REVIEW 4 major objections 6 minor 2 cited by
Imperceptible Adversarial Examples in the Physical World
T0 review · 4 major / 6 minor · reviewed 2026-08-12 · deepseek-v4-flash
Pith's one-line read Straight-through gradient estimation makes imperceptible, L-infinity-bounded adversarial examples work in the physical world, with zero accuracy on printed photos and AP50 down to 4.22 percent in a driving simulator.
desk verdict Well-executed application of known STE/BPDA trick to physical attacks; strong claims rest on an unmeasured sign-accuracy assumption and a small, confounded experiment. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The central object is the straight-through estimator (STE, also known as BPDA), defined by using the true non-differentiable distortion in the forward pass and the identity in the backward pass. In the global-perturbation setup it is expressed with a stop-gradient operation as $f(d(x+\delta)) = f(x+\delta + \mathrm{sg}[d(x+\delta)-(x+\delta)])$, so the backward pass sees $x+\delta$ with a constant offset. In the patch setup the distortion is written as $g_d(\delta,x,e)=r(x+\delta)+\mathrm{sg}[c(p(x+\delta),e)-r(x+\delta)]$, where $r$ is a differentiable renderer and the non-differentiable camera-plus-print pipeline only supplies the forward value. The mechanism works because the sign of the identity-backward gradient is asserted to match the true sign whenever the distortion preserves a similar image, and sign-based attacks such as FGSM and PGD only need the sign.
What would settle it
Print the same six images again with a different printer or camera, generate STE-augmented PGD perturbations at $\ell_\infty=4/255$, and count correct predictions of the target classifier; any nonzero correct count would falsify the zero-accuracy claim. A more direct test of the mechanism: for random perturbations, compare the sign of the identity-backward gradient with the sign obtained by finite differences through the physical pipeline; if sign agreement falls well below 100% of pixels, the assertion that the sign is always accurate is refuted.
Extended reading notes
Core claim
The paper's central claim is that non-differentiability in physical imaging is not a barrier to imperceptible adversarial examples. On the paper's own terms: apply the true distortion $d(\cdot)$ in the forward pass, so the loss is exact, and backpropagate through the identity, so the gradient is approximate but cheap. The stop-gradient identity $f(d(x+\delta)) = f(x+\delta + \mathrm{sg}[d(x+\delta)-(x+\delta)])$ makes this concrete. For the patch threat model, the same construction uses a differentiable renderer $r(x+\delta)$ in place of the non-differentiable renderer, with the residual detached as a constant. With this machinery, PGD bounded by $\ell_\infty=4/255$ achieves zero accuracy on the printout photos, and an unbounded STE-augmented patch reaches 0% AP50 while an $\ell_\infty=8/255$ patch reaches 4.22% AP50 in the simulator.
Load-bearing premise
The load-bearing premise is that the identity backward pass preserves the sign of the true gradient through the physical distortion; if clipping, halftoning, color shifts, perspective misalignment, or game-engine lighting ever make that sign wrong, the digitally optimized perturbation is not what the camera sees, and the zero-accuracy results would not transfer.
Editorial extensions
If this is right
- Physical adversarial examples no longer require large, visibly strange perturbations: with STE, $\ell_\infty = 4/255$ perturbations force zero accuracy on printed photos, so an attacker does not need to sacrifice imperceptibility.
- Patch-based attacks on object detection become practical: an $\ell_\infty = 8/255$ patch drops AP50 from 43.29% to 4.22% in a photorealistic driving simulator, and an unbounded patch reaches 0%.
- Because the attack is fast (a single FGSM step at $\ell_\infty=16/255$ suffices, and a few PGD iterations at $16/255$ cross the zero-accuracy threshold), physical attacks are cheap to generate once the pipeline is built.
- The method extends to 3D camouflage: the paper's differentiable-rendering construction works with mesh renderers, so imperceptible textures on 3D objects are a direct corollary.
- Defenses that flag abnormal textures will not catch these examples, since the perturbations remain small and visually benign.
Reading between the lines
- A testable prediction follows from the sign-accuracy mechanism: the attack's effectiveness should degrade as physical distortion becomes more nonlinear or misaligned, so printers with stronger color shifts or cameras with larger perspective error should require larger $\epsilon$ to reach zero accuracy.
- The zero-accuracy result rests on six images and one printer-camera pair; if the threat model is as general as the paper suggests, the same STE recipe should transfer to other classifier architectures and capture devices, a claim the experiments do not yet cover.
- Combining STE with expectation-over-transformation noise, which the paper mentions as future work, should yield physical perturbations robust to viewpoint and lighting variation; the mechanism's design allows this without changing the forward-pass trick.
- The same stop-gradient construction could be reused as a diagnostic for defenses: a defense that deliberately breaks the sign correspondence between the digital perturbation and the physical loss would neutralize the attack, pointing to a cheap defensive direction.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper proposes using a straight-through estimator (STE, also called BPDA) to generate ℓ∞-bounded adversarial examples that survive non-differentiable physical distortions. In the global perturbation threat model, the method applies the true non-differentiable distortion in the forward pass and an identity backward pass, then uses FGSM or PGD on the resulting surrogate gradient. Experiments with printed ImageNet images report zero classification accuracy for PGD at ℓ∞ = 4/255 and for FGSM at ℓ∞ = 16/255. In the patch threat model, STE is combined with a differentiable perspective renderer in the CARLA simulator; the paper reports AP50 dropping from 43.29% to 4.22% for an ℓ∞ = 8/255 patch and to 0% for an unbounded patch. The authors claim these are the first imperceptible, physically realizable adversarial examples with small ℓ∞ bounds that force near-zero accuracy.
Significance. If the empirical claims hold, this is a significant result: it would show that small ℓ∞-bounded perturbations, imperceptible to humans, can survive print-and-camera pipelines and simulator-based rendering, contradicting the common assumption that physical distortions act as a defense. The mathematical formulation is clean and the stop-gradient identities in Eq. (3) and Eq. (5) are exact. The use of an external pre-trained ResNet-50 and a public CARLA detection model, rather than a model trained by the authors, is a strength, as is the internal consistency of the reported trends: larger budgets monotonically reduce accuracy in nearly all rows. However, the central claims rest on an unmeasured sign-fidelity assumption for the identity backward pass, on six images with no repeated trials, and on CARLA scenes that were recreated rather than taken from the official GARD dataset. The significance is therefore conditional on additional measurement and control experiments.
major comments (4)
- The assertion that 'the sign of the approximate gradient is always accurate' is load-bearing for the zero-accuracy claim but is never measured. The argument only requires d(x + δ) to be similar to x + δ; for sign-based PGD, one needs per-coordinate sign agreement between the identity backward pass and the true distortion. The printout pipeline in Section 3.2 applies a perspective transform from handheld photos and a manual crop, so after the homography d(x + δ) is not pixel-wise close to x + δ. A one-pixel misalignment can flip the sign of high-frequency components at ε = 4/255. The paper itself concedes in Section 3.4 that any pixel misalignment breaks the assumption, and Figure A.1 shows white edges from imperfect cropping on the images used for the zero-accuracy claim. Please quantify the sign agreement between the identity backward pass and the true distortion (for example, by finite differences on registered images), and either eliminate cropping artifacts or report results separately for cleanly registered images. Without this, the Physical column of Table 1 may reflect misalignment plus cropping artifacts rather than the bounded perturbation alone.
- The detached residual C = c(p(x + δ), e) - r(x + δ) is assumed small because the differentiable renderer places the patch at the same location as the UE4 renderer, but this assumption is never quantified. UE4 applies lighting, weather, materials, and occlusion, while the differentiable renderer is only a perspective transformation. Furthermore, Section 4.2 states that the GARD scenes had to be recreated with the OSCAR toolkit because the released CARLA metadata was incomplete, so the evaluation is not on the official GARD images. Please report the distribution of pixel residuals between the UE4 render and the differentiable renderer across the 20 scenes (for example, mean and maximum absolute difference per patch), and ideally include a comparison with digitally composed patches as in the original GARD setup. If C is not small, the 4.22% AP50 result may be an artifact of renderer mismatch rather than evidence that the bounded perturbation survives the full pipeline.
- The headline zero-accuracy result is based on six images with no repeated trials. The 113 printouts described in Section 3.2 correspond to one print per condition, so each row in the Physical column is a single observation per image. The claim that STE 'forces zero accuracy' therefore rests on 6 correct classifications becoming 0, a very small sample. Please report per-image results, provide confidence intervals or repeated print/capture trials, and include a control with random bounded perturbations (or an unprinted digital perturbation) to confirm that the effect is attributable to the optimized perturbation under the stated ε bound rather than to cropping, perspective, or printing artifacts. The visible white edges in Figure A.1 make this control particularly important.
- The digital and physical columns of Table 1 are surprising in a way that needs explanation: for PGD + STE at ε = 4, the digital accuracy is 3/6 but the physical accuracy is 0/6, meaning the attack is stronger after the print-and-camera distortion than in the digital domain. If STE is only a backward-pass approximation, one would expect physical effectiveness to be no better than digital effectiveness. The current text addresses the gap between digital PGD and STE-physical PGD, but not the comparison between STE-physical and STE-digital. Please measure the realized perturbation in the captured image after registration (for example, the ℓ∞ difference between the registered photo of the benign printout and the attacked printout) and discuss whether the physical distortion itself contributes to the drop. Without this measurement, it is difficult to attribute the zero-accuracy result to the small ℓ∞-bounded perturbation rather than to unintended artifacts.
minor comments (6)
- The notation 'where C is a constant' is misleading because C = d(x + δ) - (x + δ) depends on x and δ; it is a term detached from differentiation, not a constant in the mathematical sense. Please rephrase as 'a term treated as constant by the stop-gradient operation.'
- The terms 'global perturbation threat model' and 'patch perturbation threat model' are used without definition until Sections 3 and 4. Please define them at first use, since they are central to the claimed contributions.
- The caption refers to an 'empirical threshold of loss' that yields zero accuracy, but does not explain how this threshold was computed. Please describe the procedure used to set the dashed cyan line.
- The TIDE error columns (Class, Box, Other, Dup., Bg., Missed) lack a clear explanation of what each count represents and how the columns relate to the TIDE taxonomy. Please add a sentence or footnote explaining these counts.
- The row labels in Figures A.1 and A.2 appear to contain a typo: the third data row is labeled 'hot pot' in both figures, but the text describing the setup lists the six images as including 'ladle' and only one 'hot pot'. Please correct the labels.
- References [36] and [37] have a dangling comma before 'Accessed' in the bibliographic entries; please clean up the formatting.
Circularity Check
No significant circularity: the STE/BPDA identities are exact forward-pass constructions and the headline results are evaluated against external pretrained models, physical printouts, and the UE4 renderer.
full rationale
The derivation chain is self-contained, and the reported results are not predetermined by the method's definitions. Equation (3), f(d(x+δ)) = f(x+δ + sg[d(x+δ) − (x+δ)]), and Equation (5), g_d(δ,x,e) = r(x+δ) + sg[c(p(x+δ),e) − r(x+δ)], are exact forward-pass identities; the backward pass uses the identity function as an approximation to the true distortion gradient, not as a fitted parameter that is later renamed a prediction. The zero-accuracy and AP50 values are measured against external, pretrained models (torchvision ResNet-50 and the Armory Faster R-CNN), against physical printouts, and against CARLA's UE4 renderer, so the evaluation targets are independent of the optimization procedure. The self-citations ([11] ShapeShifter, [13] OSCAR Datagen Toolkit, [41] MART) supply related work and implementation tooling; none is load-bearing evidence that STE works, and no uniqueness theorem or fitted quantity is imported from these citations. The paper's own Section 3.4 caveat that pixel misalignment could break the STE assumption is a correctness and robustness limitation, not circularity: it concedes the sign-accuracy assumption may fail, which is the opposite of defining the result into existence. No step in the paper reduces, by construction or by self-citation, to its own input.
Assumptions & free parameters
free parameters (3)
- Global PGD/FGSM step size and iterations =
step size 1/255; 12 PGD iterations or 1 FGSM step
- Patch attack optimizer schedule =
Adam-200-1, Adam-200-2, Adam-500-12.75 (learning rates 1/255, 2/255, 12.75/255)
- ℓ∞ perturbation budgets =
2/255, 4/255, 8/255, 16/255, 255/255
assumptions (4)
- domain assumption For a non-differentiable distortion that approximately preserves pixel correspondence, the identity backward pass yields a gradient whose sign matches the true gradient.
- domain assumption The differentiable renderer r(·) renders x+δ at the same location as the non-differentiable camera-renderer c(p(x+δ), e), so the stop-gradient residual C is effectively constant with respect to δ.
- domain assumption The CARLA simulator and the particular printer-camera pair are representative of physical-world deployment conditions.
- domain assumption Six ImageNet images and 20 recreated CARLA scenes are sufficient to support zero-accuracy and near-zero-AP50 claims.
Cite this review
Pith. "Pith review of Imperceptible Adversarial Examples in the Physical World." pith.science (2026). https://pith.science/paper/B2Q43A6J
@misc{pith2026241116622,
author = {Pith},
title = {Pith review of: Imperceptible Adversarial Examples in the Physical World},
year = {2026},
howpublished = {\url{https://pith.science/paper/B2Q43A6J}},
note = {Machine review of arXiv:2411.16622}
}
abstract
Adversarial examples in the digital domain against deep learning-based computer vision models allow for perturbations that are imperceptible to human eyes. However, producing similar adversarial examples in the physical world has been difficult due to the non-differentiable image distortion functions in visual sensing systems. The existing algorithms for generating physically realizable adversarial examples often loosen their definition of adversarial examples by allowing unbounded perturbations, resulting in obvious or even strange visual patterns. In this work, we make adversarial examples imperceptible in the physical world using a straight-through estimator (STE, a.k.a. BPDA). We employ STE to overcome the non-differentiability -- applying exact, non-differentiable distortions in the forward pass of the backpropagation step, and using the identity function in the backward pass. Our differentiable rendering extension to STE also enables imperceptible adversarial patches in the physical world. Using printout photos, and experiments in the CARLA simulator, we show that STE enables fast generation of $\ell_\infty$ bounded adversarial examples despite the non-differentiable distortions. To the best of our knowledge, this is the first work demonstrating imperceptible adversarial examples bounded by small $\ell_\infty$ norms in the physical world that force zero classification accuracy in the global perturbation threat model and cause near-zero ($4.22\%$) AP50 in object detection in the patch perturbation threat model. We urge the community to re-evaluate the threat of adversarial examples in the physical world.
Figures
Figures from the paper (3 more)
Forward citations
Cited by 2 Pith papers
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ALLUDE: A Unified Evaluation System for Configurable Attacks in Differentiable Environments
A configurable, cross-platform simulator-based evaluation platform shows that object class and camera trajectory, not weather or detector choice, dominate whether 3D adversarial patch attacks succeed, and that all tes...
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UNDREAM: Bridging Differentiable Rendering and Photorealistic Simulation for End-to-end Adversarial Attacks
UnDREAM enables optimization of adversarial textures on arbitrary 3D objects inside Unreal Engine by bridging the simulator to the differentiable renderer Mitsuba.
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