Misorientation

My name is Jestine (34 years old) and my hobbies are Origami and Microscopy.

Here is my web site; http://Www.hostgator1centcoupon.info/ (support.file1.com) In physics, in the context of M-theory, the action for the N=8 M2 branes in full is (with some indices hidden):

$S=\int (-\frac{1}{2}{D}^{\mu }{X}_I{D}_{\mu }{X}_I+\frac{i}{2}\bar{\mathrm{\Psi }}{\mathrm{\Gamma }}^{\mu }{D}_{\mu }\mathrm{\Psi }+\frac{i}{4}\bar{\mathrm{\Psi }}{\mathrm{\Gamma }}_{IJ}[X^I,X^J,\mathrm{\Psi }]-\frac{1}{12}[X^I,X^J,X^K][X^I,X^J,X^K]+\frac{1}{2}{\epsilon }^{abc}Tr(A_a{\partial }_b{A}_c+\frac{2}{3}{A}_a{A}_b{A}_c))d{\sigma }^3$

where [, ] is a generalisation of a Lie bracket which gives the group constants.

The only known compatible solution however is:

${[A,B,C]}_{\eta }\equiv {\epsilon }^{\mu \nu \tau \eta }{A}_{\mu }{B}_{\nu }{C}_{\tau }$

using the Levi-Civita symbol which is invariant under SO(4) rotations. M5 branes can be introduced by using an infinite symmetry group.

The action is named after Jonathan Bagger, Neil Lambert, and Andreas Gustavsson.

Notes

43 year old Petroleum Engineer Harry from Deep River, usually spends time with hobbies and interests like renting movies, property developers in singapore new condominium and vehicle racing. Constantly enjoys going to destinations like Camino Real de Tierra Adentro.

References

• Lie 3-Algebra and Multiple M2-branes

Template:String-theory-stub