Summary
This project proposes an optical–structural hypothesis about the rotation curves of spiral galaxies. Rather than postulating the existence of invisible mass from the outset, it is suggested that the flatness of the rotation curves may, at least in part, result from the blending of light coming from different layers of the galaxy, from the scattering of central galactic light by interstellar dust and gas, and from spectral averaging along a given line of sight. In this framework, the Doppler signature of the faster inner layers can appear in the spectrum of the outer regions and make the true orbital speed of edge stars appear artificially higher.
1) Introduction to the dark matter problem and the measurement of galactic rotation
One of the main observational arguments for the existence of “dark matter” comes from galaxy rotation curves. These curves are derived from the light of the galaxy, not from a direct tracking of the motion of individual stars.
1.1. How do we measure the rotation of a galaxy from its light?
When a massive object such as a galaxy is rotating, one side of the galactic disk is moving towards us, while the opposite side is moving away from us.
Using the Doppler effect applied to light:
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the light coming from the part of the galaxy that is approaching us is slightly shifted toward shorter wavelengths → it appears bluer (blueshift);
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the light coming from the part that is receding from us is slightly shifted toward longer wavelengths → it appears redder (redshift).
In the spectrum of the light emitted by the gas and stars in the galaxy, the well-known spectral lines (for example, hydrogen lines) are therefore shifted slightly toward the blue on the approaching side and slightly toward the red on the receding side.
By measuring the amplitude of this Doppler shift:
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we determine the direction of rotation of the galaxy,
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and from the value of the shift, we compute the linear rotation speed of gas and stars at different distances from the galactic centre.
In this way, for each radial distance from the centre of the galaxy, one obtains a rotation speed v(r), and a diagram called the galactic rotation curve can be plotted.
1.2. Theoretical expectation versus observation
In a “normal” gravitational disk where the mass is mainly concentrated in the centre (as in the Solar System, where the dominant mass is the Sun), we expect the orbital speed to decrease with distance from the centre as
v(r) ∝ 1 / sqrt(r).
However, for many spiral galaxies, the rotation curves derived from Doppler observations show that
v(r) ≈ constant.
That is, stars and gas in the outer regions rotate at almost the same speed as in the intermediate regions, while the visible mass (stars and gas in the disk) is not sufficient to generate such high velocities.
To explain this discrepancy, the concept of dark matter was introduced: an invisible mass distributed in the galactic halo, providing the additional gravity required for these large rotation speeds.
Nevertheless, up to now no dark-matter particle has been directly detected, and this has motivated a re-examination of the observation process and of the interpretation of rotation curves with greater care and precision.
2) Nature of optical observation and its limitations
The rotation speed of galaxies is not measured from the actual motion of individual stars; we never directly see the position or displacement of stars in a distant galaxy.
What we observe is only light. And all inferences — speed, disk structure, and even the existence of dark matter — are based on spectral analysis of that light.
Yet, on its way to the telescope, light:
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travels across extremely large distances,
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passes through several layers of gas and dust,
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undergoes multiple events of scattering, absorption, reflection and path change,
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and finally ends up being mixed, within a single pixel of the telescope detector, with light from other sources.
This implies that:
The rotation speed we derive from the light is not necessarily equal to the true orbital speed of the stars at that location.
Our line of sight toward the edge of a galaxy passes through several structural layers, and the received light is essentially an average of the emission from these layers.
2.1. Accumulation of light from several layers along one line of sight
A galaxy is not a single-layer structure. When a telescope looks at a given point on the edge of the galactic disk, it actually receives the combined light of several regions and layers:
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the thin disk layer (Thin Disk),
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the thick disk layer (Thick Disk),
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part of the spiral arms,
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the light of the stellar halo,
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the scattered light from the central region.
Each of these layers has a different orbital speed, but their light contributions are added together along the path.
Symbolically:
I_obs(λ) = Σ I_i(λ, v_i)
where I_i is the light intensity of layer i and v_i is the effective velocity associated with that layer.
In practice, telescopes therefore record a spectral average of several layers, rather than the velocity of a single, isolated layer.
2.2. Limits of spatial and spectral resolution
Even the most advanced telescopes, because of the huge distance to external galaxies, effectively add together, in each image pixel:
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the light from thousands of stars,
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originating from hundreds of different layers.
This effect is known in astrophysics as beam smearing.
Under such conditions, the observed Doppler line is influenced by:
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the intensity of each layer,
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the scattering of light along the path,
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the relative brightness between layers,
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and small deflections of the light path.
Important result:
The apparent velocity is not necessarily equal to the true velocity of the outer layer.
2.3. Combined effect of light on the apparent velocity
If a brighter, faster layer is combined along the same line of sight with a fainter, slower layer, the resulting spectrum:
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is mainly dominated by the brighter layer,
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is less representative of the outer layer’s velocity,
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and looks more like the velocity of the inner layers.
This is exactly the phenomenon that will play a key role later in the section presenting the main hypothesis.
3) Multilayer structure of the galaxy and its importance
Spiral galaxies are, from both a spatial and dynamical point of view, multilayer structures. Each layer hosts a population of stars and gas with different properties, and each one shows distinct behaviour in terms of orbital speed, luminosity and density.
Understanding these layers is essential, because:
The light observed at the edge of a galaxy is a combination of the emission from these layers, not just from the outer stars.
3.1. Thin disk layer (Thin Disk)
This layer:
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is the thinnest part of the galactic disk,
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contains relatively young and bright stars,
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has a high density in the main plane of the disk,
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and exhibits relatively high orbital speeds.
A large fraction of the galaxy’s visible light comes from this thin disk layer.
3.2. Thick disk layer (Thick Disk)
This layer lies at greater heights above and below the main plane of the disk.
Its properties:
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lower density,
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older and fainter stars,
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slightly lower orbital speeds,
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a broader presence along many lines of sight.
The light from this layer is weaker, but because it occupies a large volume, it makes a significant contribution to the total observed light.
3.3. Central region and bulge (Central Region & Bulge)
The centre of a galaxy is one of its most energetic and brightest regions. This area includes:
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a very dense population of stars,
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extremely bright stars,
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hot, ionised gas,
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a strong gravitational field,
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faster rotation compared to the outer layers.
The central luminosity is tens to hundreds of times higher than that of the outer parts of the galaxy. This brightness contrast is one of the key factors behind the “dominance of inner light” over the light from outer regions.
3.4. Spiral arms (Spiral Arms)
The spiral arms:
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contain highly active star-forming regions,
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host variable clouds of dust and gas,
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include young and very bright stars,
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exhibit a strongly non-uniform structure.
The arms redistribute light in a non-uniform way in different directions and, along certain lines of sight, they cause scattering and local enhancement of the brightness.
3.5. Stellar halo (Stellar Halo)
The stellar halo is an extended structure composed of:
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very old stars,
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extremely faint in luminosity,
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scattered throughout a large volume surrounding the galactic disk.
Although the individual light contribution of these stars is small, their wide spatial distribution makes the halo a non-negligible component of the total integrated light of the galaxy.
Because it lies along many lines of sight, halo light still enters spectral analysis.
3.6. Summary: importance of the layered structure
These layers:
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have different luminosities,
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have different orbital speeds,
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have different densities,
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and appear along a common line of sight.
Therefore, the light observed at the edge of the galaxy is not only the light coming from the stars located locally at that radius.
This essentially means that:
We never see the speed of “a single layer”; instead, we measure an apparent speed that results from the combination of several layers with different luminosities.
4) Role of light scattering in galactic dust and gas
So far, we have seen that:
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the galaxy has a multilayer structure,
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the observed light is an average of the emission from these layers,
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the line of sight toward the edge of the galaxy passes through several layers.
In this section, we focus on the key mechanism that provides a physical pathway for the “penetration” of central light into the outer regions.
4.1. Interstellar dust as the main scattering medium
Galactic dust consists of extremely small particles (silicates, carbon and other compounds), mainly concentrated in:
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the disk plane,
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the spiral arms.
These grains:
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absorb starlight,
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scatter part of it into other directions,
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and create diffuse light in different regions of the disk.
In such an environment:
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photons emitted from the galactic centre
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can, after multiple scattering events, emerge in directions which, from the telescope’s point of view, correspond to regions recorded as “outer parts of the disk”.
Thus:
Part of the light seen in images of the galactic edge does not necessarily come from the stars actually located there but may be scattered light originating from the centre.
4.2. Role of neutral hydrogen (H I)
In addition to dust, large clouds of neutral hydrogen (H I):
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are abundant in the outer regions of galaxies,
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have relatively low density but occupy a very large volume.
Light scattering in H I is not, by itself, as strong as scattering by dust, but:
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the path of light inside a galaxy is very long,
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and light can pass through several H I clouds,
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even small scattering effects along the light path can add up.
As a result, H I gas plays a cumulative role in building a diffuse light background in the outer regions of the galaxy.
4.3. Diffuse galactic light (Diffuse Galactic Light)
The combined effect of:
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scattering by dust,
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and spreading/scattering in H I gas,
leads to what can be called diffuse galactic light:
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light that does not come directly from a single well-defined star,
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but is produced by the scattering and redistribution of photons in the interstellar medium,
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and which can appear in parts of the image that do not coincide with the true position of the original source.
In the outer regions of a galaxy, this means that:
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part of the light really does come from stars located in that region,
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and another part is scattered light originating from the inner layers.
This “light contamination” can, in Doppler analysis, cause the velocity signature of the inner layers to appear in the spectrum of the outer region.
4.4. Consequences for measuring the rotation speed
If, along a given line of sight:
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the outer stars are faint and relatively slow,
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but scattered light from the very bright central regions of the galaxy (where the orbital speed is higher) enters the same line of sight,
then:
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the resulting spectrum in that region will be dominated by the light from the inner layers,
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the spectral contribution of the outer stars will be washed out in the average.
In that case, the velocity derived from the spectrum reflects the inner dynamics more than the true orbital speed of the edge stars. And the apparent velocity is then pulled towards the velocity of the central layers.
This is precisely the idea that will be explicitly formulated in the next section:
The mixing of light from fast inner layers with light from slower outer layers transfers the Doppler signature of the inner layer to the edge.
5) Formulation of the “layered-light interpretation” (LLI hypothesis)
In this section, the proposed idea is expressed as an explicit, discussable hypothesis. This hypothesis does not attempt to deny the presence of extra mass, but first raises the following question:
Have the apparent velocities at the edge of a galaxy been correctly interpreted, in optical and structural terms, before introducing any new gravitational component?
5.1. Qualitative statement of the hypothesis
The layered-light interpretation hypothesis can be summarised as follows:
The high rotation speed inferred from the light spectrum for the outer regions of galaxies may, to a significant extent, result from the mixing of light from faster inner layers with light from slower outer layers, such that the Doppler effect of the inner layers appears in the spectrum of the edge region and makes the true speed of the outer stars appear larger than it really is.
In other words:
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the light from the inner layers (the centre and thin disk), due to their high brightness and scattering in dust and gas, accounts for a large fraction of the spectrum recorded in the outer regions;
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the light from the outer layers, because of their lower brightness and lower density, contributes less to the final spectrum.
Under these conditions:
The mixing of light from fast inner layers with light from slow outer layers transfers the Doppler signature of the inner layer to the edge.
As a result, the apparent edge velocity plotted on the rotation curve does not necessarily correspond directly to the orbital velocity of the stars actually located in that outer region.
5.2. Simple symbolic formulation
For a given line of sight in the outer region of a galaxy, the observed spectral intensity can be written, to a first approximation, as:
I_obs(λ) ≈ I_out(λ, v_out) + I_in->out(λ, v_in)
where:
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I_out(λ, v_out): light contribution from the stars and gas actually located in the outer region, with orbital speedv_out; -
I_in->out(λ, v_in): light contribution scattered from the inner layers (centre and inner disk) which, due to scattering in dust and gas, appears along the same line of sight and carries the Doppler signature associated with the inner speedv_in.
If
I_in->out >> I_out,
i.e. the inner layers contribute much more light than the truly outer stars, then:
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the observed Doppler spectrum mostly represents
v_in, and only weakly reflects the truev_out.
In practice, the effective speed extracted from the spectrum can be written as a weighted average:
v_eff ≈ (I_out * v_out + I_in->out * v_in) / (I_out + I_in->out).
If I_in->out dominates and v_in > v_out, then:
v_eff ≈ v_in,
and the apparent edge velocity is artificially pulled towards the speed of the inner layers.
5.3. Connection with the flat rotation curve
If this mechanism is active over a significant fraction of the outer radii of the galaxy, then:
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the effective speed
v_eff(r)remains strongly influenced by the inner layers, -
the true speed differences between the various layers are smoothed out in the spectral averaging,
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and the rotation curve constructed from these apparent velocities can become approximately flat, even if the true outer-layer speed
v_out,real(r)actually decreases with radius.
In other words, this hypothesis suggests that:
Part of the flatness of galactic rotation curves may result from light averaging and contamination of the outer-layer spectrum by inner-layer light, rather than necessarily from the presence of unseen mass.
5.4. Scope of the hypothesis
This hypothesis:
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does not categorically deny the existence of dark matter,
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but emphasises a prior methodological point:
Before introducing new gravitational components, we should assess to what extent the apparent edge velocities may be the product of light blending from different galactic layers.
If detailed modelling shows that:
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the contribution of scattered light from the centre,
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and the ratio
I_in->out / I_out,
are sufficient to reproduce the observed flat curves, then part of the galactic rotation problem could be explained without invoking invisible mass.
6) Summary and conclusion
In standard cosmology, the “flat rotation curves of galaxies” are regarded as one of the strongest observational arguments for the existence of dark matter. However, all these conclusions rely on a conceptual chain:
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light received from different regions of the galaxy,
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its conversion into a spectrum and measurement of the Doppler shift,
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interpreting this shift as the local orbital speed,
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computing the dynamical mass from that speed,
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comparing it with the luminous mass,
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and finally inferring missing mass (dark matter).
The layered-light interpretation intervenes in the middle of this chain and raises the question:
To what extent do the velocities extracted from the light spectrum truly represent the dynamics of the outer layers of a galaxy?
6.1. Core results of the hypothesis
Given:
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the multilayer structure of galaxies,
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the dominant brightness of the centre and inner disk,
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the scattering of light in interstellar dust and neutral hydrogen gas,
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and spectral averaging along a single line of sight (beam smearing),
the present hypothesis proposes that:
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The light recorded from the edge region of a galaxy is a combination of emission from the outer stars and scattered light from the inner layers.
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If the light contribution from the inner layers exceeds that of the truly outer stars, then the Doppler signature of the inner layers will appear in the spectrum of the outer region.
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In such a case, the effective velocity extracted from the spectrum is closer to the speed of the inner layers than to the true speed of the outer orbits.
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This mechanism can produce an artificial flattening of the rotation curve, without necessarily requiring the addition of unseen mass.
6.2. Position of this hypothesis in the dark-matter discussion
This hypothesis does not claim to be a complete replacement for all dark-matter models, nor does it categorically deny the possible existence of dark matter.
Rather, it emphasises a methodological point:
Before concluding that a new mass component exists in the Universe, we must, as far as possible, ensure that the velocities inferred from the light spectrum faithfully represent the actual dynamics of the layer to which they are being assigned.
If optical and structural effects (layer blending, scattering in dust, diffuse luminosity) are not carefully included in the modelling of rotation curves, then part of the “missing mass” might in fact arise from an incomplete or biased interpretation of the light signals, and may, at least in part, be the result of a misinterpretation of light signals rather than the absence of a new material component.
6.3. Research outlook
The layered-light interpretation is not a fully developed model based on numerical simulations and detailed calculations, but rather:
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a conceptual framework,
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and an open question for future research.
Possible directions for further work (only mentioned here, not developed) include:
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numerical modelling of radiative transfer in a dusty, multilayer galactic disk,
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quantitative estimation of the contribution of scattered light from the central regions,
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simulation of apparent rotation curves in the presence of diffuse luminosity,
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systematic comparison between dusty galaxies and dust-poor galaxies.
The aim of this hypothesis is to show that:
Even at a very preliminary level, one can construct scenarios in which part of the “dynamical anomaly” attributed to dark matter actually has its origin in optics and in the multilayer structure of galaxies.
In this sense, the hypothesis is not the end of the discussion, but an invitation to re-examine in more detail the relationship between light, structure and dynamics in spiral galaxies.
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Younes HASSANABADI