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A Verifiable Multi-Secret Sharing Scheme Based on Hermite Interpolation
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作者 Tomoko Adachi Chie Okazaki 《Journal of Mathematics and System Science》 2014年第9期587-592,共6页
A threshold scheme, which is introduced by Shamir in 1979, is very famous as a secret sharing scheme. We can consider that this scheme is based on Lagrange's interpolation formula. A secret sharing scheme has one key... A threshold scheme, which is introduced by Shamir in 1979, is very famous as a secret sharing scheme. We can consider that this scheme is based on Lagrange's interpolation formula. A secret sharing scheme has one key. On the other hand, a multi-secret sharing scheme has more than one key, that is, a multi-secret sharing scheme has p (〉_ 2) keys. Dealer distribute shares of keys among n participants. Gathering t (〈 n) participants, keys can be reconstructed. Yang et al. (2004) gave a scheme of a (t, n) multi-secret sharing based on Lagrange's interpolation. Zhao et al. (2007) gave a scheme of a (t, n) verifiable multi-secret sharing based on Lagrange's interpolation. Recently, Adachi and Okazaki give a scheme of a (t, n) multi-secret sharing based on Hermite interpolation, in the case ofp 〈 t. In this paper, we give a scheme ofa (t, n) verifiable multi-secret sharing based on Hermite interpolation. 展开更多
关键词 Verifiable secret sharing scheme Multi-secret sharing scheme Hermite interpolation
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不可分的么模定Hermite型的构作 被引量:1
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作者 朱福祖 《科学通报》 EI CAS CSCD 北大核心 1994年第12期1059-1061,共3页
设F=Q((-m)^(1/2))(m>0且无平方因子)为虚二次域,D_m为它的代数整数环.域F有一个非平凡的对合即复共轭,它的不动点域是Q.设V为域F上n维非退化的Hermite空间,并有关于上述对合的V上半双线性型φ以及与φ相伴的Hermite型H.设L为V上的D_... 设F=Q((-m)^(1/2))(m>0且无平方因子)为虚二次域,D_m为它的代数整数环.域F有一个非平凡的对合即复共轭,它的不动点域是Q.设V为域F上n维非退化的Hermite空间,并有关于上述对合的V上半双线性型φ以及与φ相伴的Hermite型H.设L为V上的D_m格,即L是V中的一个有限生成D_m模且FL=V.一个D_m格L称为偶格,是指对一切x∈L有H(x) 展开更多
关键词 不可分格 么模格 奇格 埃尔米特格
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Anti-(conjugate) linearity 被引量:1
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作者 Armin Uhlmann 《Science China(Physics,Mechanics & Astronomy)》 SCIE EI CAS CSCD 2016年第3期1-38,共38页
This is an introduction to antilinear operators. In following Wigner the terminus antilinear is used as it is standard in Physics.Mathematicians prefer to say conjugate linear. By restricting to finite-dimensional com... This is an introduction to antilinear operators. In following Wigner the terminus antilinear is used as it is standard in Physics.Mathematicians prefer to say conjugate linear. By restricting to finite-dimensional complex-linear spaces, the exposition becomes elementary in the functional analytic sense. Nevertheless it shows the amazing differences to the linear case. Basics of antilinearity is explained in sects. 2, 3, 4, 7 and in sect. 1.2: Spectrum, canonical Hermitian form, antilinear rank one and two operators,the Hermitian adjoint, classification of antilinear normal operators,(skew) conjugations, involutions, and acq-lines, the antilinear counterparts of 1-parameter operator groups. Applications include the representation of the Lagrangian Grassmannian by conjugations, its covering by acq-lines. As well as results on equivalence relations. After remembering elementary Tomita-Takesaki theory, antilinear maps, associated to a vector of a two-partite quantum system, are defined. By allowing to write modular objects as twisted products of pairs of them, they open some new ways to express EPR and teleportation tasks. The appendix presents a look onto the rich structure of antilinear operator spaces. 展开更多
关键词 OPERATORS canonical form antilinear (skew) hermiticity acq-lines
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