nLab D1-D3-brane bound state

Redirected from "D1-D3 brane intersections".
Contents

Contents

Idea

The special case of Dp-D(p+2)-brane bound states for D1-D3-brane bound states.


brane intersections/bound states/wrapped branes/polarized branes

S-duality\,bound states:

intersecting\,M-branes:

References

For more see the references at Dp-D(p+2)-brane bound state:

Parallel intersection

  • Gianluca Grignani, Troels Harmark, Andrea Marini, Marta Orselli, Thermal DBI action for the D3-brane at weak and strong coupling, JHEP 03 (2014) 114 (arxiv:1311.3834)

Transversal intersection

As spikes/BIons (D3-brane perspective)

As spikes/BIons in the D3-brane DBI-theory:

from the M5-brane:

As fuzzy funnels (D1-brane perspective)

As fuzzy funnels (the D1-brane matrix model perspective):

As monopoles

Identification with Yang-Mills monopoles:

  • Duiliu-Emanuel Diaconescu, D-branes, Monopoles and Nahm Equations, Nucl. Phys. B503 (1997) 220-238 (arxiv:hep-th/9608163)

  • 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)

D1-D3 brane intersections in AdS 2/CFT 1AdS_2/CFT_1

On D1-D3 brane intersections in AdS2/CFT1:

Via T-duality from D6-D8 brane intersections:

Lift to M2-M5-brane bound states

The lift of Dp-D(p+2)-brane 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 (this eventually motivated the BLG-model/ABJM model):

Last revised on April 2, 2020 at 13:20:27. See the history of this page for a list of all contributions to it.