Tired light: Difference between revisions
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A number of tired light mechanisms have been suggested over the years. [[Fritz Zwicky]], in his paper proposing these models investigated a number of redshift explanations, ruling out some himself. The simplest form of a tired light theory assumes an exponential decrease in photon energy with distance traveled: |
A number of tired light mechanisms have been suggested over the years. [[Fritz Zwicky]], in his paper proposing these models investigated a number of redshift explanations, ruling out some himself. The simplest form of a tired light theory assumes an exponential decrease in photon energy with distance traveled: |
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:<math>E(x)= |
:<math>E(x)=E_0 \exp{-\frac{x}{R_0}}</math> |
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where |
where <math>E(x)</math> is the energy of the photon at distance <math>x</math> from the source of light, <math>E_0</math> is the energy of the photon at the source of light, and <math>R</math> is a large constant characterizing the "resistance of the space". To correspond to [[Hubble's law]], the constant <math>R_0</math> must be several giga[[parsec]]s. <!--It must be large enough to take into account any deviation from Hubble's law--> For example, Zwicky considered whether an integrated [[Compton Effect]] could account for the scale normalization of the above model: |
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{{quote|... light coming from distant nebulae would undergo a shift to the red by [[Compton effect]] on those free electrons [in interstellar spaces] [...] But then the light scattered in all directions would make the interstellar space intolerably opaque which disposes of the above explanation. [...] it is evident that any explanation based on a scattering process like the Compton effect or the [[Raman effect]], etc., will be in a hopeless position regarding the good definition of the images.<ref name="Zwicky" />}} |
{{quote|... light coming from distant nebulae would undergo a shift to the red by [[Compton effect]] on those free electrons [in interstellar spaces] [...] But then the light scattered in all directions would make the interstellar space intolerably opaque which disposes of the above explanation. [...] it is evident that any explanation based on a scattering process like the Compton effect or the [[Raman effect]], etc., will be in a hopeless position regarding the good definition of the images.<ref name="Zwicky" />}} |
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Tired light is a class of hypothetical redshift mechanisms that was proposed as an alternative explanation for the redshift-distance relationship. Generally, these models are proposed as alternatives to the metric expansion of space of which the Big Bang and the Steady State cosmologies are the most famous examples. The concept was first proposed in 1929 by Fritz Zwicky, who suggested that photons lose energy over time through collisions with other particles. This idea was first criticized because such scattering would blur the images of distant objects more than what is seen and the expected time dilation of cosmological sources has also been observed — and effect that should not be present if the cosmological redshift was due to a tired light scattering mechanism. Today, tired light is remembered mainly for historical interest as an example of a falsified hypothesis.
History and reception
Tired light was an idea that came about due to the observation made by Edwin Hubble that distant galaxies have redshifts proportional to their distance. Redshift is a shift in the spectrum of the emitted electromagnetic radiation from an object toward lower energies and frequencies, associated with the phenomenon of the Doppler Effect. Observers of spiral nebulae such as Vesto Slipher observed that regardless of their position in the sky, these objects (now known to be separate galaxies) were all redshifted, and only two (M 31 and M 33 were "blue-shifted". Since the relation holds in all directions it cannot be attributed to normal movement with respect to a background which would show an assortment of redshifts and blueshifts. Everything is moving away from the Milky Way galaxies. Hubble's contribution was to show that the magnitude of the redshift was correlated strongly with the distance to the distant galaxies.
Immediately upon publishing these results, Willem de Sitter who was working with Einstein's Theory of General Relativity recognized that these observations fit a set of solutions to Einstein equations now collectively known as the FRW metric. The universal redshift-distance relation in this solution is attributable to the effect an expanding universe has on a photon traveling on a null spacetime interval (also known as a "light-like" geodesic). In this formulation, there was still an analogous effect to the Doppler Effect, though relative velocities need to be handled with more care since distances can be defined in different ways in expanding metrics.
At the same time, other explanations were proposed that did not concord with general relativity. Edward Milne proposed an explanation compatible with special relativity but not general relativity that there was a giant explosion that could explain redshifts (see Milne universe). Others proposed thatsystematic effects could explain the redshift-distance correlation. Along this line, Fritz Zwicky proposed a "tired light" mechanism in 1929.[1] Zwicky suggested that photons might slowly lose energy as they travel vast distances through a static universe by interaction with matter or other photons, or by some novel physical mechanism. Since a decrease in energy corresponds to an increase in light's wavelength, this effect would produce a redshift in spectral lines that increase proportionally with the distance of the source. The term "tired light" was coined by Richard Tolman in the early 1930s as a way to refer to this idea.[2]
Tired light mechanisms were among the proposed alternatives to the Big Bang and the Steady State cosmologies, both of which relied on the general relativistic expansion of the universe of the FRW metric. Through the middle of the twentieth century, most cosmologists supported one of these two paradigms, but there were a few scientists, especially those who were working on alternatives to general relativity, who worked with the tired light alternative.[3] As the discipline of observational cosmology developed in the late twentieth century and the associated data became more numerous and accurate, the Big Bang emerged as the cosmological theory most supported by the observational evidence, and it remains the accepted consensus model with a current parametrization that precisely specifies the state and evolution of the universe. Additionally, a number of falsifying observations have shown that "tired light" hypotheses are not viable explanations for cosmological redshifts. For example, in a static universe with tired light mechanisms, the surface brightness of stars and galaxies should be constant, that is, the farther an object is, the less light we receive, but its apparent area diminishes as well, so the light received divided by the apparent area should be constant. In an expanding universe, the surface brightness diminishes with distance. As the observed object recedes, photons are emitted at a reduced rate because each photon has to travel a distance that is a little longer than the previous one, while its energy is reduced a little because of increasing redshift at a larger distance. On the other hand, in an expanding Universe, the object appears to be larger than it really is, because it was closer to us when the photons started their travel. This causes a difference in surface brilliance of objects between a static and an expanding Universe. This is known as the Tolman surface brightness test that in those studies favors the expanding universe hypothesis and rules out static tired light models.[4][5][6]
Redshift is directly observable and used by cosmologists as a direct measure of lookback time. They often refer to age and distance to objects in terms of redshift rather than years or light-years. In such a scale, the Big Bang corresponds to a redshift of infinity.[4] Alternative theories of gravity that do not have an expanding universe in them need an alternative to explain the correspondence between redshift and distance that is sui generis to the expanding metrics of general relativity. Such theories are sometimes referred to as "tired-light cosmologies", though not all authors are necessarily aware of the historical antecedents.[7]
Specific falsified models
![](http://upload.wikimedia.org/wikipedia/commons/thumb/0/0d/Hubble_ultra_deep_field_high_rez_edit1.jpg/275px-Hubble_ultra_deep_field_high_rez_edit1.jpg)
In general, any "tired light" mechanism must solve some basic problems, in that the observed redshift must:
- admit the same measurement in any wavelength-band
- not exhibit blurring
- follow the detailed Hubble relation observed with supernova data (see accelerating universe)
- explain associated time dilation of cosmologically distant events.[8]
A number of tired light mechanisms have been suggested over the years. Fritz Zwicky, in his paper proposing these models investigated a number of redshift explanations, ruling out some himself. The simplest form of a tired light theory assumes an exponential decrease in photon energy with distance traveled:
where is the energy of the photon at distance from the source of light, is the energy of the photon at the source of light, and is a large constant characterizing the "resistance of the space". To correspond to Hubble's law, the constant must be several gigaparsecs. For example, Zwicky considered whether an integrated Compton Effect could account for the scale normalization of the above model:
... light coming from distant nebulae would undergo a shift to the red by Compton effect on those free electrons [in interstellar spaces] [...] But then the light scattered in all directions would make the interstellar space intolerably opaque which disposes of the above explanation. [...] it is evident that any explanation based on a scattering process like the Compton effect or the Raman effect, etc., will be in a hopeless position regarding the good definition of the images.[1]
This expected "blurring" of cosmologically distant objects is not seen in the observational evidence, though it would take much larger telescopes than those available at that time to show this with certainty. Alternatively, Zwicky proposed a kind of Sachs-Wolfe Effect explanation for the redshift distance relation:
One might expect a shift of spectral lines due to the difference of the static gravitational potential at different distances from the center of a galaxy. This effect, of course, has no relation to the distance of the observed galaxy from our own system and, therefore, cannot provide any explanation of the phenomenon discussed in this paper.[1]
Zwicky's proposals were carefully presented as falsifiable according to later observations:
... [a] gravitational analogue of the Compton effect [...] It is easy to see that the above redshift should broaden these absorption lines asymmetrically toward the red. If these lines can be photographed with a high enough dispersion, the displacement of the center of gravity of the line will give the redshift independent of the velocity of the system from which the light is emitted.[1]
Such broadening of absorption lines is not seen in high-redshift objects, thus falsifying this particular hypothesis.[9]
Zwicky also notes, in the same paper, that according to a tired light model a distance-redshift relationship would necessarily be present in the light from sources within our own galaxy (even if the redshift would be so small that it would be hard to measure), that do not appear under a recessional-velocity based theory. He writes, referring to sources of light within our galaxy: "It is especially desirable to determine the redshift independent of the proper velocities of the objects observed".[1] Subsequent to this, astronomers have patiently mapped out the three-dimensional velocity-position phase space for the galaxy and found the redshifts and blueshifts of galactic objects to accord well with the statistical distribution of a spiral galaxy, eliminating the intrinsic redshift component as an effect.[10]
Following after Zwicky in 1935, Edwin Hubble and Richard Tolman compared recessional redshift with a non-recessional one, writing that they:
... both incline to the opinion, however, that if the red-shift is not due to recessional motion, its explanation will probably involve some quite new physical principles [... and] use of a static Einstein model of the universe, combined with the assumption that the photons emitted by a nebula lose energy on their journey to the observer by some unknown effect, which is linear with distance, and which leads to a decrease in frequency, without appreciable transverse deflection.[11]
These conditions became almost impossible to meet and the overall success of general relativistic explanations for the redshift-distance relation is one of the core reasons that the Big Bang model of the universe remains the cosmology preferred by researchers.
In the early 1950s, Erwin Finlay-Freundlich proposed a redshift as "the result of loss of energy by observed photons traversing a radiation field."[12] R.A. Alpher noted, "No generally accepted physical mechanism has been proposed for this loss,"[13] though P.F. Brown "... proposed that the energy lost reappears as neutrino pairs resulting from the exchange of a graviton between two photons."[14] This exotic proposal was already falsified by the same observations that falsified the other mechanisms proposed above. From time to time, additional tired light models are proposed including one that was published in a 1979 Nature paper where a type of Integrated Sachs-Wolfe Effect (ISW) was proposed as a possible mechanism.[15] Unfortunately, the observed magnitude of the ISW seen in the low-l mode anisotropies of the cosmic microwave background falsifies this proposal as well.
Notes
- ^ a b c d e Zwicky, F. 1929. On the Red Shift of Spectral Lines through Interstellar Space. PNAS 15:773-779. Abstract (ADS) Full article (PDF)
- ^ Evans, Myron W.; Vigier, Jean-Pierre (1996). The Enigmatic Photon: Theory and Practice of the B3 Field. Springer. p. 29. ISBN 0792340442.
- ^ Wilson, O. C. 1939. Possible applications of supernovae to the study of the nebular red shifts. Astrophysical Journal 90:634-636. Archived article (ADS)
- ^ a b Geller J. et al.,Test of the expanding universe postulate The astrophysical journal 174, p.1 (1972)
- ^ Goldhaber, et al. (2001) Timescale Stretch Parameterization of Type Ia Supernova B-band Light Curves url
- ^ Lubin and Sandage(2001), The Tolman Surface Brightness Test for the Reality of the Expansion. IV. A Measurement of the Tolman Signal and the Luminosity Evolution of Early-Type Galaxies, url
- ^ Barrow, John D. (2001). Peter Coles (ed.). The Routledge Companion to the New Cosmology. Routledge. p. 308. ISBN 0-415-24312-2.
- ^ While supernova light curve data are consistent with time dilation and rule out some static cosmologies, a 2010 comparison of quasar light curves at high and low redshifts did not show the expected evidence of time dilation, see Hawkins, M. R. S. (9 April 2010). "On time dilation in quasar light curves". Monthly Notices of the Royal Astronomical Society. Bibcode:2010MNRAS.405.1940H. doi:10.1111/j.1365-2966.2010.16581.x. ISSN 1365-2966.
In this paper we set out to measure time dilation in quasar light curves. In order to detect the effects of time dilation, sets of light curves from two monitoring programmes are used to construct Fourier power spectra covering time-scales from 50 d to 28 yr. Data from high- and low-redshift samples are compared to look for the changes expected from time dilation. The main result of the paper is that quasar light curves do not show the effects of time dilation.
{{cite journal}}
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requires|url=
(help)CS1 maint: unflagged free DOI (link) - ^ See, for example, high-redshift spectra shown at http://astrobites.com/2011/04/27/prospecting-for-c-iv-at-high-redshifts/
- ^ Binney & Merrifield: GALACTIC ASTRONOMY, Princeton University Press, ISBN13: 978-0-691-02565-0
- ^ Hubble, Edwin; Tolman, Richard C. (11/1935). "Two Methods of Investigating the Nature of the Nebular Redshift". Astrophysical Journal. 82: 302. Bibcode:1935ApJ....82..302H. doi:10.1086/143682.
{{cite journal}}
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(help) - ^ Finlay-Freundlich, E. (1954). "Red-Shifts in the Spectra of Celestial Bodies". Proc. Phys. Soc. A. 67 (2): 192–193. Bibcode:1954PPSA...67..192F. doi:10.1088/0370-1298/67/2/114.
- ^ Alpher, R.A. (1962). "Laboratory Test of the Finlay-Freundlich Red Shift Hypothesis". Nature. 196 (4852): 367–368. Bibcode:1962Natur.196..367A. doi:10.1038/196367b0.
- ^ Brown, P.F. (1962). "The Case for an Exponential Red Shift Law". Nature. 193 (4820): 1019–1021. Bibcode:1962Natur.193.1019B. doi:10.1038/1931019a0.
- ^ D.F. Crawford, Photon Decay in Curved Space-time, Nature, 277(5698), 633-635 (1979).