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利用光子自旋霍尔效应的物理不可克隆函数

Physical unclonable function using photonic spin Hall effect.

作者信息

Divyanshu Divyanshu, Goyal Amit Kumar, Massoud Yehia

机构信息

Innovative Technologies Laboratories (ITL), King Abdullah University of Science and Technology (KAUST), 23955, Thuwal, Saudi Arabia.

出版信息

Sci Rep. 2024 Jun 22;14(1):14393. doi: 10.1038/s41598-024-65176-0.

DOI:10.1038/s41598-024-65176-0
PMID:38909056
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11193811/
Abstract

This study presents a novel method leveraging surface wave-assisted photonic spin Hall effect (PSHE) to construct physical unclonable functions (PUFs). PUFs exploit inherent physical variations to generate unique Challenge-Response pairs, which are critical for hardware security and arise from manufacturing discrepancies, device characteristics, or timing deviations. We explore PSHE generation-based PUF design, expanding existing design possibilities. With recent applications in precise sensing and computing, PSHE offers promising performance metrics for our proposed PUFs, including an inter-Hamming distance of 47.50% , an average proportion of unique responses of 62.5% , and a Pearson correlation coefficient of - 0.198. The PUF token demonstrates robustness to simulated noise. Additionally, we evaluate security using a machine learning-based attack model, employing a multi-layer perceptron (MLP) regression model with a randomized search method. The average accuracy of successful attack prediction is 9.70% for the selected dataset. Our novel PUF token exhibits high non-linearity due to the PSHE effect, resilience to MLP-based attacks, and sensitivity to process variation.

摘要

本研究提出了一种利用表面波辅助光子自旋霍尔效应(PSHE)来构建物理不可克隆函数(PUF)的新方法。PUF利用固有的物理变化来生成独特的挑战-响应对,这对于硬件安全至关重要,并且源于制造差异、器件特性或时序偏差。我们探索基于PSHE生成的PUF设计,扩展了现有的设计可能性。随着PSHE在精确传感和计算中的最新应用,它为我们提出的PUF提供了有前景的性能指标,包括汉明间距为47.50%、唯一响应的平均比例为62.5%以及皮尔逊相关系数为-0.198。PUF令牌对模拟噪声具有鲁棒性。此外,我们使用基于机器学习的攻击模型来评估安全性,采用具有随机搜索方法的多层感知器(MLP)回归模型。对于所选数据集,成功攻击预测的平均准确率为9.70%。由于PSHE效应,我们新颖的PUF令牌表现出高度非线性、对基于MLP的攻击具有弹性以及对工艺变化敏感。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6ae9/11193811/2ba99405959c/41598_2024_65176_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6ae9/11193811/dbe456cf775a/41598_2024_65176_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6ae9/11193811/5d27385775a2/41598_2024_65176_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6ae9/11193811/44fc51136414/41598_2024_65176_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6ae9/11193811/f6c9056a3d21/41598_2024_65176_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6ae9/11193811/b65d162bc910/41598_2024_65176_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6ae9/11193811/01626c0d4ec9/41598_2024_65176_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6ae9/11193811/2ba99405959c/41598_2024_65176_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6ae9/11193811/dbe456cf775a/41598_2024_65176_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6ae9/11193811/5d27385775a2/41598_2024_65176_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6ae9/11193811/44fc51136414/41598_2024_65176_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6ae9/11193811/f6c9056a3d21/41598_2024_65176_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6ae9/11193811/b65d162bc910/41598_2024_65176_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6ae9/11193811/01626c0d4ec9/41598_2024_65176_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6ae9/11193811/2ba99405959c/41598_2024_65176_Fig8_HTML.jpg

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