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By the Nahm transform, the moduli space of time-translation invariant self-dual Yang-Mills theory solitons on 4d Minkowski spacetime is equivalently the space of solutions to the Bogomolny equations on 3d Euclidean space, which in tur# iN n may be thought of as magnetic monopoles in 3d Euclidean Yang-Mills theory coupled to a charged scalar field (a “Higgs field”). Therefore this moduli space is traditionally referred to simply as the moduli space of magnetic monopoles (e.g. Atiyah-Hitchin 88) or just the moduli space of monopoles.
The moduli space
of monopoles is … (Atiyah-Hitchin 88, p. 15-16).
Write
for the space of pointed rational functions from the Riemann sphere to itself, of degree , inside the full Cohomotopy cocycle space. The homotopy type of is discussed in Segal 79.
To each configuration of magnetic monopoles is associated a scattering amplitude
(moduli space of k monopoles is space of degree complex-rational functions from Riemann sphere to itself)
The assignment (3) is a diffeomorphism identifying the moduli space (1) of magnetic monopoles with the space (2) of complex-rational functions from the Riemann sphere to itself, of degree (hence the cocycle space of complex-rational 2-Cohomotopy)
(due to Donaldson 84, see also Atiyah-Hitchin 88, Theorem 2.10).
(space of degree complex-rational functions from Riemann sphere to itself is k-equivalent to Cohomotopy cocycle space in degree )
The inclusion of the complex rational self-maps maps of degree into the full based space of maps of degree (hence the -component of the second iterated loop space of the 2-sphere, and hence the plain Cohomotopy cocycle space) induces an isomorphism of homotopy groups in degrees (in particular a k-equivalence):
Hence, Prop. and Prop. together say that the moduli space of -monopoles is -equivalent to the Cohomotopy cocycle space .
This is a non-abelian analog of the Dirac charge quantization of the electromagnetic field, with ordinary cohomology replaced by Cohomotopy cohomology theory:
(moduli space of monopoles is stably weak homotopy equivalent to classifying space of braid group)
For there is a stable weak homotopy equivalence between the moduli space of k monopoles (?) and the classifying space of the braid group on strands:
Generally Dp-D(p+2)-brane intersections geometrically engineer Yang-Mills monopoles in the worldvolume of the higher dimensional D-branes.
Specifically for , i.e. for D6-D8-brane intersections, this fits with the Witten-Sakai-Sugimoto model geometrically engineering quantum chromodynamics, and then gives a geometric engineering of the Yang-Mills monopoles in actual QCD (HLPY 08, p. 16).
Here we are showing
with
the 5d Chern-Simons theory on their worldvolume
the corresponding 4d WZW model on the boundary
both exhibiting the meson fields
(see below at WSS – Baryons)
the Yang-Mills monopole D6-branes
(see at D6-D8-brane bound state)
the NS5-branes.
Simon Donaldson, Nahm’s Equations and the Classification of Monopoles, Comm. Math. Phys., Volume 96, Number 3 (1984), 387-407, (euclid:cmp.1103941858)
Michael Atiyah, Nigel Hitchin, The geometry and dynamics of magnetic monopoles M. B. Porter Lectures. Princeton University Press, Princeton, NJ, 1988 (jstor:j.ctt7zv206)
Graeme Segal, The topology of spaces of rational functions, Acta Math. Volume 143 (1979), 39-72 (euclid:1485890033)
Michael Atiyah, Nigel Hitchin, J. T. Stuart and M. Tabor, Low-Energy Scattering of Non-Abelian Magnetic Monopoles, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences Vol. 315, No. 1533, New Developments in the Theory and Application of Solitons (Aug. 13, 1985), pp. 459-469 (jstor:37546)
Gary Gibbons, Nicholas Manton, Classical and Quantum Dynamics of BPS Monopoles, Nucl. Phys. B274 (1986) 183-224 (spire:18322, doi:10.1016/0550-3213(86)90624-3)
Ralph Cohen, Stability phenomena in the topology of moduli spaces (arXiv:0908.1938)
See also
In string theory Yang-Mills monopoles are geometrically engineeted as transversally intersecting Dp-D(p+2)-brane bound states:
For transversal D1-D3-brane bound states:
Duiliu-Emanuel Diaconescu, D-branes, Monopoles and Nahm Equations, Nucl. Phys. B503 (1997) 220-238 (arxiv:hep-th/9608163)
Amihay Hanany, Edward Witten, Type IIB Superstrings, BPS Monopoles, And Three-Dimensional Gauge Dynamics, Nucl. Phys. B492:152-190, 1997 (arxiv:hep-th/9611230)
Jessica K. Barrett, Peter Bowcock, Using D-Strings to Describe Monopole Scattering (arxiv:hep-th/0402163)
Jessica K. Barrett, Peter Bowcock, Using D-Strings to Describe Monopole Scattering - Numerical Calculations (arxiv:hep-th/0512211)
For transversal D2-D4 brane intersections (with an eye towards AdS/QCD):
For transversal D3-D5 brane intersections:
For transversal D6-D8-brane intersections (with an eye towards AdS/QCD):
With emphasis on half NS5-branes in type I' string theory:
The moduli space of monopoles appears also in the KK-compactification of the M5-brane on a complex surface (AGT-correspondence):
Relation to braid groups:
Fred Cohen, Ralph Cohen, B. M. Mann, R. J. Milgram, The topology of rational functions and divisors of surfaces, Acta Math (1991) 166: 163 (doi:10.1007/BF02398886)
Ralph Cohen, John D. S. Jones Monopoles, braid groups, and the Dirac operator, Comm. Math. Phys. Volume 158, Number 2 (1993), 241-266 (euclid:cmp/1104254240)
Relation of Dp-D(p+2)-brane bound states (hence Yang-Mills monopoles) to Vassiliev braid invariants via chord diagrams computing radii of fuzzy spheres:
Sanyaje Ramgoolam, Bill Spence, S. Thomas, Section 3.2 of: Resolving brane collapse with corrections in non-Abelian DBI, Nucl. Phys. B703 (2004) 236-276 (arxiv:hep-th/0405256)
Simon McNamara, Constantinos Papageorgakis, Sanyaje Ramgoolam, Bill Spence, Appendix A of: Finite effects on the collapse of fuzzy spheres, JHEP 0605:060, 2006 (arxiv:hep-th/0512145)
Simon McNamara, Section 4 of: Twistor Inspired Methods in Perturbative FieldTheory and Fuzzy Funnels, 2006 (spire:1351861, pdf, pdf)
Constantinos Papageorgakis, p. 161-162 of: On matrix D-brane dynamics and fuzzy spheres, 2006 (pdf)
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