射频识别椭圆曲线密码处理器的高效架构

Lawrence Leinweber, C. Papachristou, F. Wolff
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引用次数: 7

摘要

RFID标签将取代条形码在供应链中进行产品识别。在视线之外读取标签的能力是它的主要优点,但会损害标签所有者的隐私。公钥加密可以恢复这种隐私。由于应用的极端经济限制,必须最小化加密功能的芯片面积和功耗。椭圆曲线处理器有效地提供了RFID所需的加密能力。本文提出了GF(2m)中椭圆曲线处理器的高效架构。一种设计需要6个m位寄存器和每个键位6个伽罗瓦域乘法运算。另一种设计需要5个m位寄存器和每个键位7个伽罗瓦域乘法运算。这些处理器需要少量的电路元件和时钟周期,同时提供对简单侧信道攻击的保护。给出了250nm、130nm和90nm工艺的功耗、面积和延迟的综合结果。与文献中先前的设计相比,所提出的处理器需要更少的面积和能量。对于具有位串行乘法器的B-163曲线,采用IBM低功耗130 nm技术合成的首次提出的设计需要9613栅极当量的面积,163,355个周期和4.14µJ的椭圆曲线点乘法。另一种提出的设计需要8756个栅极等效,190,570个周期和4.19µJ。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Efficient architectures for elliptic curve cryptography processors for RFID
RFID tags will supplant barcodes for product identification in the supply chain. The capability of a tag to be read without a line of sight is its principal benefit, but compromises the privacy of the tag owner. Public key cryptography can restore this privacy. Because of the extreme economic constraints of the application, die area and power consumption for cryptographic functions must be minimized. Elliptic curve processors efficiently provide the cryptographic capability needed for RFID. This paper proposes efficient architectures for elliptic curve processors in GF(2m). One design requires six m-bit registers and six Galois field multiply operations per key bit. The other design requires five m-bit registers and seven Galois field multiply operations per key bit. These processors require a small number of circuit elements and clock cycles while providing protection from simple side-channel attacks. Synthesis results are presented for power, area, and delay in 250, 130 and 90 nm technologies. Compared with prior designs from the literature, the proposed processors require less area and energy. For the B-163 curve, with bit-serial multiplier, the first proposed design synthesized in an IBM low-power 130 nm technology requires an area of 9613 gate equivalents, 163,355 cycles and 4.14 µJ for an elliptic curve point multiplication. The other proposed design requires 8756 gate equivalents, 190,570 cycles and 4.19 µJ.
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