Fred Hutchinson Cancer Center / Howard Hughes Medical Institute
3 Mar 2025
CEPR Seminar
London School of Hygiene and Tropical Medicine
$x' = \frac{x \, (1+s)}{x \, (1+s) + (1-x)}$ for frequency $x$ over one generation with selective advantage $s$
$x(t) = \frac{x_0 \, (1+s)^t}{x_0 \, (1+s)^t + (1-x_0)}$ for initial frequency $x_0$ over $t$ generations
Trajectories are linear once logit transformed via $\mathrm{log}(\frac{x}{1 - x})$
Multinomial logistic regression across $n$ variants models the probability of a virus sampled at time $t$ belonging to variant $i$ as
$$\mathrm{Pr}(X = i) = x_i(t) = \frac{p_i \, \mathrm{exp}(f_i \, t)}{\sum_j p_j \, \mathrm{exp}(f_j \, t) }$$
with $2n$ parameters consisting of $p_i$ the frequency of variant $i$ at initial timepoint and $f_i$ the growth rate or fitness of variant $i$.
location variant date sequences Japan 22B 2023-02-10 242 Japan 22B 2023-02-11 56 Japan 22B 2023-02-12 70 Japan 22E 2023-02-10 80 Japan 22E 2023-02-11 21 Japan 22E 2023-02-12 27 USA 22B 2023-02-10 41 USA 22B 2023-02-11 23 USA 22B 2023-02-12 23 USA 22E 2023-02-10 368 USA 22E 2023-02-11 236 USA 22E 2023-02-12 246 ...
Rapid sweep of JN.1 over Dec to Jan 2024
Retrospective projections twice monthly during 2022
30 days out, countries range from 5 to 15% mean absolute error
Correlates with data availability (median number of sequences available from the previous 30 days):
Fitness flux $\phi(t) = \left( \sum_i \Delta x_i \, f_i \right) / \Delta t$
With constant variant fitness, fitness flux equals the rate of change of mean population fitness
Mean population fitness $\bar{f}(t) = \sum_i x_i(t) \, f_i$ Fitness flux $\phi(t) = \Delta \bar{f}(t) / \Delta t$
Mean population fitness | $\bar{f}(t) = \sum_i x_i(t) \, f_i$ |
Variance in fitness across population | $\mathrm{Var}[f(t)] = \sum_i x_i(t) \, (f_i - \bar{f}(t))^2$ |
Velocity of mean population fitness | $\psi(t) = \Delta \bar{f}(t) / \Delta t$ |
Fitness flux | $\phi(t) = \left( \sum_i \Delta x_i \, f_i \right) / \Delta t$ |
Constant clade fitness within each window, USA data only, ignores within-clade fitness variation
Line thickness is proportional to variant frequency, 36 total variants
Constant clade fitness within each window, USA data only, ignores within-clade fitness variation
Line thickness is proportional to variant frequency, 32 total variants
Richard Neher and others have analytically characterized these waves
Diffusion constant $D = \mu \, \langle \delta^2 \rangle/2$, where the average $\langle \ldots \rangle$ is over the distribution of mutational effects $K(\delta)$
SARS-CoV-2
"The rate of increase in fitness of any organism at any time is equal to
its genetic variance in fitness at that time," ie
$$\frac{d\bar{f}}{dt} = Var(f)$$
$$\psi(t) = \Delta \bar{f}(t) / \Delta t = \mathbb{E}_{x(t)} \left[ \frac{d f_i}{d t}\right] + \mathbb{V}_{x(t)}[f_{i}]$$
Fitness effects of fixed mutations are ~0.05 for SARS-CoV-2 and ~0.02 for H3N2
Collapsed to 367 Pango lineages with at least 1000 sequence counts in the US
Rather than estimate variant specific fitness $f_i$ directly, instead parameterize the "innovation" in fitness in going from parent lineage $p$ to child lineage $i$ as $\delta_i = (f_i - f_p)$.
Compare a non-informative model of $$\delta_i = (f_i - f_p) \sim \mathrm{Normal}(0, \sigma)$$ to a model where each "innovation" value has an informed prior based on a linear combination of predictors such as ACE2 binding, immune escape and spike mutations, where $z_k$ represents the value of predictor $k$ $$\delta_i = (f_i - f_p) \sim \mathrm{Normal}\left(\sum_k \beta_k \, z_k, \sigma\right)$$
Seasonal influenza and SARS-CoV-2 genomics: Data producers from all over the world, GISAID
Nextstrain: Richard Neher, Ivan Aksamentov, John SJ Anderson, Kim Andrews, Jennifer Chang, James Hadfield, Emma Hodcroft, John Huddleston, Jover Lee, Victor Lin, Cornelius Roemer, Thomas Sibley
MLR and fitness modeling: Marlin Figgins, Eslam Abousamra, Jover Lee, James Hadfield, John Huddleston, Philippa Steinberg, Jesse Bloom, Cornelius Roemer, Richard Neher
Bedford Lab:
John Huddleston,  
James Hadfield,  
Katie Kistler,  
Thomas Sibley,  
Jover Lee,  
Miguel Paredes,  
Marlin Figgins,  
Victor Lin,  
Jennifer Chang,  
Nashwa Ahmed,  
Cécile Tran Kiem,  
Kim Andrews,  
Cristian Ovaduic,  
Philippa Steinberg,  
Jacob Dodds,  
John SJ Anderson  
Nobuaki Masaki  
Amin Bemanian