Neural Compression and Neural Density Estimation for Cosmological Inference

PhD Defense, at APC, Paris

September 30, 2024

Justine Zeghal

Lambda Cold Dark Matter (   CDM)

\Lambda

The simplest model that best describes our observations is

\Lambda \text{CDM}

Relying only on a few parameters:

\Omega_c,\: \Omega_b,\:\Omega_\Lambda,\: h_0, \: n_s, \sigma_8\:.

Suggesting: ordinary matter, cold dark matter (CDM), and dark energy Λ as an explanation of the accelerated expansion.

Goal: determine the value of those parameters based on our observations.

\Omega_b
\Omega_c
\Omega_\Lambda

Credit: ESA

Planck Collaboration et al. (2020)

Credit:  ESA and the Planck Collaboration

Mysterious components 

Our universe is composed of 95% unknown components.

"Dark" because they do not interact electromagnetically. 

→ Difficult to study their nature.

For instance, a question we would like to answer is whether dark energy is a cosmological constant or evolves with time?

\Lambda \text{CDM}
w \text{CDM}
\Omega_b
\Omega_c
\Omega_\Lambda

Planck Collaboration et al. (2020)

we free the dark energy equation-of-state parameter  

w

Dark Energy

We can study the impacts of

dark energy on large-scale structures of the Universe at different cosmic times.

To study large-scale structures we need to map the distribution of matter in the Universe over time.

Credit: Institute of Statistical Mathematics (ISN) 

How to study something we cannot see?

Planck Collaboration et al. (2020)

Dark energy acts as a negative pressure that counteracts gravitational forces on large scales.

Gravitational Lensing

Credit: NASA's Goddard Space Flight Center Conceptual Image Lab

 

Weak Gravitational Lensing

Weak Gravitational Lensing

Galaxy shape

Weak Gravitational Lensing

Galaxy shape

Weak Gravitational Lensing

Galaxy shape

Convergence

\kappa

Weak Gravitational Lensing

Galaxy shape

Convergence

\kappa

Shear

\gamma

Weak Gravitational Lensing

Galaxy shape

Convergence

\kappa

Shear

\gamma

This phenomenon happens everywhere.

Weak Gravitational Lensing

Galaxy shape

Shear

\gamma

This phenomenon happens everywhere.

Credit: Alexandre Refregier and numerical simulations by Jain, Seljak & White 2000

 

Weak Gravitational Lensing

Map of the distribution of matter in the Universe.

To study dark energy we need this matter distribution at different cosmic times.

Weak Gravitational Lensing

Weak Gravitational Lensing

Weak Gravitational Lensing

Weak Gravitational Lensing

Weak Gravitational Lensing

Weak Gravitational Lensing

Weak Gravitational Lensing

Weak Gravitational Lensing

Weak Gravitational Lensing

How to constrain cosmological parameters?

x

For which we have an analytical likelihood function.

This likelihood function connects our compressed observations to the cosmological parameters.

p(t|\theta)
t = f(x)

Bayes theorem:

\underbrace{p(\theta|t=t_0)}_{\text{posterior}}
\underbrace{p(\theta)}_{\text{prior}}
\underbrace{p(t = t_0|\theta)}_{\text{likelihood}}
\propto

Planck Collaboration et al. (2020)

Cosmological constraints

From stage III galaxy surveys: we know it is one of the most informative of the low redshift probes.

For this reason, future surveys such as LSST, Euclid, and Roman have chosen it as their primary probe.

Secco et al. (2022)

DES Y3 Results

Vera C. Rubin Observatory

The Legacy Survey of Space and Time (LSST) will map the large-scale structure of the Universe with finer precision than ever before.

Telescope located in Chile.

It will observe the sky for 10 years taking ~1000 images every night.

Over the next 10 years, it will observe 20 billion galaxies.

Field of view: 9.6 square degrees with a pixel size of 0.2 arcsec.

We need to update our inference methods

The traditional way of constraining cosmological parameters misses information.

x
t = f(x)

This results in constraints on cosmological parameters that are not precise.

Credit: Natalia Porqueres

DES Y3 Results (with SBI).

Planck Collaboration et al. (2020)

Jeffrey et al. (2024)

\underbrace{p(\theta|x=x_0)}_{\text{posterior}}
\underbrace{p(\theta)}_{\text{prior}}
\underbrace{p(x = x_0|\theta)}_{\text{likelihood}}
\propto

Bayes theorem:

We can build a simulator to map the cosmological parameters to the data.

Prediction

Inference

Full-field inference: extracting all cosmological information

x
\theta

 Simulator

Full-field inference: extracting all cosmological information

Depending on the simulator’s nature we can either perform

  • Explicit inference 
  • Implicit inference 
x
\theta
z
f

 Simulator

Full-field inference: extracting all cosmological information

  • Explicit inference 

Explicit joint likelihood

 

p(x| \theta, z)
z
x

Initial conditions of the Universe

Large Scale Structure

p(\theta, z \: | \: x) \propto
p(z\:|\:\theta) p(\theta)

Needs an explicit simulator to sample the joint posterior through MCMC:

p(x| \theta, z)

We need to sample in extremely

high-dimension

→ gradient-based sampling schemes.

x
\theta
z
f
\sigma^2
\mathcal{N}

Credit:  Chirag Modi, François Lanusse, Mustafa Mustafa, Uroŝ Seljak

Depending on the simulator’s nature we can either perform

  • Explicit inference 
  • Implicit inference 

Full-field inference: extracting all cosmological information

x
\theta

 Simulator

z
f

  • Implicit inference 

It does not matter if the simulator is explicit or implicit because all we need are simulations

(\theta_i, x_i)_{i=1...N}

This approach typically involve 2 steps:

2) Implicit inference on these summary statistics to approximate the posterior.

1) compression of the high dimensional data into summary statistics. Without loosing cosmological information!

Summary statistics

t = f_{\varphi}(x)
p_{\Phi}(\theta | f_{\varphi}(x))

Full-field inference: extracting all cosmological information

x
\theta

 Simulator

z
f

My contributions

All the work of this thesis aims to contribute to making 

full-field inference applicable to next-generation surveys.

  • Which full-field inference methods require the fewest simulations?

  • How to build sufficient statistics?

  • Can we perform implicit inference with fewer simulations?

Summary statistics

t = f_{\varphi}(x)
p_{\Phi}(\theta | f_{\varphi}(x))
x
\theta

 Simulator

z
f

My contributions

Summary statistics

t = f_{\varphi}(x)
p_{\Phi}(\theta | f_{\varphi}(x))
x
\theta

 Simulator

z
f

My contributions

1. A new implicit inference method with fewer simulations.

Zeghal et al. (2022)

Summary statistics

t = f_{\varphi}(x)
p_{\Phi}(\theta | f_{\varphi}(x))
x
\theta

 Simulator

z
f

My contributions

1. A new implicit inference method with fewer simulations.

2. Benchmarking simulation-based inference for full-field inference.

Zeghal et al. (2022)

Zeghal et al. (2024)

Summary statistics

t = f_{\varphi}(x)
p_{\Phi}(\theta | f_{\varphi}(x))
x
\theta

 Simulator

z
f

3. Benchmarking neural compression for implicit full-field inference.

My contributions

1. A new implicit inference method with fewer simulations.

2. Benchmarking simulation-based inference for full-field inference.

Zeghal et al. (2022)

Zeghal et al. (2024)

Lanzieri & Zeghal et al. (2024)

Neural Posterior Estimation with Differentiable Simulators

ICML 2022 Workshop on Machine Learning for Astrophysics

 

Justine Zeghal, François Lanusse, Alexandre Boucaud,

Benjamin Remy and Eric Aubourg

Implicit Inference

1) Draw N parameters 

\theta_i \sim p(\theta)

2) Draw N simulations 

x_i \sim p(x\:|\:\theta = \theta_i)

3) Train a neural density estimator on                                           to approximate the quantity of interest

(\theta_i, x_i)_{i=1...N}

4) Approximate the posterior from the learned quantity

\text{Sample } x \sim p(x)
p_{\phi}(x)

Algorithm

Normalizing Flows

p_x(x)
p_z(z)
f^{-1}_1
f^{-1}_2
f_1
f_2

Normalizing Flows

p_x(x)
p_z(z)
f_1

Normalizing Flows

p_x(x)
p_z(z)
f_1

Normalizing Flows

p_x(x)
p_z(z)
f_1
f_2

Normalizing Flows

p_x(x)
p_z(z)
f^{-1}_2
f_1
f_2

Normalizing Flows

p_x(x)
p_z(z)
f^{-1}_2
f_1
f_2
f^{-1}_1

Normalizing Flows

p_x(x)
p_z(z)
\log p_z(f^{-1}(x))
+ \log \displaystyle\left\lvert det \frac{\partial f^{-1}(x)}{\partial x}\right\rvert

Change of Variable Formula:

f^{-1}_1
f^{-1}_2
f_1
f_2
\log p_x(x)
=

Normalizing Flows

p_x(x)
p_z(z)
\log p_z(f^{-1}(x))
+ \log \displaystyle\left\lvert det \frac{\partial f^{-1}(x)}{\partial x}\right\rvert

Change of Variable Formula:

f^{-1}_1
f^{-1}_2
f_1
f_2
\log p_x(x)
=

Normalizing Flows

p_x(x)
p_z(z)
f^{-1}_1
f^{-1}_2
f_1
f_2

We need to learn the mapping

to approximate the complex distribution.

\begin{array}{ll} D_{KL}(p_x(x)||p_x^{\phi}(x)) &=\mathbb{E}_{p_x(x)}\left[ \log\left(p_x(x)\right) \right] - \mathbb{E}_{p_x(x)}\left[ \log\left(p_x^{\phi}(x)\right) \right] \end{array}
\begin{array}{ll} \implies Loss = - \mathbb{E}_{x \sim p_x(x)}\left[ \log\left(p_x^{\phi}(x)\right) \right]\\ \end{array}

From simulations only!

A lot of simulations..

Truth

Approximation

With a few simulations it's hard to approximate the posterior distribution.

→ we need more simulations

BUT if we have a few simulations

and the gradients

 

(also know as the score)

\nabla_{\theta} \log p(\theta | x)

then it's possible to have an idea of the shape of the distribution.

How gradients can help reduce the number of simulations?

How to train NFs with gradients?

How to train NFs with gradients?

Normalizing flows are trained by minimizing the negative log likelihood:

- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(\theta | x)\right) \right]

How to train NFs with gradients?

But to train the NF, we want to use both simulations and the gradients from the simulator:

Normalizing flows are trained by minimizing the negative log likelihood:

- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(\theta | x)\right) \right]
\nabla_{\theta} \log p(\theta, z |x)

How to train NFs with gradients?

But to train the NF, we want to use both simulations and the gradients from the simulator:

Normalizing flows are trained by minimizing the negative log likelihood:

- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(\theta | x)\right) \right]
\nabla_{\theta} \log p(\theta, z |x)

These gradients are the joint gradients and we want to approximate​

p(\theta|x)

How to train NFs with gradients?

But to train the NF, we want to use both simulations and the gradients from the simulator:

Normalizing flows are trained by minimizing the negative log likelihood:

- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(\theta | x)\right) \right]
\nabla_{\theta} \log p(\theta, z |x)

These gradients are the joint gradients and we want to approximate​

\nabla_\theta \log p(\theta|x)

How to train NFs with gradients?

But to train the NF, we want to use both simulations and the gradients from the simulator:

Normalizing flows are trained by minimizing the negative log likelihood:

- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(\theta | x)\right) \right]
\nabla_{\theta} \log p(\theta, z |x)

These gradients are the joint gradients and we want to approximate​

\nabla_\theta \log p(\theta|x)
= \nabla_\theta \log \int p(\theta,z|x)dz
\nabla_{\theta} \log p(\theta, z |x)

How to train NFs with gradients?

But to train the NF, we want to use both simulations and the gradients from the simulator:

Normalizing flows are trained by minimizing the negative log likelihood:

- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(\theta | x)\right) \right]
\nabla_{\theta} \log p(\theta, z |x)

These gradients are the joint gradients and we want to approximate​

\nabla_\theta \log p(\theta|x)
= \nabla_\theta \log \int p(\theta,z|x)dz
\neq \int \nabla_{\theta} \log p(\theta, z |x) dz

How to train NFs with gradients?

Normalizing flows are trained by minimizing the negative log likelihood:

- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(\theta | x)\right) \right]
\nabla_{\theta} \log p(\theta, z |x)

How to train NFs with gradients?

Normalizing flows are trained by minimizing the negative log likelihood:

- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(\theta | x)\right) \right]
\displaystyle \mathbb{E}\left[ \parallel \nabla_{\theta} \log p(\theta, z |x) - \nabla_{\theta} \log p^{\phi}(\theta |x)\parallel_2^2 \right]

Similarly to Brehmer et al., 2020, we can show that minimizing this Mean Squared Error (MSE)

How to train NFs with gradients?

Normalizing flows are trained by minimizing the negative log likelihood:

- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(\theta | x)\right) \right]
\displaystyle \mathbb{E}\left[ \parallel \nabla_{\theta} \log p(\theta, z |x) - \nabla_{\theta} \log p^{\phi}(\theta |x)\parallel_2^2 \right]

yields

\nabla_{\theta} \log p^{\phi}(\theta |x) \approx \nabla_{\theta} \log p(\theta|x)
- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(\theta | x)\right) \right]
\displaystyle \mathbb{E}\left[ \parallel \nabla_{\theta} \log p(\theta, z |x) - \nabla_{\theta} \log p^{\phi}(\theta |x)\parallel_2^2 \right]

Similarly to Brehmer et al., 2020, we can show that minimizing this Mean Squared Error (MSE)

How to train NFs with gradients?

Finally, the loss function that take into account simulations and gradients information is

Normalizing flows are trained by minimizing the negative log likelihood:

- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(\theta | x)\right) \right]
\displaystyle \mathbb{E}\left[ \parallel \nabla_{\theta} \log p(\theta, z |x) - \nabla_{\theta} \log p^{\phi}(\theta |x)\parallel_2^2 \right]

yields

\nabla_{\theta} \log p^{\phi}(\theta |x) \approx \nabla_{\theta} \log p(\theta|x)
- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(\theta | x)\right) \right]
\displaystyle \mathbb{E}\left[ \parallel \nabla_{\theta} \log p(\theta, z |x) - \nabla_{\theta} \log p^{\phi}(\theta |x)\parallel_2^2 \right]

Similarly to Brehmer et al., 2020, we can show that minimizing this Mean Squared Error (MSE)

How to train NFs with gradients?

Finally, the loss function that take into account simulations and gradients information is

Normalizing flows are trained by minimizing the negative log likelihood:

- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(\theta | x)\right) \right]
\displaystyle \mathbb{E}\left[ \parallel \nabla_{\theta} \log p(\theta, z |x) - \nabla_{\theta} \log p^{\phi}(\theta |x)\parallel_2^2 \right]

yields

\nabla_{\theta} \log p^{\phi}(\theta |x) \approx \nabla_{\theta} \log p(\theta|x)
- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(\theta | x)\right) \right]
+ \: \lambda \: \displaystyle \mathbb{E}\left[ \parallel \nabla_{\theta} \log p(\theta, z |x) - \nabla_{\theta} \log p^{\phi}(\theta |x)\parallel_2^2 \right]

Similarly to Brehmer et al., 2020, we can show that minimizing this Mean Squared Error (MSE)

How to train NFs with gradients?

- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(\theta | x)\right) \right]
+ \: \lambda \: \displaystyle \mathbb{E}\left[ \parallel \nabla_{\theta} \log p(\theta, z |x) - \nabla_{\theta} \log p^{\phi}(\theta |x)\parallel_2^2 \right]

How to train NFs with gradients?

- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(\theta | x)\right) \right]
+ \: \lambda \: \displaystyle \mathbb{E}\left[ \parallel \nabla_{\theta} \log p(\theta, z |x) - \nabla_{\theta} \log p^{\phi}(\theta |x)\parallel_2^2 \right]

Problem: the gradient of current NFs lack expressivity

How to train NFs with gradients?

- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(\theta | x)\right) \right]
+ \: \lambda \: \displaystyle \mathbb{E}\left[ \parallel \nabla_{\theta} \log p(\theta, z |x) - \nabla_{\theta} \log p^{\phi}(\theta |x)\parallel_2^2 \right]

Problem: the gradient of current NFs lack expressivity

How to train NFs with gradients?

- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(\theta | x)\right) \right]
+ \: \lambda \: \displaystyle \mathbb{E}\left[ \parallel \nabla_{\theta} \log p(\theta, z |x) - \nabla_{\theta} \log p^{\phi}(\theta |x)\parallel_2^2 \right]

Problem: the gradient of current NFs lack expressivity

How to train NFs with gradients?

- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(\theta | x)\right) \right]
+ \: \lambda \: \displaystyle \mathbb{E}\left[ \parallel \nabla_{\theta} \log p(\theta, z |x) - \nabla_{\theta} \log p^{\phi}(\theta |x)\parallel_2^2 \right]

Problem: the gradient of current NFs lack expressivity

How to train NFs with gradients?

- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(\theta | x)\right) \right]
+ \: \lambda \: \displaystyle \mathbb{E}\left[ \parallel \nabla_{\theta} \log p(\theta, z |x) - \nabla_{\theta} \log p^{\phi}(\theta |x)\parallel_2^2 \right]

Problem: the gradient of current NFs lack expressivity

→ 1cm

→ 0.01 cm

→ 0.01 cm

Benchmark Metric

A metric

We use the Classifier 2-Sample Tests (C2ST) metric.

  • C2ST=0.5 (i.e “Impossible to differentiate 👍🏼”)
  • C2ST=1(i.e “Too easy to differentiate 👎🏻”)

distribution 1

distribution 2

Requirement: the true distributions is needed.

Results on a toy model

→ On a toy Lotka Volterra model, the gradients helps to constrain the distribution shape.

Results on a toy model

Without gradients

With gradients

Summary

First Neural Posterior Estimation (NPE) algorithm that can utilize the gradient information from the simulator.

We use an MSE loss to connect the joint gradient to the marginal one.

This loss requires the use of a specific NF architecture that is smooth.

Takeaway message

ML4Astro Workshop

Can we perform implicit inference with fewer simulations?

Yes! The gradient information helps implicit inference to reduce the number of simulations required when only a few simulations are available.

\theta
f
\mathcal{N}

 Simulator

Summary statistics

t = f_{\varphi}(x)
x
p_{\Phi}(\theta | f_{\varphi}(x))

My contributions

3. Benchmarking neural compression for implicit full-field inference.

1. A new implicit inference method with fewer simulations.

2. Benchmarking simulation-based inference for full-field inference.

Zeghal et al. (2022)

Zeghal et al. (2024)

Lanzieri & Zeghal et al. (2024)

\theta
f
\mathcal{N}

 Simulator

Summary statistics

t = f_{\varphi}(x)
x
p_{\Phi}(\theta | f_{\varphi}(x))

My contributions

3. Benchmarking neural compression for implicit full-field inference.

1. A new implicit inference method with fewer simulations.

2. Benchmarking simulation-based inference for full-field inference.

Zeghal et al. (2022)

Zeghal et al. (2024)

Lanzieri & Zeghal et al. (2024)

Simulation-Based Inference Benchmark for LSST Weak Lensing Cosmology

Justine Zeghal, Denise Lanzieri, François Lanusse, Alexandre Boucaud, Gilles Louppe, Eric Aubourg, Adrian E. Bayer

and The LSST Dark Energy Science Collaboration (LSST DESC)

  • do gradients help implicit inference methods?

In the case of weak lensing full-field analysis,

  • which inference method requires the fewest simulations?

x
\theta
z
f
\sigma^2
\mathcal{N}

We developed a fast and differentiable (JAX) log-normal mass maps simulator.

For our benchmark: a Differentiable Mass Maps Simulator

DifferentiableUniverseInitiative/​sbi-lens

Benchmark metric

Explicit inference theoretically and asymptotically converges to the truth.

Explicit inference and implicit inference yield comparable constraints.

C2ST = 0.6!

To use the C2ST we need the true posterior distribution.

→ We use the explicit full-field posterior.

Why?

  • Do gradients help implicit inference methods?             

- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(x | \theta)\right) \right]
+ \: \lambda \: \displaystyle \mathbb{E}\left[ \parallel \nabla_{\theta} \log p(x, z |\theta) -{\nabla_{\theta} \log p^{\phi}(x|\theta )}\parallel_2^2 \right]

Training the NF with simulations and gradients:

Loss = 

  • Do gradients help implicit inference methods? 

- \mathbb{E}_{p(x, \theta)}\left[ \log\left(p^{\phi}(x | \theta)\right) \right]

Training the NF with simulations and gradients:

Loss = 

  • Do gradients help implicit inference methods? 

(\theta_i, x_i)_{i=1...N}
\nabla_{\theta} \log \hat{p}(x |\theta)
+ \: \lambda \: \displaystyle \mathbb{E}\left[ \parallel \nabla_{\theta} \log p(x, z |\theta) -{\nabla_{\theta} \log p^{\phi}(x|\theta )}\parallel_2^2 \right]
\nabla_{\theta}\log p(x|\theta)
\nabla_{\theta}\log p(x,z|\theta)

(from the simulator)

→ For this particular problem, the gradients from the simulator are too noisy to help.

  • Do gradients help implicit inference methods?     

→ Implicit inference requires 1500 simulations.

→ In the case of perfect gradients it does not significantly help.

→ Simple distribution all the simulations seems to help locate the posterior distribution.

  • do gradients help implicit inference methods?

In the case of weak lensing full-field analysis,

  • which inference method requires the fewest simulations?

x
\theta
z
f
\sigma^2
\mathcal{N}

→  No, it does not help to reduce the number of simulations because the gradients of the simulator are too noisy.

→  Even with marginal gradients the gain is not significant.

→  For now, we now that implicit inference requires 1500 simulations.

  • which inference method requires the fewest simulations?

What about explicit inference?

  • which inference method requires the fewest simulations?

What about explicit inference?

→ Explicit inference requires

simulations.

10^5

  • which inference method requires the fewest simulations?

Summary

Takeaway message

Two different simulation-based inference approaches to perform full-field inference.

They yield the same constraints.

Explicit inference requires 100 times more simulations than implicit inference.

We developed a fast and differentiable log-normal simulator.

Implicit inference with gradients does not significantly help to reduce the number of simulations.

Which full-field inference methods require the fewest simulations?

\theta
f
\mathcal{N}

 Simulator

Summary statistics

t = f_{\varphi}(x)
x
p_{\Phi}(\theta | f_{\varphi}(x))

My contributions

3. Benchmarking neural compression for implicit full-field inference.

1. A new implicit inference method with fewer simulations.

2. Benchmarking simulation-based inference for full-field inference.

Zeghal et al. (2022)

Zeghal et al. (2024)

Lanzieri & Zeghal et al. (2024)

\theta
f
\mathcal{N}

 Simulator

Summary statistics

t = f_{\varphi}(x)
x
p_{\Phi}(\theta | f_{\varphi}(x))

My contributions

3. Benchmarking neural compression for implicit full-field inference.

1. A new implicit inference method with fewer simulations.

2. Benchmarking simulation-based inference for full-field inference.

Zeghal et al. (2022)

Zeghal et al. (2024)

Lanzieri & Zeghal et al. (2024)

\theta
f
\mathcal{N}

 Simulator

Summary statistics

t = f_{\varphi}(x)
x
p_{\Phi}(\theta | f_{\varphi}(x))

My contributions

3. Benchmarking neural compression for implicit full-field inference.

1. A new implicit inference method with fewer simulations.

2. Benchmarking simulation-based inference for full-field inference.

Zeghal et al. (2022)

Zeghal et al. (2024)

Lanzieri & Zeghal et al. (2024)

Optimal Neural Summarisation for Full-Field Weak Lensing Cosmological Implicit Inference

Denise Lanzieri*, Justine Zeghal*, T. Lucas Makinen, François Lanusse, Alexandre Boucaud and Jean-Luc Starck

​* equal contibutions

x
t = f_{\varphi}(x)
\text{A statistic } t \text{ is said to be sufficient for the parameters } \theta \text{ if }
p(\theta \: | \: x) = p(\theta \: | \: t) \: \text{ with } \: t=f(x)

How to extract all the information?

It is only a matter of the loss function used to train the compressor.

Definition: Sufficient Statistic

Two main compression schemes

\hat{\theta} = f_\varphi(x)

Regression Losses

Two main compression schemes

Text

\hat{\theta} = f_\varphi(x)

Regression Losses

Two main compression schemes

Which learns a moment of the posterior distribution.

Mean Squared Error (MSE) loss:

\mathcal{L}_{\text{MSE}} = \mathbb{E}_{p(x,\theta)} \left[\parallel \theta - f_\varphi(x) \parallel ^2 \right]

Which learns a moment of the posterior distribution.

\hat{\theta} = f_\varphi(x)

Regression Losses

Two main compression schemes

Mean Squared Error (MSE) loss:

\mathcal{L}_{\text{MSE}} = \mathbb{E}_{p(x,\theta)} \left[\parallel \theta - f_\varphi(x) \parallel ^2 \right]

→ Approximate the mean of the posterior.

\hat{\theta} = f_\varphi(x)

Regression Losses

Two main compression schemes

Which learns a moment of the posterior distribution.

Mean Squared Error (MSE) loss:

\mathcal{L}_{\text{MSE}} = \mathbb{E}_{p(x,\theta)} \left[\parallel \theta - f_\varphi(x) \parallel ^2 \right]

→ Approximate the mean of the posterior.

\hat{\theta} = f_\varphi(x)

Regression Losses

Mean Absolute Error (MAE) loss:

\mathcal{L}_{\text{MAE}} = \mathbb{E}_{p(x,\theta)} \left[| \theta - f_\varphi(x) |\right]

Two main compression schemes

Which learns a moment of the posterior distribution.

Mean Squared Error (MSE) loss:

\mathcal{L}_{\text{MSE}} = \mathbb{E}_{p(x,\theta)} \left[\parallel \theta - f_\varphi(x) \parallel ^2 \right]

→ Approximate the mean of the posterior.

\hat{\theta} = f_\varphi(x)

Regression Losses

Mean Absolute Error (MAE) loss:

\mathcal{L}_{\text{MAE}} = \mathbb{E}_{p(x,\theta)} \left[| \theta - f_\varphi(x) |\right]

→ Approximate the median of the posterior.

Two main compression schemes

Which learns a moment of the posterior distribution.

Regression Losses

Two main compression schemes

\mu_1 = \mu_2

Regression Losses

Two main compression schemes

\mu_1 = \mu_2

Regression Losses

Two main compression schemes

\mu_1 = \mu_2

Regression Losses

Two main compression schemes

\mu_1 = \mu_2

Regression Losses

\neq

The mean is not guaranteed to be a sufficient statistic.

Two main compression schemes

Mutual information maximization

Two main compression schemes

p(\theta \: | \: x) = p(\theta \: | \: t(x)) \: \Leftrightarrow I(\theta, x) = I (\theta, t(x))

Mutual information maximization

By definition:

Two main compression schemes

I(\theta,t)
H(\theta)
H(t)
H(\theta|t)
H(t|\theta)
I(\theta,t) = H(t) - H(t|\theta)
p(\theta \: | \: x) = p(\theta \: | \: t(x)) \: \Leftrightarrow I(\theta, x) = I (\theta, t(x))

Mutual information maximization

By definition:

Two main compression schemes

I(\theta,t)
H(\theta)
H(t)
H(\theta|t)
H(t|\theta)
I(\theta,t) = H(t) - H(t|\theta)
p(\theta \: | \: x) = p(\theta \: | \: t(x)) \: \Leftrightarrow I(\theta, x) = I (\theta, t(x))

Mutual information maximization

By definition:

Two main compression schemes

I(\theta,x)
I(\theta,t) = H(t) - H(t|\theta)
p(\theta \: | \: x) = p(\theta \: | \: t(x)) \: \Leftrightarrow I(\theta, x) = I (\theta, t(x))

Mutual information maximization

By definition:

Two main compression schemes

I(\theta,t) = H(t) - H(t|\theta)
p(\theta \: | \: x) = p(\theta \: | \: t(x)) \: \Leftrightarrow I(\theta, x) = I (\theta, t(x))

Mutual information maximization

By definition:

Two main compression schemes

I(\theta,t) = H(t) - H(t|\theta)
p(\theta \: | \: x) = p(\theta \: | \: t(x)) \: \Leftrightarrow I(\theta, x) = I (\theta, t(x))

Mutual information maximization

By definition:

Two main compression schemes

I(\theta,t) = H(t) - H(t|\theta)

→ should build sufficient statistics according to the definition.

p(\theta \: | \: x) = p(\theta \: | \: t(x)) \: \Leftrightarrow I(\theta, x) = I (\theta, t(x))

Mutual information maximization

By definition:

Two main compression schemes

For our benchmark

Log-normal LSST Y10 like

differentiable

simulator

t = f_{\varphi}(x)
DifferentiableUniverseInitiative/​sbi-lens

1. We compress using one of the losses.

Benchmark procedure:

2. We compare their extraction power by comparing their posteriors.

For this, we use implicit inference, which is fixed for all the compression strategies.

p(\theta \: | \: x) = p(\theta \: | \: t) \: \text{ with } \: t=f(x)

Numerical results

Summary

Takeaway message

Compression is the first step of the two-stage implicit full-field inference approach.

To perform implicit full-field inference this compression has to extract all cosmological information.

How to build sufficient statistics?

Compression schemes based on maximizing mutual information can generate sufficient statistics, while compression schemes based on regression losses do not guarantee the generation of such statistics.

Design an experimental setup that enables the isolation of the impact of the loss function.

In recent years, there has been a shift from analytical likelihood-based to simulation-based inference to enhance the precision of constraints on cosmological parameters.

Conclusion

The goal of my thesis was to conduct a cutting-edge methodological study focused on enhancing both performance (the amount of information extracted) and efficiency (the number of simulations required).

I demonstrated that achieving near-optimal implicit full-field inference is possible with just a few simulations.

Open challenges..

For instance, the fidelity of the simulator.

  • Corrected the simulator with variational inference.
  • Modeling the impact of baryons.
\theta
f
\mathcal{N}

 Simulator

Summary statistics

t = f_{\varphi}(x)
x
p_{\Phi}(\theta | f_{\varphi}(x))

Thank you for your attention!

Backup

Coupling flows

\text{conditionner}
\text{coupling function}
\text{coupling flow}
\begin{array}{ll} x^A &= z^A\\ x^B &= g(z^B, h(z^A)) \\ \end{array} \\ \text{with $g(\cdot; \theta)$ a bijection}\\ \text{and $h$ any arbitrary function.}
\text{Have to choose how to split $x$.}
\implies \displaystyle\left\lvert det \frac{\partial f^{-1}(x)}{\partial x}\right\rvert = \frac{\partial g^{-1}(x^B)}{\partial x^B}
\frac{\partial f^{-1}(x)}{\partial x} = \begin{bmatrix} \mathbb{I} & 0 \\ \frac{\partial g^{-1}(x^B)}{\partial x^A} & \frac{\partial g^{-1}(x^B)}{\partial x^B} \end{bmatrix}
\text{The power of a coupling flow resides in the ability of a conditioner}
\text{$h$ to be arbitrarily complex (usually modelled as a neural network).}
\text{A coupling flow is invertible if and only if $g$ is invertible.}

Combine multiple mappings

f_1(z_0)
p_x(x)
p_{z_0}(z_0)
p_{z_1}(z_1)
f_2(z_1)
f_2^{-1}(z_2)
f_1^{-1}(z_1)
f = f_k \circ ... \circ f_2 \circ f_1
\text{with $x = z_2$}
\log p_x(x) = \log p_z(f^{-1}(x))
+ \sum_{i=1}^{k}\log \displaystyle\left\lvert det \frac{\partial f^{-1}_i(z_i)}{\partial z_{i+1}}\right\rvert \\
f^{-1} = f_1^{-1} \circ ... \circ f_{k-1}^{-1} \circ f_k^{-1}

Smooth Normalizing Flows

p_x(x)
p_z(z)
f(z)
f^{-1}(z)
\left\{ \begin{array}{ll} f_{y}^\varphi(x) &= \frac{\sigma(x) - \sigma(x_0)}{\sigma(x_1) - \sigma(x_0)}\cdot (1-c_\varphi(y)) +c_\varphi(y)\cdot x \\ \\ \sigma(x) &= c_\varphi(y)\cdot x + \frac{1-c_\varphi(y)}{1+\exp({-\rho(x)})}\\ \\ \rho(x) &= a_\varphi(y) \cdot \left(\log\left(\frac{x}{1-x}\right) + b_\varphi(y)\right) \end{array} \right.

Smooth diffeomorphism (Köhler et al. (2021a)):

This function is not very expressive but a mixture of this transformation is.

Mixture of 5 transformations.

x
f(x)
0
0
1
1
\log p_x(x) = \log p_z(f^{-1}(x))
+ \log \displaystyle\left\lvert det \frac{\partial f^{-1}(x)}{\partial x}\right\rvert

Inversing Smooth Transformations

f(y) - x = 0

We define                  as an implicit function:

f^{-1}(x)

and use a root-finding algorithm.

y_0, y_1, ..., y_N \approx y
\log p_x(x) = \log p_z(f^{-1}(x))
+ \log \displaystyle\left\lvert det \frac{\partial f^{-1}(x)}{\partial x}\right\rvert

Inversing Smooth Transformations

y_0, y_1, ..., y_N \approx y

Using automatic differentiation requires storing the value of each iteration and its gradient.

→ Inefficient.

From the Implicit Function Theorem:

\frac{\partial f^{-1}}{\partial x}(x) \approx \left[ \dfrac{\partial f}{\partial y}(y) \right]^{-1}

Perspectives

→ Quality of inference solely tied to the simulator's quality. Realistic simulations are costly.

State-of-the-art explicit full-field inference results are performed on a 1LPT model.

We need a more realistic gravity model, but are we able to sample it?

Project with: Yuuki Omori, Chihway Chang, and François Lanusse.

Porqueres et al. (2023)

Perspectives

→ Quality of inference solely tied to the simulator's quality. Realistic simulations are costly.

Project with: François Lanusse, Benjamin Remy, and Alexandre Boucaud.

Even the most accurate simulations will never perfectly match our data.

We learn the mapping between simulations and real data.

x
\theta
z
f
\sigma^2
\mathcal{N}

Explicit joint likelihood

 

p(x| \theta, z)
p(x| \theta, z)

Extracting gradient information

\nabla_{\theta} \log p(\theta, z |x) =
x
\theta
z
f
\sigma^2

Explicit joint likelihood

 

p(x| \theta, z)
p(x| \theta, z)

Extracting gradient information

\mathcal{N}
\nabla_{\theta} \log p(\theta, z |x) =
x
\theta
f
\sigma^2

Explicit joint likelihood

 

p(x| \theta, z)
\nabla_\theta \log p(x| \theta, z)

Extracting gradient information

z
\mathcal{N}
+ \nabla_{\theta} \log p(\theta)
+ \sum_{i}^N \nabla_{\theta} \log p(z_i|z_1, .., z_{i-1},\theta)
\nabla_{\theta} \log p(\theta, z |x) =
x
\theta
f
\sigma^2

Explicit joint likelihood

 

p(x| \theta, z)
\nabla_\theta \log p(x| \theta, z)

Extracting gradient information

z
\mathcal{N}

a framework for automatic differentiation following the NumPy API, and using GPU

probabilistic programming library

powered by JAX

+ \nabla_{\theta} \log p(\theta)
+ \sum_{i}^N \nabla_{\theta} \log p(z_i|z_1, .., z_{i-1},\theta)
\nabla_{\theta} \log p(\theta, z |x) =
x
\theta
f
\sigma^2

Explicit joint likelihood

 

p(x| \theta, z)
\nabla_\theta \log p(x| \theta, z)

Extracting gradient information

z
\mathcal{N}

PhD Defense

By Justine Zgh

PhD Defense

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