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Michael S. Turner

Publications and source records attributed to Michael S. Turner.

At least 19 recordsLinked to original sources

DESI Dark Secrets

We critically examine the results of the Dark Energy Spectroscopic Instrument (DESI), which provide evidence that dark energy may not be quantum vacuum energy. We find that the best-fit $w_0w_a$ models for dark energy, which underpin the claim, have unusual behavior. They achieve a maximum energy density around $z\simeq 0.5 $ and rapidly decrease before and after (this redshift is also the pivot point for the DESI results). We show that this could be explained by the fact that the $w_0w_a$ parameterization is limited in its ability to model dark energy as it only allows four generic behaviors -- monotonically increasing or decreasing, or with a maximum or minimum -- and $w_a \not= 0$ and $w=-1$ can only be achieved at a minimum or maximum of the dark energy. Further, $w_0w_a$ is a one-parameter characterization of scalar-field models and it cannot represent them to the precision needed for the DESI results. We explore scalar-field models characterized by one dimensionless parameter $β$, which for $β\rightarrow 0$, reduce to $Λ$CDM. None of these models fit the DESI data significantly better than $Λ$CDM or as well as the best-fit DESI $w_0w_a$ models. We also examine the CMB and SN data that strengthen the DESI case for evolving dark energy. The combination of DESI, CMB, and SN data favors a 95\% credible interval $β= 0.33 - 0.96$, providing weak evidence for a scalar-field explanation for dark energy. While the DESI data prefer $w_0w_a$, the SN data prefer a scalar field, and together they favor a $w_0w_a$ model. Finally, the unusual behavior of the best-fit DESI $w_0w_a$ models could arise due to the matter density not varying as expected or an unaccounted-for component of energy density in the Universe. In sum, the evidence for evolving dark energy is intriguing but not conclusive, and at this point, the DESI results raise more questions than they answer.

astro-ph.CO

Particle Dark Matter in the 1980s and 1990s

In 1980, the Universe was made of stars, cosmology was the province of less than 100 astronomers, the Hubble constant was only known to within a factor of two, and the hot big bang was the ``the standard model of cosmology.'' Particle physics was a thriving enterprise concerned with the inner space of quarks, leptons and the strong, weak and electromagnetic interactions. The Standard Model was newly established and the aspirations were for a ``grand unification'' of the forces and particles. By 2000, the agendas of inner space and outer space were inextricably linked, and $Λ$CDM with its inflation, particle dark matter and dark energy -- and a Hubble constant reliably known to better than 10\% -- was the new standard model. The big questions connecting inner space and outer space included the origin of ordinary matter, the identity of dark matter, the nature of dark energy, and an understanding of the origin of space, time and the Universe. Particle dark matter, the idea that the bulk of the mysterious dark matter is a new, long-lived or stable elementary particle, played a central in bringing together inner space and outer space, and today is still a hot topic in both fields.

astro-ph.CO

The DESI results impact the local determination of $H_0$

Measurements of baryon acoustic oscillations (BAO) by the Dark Energy Spectroscopic Instrument (DESI) have revealed evidence for dark energy that evolves. If local distance measurements are analyzed with the $w_0w_a$ models preferred by the DESI measurements, the value for the Hubble constant can be as much as $2.5\,\mathrm{km\,s^{-1}Mpc^{-1}}$ smaller than the value obtained assuming $Λ$CDM. When these $w_0w_a$ models are further constrained by cosmic microwave background (CMB) and type Ia supernova (SNIa) data, the downward shift is $1.1 \pm 0.38\,\mathrm{km\,s^{-1}Mpc^{-1}}$ (DESI + CMB) and $0.5 \pm 0.1\,\mathrm{km\,s^{-1}Mpc^{-1}}$ (DESI + CMB + SNIa). The dependence of local determinations of $H_0$ on the background cosmology, combined with the fact that the low-redshift cosmology is not well constrained, is relevant to the Hubble tension.

astro-ph.CO

$Λ$CDM: The path forward

The current cosmological paradigm, $Λ$CDM, is characterized its expansive description of the history of the Universe, its deep connections to particle physics and the large amounts of data that support it. Nonetheless, $Λ$CDM's critics and boosters alike agree on one thing: it is the not the final cosmological theory and they are anxious to see it replaced by something better! After reviewing some of the impactful events in cosmology since the last \Le Workshop, I focus on the role that the recent evidence for evolving dark energy may play in getting cosmology that better theory.

astro-ph.CO

Everyone wants something better than $Λ$CDM

The current cosmological paradigm, $Λ$CDM, is characterized its expansive description of the history of the Universe, its deep connections to particle physics and the large amounts of data that support it. Nonetheless, $Λ$CDM's critics argue that it has been falsified or must be discarded for various reasons. Critics and boosters alike do agree on one thing: it is the not the final cosmological theory and they are anxious to see it replaced by something better! I review the status of $Λ$CDM, provide my views of the path forward, and discuss the role that the ``Hubble tension'' might play.

astro-ph.CO

Quantifying the uncertainty in the time-redshift relationship

The age of the Universe at a given redshift is a fundamental relationship in cosmology. For many years, the uncertainties in it were dauntingly large, close to a factor of 2. In this age of precision cosmology, they are now at the percent level and dominated by the uncertainty in the Hubble constant. The uncertainties due to the parameters that describe the current cosmological model, $Λ$CDM, are much less important. In decreasing order they are: uncertainty due to the matter density $Ω_M$ around 0.9\% for $z> 3$; uncertainty due to the dark energy equation-of-state parameter $w$, less than 0.3\% for $z>3$; and uncertainty due to the curvature parameter $Ω_k$, at most 0.07\%.

astro-ph.CO

Understanding BBN: the physics and its history

Big-bang nucleosynthesis (BBN), today a pillar of modern cosmology, began with the trailblazing 1948 paper of Alpher, Bethe and Gamow. In it, they proposed non-equilibrium nuclear processes in the early Universe ($t \sim 1000\,$sec) and an early radiation-dominated phase to explain the abundances of all the chemical elements. Their model was fundamentally flawed, but initiated a complex and interesting path to the modern theory of BBN, which explains only the abundances of the lightest chemical elements (mostly $^4$He) and the discovery of the cosmic microwave background (CMB). The purpose of this paper is to clarify the basic physics of BBN, adding some new insights, and to describe how the modern theory developed. I finish with a discussion of two misunderstandings about BBN that still persist and the tale of the pre-discovery predictions of the temperature of the CMB and the missed opportunity it turned out to be.

astro-ph.CO

The Road to Precision Cosmology

The past 50 years has seen cosmology go from a field known for the errors being in the exponents to precision science. The transformation, powered by ideas, technology, a paradigm shift and culture change, has revolutionized our understanding of the Universe, with the $Λ$CDM paradigm as its crowning achievement. I chronicle the journey of precision cosmology and finish with my thoughts about what lies ahead.

astro-ph.CO

The third cosmological paradigm

I begin by briefly discussing the first two cosmological paradigms, the hot big-bang model and $Λ$CDM. In discussing the third paradigm, I focus on the issues it must address, what its aspirations should be, and how it might be initiated. I end with a brief history of my collaborations with Frank Wilczek.

astro-ph.CO

$Λ$CDM: Much more than we expected, but now less than what we want

The $\rmΛ$CDM cosmological model is remarkable: with just 6 parameters it describes the evolution of the Universe from a very early time when all structures were quantum fluctuations on subatomic scales to the present, and it is consistent with a wealth of high-precision data, both laboratory measurements and astronomical observations. However, the foundation of $\rmΛ$CDM involves physics beyond the standard model of particle physics: particle dark matter, dark energy and cosmic inflation. Until this `new physics' is clarified, $\rmΛ$CDM is at best incomplete and at worst a phenomenological construct that accommodates the data. I discuss the path forward, which involves both discovery and disruption, some grand challenges and finally the limits of scientific cosmology.

astro-ph.CO

Diffusion-limited Relic Particle Production

We examine the thermal evolution of particle number densities in the early universe when the particles have a finite diffusion length. Assuming that annihilations are impossible when the mean separation of the particles is larger than their diffusion length, we derive a version of the Boltzmann equation for freeze out in this scenario and an approximate solution, accurate to better than 2\%. The effect of a finite diffusion length is to increase the final relic freeze-out abundance over its corresponding value when diffusion effects are ignored. When diffusion is limited only by scattering off of the thermal background, and the annihilation cross section is bounded by unitarity, a significant effect on the freeze-out abundance requires a scattering cross section much larger than the annihilation cross section. A similar effect is demonstrated when the relic particles are produced via the freeze-in mechanism, but in this case the finite diffusion length is due to the scattering of particles that annihilate into the relic particle of interest. For freeze in, the effect of a finite diffusion length is to reduce the final relic particle abundance. The effects of a finite diffusion length are most important when the scattering cross section or the relic mass are very large. While we have not found a particularly compelling example where this would affect previous results, with the current interest in new dark matter candidates it could become an important consideration.

astro-ph.CO

Nuclear Kinetic Equilibrium During Big Bang Nucleosynthesis

Sasankan et al, have recently claimed that there are significant deviations in the phase-space distributions of the kinetic energies of nuclei from the Maxwell-Boltzmann form usually assumed in BBN, and further, that these deviations lead to big changes in the predicted light-element abundances. Solving the relativistic Boltzmann equation perturbatively, we explicitly show that these deviations are not 20% as claimed, but rather are about 10^-17 in size and hence cannot significantly alter the predicted light-element abundances. We discuss and compute two related effects: O(0.1%) corrections to the kinetic distributions of nuclei that arise from small relativistic corrections to the MB distribution and a much smaller effect, nuclear kinetic drag, which arises from the heat transferred from the EM plasma to nuclei that is needed to maintain kinetic equilibrium.

hep-ph

Dibaryons cannot be the dark matter

The hypothetical $SU(3)$ flavor-singlet dibaryon state $S$ with strangeness $-2$ has been discussed as a dark-matter candidate capable of explaining the curious 5-to-1 ratio of the mass density of dark matter to that of baryons. We study the early-universe production of dibaryons and find that irrespective of the hadron abundances produced by the QCD quark/hadron transition, rapid particle reactions thermalized the $S$ abundance, and it tracked equilibrium until it "froze out" at a tiny value. For the plausible range of dibaryon masses (1860 - 1890 MeV) and generous assumptions about its interaction cross sections, $S$'s account for at most $10^{-11}$ of the baryon number, and thus cannot be the dark matter. Although it is not the dark matter, if the $S$ exists it might be an interesting relic.

hep-ph

Beyond H_0 and q_0: Cosmology is no longer just two numbers

For decades, H_0 and q_0 were the quest of cosmology, as they promised to characterize our "world model" without reference to a specific cosmological framework. Using Monte Carlo simulations, we show that q_0 cannot be directly measured using distance indicators with both accuracy (without offset away from its true value) and precision (small error bar). While H_0 can be measured with accuracy and precision, to avoid a small bias in its direct measurement (of order 5%) we demonstrate that the pair H_0 and Omega_M (assuming flatness and w = -1) is a better choice of two parameters, even if our world model is not precisely LambdaCDM. We illustrate with analysis of the Constitution set of supernovae and indirectly infer q_0 = -0.57+/-0.04. Finally, we show that it may be possible to directly determine q_0 with both accuracy and precision using the time dependence of redshifts ("redshift drift").

astro-ph.CO

Cosmic Acceleration, Dark Energy and Fundamental Physics

A web of interlocking observations has established that the expansion of the Universe is speeding up and not slowing, revealing the presence of some form of repulsive gravity. Within the context of general relativity the cause of cosmic acceleration is a highly elastic (p\sim -rho), very smooth form of energy called ``dark energy'' accounting for about 75% of the Universe. The ``simplest'' explanation for dark energy is the zero-point energy density associated with the quantum vacuum; however, all estimates for its value are many orders-of-magnitude too large. Other ideas for dark energy include a very light scalar field or a tangled network of topological defects. An alternate explanation invokes gravitational physics beyond general relativity. Observations and experiments underway and more precise cosmological measurements and laboratory experiments planned for the next decade will test whether or not dark energy is the quantum energy of the vacuum or something more exotic, and whether or not general relativity can self consistently explain cosmic acceleration. Dark energy is the most conspicuous example of physics beyond the standard model and perhaps the most profound mystery in all of science.

astro-ph

What Do We Really Know About Cosmic Acceleration?

Essentially all of our knowledge of the acceleration history of the Universe - including the acceleration itself - is predicated upon the validity of general relativity. Without recourse to this assumption, we use SNeIa to analyze the expansion history and find (i) very strong (5 sigma) evidence for a period of acceleration, (ii) strong evidence that the acceleration has not been constant, (iii) evidence for an earlier period of deceleration and (iv) only weak evidence that the Universe has not been decelerating since z~0.3.

astro-ph

The Cosmology of Generalized Modified Gravity Models

We consider general curvature-invariant modifications of the Einstein-Hilbert action that become important only in regions of extremely low space-time curvature. We investigate the far future evolution of the universe in such models, examining the possibilities for cosmic acceleration and other ultimate destinies. The models generically possess de Sitter space as an unstable solution and exhibit an interesting set of attractor solutions which, in some cases, provide alternatives to dark energy models.

astro-ph

Measuring and Understanding the Universe

Revolutionary advances in both theory and technology have launched cosmology into its most exciting period of discovery yet. Unanticipated components of the universe have been identified, promising ideas for understanding the basic features of the universe are being tested, and deep connections between physics on the smallest scales and on the largest scales are being revealed.

astro-ph