
Information-Driven Design of Imaging Systems
Quick Answer
Berkeley AI Research introduces a framework for evaluating imaging systems based on mutual information, predicting performance across four domains.
Quick Take
Berkeley AI Research introduces a framework for evaluating imaging systems based on mutual information, predicting performance across four domains. This method optimizes designs to match state-of-the-art systems while requiring less memory and computation, addressing limitations of traditional metrics.
Key Points
- Mutual information quantifies measurement effectiveness in distinguishing objects.
- Framework enables direct evaluation, optimizing imaging systems' information content.
- Optimized designs match state-of-the-art methods with lower resource requirements.
- Traditional metrics fail to unify quality aspects like noise and resolution.
- Imaging systems' noise characteristics allow for direct information estimation.
Paper Resources
Article Content
From source RSS / original summaryAn encoder (optical system) maps objects to noiseless images, which noise corrupts into measurements. Our information estimator uses only these noisy measurements and a noise model to quantify how well measurements distinguish objects. Many imaging systems produce measurements that humans never see or cannot interpret directly. Your smartphone processes raw sensor data through algorithms before producing the final photo.
MRI scanners collect frequency-space measurements that require reconstruction before doctors can view them. Self-driving cars process camera and LiDAR data directly with neural networks. What matters in these systems is not how measurements look, but how much useful information they contain. AI can extract this information even when it is encoded in ways that humans cannot interpret. And yet we rarely evaluate information content directly.
Traditional metrics like resolution and signal-to-noise ratio assess individual aspects of quality separately, making it difficult to compare systems that trade off between these factors. The common alternative, training neural networks to reconstruct or classify images, conflates the quality of the imaging hardware with the quality of the algorithm. We developed a framework that enables direct evaluation and optimization of imaging systems based on their information content.
In our NeurIPS 2025 paper, we show that this information metric predicts system performance across four imaging domains, and that optimizing it produces designs that match state-of-the-art end-to-end methods while requiring less memory, less compute, and no task-specific decoder design. Why mutual information? Mutual information quantifies how much a measurement reduces uncertainty about the object that produced it.
Two systems with the same mutual information are equivalent in their ability to distinguish objects, even if their measurements look completely different. This single number captures the combined effect of resolution, noise, sampling, and all other factors that affect measurement quality. A blurry, noisy image that preserves the features needed to distinguish objects can contain more information than a sharp, clean image that loses those features. Information unifies traditionally separate quality metrics.
It accounts for noise, resolution, and spectral sensitivity together rather than treating them as independent factors. Previous attempts to apply information theory to imaging faced two problems. The first approach treated imaging systems as unconstrained communication channels, ignoring the physical limitations of lenses and sensors. This produced wildly inaccurate estimates. The second approach required explicit models of the objects being imaged, limiting generality.
Our method avoids both problems by estimating information directly from measurements. Estimating information from measurements Estimating mutual information between high-dimensional variables is notoriously difficult. Sample requirements grow exponentially with dimensionality, and estimates suffer from high bias and variance. However, imaging systems have properties that enable decomposing this hard problem into simpler subproblems.
Mutual information can be written as: The first term, $H(Y)$, measures total variation in measurements from both object differences and noise. The second term, $H(Y \mid X)$, measures variation from noise alone. Mutual information equals the difference between total measurement variation and noise-only variation. Imaging systems have well-characterized noise. Photon shot noise follows a Poisson distribution. Electronic readout noise is Gaussian.
This known noise physics means we can compute $H(Y \mid X)$ directly, leaving only $H(Y)$ to be learned from data. For $H(Y)$, we fit a probabilistic model (e. g. a transformer or other autoregressive model) to a dataset of measurements. The model learns the distribution of all possible measurements. We tested three models spanning efficiency-accuracy…
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