naphtalene, the last transition is from 4 to 5).
Due to spontaneous emission, electron in an excited state will have a finite lifetime to stay in that state. Therefore, it cannot consecutively absorbs photon to get excited to a higher and higher levels. After hitting certain upper level, spontaneous emission becomes much more probable and faster that the probability to de-excite exceed that of excitation.
 
Last edited:
goldenboy said:
So, the exercise is resolved. But my question is : when ALL the electrons at state n = 1 go to n = 2, and n = 2 go to n = 3, ... considering that light is always available, why molecules don't stop absorbing the wave length of the first transition states (consecutively, why the sample doesn't change its colour) through time. And why after a certain state, electron doesn't absorbe the wave length corresponding to it's transition (like in naphtalene, the last transition is from 4 to 5).

An important point to recognize here is the fact that a molecule, which has been excited, will fall back very rapidly to the ground state again, by so called radiationless transitions. Basically, the electronic excitation energy dissipates rapidly into molecular vibrations. So the probability to sequentially excite various electrons within one molecule are vanishingly small with the exception of molecules in highest power laser fields.
 

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