2016
DOI: 10.21711/217504322016/em304
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An algorithm for computing the Seifert matrix of a link from a braid representation

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Cited by 9 publications
(11 citation statements)
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“…Essentially, drumhead states are boundary projections of a bulk surface stretched across the NLs i.e. a taut Seifert surface [14,15] of the NLs, with degeneracy corresponding to the multiplicity of the projection. But it has to be emphasized that this Seifert surface of a 3D nodal system is an entirely abstract construction [47] not verifiable from 2D boundary states, insofar as 3D geometric information, particularly of the knot over/under-crossings, is already lost in the surface projection.…”
Section: Drumhead States Versus Seifert Surfacesmentioning
confidence: 99%
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“…Essentially, drumhead states are boundary projections of a bulk surface stretched across the NLs i.e. a taut Seifert surface [14,15] of the NLs, with degeneracy corresponding to the multiplicity of the projection. But it has to be emphasized that this Seifert surface of a 3D nodal system is an entirely abstract construction [47] not verifiable from 2D boundary states, insofar as 3D geometric information, particularly of the knot over/under-crossings, is already lost in the surface projection.…”
Section: Drumhead States Versus Seifert Surfacesmentioning
confidence: 99%
“…A quintessential example is given by nodal knots existing in momentum space, where the knotted structure leads to new phases of matter protected by topological knot invariants. Unlike knotted molecules or optical vortices in real space [1][2][3], nodal knots consist of valence and conduction bands intersecting along one-dimensional (1D) lines in momentum space, which intertwine to form knotted nodal loops (NLs) [4][5][6][7][8][9][10][11][12][13] so multifarious that topological invariants take the form of polynomials rather than the Z 2 or Z integers [11][12][13][14][15] of ordinary topological insulators. Fundamental in constructing such invariants are the Seifert surfaces bounded by the nodal structure [14,15], which assume interesting, bubble-like shapes demarcating "drumhead" topological regions in the projected 2D surface Brillouin zone (BZ) [16][17][18][19].…”
Section: Introductionmentioning
confidence: 99%
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“…In this standard form, it is easy to define a homology basis (green) consisting of the independent closed loops traversing the twist operators. From this wedding cake, it is also not difficult to deduce the a representative braid for the knot/link by identifying the twist operators as braid operations, and the layers of the cake as the strands [62]. 2a, together with its lifted l # .…”
Section: Section I: Calculation Of the Topological Invariants Of The ...mentioning
confidence: 99%
“…We refer to Stallings [152], Gambaudo and Ghys [57], Cohen and van Wijk [41], Collins [42], Bourrigan [31] and Palmer [125] for more detailed accounts of the Seifert surfaces and Seifert matrices of braids.…”
Section: I+1 I+1 Imentioning
confidence: 99%