A bound state/brane intersection of D0-branes with D2-branes. Special case of Dp-D(p+2) brane bound states.
What is called the Myers effect (Myers 99) in string theory is the claimed phenomenon that given $N$ D0-branes in a constant background RR field $F_4$ (the field strength associated with D2-brane charge) with, crucially, nonabelian effects included, then these D0-branes expand into a fuzzy 2-sphere which represents a spherical D0-D2 brane bound state of a D2-brane and $N$ D0-branes (Myers 99, section 6, see p. 22, Myers 03, section 4).
brane intersections/bound states/wrapped branes
D-branes and anti D-branes form bound states by tachyon condensation, thought to imply the classification of D-brane charge by K-theory
intersecting D-branes/fuzzy funnels:
Dp-D(p+6) brane bound state
intersecting$\,$M-branes:
(…)
The effect now known as the “Myers effect” in D-brane theory was first described in:
Review includes
See also
Pedro J. Silva, Quantum Myers effect and its supergravity dual for D0/D4 systems (arXiv:hep-th/0109112)
Yoshifumi Hyakutake, Gravitational Dielectric Effect and Myers Effect, Phys.Rev.D71:046007,2005 (arXiv:hep-th/0401026)
Yoshinao Sato, Dissolving D0-brane into D2-brane with background B-field, JHEP 0512 (2005) 032 (arXiv:hep-th/0505045)
On solutions of the BMN matrix model in relation to the Myers effect and D0-D2 brane bound states:
Last revised on January 12, 2020 at 16:33:28. See the history of this page for a list of all contributions to it.