Magnetic Domains
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"Magnetic Domains" refers methods in this paper
...This equation is a BPS equation of the ABJM model [46, 47] just as the Basu-Harvey equation (4....
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...Now f and ω have the same volume type, so the non-compact version of Moser’s theorem [30] implies that there is a diffeomorphism w : M → Σφ0 and a constant q ∈ R such that w∗i∗f = q 4πω (see also [32])....
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"Magnetic Domains" refers background in this paper
...5) is a BPS equation of the BLG model [48, 49]....
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"Magnetic Domains" refers background or methods in this paper
...If we insert a D5-brane at s = 0 parallel to the NS5-branes and such that the D3-branes can intersect it, the strings connecting the D3- and D5-branes yield an additional fundamental hypermultiplet [34]....
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...To see this, let us T-dualize along T 212, and we arrive at the configuration 0 1 2 3 4 5 6 . . . D5 × × × 0 × × ` NS5 × × × ` × × 0 (1,1) × × × ` × × ` NS5 D5 (1, 1)-brane - 6 x3 x6 The NS5-brane ends at x3 = 0 and turns into a (p, q)-fivebrane with p = q = 1 which extends diagonally in R236 as indicated by the symbol `....
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...The alternative is to insert an NS5-brane....
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...This configuration is in fact related to a bound state between D5- and NS5-branes....
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...To compare with Chalmers-Hanany-Witten configurations [33, 34], we T-dualize along the x4- and x5-directions, S-dualize and obtain 0 1 2 3 4 5 6 . . . D3 × × × ` NS5 × × × × × × si (3.2) Dirac monopoles correspond to a single N = 1 NS5-brane at e.g. s = 0....
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