[PDF] from arxiv.orgS Bellucci… - Arxiv preprint arXiv:1106.2434, 2011 - arxiv.org ... It was required to find the so called Xtensor discussed in [2], and then finding a consistent set of solutions to the Bianchi identities in superspace in the torsion, curvature and H sectors at dimension zero through 3 2 . This was achieved in [1] and [7] to second order. ... Related articles - All 2 versions
[PDF] from arxiv.orgG Leithall… - Physical Review E, 2011 - APS ... 16]. The third diagram in (1) is a shorthand notation, where, eg, the first bond, together with its filled circle, represents ∑ i ∫ dr1ρi(r1)wi μ(|r1 − x|) ≡ nμ(x); tensor contraction over all Greek indices is implied. Both wi μ and nμ ... Related articles - All 7 versions
[PDF] from arxiv.orgAB Goncharov - Arxiv preprint arXiv:1107.5710, 2011 - arxiv.org Page 1. arXiv:1107.5710v1 [math.AG] 28 Jul 2011 Hidden Hodge symmetries and Hodge correlators AB Goncharov To Don Zagier for his 60-th birthday 1 Hidden Hodge symmetries There is a well known parallel between Hodge ...
Y Othmani, L Delannay… - International Journal of Solids and …, 2011 - Elsevier ... pquv pquv pquvx (x) (x) = + where 0 0 pquv jkms rauv rsam pj,kq (x) CC n (y)n (y)n (y)n (y) (xy)ds(y) x = (23) and 0 0 pquv jkms sauv am pj,kq (x) CC n (y)n (y) (xy)ds(y) x = (24) The latter integral can be derived from (23) by setting r = s. Thus, the ( )pquv xtensor can be ...
[PDF] from arxiv.orgC Ahn, J Paeng… - Arxiv preprint arXiv:1107.0640, 2011 - arxiv.org ... the 4-forms appearing in the left hand side of (2.13) occur naturally. On the other hand, the Aijkl µ (x) tensor in (2.13) appears in the scalar kinetic terms of 4-dimensional N = 8 gauged supergravity and it is given by Aijkl µ (x) = −2 √2(uij IJ ∂µvklIJ − vijIJ ∂µukl IJ ) . (2.14) ... Related articles - All 2 versions
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