books book reviews

books on high energy astrophysics

reviewed by T. Nelson

Score+4

Astrophysics At Very High Energies

by Felix Aharonian, Lars Bergström, and Charles Dermer
Springer, 2013, 361 pages
reviewed by T. Nelson

High energy astrophysics is the study of gamma rays created under the most extreme conditions known in the universe: immense gravitational fields, intense heat, crushing magnetic fields, and colossal shock waves. They interact with the atmosphere to produce a variety of radioactive and non-radioactive particles that can tell us about conditions that existed almost at the beginning of the cosmos.

One of the biggest unsolved questions in astrophysics is what the nature of dark matter could be. The experts in this book give their perspectives on this and related topics in three lengthy chapters.

Felix Aharonian

Cosmic gamma rays below 100 GeV are observable only from satellites, which have modest sensitivity (about 10−12 erg cm−2 / second). Particles and γ-rays more energetic than that (up to 100 TeV) are studied with ground-based Imaging Atmospheric Cherenkov Telescopes or IACTs, which measure the visible light, called Cherenkov radiation, that's produced when a particle exceeds the speed of light in a medium. These detectors, which are basically giant mirrors, pick up showers of photons—tiny flashes of light lasting only a few nanoseconds. At least two detectors 100 meters apart are needed to triangulate on the source and direction of the gamma rays. The number of photons allows calculation of the energy.

The gamma rays come from the most violent objects in the sky: black holes, pulsar-driven nebulae (called plerions), pulsar winds, pulsar microquasars, neutron stars, X-ray binaries, and supernova remnants. These bodies act as particle accelerators via “non-thermal” processes, i.e. nuclear reactions.

Mixed with gamma rays are a variety of charged particles, which while not exactly a nuisance are less informative than gamma rays because they are deflected by magnetic fields during transit, which makes it challenging to determine their origin. There's also a high diffuse thermal background produced by absorption of gamma rays by the interstellar medium, which happens by two important processes: inverse Compton scattering and photon-photon pair production. Absorption features in the spectra of Extragalactic Background Light (EBL) also give information about the formation of galaxies billions of years ago.

These processes are familiar to anyone who works with radiation: bremsstrahlung, or ‘braking radiation’, produced by deceleration of a charged particle; photomeson reactions, in which a proton reacts with a gamma-ray to produce a neutral π meson; photon-photon pair production, where two gamma rays interact to produce an electron and a positron, and so on. If bremsstrahlung is due to circular motion in a magnetic field, it is called synchrotron radiation.

Gamma rays are absorbed and re-emitted by various processes at rates that differ depending on the strength of the magnetic field, the accelerator processes in the star, the magnetic field, and the shock waves, often quite strong, in the atmosphere around it.

Untangling all these different processes is a tremendous challenge: the only information we have is the energy spectrum, so deduction plays a strong role. For instance, protons above 1PeV would be needed to get neutrinos in the 10–100 TeV range, which is the optimal energy for detection by IceCube or KM3NET neutrino detectors, but both of those detectors have low sensitivity, so we might miss them; instead we would have to look for synchrotron X-rays caused by secondary π± meson decay.

The authors are honest about the challenges in analyzing the results:

Remarkably, a tendency of softening [lower energy] of the energy spectrum of gamma-rays with distance from the position of the pulsar has been found in the gamma-ray image of HESS J1825-137 [a pulsar wind nebula near the center of the galaxy]. This is indeed a strong argument in favour of the inverse Compton origin of TeV emission of this source. On the other hand, the TeV gamma-ray luminosity of this source is about 10% of the pulsar spin-down luminosity . . . . This makes quite difficult the interpretation of gamma-ray emission by the current spin-down power of the pulsar. [p.89]

(The name HESS in the pulsar wind nebula HESS J1825-137 refers to the High Energy Stereoscopic System, a cosmic ray observatory in Namibia.) All this logic, which often requires sophisticated computer modeling, can become quite complex, and the reader needs to take copious notes to organize it.

 

Lars Bergström

In the second chapter, Lars Bergström focuses on dark matter. We're now certain, he says, that neutrinos are not the main form of dark matter, but only a small fraction of it. And so he gives us just enough quantum field theory to make us hate it, and then goes on to a brief introduction to SUSY or supersymmetry.

Supersymmetry, says Bergström, would be a beautiful theory if it were not ‘broken’ (by which he means it has a broken symmetry). Breaking must have occurred since no super­sym­met­ric particle has ever been detected and unbroken symmetry would mean they all have the same mass, which they probably don't.

And so he theorizes about what spectral features would be seen and what properties they could have if the various particles existed. For dark matter that means mainly light neutralinos. Neutralinos are linear combinations of neutral gauge bosons called gauginos and neutral higgsinos, so there are four (or now maybe five) states: if they are small, they're gaugino-like; if they're big, they're higgsino-like. There are also squarks, gluinos, axions, axinos, Q-balls, and WIMPS (the last being a generic term meaning weakly-interacting massive particles, not part of any specific theory, so forget that one).

You would be forgiven for never having heard of any of these particles: as I mentioned, not one has ever actually been detected in any experiment on Earth or in any cosmic rays. But the theory, known as the MSSM (minimal supersymmetric extension of the Standard Model), says that light neutralinos have to be lighter than 7 TeV to stay within the upper limit calculated from the WMAP data. So some, er, “fine-tuning” is necessary and we can make a wild guess estimate of < 600 GeV, or about 638 times as heavy as a neutron (there is still ample speculation about the mass in the literature).

One question laymen always ask is whether dark matter could be black holes. Bergström says no: black holes come in three sizes: small (2–20 solar masses); medium (a few million solar masses) such as Sgr A* in the center of the Milky Way; and big (a few billion solar masses), as in active galactic nuclei (AGN). Even added together, they are way too small. The galactic ‘halos’, i.e., stars and dust, around these AGN black holes are a thousand times heavier than the AGNs. Anyway, black holes are not really black, so they're not “dark.” (And of course they aren't holes, either.)

Bergström says the MSSM has over a hundred free parameters. Results from the Linear Hadron Collider have ruled out wide ranges of masses for the supersymmetric particles, so a pessimist might say the walls are closing in on MSSM. An optimist would say they're zeroing in on the possibilities. And Bergström is most definitely an optimist.

Charles Dermer

The third chapter focuses on categorizing various objects. The author admits that it was mostly out of date when it was incorporated into this book, but it's still a great way to become familiar with objects including some of the 1900 pulsars that have been identified through radio surveys, such as the Crab Nebula, Vega pulsar, and Cygnus X-3. Some of the theory presented in the first chapter is also repeated, but from a different angle and a bit more math.

Nice color images of gamma-ray sky maps, color graphs, and a good index, but since publication better γ-ray data have come in, so read it for the background theory more than for the astronomy.

aug 13, 2024

Score+4

Dark Matter: Evidence, Theory, and Constraints

by David J.E. Marsh, David Ellis, and Viraf M. Mehta
Princeton University Press, 2024, 328 pages
reviewed by T. Nelson

How do you write a scientific book on something that may or may not be real? In many ways, it's like starting a new religion: your first task is to convince people the entity exists. And so nearly half of this book (37.6% if you want to be precise) is a series of proofs intended to show that dark matter really exists.

We've known for almost a century that galaxies rotate too fast. In 1933, Fritz Zwicky measured the Doppler velocity dispersion in the Coma galaxy Cluster. Instead of 80 km/s, as he calculated from the visible mass, the dispersion was 12.5 times faster, indicating that the total mass was 200 times more than the visible mass. Similar but smaller discrepancies were found in other celestial bodies, including Andromeda and the Milky Way.

For a long time it was assumed that something was wrong with the models. The most popular model for the density profile of a galaxy is the Navarro-Frenk-White (NFW) model, which defines its “halo” or visible profile as having a slope of 1/r at small radius, 1/r2 at medium radius, 1/r3 at a large radius. The easiest thing to do was to tweak the NFW model by adding dark matter. The density of dark matter you'd need, in terms of particles per cubic centi­meter, would be infinitesimal: a grand total of one, creating a density about 1 / 3.346×1022 that of water. Those few particles over galactic distances add up to an astronom­ic­ally big mass. (The authors calculate it wrong in the book, but for sure it's tiny. There are other minor errors: one TeV is 1012 eV, not 109 as they say on page 7.)

Alternative theories predate even Zwicky, originating with Einstein's cosmological constant. The strongest evidence for the dominant theory today, called ΛCDM, where Λ (lambda) is the cosmological constant and CDM means cold dark matter, comes from measurements of the cosmic microwave background (CMB). The authors write:

The existence of a new, very cold, and almost pressureless degree of freedom is required to explain the detailed shape of the CMB anisotropies and to achieve consistency with the observed distribution of galaxies. Cosmological measurements are extremely statistically accurate and measure the required density of DM [dark matter] to within 1%.

At redshift (z) below 1100, after recombination happens, baryons behave like dark matter: they're decoupled from photons and are non-relativistic. At earlier times, where z is above 1100, baryons are tightly coupled to photons. This is important to the CMB because the sub-horizon modes oscillate in baryon acoustic oscillations. The term sub-horizon refers to length scales within the physical reach of some perturbation in the CMB. There is also a damping term called Silk damping or diffusion damping, which comes from Thomson scattering and the non-zero photon quadrupole. These factors go into elaborate computer simulations to calculate the CMB power spectrum, which displays the amount of correlation in the temperature as a function of angular scale.

The CMB power spectrum, shown in the graph on page 102, has many peaks and valleys. Small-scale modes (i.e., peaks) create galaxies. Computer simulations with and without CDM show huge differences in the spectrum, particularly at an angular scale (called a multipole) of 200, which is the angular size of the acoustic horizon as measured at the redshift where decoupl­ing occurs.

The authors say that logarithmic growth of CDM perturb­ations makes CDM necessary for galaxy formation. In the absence of dark matter (DM), acoustic oscillations would have large amplitude. With DM they're smaller because DM provides gravitational potential wells for the baryon-photon fluid. Thus, the authors say, dark matter is needed to reconcile the theory of structural growth of galaxies due to gravitational instability with the observed fluctuation amplitude in the CMB.

Dark energy

This is not to be confused with dark energy. Dark energy is a hypo­thet­ical force thought to accelerate expan­sion of the universe and is totally different from dark matter. In some ways they're opposites. Dark matter is thought to make up 27% of the matter-energy content of the universe, while dark energy takes 69%, leaving only four to five percent as what we can see.

The news media are saying a new paper has proved dark energy is not real. The ‘new’ theory is David Wiltshire's “timescape” model, which has actually been floating around for a number of years. The new paper isn't proof, but another model based on supernova data that tweaks the FLRW model used by ΛCDM. Dark energy was also recently challenged in a 109-author article based on data of early supernovae.

Pop science sites all over the Internet have suddenly decided that Wiltshire's most recent paper is a break­through: “Huge if true” says one. “Debunked” says another. NASA still says they're sure dark energy exists. It's remarkable how fast “It's just a placeholder for something we don't understand” changed into “We're sure it's real.” If two-thirds of the universe was all an artifact, people were too confident in the old model. It's reasonable to ask how we can trust the new one. Maybe if there is no dark energy, the model is still wrong and there's no dark matter either.

MOND

One possible alternative, which the authors strongly oppose, is modified Newtonian dynamics or MOND. Instead of changing NFW, which most people have never heard of, MOND changes the famous Einstein-Hilbert action, which is S = d4x √−gR (where R is the Ricci scalar), by adding two new fields. Physicists regard making ad hoc changes to a formula for every new thing that comes along as too risky. But either our fundamental equations of gravity need tweaking, or the total amount of matter we can detect is only a small fraction of what's out there.

There's considerable resurging interest in MOND (see here and here). A recent article by Stacy S. McGaugh et al. claims that MOND predicted the early emergence of massive galaxies and clusters of galaxies, while ΛCDM did not.

There are many other formulations of modified gravity besides MOND, including a “post-Friedmann” frame­work and Hořava-Lifshitz gravity. Philip Bull et al. summarize their status. Giving fair treatment to these blasphemers rather than focusing exclusively on ΛCDM would have strengthened the book.

If you reject the idea of modifying the theory of gravity, you have an even worse problem: there are no known particles with the right properties.

The Standard Model

Before speculating on the particles, the authors provide a very nice overview of the Standard Model (SM) and Higgs mechan­ism. They break down each of the terms in the formulas such as the SM Lagrangian and explain individually what they do. They also explain spinors and why they're important for particles with left or right handedness; and what a gauge transformation is and why there can be no such a thing as a right-handed neutrino.

If you've been looking for a clear description of particle physics math and don't have any strength left to lift a copy of Weinberg's excellent two-volume set, get this book and a copy of Penrose's Road To Reality today.

Neutrinos

At this point the book turns to categorizing the particles in the ΛCDM gospel. Neutrinos with a mass greater than 12 eV would be too heavy to account for dark matter. But they must be less than 1 eV to be consistent with the CMB. So ordinary neutrinos are ruled out. The authors drop a big hint about what they're really thinking. The theory says there's no such thing as a right-handed neutrino, but if there were, it wouldn't interact with photons or with any known particles. (This is heresy and they'd be crucified if they proposed it, but . . . hint hint!)

WIMPs

Some physicists suggest that dark matter could be weakly-interacting massive particles or WIMPs. The “wimp miracle” is that the numbers calculated for WIMPs are all at the exact scale needed for relic density. Sadly, WIMPS, like right-handed neutrinos, face the challenge of non-existence, which may be an insurmountable obstacle: in order for WIMPs to exist, we must invoke supersymmetry, which postulates a large number of gigantic hypothetical particles (see Astrophysics At Very High Energies reviewed at left).

Axions and primordial black holes

Axions are particles with such a low mass they'd be extremely hard to detect if even they existed, and—even worse—the theory doesn't favor any particular mass, so nobody knows where in the spectrum to look. Primordial black holes, which are much smaller than ordinary everyday black holes (which are ruled out), likewise face the challenge of non-existence. If they existed, they'd have to form by some unknown ‘exotic mechanism’ (such as divine intervention).

People have searched for primordial black holes and concluded that their mass is most likely between 10−15 and 10−11 solar masses, or at least two billion metric tons. The authors say such tiny black holes are still big enough to cause a Richter 4 earthquake if they smashed into the Earth, so they should be fairly easy to detect if they exist.

So the authors return to their favorite candidate: the sterile neutrino. These hypothetical uncharged, invisible particles are only affected by gravity, so even if they exist we might never detect them. But if not, that would mean we're running out of candidates. Astrophysicists are almost desperate enough to propose spin-2 gravitons from the Randall-Sundrum model of a five-dimensional brane in string theory. As usual, the science popularizers are misinterp­ret­ing that as matter from “another dimension.” That's not exactly what it means. But string theory? That's the work of the Devil.

Unless someone finds the particle, there's a good chance that the premise of this book—that dark matter exists—will have to be abandoned. If so, it wouldn't be a failure, but a good example of self-correction in science. There are Big Clues: why would some galaxies have more dark matter than others? The theory doesn't say. Simulations can prove a theory wrong, but they can never prove a theory is correct, nor can they prove that something is real. Maybe more radio observations are needed, or maybe quantum gravity will come to the rescue. This book gives you the background to understand the science when somebody figures out the answer.

jan 05, 2025. last updated jan 11, 2025