Open main menu
Home
Random
Recent changes
Special pages
Community portal
Preferences
About Wikipedia
Disclaimers
Incubator escapee wiki
Search
User menu
Talk
Dark mode
Contributions
Create account
Log in
Editing
M-theory
(section)
Warning:
You are not logged in. Your IP address will be publicly visible if you make any edits. If you
log in
or
create an account
, your edits will be attributed to your username, along with other benefits.
Anti-spam check. Do
not
fill this in!
===ABJM superconformal field theory=== {{main article|ABJM superconformal field theory}} Another realization of the AdS/CFT correspondence states that M-theory on {{math|''AdS''<sub>4</sub>×''S''<sup>7</sup>}} is equivalent to a quantum field theory called the [[ABJM superconformal field theory|ABJM theory]] in three dimensions. In this version of the correspondence, seven of the dimensions of M-theory are curled up, leaving four non-compact dimensions. Since the spacetime of our universe is four-dimensional, this version of the correspondence provides a somewhat more realistic description of gravity.<ref name="Aharony et al. 2008">Aharony et al. 2008</ref> The ABJM theory appearing in this version of the correspondence is also interesting for a variety of reasons. Introduced by Aharony, Bergman, Jafferis, and Maldacena, it is closely related to another quantum field theory called [[Chern–Simons theory]]. The latter theory was popularized by Witten in the late 1980s because of its applications to knot theory.<ref>Witten 1989</ref> In addition, the ABJM theory serves as a semi-realistic simplified model for solving problems that arise in condensed matter physics.<ref name="Aharony et al. 2008"/>
Edit summary
(Briefly describe your changes)
By publishing changes, you agree to the
Terms of Use
, and you irrevocably agree to release your contribution under the
CC BY-SA 4.0 License
and the
GFDL
. You agree that a hyperlink or URL is sufficient attribution under the Creative Commons license.
Cancel
Editing help
(opens in new window)