By Xusheng Zhang, Kunpeng Wang, Dongdai Lin (auth.), Michel Abdalla, Tanja Lange (eds.)
This ebook constitutes the refereed lawsuits of the fifth foreign convention on Pairing-Based Cryptography, Pairing 2012, held in Cologne, Germany, in may perhaps 2012.
The 17 complete papers for presentation on the educational music and three complete papers for presentation on the business song have been conscientiously reviewed and chosen from forty nine submissions. those papers are awarded including 6 invited talks. The contributions are equipped in topical sections on: algorithms for pairing computation, safeguard types for encryption, useful encryption, implementations in and software program, tune, homes of pairings, and signature schemes and applications.
Read or Download Pairing-Based Cryptography – Pairing 2012: 5th International Conference, Cologne, Germany, May 16-18, 2012, Revised Selected Papers PDF
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Extra resources for Pairing-Based Cryptography – Pairing 2012: 5th International Conference, Cologne, Germany, May 16-18, 2012, Revised Selected Papers
ASIACRYPT 2002. LNCS, vol. 2501, pp. 46–63. Springer, Heidelberg (2002) 5. : Eﬃcient Key Agreement and Signature Schemes Using Compact Representations in GF(p10 ). In: ISIT 2004, p. 13. IEEE (2004) 6. : Public-key Cryptosystems besed on Cubic Finite Field Extensions. IEEE Trans. Inform. Theory 45, 2601–2605 (1999) 7. : Discrete Logarithms in GF(p) Using the Number Field Sieve. SIAM J. on Discrete Math. 6, 124–138 (1993) 32 T. Yonemura et al. 8. : A Fast Algorithm for Computing Multiplicative Inverses in GF(2m ) Using Normal Bases.
Then for the elliptic curves of the form Y 2 = X 3 + B, the cost of fN,P (Q) is An Improved Twisted Ate Pairing over KSS Curves with k = 18 43 CLite = (5S1 + (2e + 6)M1 + Sk + Mk ) log2 N . In the case of KSS curves, s = 18, i = 1, j = 2, e = 3, k = 18, and in order to compare the costs of two pairings explicitly, we assume S1 = M1 . Then CLite = 167S1 log2 N . Denote the costs of fT 3 ,P (Q) and A by c1 and c2 , respectively. Considering equation (3) and z0 , we have c1 = 167S1 log2 T 3 ≈ 501S1 log2 χ , c2 = 351S1 log2 z0 ≈ 351S1 log2 χ , where χ is the curve parameter.
Practically, this representation is not worse than the aﬃne representation. Although compression and decompression incur some extra ﬁeld inversions in comparison with the aﬃne representation, this fact is not a serious disadvantage of the proposed representation because the costs of compression and decompression is much smaller than the costs of encryption and decryption. It is clear that the cost of inversion in the base ﬁeld is much smaller than the cost of exponentiation in the embedding ﬁeld.