Energy tolerance for orbital of electrons

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SUMMARY

The discussion centers on the energy tolerance required for an electron to transition between orbitals, specifically in hydrogen. To move from the ground state to the third orbital, a photon with an energy of 12.09 eV is necessary. The tolerance for photon frequency is questioned, with insights indicating that photons with slightly different energies, such as 12.15 eV, can indeed excite the electron and scatter the excess energy as a lower energy photon, approximately 0.06 eV. This phenomenon is explained through the lens of the Heisenberg uncertainty principle, which relates the natural width of spectral lines to the lifetime of excited states.

PREREQUISITES
  • Understanding of quantum mechanics principles
  • Familiarity with photon energy calculations
  • Knowledge of the Heisenberg uncertainty principle
  • Basic concepts of atomic orbitals and electron transitions
NEXT STEPS
  • Research the Heisenberg uncertainty principle in detail
  • Explore the concept of natural width in spectral lines
  • Learn about photon absorption and emission processes
  • Investigate energy levels and transitions in other elements beyond hydrogen
USEFUL FOR

Students of physics, quantum mechanics enthusiasts, and researchers interested in atomic behavior and photon interactions will benefit from this discussion.

MikeGomez
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An exact energy level is required to bring an electron from one orbital to another. For example with hydrogen, for an electron to go from the ground state to the third orbital requires a photon with an energy of 12.09eV. But what is the tolerance? In other words, how close to that frequency does the photon need to be, within 1%, .001%, or what?

Also, is it ever possible for a photon with a slightly different frequency to be absorbed? Can a photon of 12.15eV cause the electron to jump to the third orbital and either …

scatter the remaining energy as a 0.06eV photon?

or

absorb the excess energy as heat?
 
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Each spectral line has a natural width, a spread in energy inversely proportional to the lifetime of the excited state, and given approximately by the (dare I say it) Heisenberg uncertainty principle. Natural widths are typically very small.

Second question is yes, the photon can excite the atom and scatter as a lower energy photon. No such thing as "heat" for a single atom.
 
Thanks Bill.
 

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