Flowers of immortality Thomas Fink and Yang-Hui He London Institute for Mathematical Sciences Royal Institution 21 Albermarle St

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Flowers of immortality
Thomas Fink and Yang-Hui He
London Institute for Mathematical Sciences, Royal Institution, 21 Albermarle St,
London W1S 4BS, UK
Abstract. There has been a recent surge of interest in what causes aging. This
has been matched by unprecedented research investment in the field from tech
companies. But, despite considerable effort from a broad range of researchers, we
do not have a rigorous mathematical theory of programmed aging. To address this,
we recently derived a mortality equation that governs the transition matrix of an
evolving population with a given maximum age. Here, we characterize the spectrum of
eigenvalues of the solution to this equation. The eigenvalues fall into two classes. The
complex and negative real eigenvalues, which we call the flower, are always contained
in the unit circle in the complex plane. They play a negligible role in controlling the
dynamics of an aging population. The positive real eigenvalues, which we call the
stem, are the only eigenvalues which can lie outside the unit circle. They control the
most important properties of the dynamics. In particular, the spectral radius increases
with the maximum allowed age. This suggests that programmed aging confers no
advantage in a constant environment. However, the spectral gap, which governs the
rate of convergence to equilibrium, decreases with the maximum allowed age. This
opens the door to an evolutionary advantage in a changing environment.
arXiv:2210.13561v1 [q-bio.PE] 24 Oct 2022
Flowers of immortality 2
1. Introduction
1.1. The mortality equation
Recently, we derived a simple mortality matrix equation that governs the transition
matrix Qof an evolving population with maximum age a[1]. It is
Qa(I+MF Q) = MF,(1)
where all of the matrices are 2n×2nand Fis a diagonal matrix with the genotype
fitnesses along the diagonal. The mutation matrix Msatisfies
Mn=Mn/n, (2)
where Mis defined recursively in block form:
Mn+1 = MnIn
InMn!,M1= 0 1
1 0 !,(3)
with Inthe 2n×2nidentity matrix. The only difference between Mand Mis that M
is a stochastic matrix, in that its rows and columns sum to 1.
Eq. (1) is actually a more compact version of
Qa=MF(I+Q+. . . +Qa1),(4)
which is the actual governing equation. Notice that while eq. (1) has degree a+ 1, it
can be reduced to degree aby dividing through by QIto give eq. (4). The solution
Q=Ito eq. (1) is spurious, and we always disregard it. For the derivation of eq. (4)
and (1), see [1].
The matrix Q=MF governs the evolution of a population with maximum age
a= 1. It has 2neigenvalues, some of which may be degenerate. They are all real and lie
in the range [1,1].
By the Cayley Hamilton theorem, the eigenvalues of Qhave the same functional
relation to the eigenvalues of MF as the matrix Qdoes to the matrix MF. For each
eigenvalue λof MF, we obtain a family of aeigenvalues belonging to Q. This family is
generated by the analogue of eq. (1), but for numbers rather than matrices:
µa(1 + λµ) = λ. (5)
Just as eq. (1) is more the compact version of eq. (4), albeit with a spurious root at
Q=I, eq. (5) is a more compact version of
µa=λ(1 + µ+µ2+. . . +µa1),(6)
with a similarly spurious root at µ= 1, which we always disregard. Eq. (6) has a
solutions, and thus there are a2neigenvalues of the matrix Q. The goal of this paper is to
characterize them, and thereby better understand the dynamics of an aging population.
Notice that while the eigenvalues λare real, the eigenvalues µcan be complex.
Whereas a real eigenvalue corresponds to exponential growth or decay of the component
Flowers of immortality 3
of the population that projects along the associated eigenvector, a complex eigenvalue
corresponds to oscillatory behavior, with the overall growth or decay set by its
magnitude.
1.2. Summary of results
In this paper, we do four things, which correspond to the following four sections.
In the section 2, we study the complex and negative real eigenvalues of the solution
Qto the mortality equation (1). Our approach is make no assumptions about the fitness
F, and therefore about the 2neigenvalues λ[1,1] of MF. Rather it is to characterize,
for any given λ, the family of aeigenvalues satisfying eq. (5). The complex and negative
real eigenvalues are always contained in the unit circle, which we call the flower (Fig.
1). These play a negligible role in controlling the dynamics of an aging population.
In the section 3, we study the real eigenvalues of Q, which we call the stem. Of the
aeigenvalues associated with a given λ, only one is positive and real, which we call ρ,
and it has the largest magnitude (Fig. 1). Only these stem eigenvalues can lie outside
the unit circle. They control most of the important properties of the dynamics of an
aging population.
We study properties of the stem in section 4. We prove that the stem eigenvalues
ρincrease with λand are convex with λ, and increase with the maximum age a. The
latter is important because it means that, in a fixed environment, programmed aging
confers no evolutionary benefit. We show that the spectral gap of the eigenvalues of Q
increases as adecreases. This is important because the rate of convergence to equilibrium
is controlled by the spectral gap [2].
In section 5, we test our predictions by calculating the actual eigenvalues for two
different fitness functions: uniform fitness and Hamming fitness. Both are plotted in Fig.
3 and perfectly agree with our predictions. We conclude with a discussion, where we
describe the implications of our results on programmed aging.
2. The flower: complex and negative real eigenvalues
In this section we consider the complex and negative real eigenvalues of the solution of
the mortality equation. We call this the flower, because of the petals that appear as the
maximum age aincreases (Fig. 1). We show that all these eigenvalues are tame, in the
sense that they are contained inside the unit circle on the complex plane.
Our protagonist is the polynomial from eqs. (5) and (6), recalling that the more
compact P= (µ1)Qhas an (a+ 1)-th spurious root at µ= 1:
P(µ) := λ+ (1 + λ)µaµa+1,(7)
Q(µ) := λ(1 + µ+µ2+. . . +µa1)µa.(8)
This canonical form makes it easier to pick off the coefficients in what follows. We first
摘要:

FlowersofimmortalityThomasFinkandYang-HuiHeLondonInstituteforMathematicalSciences,RoyalInstitution,21AlbermarleSt,LondonW1S4BS,UKAbstract.Therehasbeenarecentsurgeofinterestinwhatcausesaging.Thishasbeenmatchedbyunprecedentedresearchinvestmentinthe eldfromtechcompanies.But,despiteconsiderablee ortfrom...

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