I The definition of the spectra in quantum mechanics

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The discussion centers on the complexities of defining spectra in quantum mechanics, particularly for undergraduate students. It emphasizes the need to solve the energy eigenvalue problem and understand spectral lines resulting from transitions between energy states. The term "spectrum" is noted as vague, with various types such as atomic emission and absorption requiring different considerations. The conversation highlights the limitations of computational techniques in fully defining spectra, suggesting that spectroscopy involves intricate processes that cannot be simplified easily. Ultimately, a comprehensive understanding of quantum mechanics and its terminology is essential for accurate explanations.
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I have read that "The spectrum of a substance (gas, liquid or solid) can be defined as the set of all eigenvalues of the Schrodinger equation"

please, Can anyone explain this?
for undergraduate students how to explain this?
 
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The sentence is not entirely correct.

You can calculate the spectrum by first solving for the energy eigenvalue problem for the system. Then the spectral lines, i.e., the electromagnetic radiation emitted when the system undergoes transitions from states of higher energy to lower. In first-order perturbation theory what you get are the dipole transitions, and the frequencies of the radiation are given by the energy-differences: ##\hbar \omega_{\gamma}=E_n-E_m##, where ##E_j## are the bound-state energies of the system.
 
Asmaa said:
Summary:: I have read that "The spectrum of a substance (gas, liquid or solid) can be defined as the set of all eigenvalues of the Schrodinger equation"

please, Can anyone explain this?

for undergraduate students how to explain this?
That's like asking: explain QM to me. You need a textbook. E.g.

https://www.cambridge.org/gb/academ...nics-3rd-edition?format=HB&isbn=9781107189638
 
Can you be more specific about what is unclear? Which of these terms do you not understand?

spectrum

eigenvalues

Schrödinger equation
 
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Also,

"Spectrum" is quite vague. What kind of spectra? Atomic emission, absorption, fluorescence, inelastic scattering? There are many things to consider in some of these techniques, such as the probability of several relaxation processes, intermolecular and intramolecular interactions, solvents.

Spectroscopy is a messy thing. If we could simply use DFT and other computational techniques to define everything, then spectroscopists would be out of a job, and monkeys could do the work.

You can get close to predicting what might happen when light interacts with matter, but there is no theory that can define a "spectrum".
 
We often see discussions about what QM and QFT mean, but hardly anything on just how fundamental they are to much of physics. To rectify that, see the following; https://www.cambridge.org/engage/api-gateway/coe/assets/orp/resource/item/66a6a6005101a2ffa86cdd48/original/a-derivation-of-maxwell-s-equations-from-first-principles.pdf 'Somewhat magically, if one then applies local gauge invariance to the Dirac Lagrangian, a field appears, and from this field it is possible to derive Maxwell’s...