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added the following pointers:
Relation of Dp-D(p+2)-brane bound states to knot invariants via chord diagrams:
S. Ramgoolam, B. Spence, S. Thomas, Section 3.2 of: Resolving brane collapse with $1/N$ corrections in non-Abelian DBI, Nucl. Phys. B703 (2004) 236-276 (arxiv:hep-th/0405256)
S. McNamara, Constantinos Papageorgakis, S. Ramgoolam, B. Spence, Appendix A of: Finite $N$ effects on the collapse of fuzzy spheres, JHEP 0605:060, 2006 (arxiv:hep-th/0512145)
Constantinos Papageorgakis, p. 161-162 of: On matrix D-brane dynamics and fuzzy spheres, 2006 (Papageorgakis06.pdf:file)
added pointer also to
am adding references on the lift to M-theory:
The lift of Dp-D(p+2)-bound states in string theory to M2-M5-brane bound states/E-strings in M-theory, under duality between M-theory and type IIA string theory+T-duality, via generalization of Nahm’s equation:
Anirban Basu, Jeffrey Harvey, The M2-M5 Brane System and a Generalized Nahm’s Equation, Nucl.Phys. B713 (2005) 136-150 (arXiv:hep-th/0412310)
{#BaggerLambertMukhiPapageorgakis13} Jonathan Bagger, Neil Lambert, Sunil Mukhi, Constantinos Papageorgakis, Section 2.2.1 of Multiple Membranes in M-theory, Physics Reports, Volume 527, Issue 1, 1 June 2013, Pages 1-100 (arXiv:1203.3546, doi:10.1016/j.physrep.2013.01.006)
copied the section on fuzzy funnel shape observables as $\mathfrak{su}(2)$-weight systems on chord diagrams from fuzzy sphere also to here
added some actual content to the section “As fuzzy funnels” (here),
highlighting in the end that with the gauge field taken into account, the fuzzy funnel system is not just a $\mathfrak{sl}(2,\mathbb{C})$-rep, but in fact a $\mathfrak{gl}(2,\mathbb{C})$
(this is often ignored, but it is implicit in Gaiotto-Witten 08, Section 3.1.1)
added illustration of the passage from chord diagrams to fuzzy funnels (here)
will add this graphics also to fuzzy funnel and maybe elsewhere
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