http://wiki.naturalphilosophy.org/index.php?title=The_Doppler_Effect_of_Absorption_Spectral_Lines_in_Moving_Astronomic_Bodies:_How_Can_It_Happen%3F_(2010_John_Chappell_Memorial_Lecture)&feed=atom&action=historyThe Doppler Effect of Absorption Spectral Lines in Moving Astronomic Bodies: How Can It Happen? (2010 John Chappell Memorial Lecture) - Revision history2024-03-29T09:21:10ZRevision history for this page on the wikiMediaWiki 1.34.0http://wiki.naturalphilosophy.org/index.php?title=The_Doppler_Effect_of_Absorption_Spectral_Lines_in_Moving_Astronomic_Bodies:_How_Can_It_Happen%3F_(2010_John_Chappell_Memorial_Lecture)&diff=25410&oldid=prevMaintenance script: Imported from text file2017-01-02T03:00:38Z<p>Imported from text file</p>
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</table>Maintenance scripthttp://wiki.naturalphilosophy.org/index.php?title=The_Doppler_Effect_of_Absorption_Spectral_Lines_in_Moving_Astronomic_Bodies:_How_Can_It_Happen%3F_(2010_John_Chappell_Memorial_Lecture)&diff=21047&oldid=prevMaintenance script: Imported from text file2017-01-01T18:12:50Z<p>Imported from text file</p>
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<tr><td class='diff-marker'> </td><td style="background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;"></td><td class='diff-marker'> </td><td style="background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;"></td></tr>
<tr><td class='diff-marker'>−</td><td style="color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;"><div>Astronomers use the Doppler-shifted absorption (dark) lines in the spectra of moving astronomic bodies to measure their radial velocities respect to Earth. A dark line, however, is the absence of radiation. How, then, can it be red-shifted or blue-shifted in any sense? This paper investigates this problem trying to comply with QM, and with both, the classical Doppler effect and its relativistic version. For relativity this is the problem: the Doppler-shifted dark lines are produced by absorption in the atmosphere of the selfsame star that emits the radiation. So it looks like a Doppler shift without relative motion. For QM the problem is how to harmonize the frequency shift with Planck's quantum relation, ''E=hf'', where the frequency ''f'' is uniquely defined by a given energy level of a given atom in a stationary frame of reference. How can it be Doppler-shifted, by the macroscopic motion of the atom? <span>&nbsp;</span>Between 1918 and 1932, Bohr, Schroedinger, Dirac, and Fermi studied a similar problem, developing a quantum theory of the Doppler effect. They criticized and improved what each other said. Yet, in this paper preference will be given to the complete classical version of the Doppler formula, explained as a double Doppler effect with time difference between emission and reception. A ?bonus? prediction of the paper is a non-relativistic diffraction experiment in which the cosmic motion of the Earth might be detected.[[Category:Scientific Paper]]</div></td><td class='diff-marker'>+</td><td style="color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;"><div>Astronomers use the Doppler-shifted absorption (dark) lines in the spectra of moving astronomic bodies to measure their radial velocities respect to Earth. A dark line, however, is the absence of radiation. How, then, can it be red-shifted or blue-shifted in any sense? This paper investigates this problem trying to comply with QM, and with both, the classical Doppler effect and its relativistic version. For relativity this is the problem: the Doppler-shifted dark lines are produced by absorption in the atmosphere of the selfsame star that emits the radiation. So it looks like a Doppler shift without relative motion. For QM the problem is how to harmonize the frequency shift with Planck's quantum relation, ''E=hf'', where the frequency ''f'' is uniquely defined by a given energy level of a given atom in a stationary frame of reference. How can it be Doppler-shifted, by the macroscopic motion of the atom? <span>&nbsp;</span>Between 1918 and 1932, Bohr, Schroedinger, Dirac, and Fermi studied a similar problem, developing a quantum theory of the Doppler effect. They criticized and improved what each other said. Yet, in this paper preference will be given to the complete classical version of the Doppler formula, explained as a double Doppler effect with time difference between emission and reception. A ?bonus? prediction of the paper is a non-relativistic diffraction experiment in which the cosmic motion of the Earth might be detected.</div></td></tr>
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<p><b>New page</b></p><div>{{Infobox paper<br />
| title = The Doppler Effect of Absorption Spectral Lines in Moving Astronomic Bodies: How Can It Happen? (2010 John Chappell Memorial Lecture)<br />
| url = [http://www.naturalphilosophy.org/pdf/abstracts/abstracts_5254.pdf Link to paper]<br />
| author = [[Francisco J M?ller]]<br />
| keywords = [[Doppler effect]], [[quantum photon absorption]], [[relativistic Doppler]], [[cosmic motion]]<br />
| published = 2010<br />
| journal = [[Proceedings of the NPA]]<br />
| volume = [[7]]<br />
| num_pages = 7<br />
| pages = 336-342<br />
}}<br />
<br />
'''Read the full paper''' [http://www.naturalphilosophy.org/pdf/abstracts/abstracts_5254.pdf here]<br />
<br />
==Abstract==<br />
<br />
Astronomers use the Doppler-shifted absorption (dark) lines in the spectra of moving astronomic bodies to measure their radial velocities respect to Earth. A dark line, however, is the absence of radiation. How, then, can it be red-shifted or blue-shifted in any sense? This paper investigates this problem trying to comply with QM, and with both, the classical Doppler effect and its relativistic version. For relativity this is the problem: the Doppler-shifted dark lines are produced by absorption in the atmosphere of the selfsame star that emits the radiation. So it looks like a Doppler shift without relative motion. For QM the problem is how to harmonize the frequency shift with Planck's quantum relation, ''E=hf'', where the frequency ''f'' is uniquely defined by a given energy level of a given atom in a stationary frame of reference. How can it be Doppler-shifted, by the macroscopic motion of the atom? <span>&nbsp;</span>Between 1918 and 1932, Bohr, Schroedinger, Dirac, and Fermi studied a similar problem, developing a quantum theory of the Doppler effect. They criticized and improved what each other said. Yet, in this paper preference will be given to the complete classical version of the Doppler formula, explained as a double Doppler effect with time difference between emission and reception. A ?bonus? prediction of the paper is a non-relativistic diffraction experiment in which the cosmic motion of the Earth might be detected.[[Category:Scientific Paper]]<br />
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[[Category:Relativity]]<br />
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