7 research outputs found

    Cayley-Dickson Algebras and Finite Geometry

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    Given a 2N2^N-dimensional Cayley-Dickson algebra, where 3≤N≤63 \leq N \leq 6, we first observe that the multiplication table of its imaginary units eae_a, 1≤a≤2N−11 \leq a \leq 2^N -1, is encoded in the properties of the projective space PG(N−1,2)(N-1,2) if one regards these imaginary units as points and distinguished triads of them {ea,eb,ec}\{e_a, e_b, e_c\}, 1≤a<b<c≤2N−11 \leq a < b <c \leq 2^N -1 and eaeb=±ece_ae_b = \pm e_c, as lines. This projective space is seen to feature two distinct kinds of lines according as a+b=ca+b = c or a+b≠ca+b \neq c. Consequently, it also exhibits (at least two) different types of points in dependence on how many lines of either kind pass through each of them. In order to account for such partition of the PG(N−1,2)(N-1,2), the concept of Veldkamp space of a finite point-line incidence structure is employed. The corresponding point-line incidence structure is found to be a binomial ((N+12)N−1,(N+13)3)\left({N+1 \choose 2}_{N-1}, {N+1 \choose 3}_{3}\right)-configuration CN{\cal C}_N; in particular, C3{\cal C}_3 (octonions) is isomorphic to the Pasch (62,43)(6_2,4_3)-configuration, C4{\cal C}_4 (sedenions) is the famous Desargues (103)(10_3)-configuration, C5{\cal C}_5 (32-nions) coincides with the Cayley-Salmon (154,203)(15_4,20_3)-configuration found in the well-known Pascal mystic hexagram and C6{\cal C}_6 (64-nions) is identical with a particular (215,353)(21_5,35_3)-configuration that can be viewed as four triangles in perspective from a line where the points of perspectivity of six pairs of them form a Pasch configuration. We also draw attention to a remarkable nesting pattern formed by these configurations, where CN−1{\cal C}_{N-1} occurs as a geometric hyperplane of CN{\cal C}_N. Finally, a brief examination of the structure of generic CN{\cal C}_N leads to a conjecture that CN{\cal C}_N is isomorphic to a combinatorial Grassmannian of type G2(N+1)G_2(N+1).Comment: 26 pages, 20 figures; V2 - the basis made explicit, a footnote and a couple of references adde

    Distinguished three-qubit 'magicity' via automorphisms of the split Cayley hexagon

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    Disregarding the identity, the remaining 63 elements of the generalized three-qubit Pauli group are found to contain 12096 distinct copies of Mermin's magic pentagram. Remarkably, 12096 is also the number of automorphisms of the smallest split Cayley hexagon. We give a few solid arguments showing that this may not be a mere coincidence. These arguments are mainly tied to the structure of certain types of geometric hyperplanes of the hexagon. It is further demonstrated that also an (18_{2}, 12_{3})-type of magic configurations, recently proposed by Waegell and Aravind (J. Phys. A: Math. Theor. 45 (2012) 405301), seems to be intricately linked with automorphisms of the hexagon. Finally, the entanglement properties exhibited by edges of both pentagrams and these particular Waegell-Aravind configurations are addressed.Comment: 15 pages, 4 figures, 5 table

    Veldkamp-Space Aspects of a Sequence of Nested Binary Segre Varieties

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    Let S(N)≡PG(1, 2)×PG(1, 2)×⋯×PG(1, 2)S_{(N)} \equiv PG(1,\,2) \times PG(1,\,2) \times \cdots \times PG(1,\,2) be a Segre variety that is NN-fold direct product of projective lines of size three. Given two geometric hyperplanes H′H' and H′′H'' of S(N)S_{(N)}, let us call the triple {H′,H′′,H′ΔH′′‾}\{H', H'', \overline{H' \Delta H''}\} the Veldkamp line of S(N)S_{(N)}. We shall demonstrate, for the sequence 2≤N≤42 \leq N \leq 4, that the properties of geometric hyperplanes of S(N)S_{(N)} are fully encoded in the properties of Veldkamp {\it lines} of S(N−1)S_{(N-1)}. Using this property, a complete classification of all types of geometric hyperplanes of S(4)S_{(4)} is provided. Employing the fact that, for 2≤N≤42 \leq N \leq 4, the (ordinary part of) Veldkamp space of S(N)S_{(N)} is PG(2N−1,2)PG(2^N-1,2), we shall further describe which types of geometric hyperplanes of S(N)S_{(N)} lie on a certain hyperbolic quadric Q0+(2N−1,2)⊂PG(2N−1,2)\mathcal{Q}_0^+(2^N-1,2) \subset PG(2^N-1,2) that contains the S(N)S_{(N)} and is invariant under its stabilizer group; in the N=4N=4 case we shall also single out those of them that correspond, via the Lagrangian Grassmannian of type LG(4,8)LG(4,8), to the set of 2295 maximal subspaces of the symplectic polar space W(7,2)\mathcal{W}(7,2).Comment: 16 pages, 8 figures and 7 table

    Jordan Decompositions of Tensors

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    We expand on an idea of Vinberg to take a tensor space and the natural Lie algebra which acts on it and embed them into an auxiliary algebra. Viewed as endomorphisms of this algebra we associate adjoint operators to tensors. We show that the group actions on the tensor space and on the adjoint operators are consistent, which endows the tensor with a Jordan decomposition. We utilize aspects of the Jordan decomposition to study orbit separation and classification in examples that are relevant for quantum information

    Robust digital optimal control on IBM quantum computers

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    The ability of pulse-shaping devices to generate accurately quantum optimal control is a strong limitation to the development of quantum technologies. We propose and demonstrate a systematic procedure to design robust digital control processes adapted to such experimental constraints. We show to what extent this digital pulse can be obtained from its continuous-time counterpart. A remarkable efficiency can be achieved even for a limited number of pulse parameters. We experimentally implement the protocols on IBM quantum computers for a single qubit, obtaining an optimal robust transfer in a time T = 382 ns
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