Friday 26th of April 2024

the luck and accidental opportunism of nature…..

 

 In 1898, Hermon Bumpus gathered 136 house sparrows immobilized by an ice storm, noting that the averages of several morphological traits differed between survivors and nonsurvivors. This was one of the first attempts to measure the phenotypic selection component of Charles Darwin’s thesis, that adaptation is driven by heritable traits that affect fitness.

 

Since then, a vast literature on quantifying associations between trait values and fitness has emerged (1). The quantification of Darwin’s second evolution component—that such traits are heritable—required the development of quantitative genetics by Ronald Fisher in 1918 (2). Although the selection and genetics components can be combined to determine the expected change in any trait, of greater interest is the general adaptive potential of a population. On page 1012 of this issue, Bonnet et al. (3) present a meta-analysis of 19 studies showing the abundance of heritable variations in fitness and the potential for adaptation.

Fisher famously stated that “natural selection is not evolution,” meaning that if a trait is not heritable, no amount of selection will result in a change in the offspring of surviving parents. Fisher’s key to deciphering heritability was noting that parents pass along specific variants of a gene (alleles), rather than entire genotypes, to their offspring. The sum of all the single-allele effects for a given trait carried by an individual is defined as their breeding value (BV) for that trait. BVs are best understood in terms of deviations from the mean, so that a random individual has an expected BV of zero, which implies that its offspring will, on average, be average. The expected deviation of an offspring from the population mean is simply the average of the BVs of its parents. As a result, parents with exceptional BVs have offspring that, on average, deviate substantially from the population mean. Conversely, offspring from parents with modest BVs fall close to the mean.

The spread of individual BVs is a measure of the evolutionary potential of a trait. This is the basis of the additive variance of a trait, defined as the variance among BVs for that trait in a given population. If this variance is small, offspring have very little resemblance to their parents, whereas if it is large, exceptional parents tend to have exceptional offspring. If there is no additive variance for a trait, it will not evolve. More generally, if there is no additive variance in fitness, no trait will genetically respond to selection.

 

Thus, one of the holy grails in evolutionary genetics is to estimate the additive variation in fitness itself, which gives a general measure of the evolutionary potential of a population and places limits on the maximal response for any trait. This challenging estimation problem was tackled by Bonnet et al. using a collection of 19 long-term vertebrate population studies (covering a total of 561 cohorts and ∼250,000 individuals) from North America, Europe, Africa, and Oceania. The meta-analysis showcases an immense, but doable, effort in estimating this fundamental evolutionary parameter.

Bonnet et al. used total number of offspring, also known as lifetime reproductive success (LRS), as the measure for the fitness of an individual. The LRS parameter is converted to relative fitness simply by dividing LRS for an individual by the average LRS of the population, which allows for quantifiable comparisons across studies. In statistical terms, if a population shows a significant additive variance in fitness among its individuals, this implies that parents with higher LRSs than the population average also have a high BV for LRS, and thus their children also tend to have high LRSs.

Estimating BVs, and thus additive variance, is a common problem in modern animal breeding, built around using pedigree information. A BV exists even when the trait is not displayed, as it is a measure of how exceptional an offspring from that parent would be, if produced. In the case of milk production, information on the BV of a bull is provided by the observed yields of his mother, sisters, and daughters. The same pedigree machinery used by breeders can, in theory, be applied in natural populations to estimate the additive variance of any measured trait. Pedigrees for natural populations can be constructed using molecular markers, and closed populations of vertebrates are well suited for such analyses. Even with perfect pedigrees, the transition of pedigree methods from a large and well-structured domesticated population to a small wild population has been somewhat rocky (4). Domesticated pedigrees tend to be much deeper and denser than those for natural populations, resulting in greater precision in BV estimates. Furthermore, fitness is a problematic trait for standard pedigree methods, which assume trait values are continuous and follow a Gaussian distribution, whereas fitness data are highly discrete—a parent can only have an integer number of offspring, with a large point mass at zero, that is, individuals with zero offspring. Although there have been a few attempts to estimate the additive variance in fitness in wild populations using standard pedigree methods, the failure of the Gaussian assumption suggests that these are likely rather biased.

Bonnet et al. extended these pedigree methods by using a discrete Poisson distribution with an inflated zero value instead of a Gaussian and provided a much better fit for the fitness data. Using the improved fitting, their resulting average estimate of the additive variance in relative fitness, VA(w), was two- to fourfold larger than previous values. To put it in a more tangible context, this means that if the fitness of a population drops by a third, it would take roughly 10 generations to recover back to normal fitness levels. Hence, populations with shorter generation times might have a better chance to somewhat mitigate anthropogenic changes.

In nature, the target of selection is almost certainly a constantly shifting, high-dimensional (i.e., multi-trait) phenotype that may poorly project onto individual traits or even a set of traits. Most studies of adaptation are structured around some assumed edifice of traits that affects fitness. A poor choice of traits can give a misleading impression of population adaptation. Fortunately, an estimate of VA(w) provides an upper bound, and therefore a maximal possible change in any trait independent of selection. For example, a typical trait heritability of 0.3 will mean that 30% of the trait variation is due to variance in BVs, and the maximal possible change in the average value of a trait in the population is about one standard deviation every four generations. A more reliable way to estimate VA(w) can help to better quantify the nature of selection and the robustness of a population to major environmental changes.

 

SCIENCE

26 May 2022

Vol 376, Issue 6596

 

 

 

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repeats…...

Nature is about repeats and rhythms through "abstract harmonics" of irrelevant numbers.

67% are true

33% are not committed (random)

0% are false

 

MORE TO COME...

 

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of temperature and mass…….

Cosmological observations from the Early Universe provide an invaluable probe of Physics Beyond the Standard Model (BSM). Observations of the Cosmic Microwave Background (CMB), epitomized by the Planck mission [1] and further developed e.g. by the ACT [2] and SPT [3] collaborations, paint a picture of a Universe that is dominated by non-baryonic dark energy and dark matter, well-described by the ΛCDM model [4–6]. Equipped with the CMB inference of the small cosmological baryonic abundance, ΩB ∼ 4%, the theory of Big Bang Nucleosynthesis (BBN) within the Standard Model (SM) of Particle Physics is highly predictive, and confronted with accurate measurements of primeval elements such as the mass density fraction of helium-4, YP, and the relative abundance of deuterium, D/H, offers important constraints on New Physics (NP) [7–10] active during the first few minutes of the lifetime of the Universe [11–14].

At present, measurements of deuterium in quasar absorption spectra provide the best proxy for the determination of a primordial abundance. The most recent measurements from damped Lyman-α systems achieve better than 1% precision [15–17], yielding a weighted average of D/H × 105 = 2.547 ± 0.025 [18]. This remarkable precision appears to be in tension with the SM at about the 2σ level [19], although this remains under debate [20, 21] in light of the uncertainties plaguing our understanding of the key nuclear reactions involved. This highlights the primary importance to assess the impact of uncertainties in the nuclear network rates on the predictions from BBN [22]. A notable recent advance in this direction is the improved determination of the D(p,γ)3He rate by the LUNA collaboration [23], which has an important impact on BBN constraints from primordial deuterium on various NP scenarios....

 

READ MORE:

https://arxiv.org/pdf/2206.00693.pdf

 

What does this mean?.... 

 

According to some theories, the early universe only had leptons — while GRAVITY and mass as we know it did not exist. Why? According to the theory the temperature was too high for them to be part of the system. According to OBSERVATIONS, the Higgs boson "does not exist" passed a certain point of high temperature, yet a high mass neutrino existed in the high temperatures...

 

Massive sterile neutrinos in the early universe: From thermal decoupling to cosmological constraints

 

Leonardo MastrototaroPasquale Dario SerpicoAlessandro MirizziNinetta Saviano We consider relatively heavy neutrinos νH, mostly contributing to a sterile state νs, with mass in the range 10 MeV ≲ms≲mπ∼135 MeV, which are thermally produced in the early universe in collisional processes involving active neutrinos, and freezing out after the QCD phase transition. If these neutrinos decay after the active neutrino decoupling, they generate extra neutrino radiation, but also contribute to entropy production. Thus, they alter the value of the effective number of neutrino species Neff as for instance measured by the cosmic microwave background (CMB), as well as affect primordial nucleosynthesis (BBN), notably 4He production. We provide a detailed account of the solution of the relevant Boltzmann equations. We also identify the parameter space allowed by current Planck satellite data and forecast the parameter space probed by future Stage-4 ground-based CMB observations, expected to match or surpass BBN sensitivity.https://arxiv.org/abs/2104.11752

 

The expansion of the universe led to its cooling, at a point which mass, baryons and gravity became part of the system while the neutrinos "disengaged" into "massless" units and fields. This was the end of the Lepton-only EARLY universe... etc...

 

 

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