I Can’t Sleep - Dark Matter | Soothing Bedtime Reading for Sleep
Episode Date: July 21, 2024Drift off with this calm bedtime reading on dark matter, created to bring peace and ease insomnia or sleepless nights. In this gentle episode, Benjamin explores the mystery of dark matter—what scien...tists know, what remains unknown, and why it plays such an important role in understanding the universe. His steady, soothing voice offers comfort without whispers or hypnosis, just calm, fact-filled narration to help quiet the mind. Whether you’re battling anxiety, stress, or restlessness, this peaceful reading invites you to press play, relax, and let your thoughts fade as you drift into sleep. Want More? Request a Topic: https://www.icantsleeppodcast.com/request-a-topic Ad-Free Episodes: https://icantsleep.supportingcast.fm/ Shop Sleep-Friendly Products: https://www.icantsleeppodcast.com/sponsors Join the Discussion on Discord: https://discord.gg/myhGhVUhn7 This content is derived from the Wikipedia article on Dark Matter, available under the Creative Commons Attribution-ShareAlike (CC BY-SA) license. Read the full article: Wikipedia – Dark Matter. Happy sleeping! Learn more about your ad choices. Visit megaphone.fm/adchoices
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Welcome back or welcome to the I Can't Sleep Podcast, where I read random articles from across
the web to bore you to sleep with my soothing voice. I'm your host, Benjamin Boster.
Today's episode is from a Wikipedia article titled Dark Matter.
In astronomy, Dark Matter is a...
is a hypothetical form of matter that appears not to interact with light or the electromagnetic field.
Dark matter is implied by gravitational effects, which cannot be explained by general relativity,
unless more matter is present than can be seen.
Such effects occur in the context of formation and evolution of galaxies,
gravitational lensing, the observable universe's current structure, mass position in galactic,
galactic collisions, the motion of galaxies within galaxy clusters, and cosmic microwave background
and isotropies. In the standard Lambda CDM model of cosmology, the mass energy content of the
universe is 5% ordinary matter, 26.8% dark matter, and 68.2%, a form of energy known as dark energy.
Thus, dark matter constitutes 85% of the total mass,
while dark energy and dark matter constitute 95% of the total mass energy content.
Dark matter is not known to interact with ordinary barionic matter and radiation,
except through gravity, making it difficult to detect in the laboratory.
The most prevalent explanation is that dark matter is some as yet undiscovered subatomic particle,
such as weakly interactive massive particles,
wimps, or axions.
The other main possibility is that dark matter is composed of primordial black holes.
Dark matter is classified as cold, warm, or hot,
according to its velocity,
more precisely its free streaming length.
Recent models have favored a cold dark matter scenario
in which structures emerge by the gradual accumulation of particles.
Although the astrophysics community generally accepts dark matter's existence,
a minority of astrophysicists intrigued by specific observations
that are not well explained by ordinary dark matter,
argue for various modifications of the standard laws of general relativity.
These include modified Newtonian dynamics,
tensor, vector, scalar, gravity, and entropic gravity.
So far, none of the proposed modified gravity theories
can successfully describe every piece of observational evidence at the same time,
suggesting that even if gravity has to be modified,
some form of dark matter will still be required.
The hypothesis of dark matter has an elaborate history.
In the appendices of the book,
Baltimore lectures on molecular dynamics,
and the wave theory of light, where the main text was based on a series of lectures given in 1884,
Lord Kelvin discussed the potential number of stars around the sun from the observed velocity dispersion of the stars near the sun,
assuming that the sun was 200 to 100 million years old.
He posed what would happen if there were a thousand million stars within one kiloparse of the sun,
at which distance their parallax would be one milo-arc second.
Lord Kelvin concluded, many of our supposed thousand million stars, perhaps a great majority of them, may be dark bodies. In 1906, Henri Poincaray in the Milky Way and theory of gases used the French word matier obscure dark matter in discussing Kelvin's work. He found that the amount of dark matter would need to be less than that of visible matter. The second to suggest the existence of dark matter,
using stellar velocities, was Dutch astronomer Jacobus Capitin in 1922.
A publication from 1930 points to Swedish Newt-Lonmark being the first to realize
that the universe must contain much more mass than can be observed.
Dutch and radio astronomy pioneer Jan Urt also hypothesized the existence of dark matter in 1932.
Uart was studying stellar motions in the local galactic neighborhood
and found the mass in the galactic plane must be greater than what was observed
but this measurement was later determined to be erroneous
in 1933 Swiss astrophysicist Fritz-Wiki
who studied galaxy clusters while working at the California Institute of Technology
made a similar inference
Sviki applied the virile theorem to the comical
cluster and obtained evidence of unseen mass he called dunkel matyr dark matter.
Sviki estimated its mass based on the motions of galaxies near its edge,
and compared that to an estimate based on its brightness and number of galaxies.
He estimated the cluster had about 400 times more mass than what was visually observable.
The gravity effect of the visible galaxies was far too small for such vast orbits,
Thus, mass must be hidden from view.
Based on these conclusions, Sviki inferred some unseen matter provided the mass
and associated gravitation attraction to hold the cluster together.
Sviki's estimates were off by more than an order of magnitude,
mainly due to an obsolete value of the Hubble constant.
The same calculation today shows a smaller fraction,
using greater values for luminous mass.
nonetheless, as Vicky did correctly conclude from his calculation that the bulk of the matter was dark.
Further indications of mass-to-light ratio anomalies came from measurements of galaxy rotation curves.
In 1939, Horace W. Bamcock reported the rotation curve for the Andromeda Nebula,
known now as the Andromeda Galaxy, which suggested the mass to luminosity ratio increases radially.
He attributed it to either light absorption within the galaxy
or modified dynamics in the outer portions of the spiral
and not to the missing matter he had uncovered.
Following Babcock's 1939 report of unexpectedly rapid rotation
in the outskirts of the Andromeda galaxy
and a mass to light ratio of 50
in 1940, Yan Orr discovered and wrote about the large non-visible halo of NGC-311
1960s. Early radio astronomy observations performed by Seth Shostak, later SETI Institute senior astronomer,
showed a half-dozen galaxies spun too fast in their outer regions, pointing to the existence
of dark matter as a means of creating the gravitational pull needed to keep the stars in their orbits.
1970s.
Vera Rubin, Ken Ford, and Ken Freeman's work in the 1960s and 1970s
provided further strong evidence, also using galaxy rotation curves.
Rubin and Ford worked with a new spectrograph to measure the velocity curve of edge-on-spiral
galaxies with greater accuracy.
This result was confirmed in 1978.
An influential paper presented Rubin and Ford's
results in 1980. They showed most galaxies must contain about six times as much dark as visible mass.
Thus, by around 1980, the apparent need for dark matter was widely recognized as a major unsolved
problem in astronomy. At the same time, Rubin and Ford were exploring optical rotation curves.
Radio astronomers were making use of new radio telescopes to map the 21-centimeter line of atomic hydrogen in
nearby galaxies. The radio distribution of interstellar atomic hydrogen often extends to the much
greater galactic distances and can be observed as collective starlight, expanding the sample distances
for rotation curves and thus of the total mass distribution to a new dynamical regime. Early mapping of
Andromeda with the 300-foot telescope at Green Bank and the 250-foot dish at jaw-drill bank
already showed the hydrogen rotation curve did not trace the expected Kepleran decline.
As more sensitive receivers became available, Roberts and Whitehurst, 1975, were able to trace
the rotational velocity of Andromeda to 30 kiloparsex, much beyond the optical measurements.
illustrating the advantage of tracing the gas disk at large radii.
The papers figure 16 combines the optical data,
the clusters of points at radii of less than 15 kiloparsex,
with a single point further out,
with the hydrogen data between 20 and 30 kiloprsecs,
exhibiting the flatness of the outer galaxy rotation curve.
The solid curve peeking at the center is the optical surface density,
while the other curves shows the cumulative mass, still rising linearly at the outermost measurement.
In parallel, the use of interferometric arrays for extragalactic hydrogen spectroscopy was being deployed.
Rogstad and Shostak, 1972, published hydrogen rotation curves of five spirals mapped with the Owens Valley Interferometer.
The rotation curves of all five were very flat.
suggesting very large values of mass to light ratio in the outer parts of their extended hydrogen disks.
1980s
A stream of observations in the 1980s supported the presence of dark matter,
including gravitational lensing of background objects by galaxy clusters,
the temperature distribution of hot gas and galaxies and clusters,
and the pattern of antisotropies in the cosmic microwave background.
According to consensus among cosmologists, dark matter is composed primarily of a not yet characterized type of subatomic particle.
The search for this particle, by a variety of means, is one of the major efforts in particle physics.
In standard cosmological calculations, matter means any constituent of the universe whose energy density scales with the inverse cube of the scale factor, i.e. row is proportionally,
to A to the negative 3.
This is in contrast to radiation,
which scales as the inverse fourth power of the scale factor,
Rho is proportional to A to the negative 4.
And a cosmological constant,
which does not change the respect to A,
Rho is proportional to A to zero.
The different scaling factors for matter and radiation
are a consequence of radiation redshift.
For example, after gradually doubling the diameter of the observable universe via cosmic expansion of general relativity, the scale A has doubled.
The energy of the cosmic microwave background radiation has been halved because the wavelength of each photon has doubled.
The energy of ultra-relativistic particles, such as early era standard model neutrinos, is similarly halved.
The cosmological constant, as an intrinsic property of space, has a constant energy density regardless of the volume under consideration.
In principle, dark matter means all components of the universe which are not visible, but still obey, row, is proportional to A to the negative 3.
In practice, the term dark matter is often used to mean only the non-barianic component of dark matter,
i.e. excluding missing barons. Context will usually indicate which meaning is intended.
The arms of spiral galaxies rotate around the galactic center. The luminous mass density of a spiral galaxy
decreases as one goes from the center to the outskirts. If luminous mass were all the matter,
then we can model the galaxy as a point mass in the center and test masses orbiting around it.
similar to the solar system.
From Kepler's third law, it is expected that the rotation velocities
will decrease with distance from the center similar to the solar system.
This is not observed. Instead, the galaxy rotation curve remains flat as distance from the center
increases. If Kepler's laws are correct, then the obvious way to resolve this
discrepancy is to conclude the mass distribution in spiral galaxies is not similar.
similar to that of the solar system. In particular, there is a lot of non-luminous matter, dark matter,
in the outskirts of the galaxy. Stars and bound systems must obey the virial theorem. The theorem,
together with the measured velocity distribution, can be used to measure the mass distribution
in a bound system, such as elliptical galaxies or globular clusters. With some exceptions,
Velocity dispersion estimates of elliptical galaxies do not match the predicted velocity dispersion
from the observed mass distribution, even assuming complicated distributions of stellar orbits.
As with galaxy rotation curves, the obvious way to resolve the discrepancy is to postulate the
existence of non-luminous matter. Galaxy clusters are particularly important for dark matter studies,
since their masses can be estimated in three independent ways.
From the scatter and radial velocities of the galaxies within clusters,
from x-rays emitted by hot gas in the clusters,
from the x-ray energy spectrum and flux,
the gas temperature and density can be estimated,
hence giving the pressure,
assuming pressure and gravity balance determines the cluster's mass profile.
Gravitational lensing,
usually of more distant galaxies,
can measure cluster masses without relying on observations of dynamics, e.g. velocity.
Generally, these three methods are in reasonable agreement that dark matter outweighs visible matter by approximately 5 to 1.
One of the consequences of general relativity is the gravitational lens.
Gravitational lensing occurs when massive objects between a source of light and the observer
act as a lens to bend light from the source.
One example is a cluster of galaxies lying between a more distant source, such as a quasar, and an observer.
The more mass of an object, the more lensing is observed.
Strong lensing is the observed distortion of background galaxies into arcs when their light passes through such a gravitational lens.
It has been observed around many distant clusters, including ABLE 1689.
By measuring the distortion geometry, the mass of the intervening cluster can be obtained.
In the dozens of cases where this has been done,
the mass to light ratios obtained correspond to the dynamical dark matter measurements of clusters.
Lensing can lead to multiple copies of an image.
By analyzing the distribution of multiple image copies,
scientists have been able to deduce and map the distribution of dark matter around the MACA,
J0-416.1-2403 galaxy cluster.
Weak gravitational lensing investigates minute distortions of galaxies using statistical analyses
from vast galaxy surveys.
By examining the apparent sheer deformation of the adjacent background galaxies,
the mean distribution of dark matter can be characterized.
The mass to light ratios correspond to dark matter
densities predicted by other large-scale structure measurements.
Dark matter does not bend light itself.
Mass, in this case the mass of the dark matter, bends space-time.
Light follows the curvature of space-time, resulting in the lensing effect.
In May 2021, a new detailed dark matter map was revealed by the Dark Energy Survey collaboration.
In addition, the map revealed previously undiscovered filamentary,
structures connecting galaxies by using a machine learning method.
In April 2023, study in Nature Astronomy
examine the inferred distribution of the dark matter
responsible for the lensing of the elliptical galaxy
HS0810 plus 2554,
and found tentative evidence of interference patterns within the dark matter.
The observation of the interference patterns is incompatible
with the WIMPS, but would be compatible with simulations involving 10 to the negative 22 electron
voltaxeons. While acknowledging the need to corroborate the findings by examining other
astrophysical lenses, the authors argued that the ability of axion-based dark matter to resolve
lensing anomalies, even in demanding cases such as HS 081 plus 2554, together with its success and
reproducing other astrophysical observations tilt the balance toward new physics invoking axioms.
Although both dark matter and ordinary matter or matter, they do not behave in the same way.
In particular, in the early universe, ordinary matter was ionized and interacted strongly with radiation via Thompson scattering.
Dark matter does not interact directly with radiation, but it does not interact directly with radiation, but it
does affect the cosmic microwave background, Cmb, by its gravitational potential, mainly on large scales,
and by its effects on the density and velocity of ordinary matter.
Ordinary and dark matter perturbations, therefore, evolve differently with time and leave different
imprints on the Cmb.
The cosmic microwave background is very close to a perfect black body, but contains very small
temperature anisotropies of a few parts in 100,000. A sky map of anisotropies can be decomposed into
an angular power spectrum, which is observed to contain a series of acoustic peaks at near-equal
spacing but different heights. A series of peaks can be predicted for any assumed set of cosmological
patterns by modern computer codes, such as CMB-FAST and C-A-M-B.
and matching theory to data, therefore constrains cosmological parameters.
The first peak mostly shows the density of baryonic matter,
while the third peak relates mostly to the density of dark matter,
measuring the density of matter and the density of atoms.
The CMB anestotropy was first discovered by C-O-B-E in 1992,
though this had two-course resolution to detect the acoustic peaks.
After the discovery of the first acoustic peak by the balloon-born boomerang experiment in 2000,
the power spectrum was precisely observed by WMAP in 2003-2012,
and even more precisely by the Planck spacecraft in 2013-2015.
The results support the Lambda CDM model.
The observed CMB angular power spectrum provides powerful evidence in support of dark matter,
as its precise structure is well fitted by the Lambda CDM model,
but difficult to reproduce with any competing model,
such as modified Newtonian dynamics, M-O-N-D.
Structure formation refers to the period after the Big Bang
when density perturbations collapse to form stars, galaxies, and clusters.
Prior to structure formation, the Friedman Solutions to General Relativity
describe a homogenous universe.
Later, small anisotropies gradually grew and condensed the homogeneous universe into stars, galaxies, and larger structures.
Ordinary matter is affected by radiation, which is a dominant element of the universe at very early times.
As a result, its density perturbations are washed out and unable to condense into structure.
If there were only ordinary matter in the universe, there would not have been enough time for density perturbations to grow,
into the galaxies and clusters currently seen.
Dark matter provides a solution to this problem because it is unaffected by radiation.
Therefore, its density perturbations can grow first.
The resulting gravitational potential acts as an attractive potential well
for ordinary matter collapsing later, speeding up the structure formation process.
The bullet cluster, the result of a recent collision of two galaxy clusters,
provides model-independent observational evidence for dark matter.
Alternatives like modified gravity theories have a difficult time explaining this system
because as apparent center of mass is far displaced from the baryonic center of mass.
Type IA supernovae can be used as standard candles to measure extra-galactic distances,
which can in turn be used to measure how fast the universe has expanded in the past.
Data indicates the universe is expanding at an accelerating rate,
the cause of which is usually described as dark energy.
Since observations indicate the universe is almost flat,
it is expected the total energy density of everything in the universe should sum to one.
Barionic acoustic oscillations B-A-O are fluctuations in the density of the visible barionic matter,
normal matter, of the universe on large scales.
These are predicted to arise in the Lambda CDM model due to acoustic oscillations in the photon baryon fluid of the early universe,
and can be observed in the cosmic microwave background angular power spectrum.
B.A.O.s set up a preferred length scale for baryons.
Has the dark matter in baryons clumped together after recombination,
the effect is much weaker in the galaxy distribution in the nearby universe,
but as detectable as a subtle preference for pairs of galaxies to be separated by 147 megaparsecs,
compared to those separated by 130 to 160 megaparsecs.
This feature was predicted theoretically in the 1990s,
and then discovered in 2005 and two large galaxy redshift surveys,
the Sloan Digital Sky Survey, and the 2DF Galaxy Redshift Survey.
Combining the CMB observations was BAL,
measurements from galaxy redshift surveys provides a precise estimate of the Hubble constant and the
average matter density in the universe. The results support the Lambda CDM model. Large galaxy redshift
surveys may be used to make a three-dimensional map of the galaxy distribution. These maps are
slightly distorted because distances are estimated from observed redshift. The redshift contains a
contribution from the galaxy's so-called peculiar velocity in addition to the dominant Hubble
expansion term. On average, superclusters are expanding more slowly than the cosmic mean,
due to their gravity, while voids are expanding faster than average. In a redshift map,
galaxies in front of a supercluster have excess radio velocity towards it and have redshifts
slightly higher than their distance would imply, while galaxies behind the supercluster
have red shifts slightly low for their distance. This effect causes superclusters to appear
squashed in the radial direction, and likewise voids are stretched. Their angular positions
are unaffected. This effect is not detectable for any one structure since the true shape is not
known, but can be measured by averaging over many structures.
It was predicted quantitatively by Nick Kaiser in 1987, and first decisively measured in 2001
by the 2DF Galaxy Redshift survey.
Results are in agreement with the Lambda-CTM model.
In astronomical spectroscopy, the Lyman Alpha Forest is the sum of the absorption lines
arising from the Lyman Alpha transition of neutral hydrogen
and the spectra of distant galaxies and quasars.
Lyman Alpha forest observations can also constrain cosmological models.
These constraints agree with those obtained with WMAP data.
The exact identity of dark matter is unknown,
but there are many hypotheses about what dark matter could consist of.
Dark matter can refer to any substance which interacts predominantly
via gravity with visible matter, e.g. stars and planets. Hence, in principle, it need not be composed of a new
type of fundamental particle, but could, at least in part, be made up of standard baryonic matter,
such as protons or neutrons. Most of the ordinary matter familiar to astronomers,
including planets, brown dwarfs, red dwarfs, visible stars, white dwarfs, neutron stars, and black
holes fall into this category. Solitary black holes, neutron stars, burned out dwarfs,
and other massive objects that are hard to detect are collectively known as machos.
Some scientists initially hoped that barionic machos could account for and explain all the dark matter.
However, multiple lines of evidence suggests the majority of dark matter is not barionic.
Sufficient diffuse, barionic gas or dust would be
visible when back led by stars.
The theory of Big Bang
nucleosynthesis predicts the observed abundance of the chemical
elements. If there are more baryons,
then there should also be more helium,
lithium, and heavier elements
synthesized during the Big Bang.
Agreement with observed abundances requires that
barionic matter makes up between
4 to 5% of the universe's
critical density.
In contrast, large
scale structure and other observations indicate that the total matter density is about 30% of the
critical density. Astronomical searches for gravitational microlensing in the Milky Way found at most
only a small fraction of the dark matter may be in dark, compact, conventional objects, machos, etc.
The excluded range of object masses is from half the Earth's mass, up to 30 solar masses,
which covers nearly all the plausible candidates.
Detailed analysis of the small irregularities in esotropies in cosmic microwave background.
Observations by WMAP and Planck indicate that around 5-6 of the total matter
is in a form that interacts significantly with ordinary matter or photons only through gravitational
effects.
There are two main candidates for non-barionic dark matter.
hypothetical particles such as axions, sterile neutrinos, weakly interacting massive particles,
whims, supersymmetric particles, atomic dark matter, or geons, and primordial black holes.
Once a black hole ingests either kind of matter, baryonic or not, the distinction is lost.
Unlike baryonic matter, non-barionic particles do not contribute to the formation of the elements
in the early universe.
Big Bang nucleosynthesis.
And so its presence is revealed only via its gravitational effects or weak lensing.
In addition, if the particles of which is composed are supersymmetric, they can undergo annihilation
interactions with themselves, possibly resulting in observable byproducts such as gamma rays
and neutrinos in direct detection.
In 2015, the idea that dense dark matter was composed of primordial black holes,
made a comeback following results of gravitational wave measurements, which detected the merger
of intermediate mass black holes. Black holes with about 30 solar masses are not predicted
to form by either stellar collapse, typically less than 15 solar masses, or by the merger of
black holes in galactic centers, millions or billions of solar masses. It was proposed that
the intermediate mass black holes caused the detected merger formed in the hot, dense, early
phase of the universe due to denser regions collapsing. A later survey of about a thousand
supernovae detected no gravitational lensing events when about eight would be expected if
intermediate mass primordial black holes above a certain mass range accounted for over 60% of
dark matter. However, the study assumed a monochromatic distribution to represent the
LIGO-Virgo mass range, which is inapplicable to the broadly platicic
mass distribution suggested by subsequent James Webb Space Telescope observations.
