The theory of 11-dimensional supergravity contains a higher gauge field – the supergravity C-field – that naturally couples to higher electrically charged 2-branes, membranes (Bergshoeff-Sezgin-Townsend 87). By double dimensional reduction, these turn into the superstrings of type IIA string theory (Duff-Howe-Inami-Stelle 87). (See at duality between M-theory and type IIA string theory.)
When in (Witten95) it was argued that the 10-dimensional target space theories of the five types of superstring theories are all limiting cases of one single 11-dimensional target space theory that extends 11-dimensional supergravity (M-theory), it was natural to guess that this supergravity membrane accordingly yields a 3-dimensional sigma-model that reduces in limiting cases to the string sigma-models.
But there were two aspects that make this idea a little subtle, even at this vague level: first, there is no good theory of the quantization of the membrane sigma-model, as opposed to the well understood quantum string. Secondly, that hypothetical “theory extending 11-dimensional supergravity” (“M-theory”) has remained elusive enough that it is not clear in which sense the membrane would relate to it in a way analogous to how the string relates to its target space theories (which is fairly well understood).
Later, with the BFSS matrix model some people gained more confidence in the idea, by identifying the corresponding degrees of freedom in a special case (Nicolai-Helling 98, Dasgupta-Nicolai-Plefka 02). See also at membrane matrix model.
In a more modern perspective, the M2-brane worldvolume theory appears under AdS4-CFT3 duality as a holographic dual of a 4-dimensional Chern-Simons theory. Indeed, its Green-Schwarz action functional is entirely controled by the super-Lie algebra 4-cocycle of super Minkowski spacetime given by the brane scan. This exhibits the M2-brane worldvolume theory as a 3-dimensional higher dimensional WZW model.
There are two different incarnations of the M2-brane. On the one hand it is defined as a Green-Schwarz sigma model with target space a spacetime that is a solution to the equations of motion of 11-dimensional supergravity. One would call this the “fundamental” M2 in analogy with the “fundamental string”, if only there were an “M2-perturbation series” which however is essentially ruled out.
On the other hand the M2 also appears as a black brane, hence as a solution to the equations of motion of 11-dimensional supergravity with singularity that looks from outside like a charged 2 dimensional object.
See at Green-Schwarz sigma model and brane scan.
As a black brane solution to the equations of motion of 11-dimensional supergravity, with vanishing C-field flux, the M2 is the spacetime $\mathbb{R}^{2,1} \times (\mathbb{R}^8-\{0\})$ with pseudo-Riemannian metric being
where
for $(\alpha,\beta) \in \mathbb{R}^2 \setminus \{(0,0)\}$;
and the field strength of the supergravity C-field is
For $\alpha \beta \neq 0$ this is a 1/2 BPS state of 11d sugra.
In the above coordinates the metric is ill-defined at $r = - \beta^{1/6} \alpha$, but in fact it may be smoothly continued through this point (Duff-Gibbons-Townsend 94, section 3), which is a event horizon. An actual singularity is at $r = 0$.
The near horizon geometry of this spacetime is the Freund-Rubin compactification AdS4$\times$S7. For more on this see at AdS-CFT.
1/2 BPS black branes in supergravity: D-branes, F1-brane, NS5-brane, M2-brane, M5-brane
(table taken from Blumenhagen-Lüst-Theisen 13, Chapter 18.5)
More generally, one may classify those solutions of 11-dimensional supergravity of the form $AdS_4 \times X_7$ for some closed manifold $X_7$, that are at least 1/2 BPS states. One finds (Medeiros-Figueroa 10) that all these are of the form $AdS_4 \times S^7/G_{ADE}$, where $S^7 / G_{ADE}$ is an orbifold of the 7-sphere (a spherical space form in the smooth case, see there) by a finite subgroup of SU(2) $G_{ADE} \hookrightarrow SU(2)$, i.e. a finite group in the ADE-classification
ADE classification and McKay correspondence
Here for $5 \leq \mathcal{N} \leq 8$-supersymmetry then the action of $G_{ADE}$ on $S^7$ is via the canonical action of $SU(2)$ as in the quaternionic Hopf fibration (Medeiros-Figueroa 10), while for $\mathcal{N} = 4$ then there is an extra twist to the action (MFFGME 09). See the table below.
In the presence of non-vanishing C-field flux $G_4$, the electric flux density of M2-branes is not $G_7 \coloneqq \star G_4$ alone, but receives corrections, first due to the quadratic C-field self-interaction in D=11 supergravity, but then also due to the shifted C-field flux quantization expected in M-theory:
The 11d supergravity literature states the corrected 7-flux to be the following combination, also known as the Page charge (due to Page 83 (8), Duff-Stelle 91 (43), reviewed e.g. in BLMP 13, p. 21):
where the second term subtracts the electric flux induced by the self-intersection of the field, and also ensures that the full expression is a closed differential form if the naive 11d supergravity equations of motion hold:
But in fact (1) does not quite make general sense, for two reasons:
In general $G_4 = 0$ is not an admissible condition and is not the actual vanshing of the C-field, due to the shifted C-field flux quantization.
Even if $G_4$ happens to be intregrally quantizaed (if $\tfrac{1}{4}p_1$ is integral) the appearance of a globally defined C-field potential $C_3$ in (1),means that the total flux actually does vanish after all.
Charge-quantized $\widetilde G_7$-flux with shifted C-field flux quantization (FSS 19b, Prop. 4.3, FSS 19c, Section 4)
Both of these issues are solved if the C-field is taken to be charge quantized in J-twisted Cohomotopy (Hypothesis H). This gives the corrected formula
where
the expression lives on the homotopy pullback of the Sp(2)-parametrized quaternionic Hopf fibration
to spacetime, along the twisted Cohomotopy-cocycle that represents the C-field under Hypothesis H;
$\widetilde G_4 \coloneqq h^\ast G_4 + \tfrac{1}{4}h^\ast p_1(\nabla)$ is the integral shifted C-field pulled back to that 3-spherical fibration over spacetime;
$d H_3 = h^\ast G_4 - \tfrac{1}{4}h^\ast p_1(\nabla)$ trivializes not the C-field itself, but its pullback, and not absolutely but relative to the background charge implied by shifted C-field flux quantization.
With the corrected 7-flux in twisted Cohomotopy it becomes true that
the integral of $G_7$ around the 7-sphere linking a black M2-brane is always integer (FSS 19c, Theorem 4.6);
this integer satisfies the C-field tadpole cancellation condition (FSS 19b, Section 4.6).
A regularized quantization of the Green-Schwarz sigma-model for the M2-brane yields the BFSS matrix model (Nicolai-Helling 98, Dasgupta-Nicolai-Plefka 02).
In this correspondence, matrix blocks around the diagonal correspond to blobs of membrane, while off-diagonal matrix elements correspond to thin tubes of membrane connecting these blobs.
graphics grabbed from Dasgupta-Nicolai-Plefka 02
The worldvolume QFT of black M2-branes is a 3d superconformal gauge field theory:
$d$ | $N$ | superconformal super Lie algebra | R-symmetry | black brane worldvolume superconformal field theory via AdS-CFT |
---|---|---|---|---|
$\phantom{A}3\phantom{A}$ | $\phantom{A}2k+1\phantom{A}$ | $\phantom{A}B(k,2) \simeq$ osp$(2k+1 \vert 4)\phantom{A}$ | $\phantom{A}SO(2k+1)\phantom{A}$ | |
$\phantom{A}3\phantom{A}$ | $\phantom{A}2k\phantom{A}$ | $\phantom{A}D(k,2)\simeq$ osp$(2k \vert 4)\phantom{A}$ | $\phantom{A}SO(2k)\phantom{A}$ | M2-brane D=3 SYM BLG model ABJM model |
$\phantom{A}4\phantom{A}$ | $\phantom{A}k+1\phantom{A}$ | $\phantom{A}A(3,k)\simeq \mathfrak{sl}(4 \vert k+1)\phantom{A}$ | $\phantom{A}U(k+1)\phantom{A}$ | D3-brane D=4 N=4 SYM D=4 N=2 SYM D=4 N=1 SYM |
$\phantom{A}5\phantom{A}$ | $\phantom{A}1\phantom{A}$ | $\phantom{A}F(4)\phantom{A}$ | $\phantom{A}SO(3)\phantom{A}$ | D4-brane D=5 SYM |
$\phantom{A}6\phantom{A}$ | $\phantom{A}k\phantom{A}$ | $\phantom{A}D(4,k) \simeq$ osp$(8 \vert 2k)\phantom{A}$ | $\phantom{A}Sp(k)\phantom{A}$ | M5-brane D=6 N=(2,0) SCFT D=6 N=(1,0) SCFT |
(Shnider 88, also Nahm 78, see Minwalla 98, section 4.2)
Specifically, worldvolume quantum field theory of M2-branes sitting at ADE singularities (as above) is supposed to be described by ABJM theory and, for the special case of $SU(2)$ gauge group, by the BLG model. See also at gauge enhancement.
$N$ Killing spinors on spherical space form $S^7/\widehat{G}$ | $\phantom{AA}\widehat{G} =$ | spin-lift of subgroup of isometry group of 7-sphere | 3d superconformal gauge field theory on back M2-branes with near horizon geometry $AdS_4 \times S^7/\widehat{G}$ |
---|---|---|---|
$\phantom{AA}N = 8\phantom{AA}$ | $\phantom{AA}\mathbb{Z}_2$ | cyclic group of order 2 | BLG model |
$\phantom{AA}N = 7\phantom{AA}$ | — | — | — |
$\phantom{AA}N = 6\phantom{AA}$ | $\phantom{AA}\mathbb{Z}_{k\gt 2}$ | cyclic group | ABJM model |
$\phantom{AA}N = 5\phantom{AA}$ | $\phantom{AA}2 D_{k+2}$ $2 T$, $2 O$, $2 I$ | binary dihedral group, binary tetrahedral group, binary octahedral group, binary icosahedral group | (HLLLP 08a, BHRSS 08) |
$\phantom{AA}N = 4\phantom{AA}$ | $\phantom{A}2 D_{k+2}$ $2 O$, $2 I$ | binary dihedral group, binary octahedral group, binary icosahedral group | (HLLLP 08b, Chen-Wu 10) |
Under AdS-CFT duality the M2-brane is given by AdS4-CFT3 duality. (Maldacena 97, section 3.2, Klebanov-Torri 10).
For M2-M5 brane bound states, i.e. bound states of M2-branes with M5-branes (dyonic M2-branes and giant gravitons), see the references below.
For the type II string theory-version see at NS5-brane the sectoin NS5/D4/D2 bound states.
Table of branes appearing in supergravity/string theory (for classification see at brane scan).
The Green-Schwarz sigma-model-type formulation of the supermembrane (as in the brane scan) first appears in
The equations of motion of the super membrane are derived via the superembedding approach in
and the Lagrangian density for the super membrane is derived via the superembedding approach in
Discussion from the point of view of Green-Schwarz action functional-∞-Wess-Zumino-Witten theory is in
Its quantization of the was explored in
Mike Duff, T. Inami, Christopher Pope, Ergin Sezgin, Kellogg Stelle, Semiclassical Quantization of the Supermembrane, Nucl.Phys. B297 (1988) 515-538 (spire:247064)
Bernard de Wit, Jens Hoppe, Hermann Nicolai, On the Quantum Mechanics of Supermembranes, Nucl. Phys. B305 (1988) 545. (pdf, pdf, spire:261702)
Bernard de Wit, W. Lüscher, Hermann Nicolai, The supermembrane is unstable, Nucl. Phys. B320 (1989) 135 (spire:266584, doi:10.1016/0550-3213(89)90214-9)
Daniel Kabat, Washington Taylor, section 2 of Spherical membranes in Matrix theory, Adv.Theor.Math.Phys.2:181-206,1998 (arXiv:hep-th/9711078)
The double dimensional reduction of the M2-brane to the Green-Schwarz superstring was observed in
The interpretation of the membrane as an object related to string theory via double dimensional reduction, hence as the M2-brane was proposed in
around the time when M-theory became accepted due to
The proposed regularization, due to deWit-Hoppe-Nicolai 88, of area-preserving diffeomorphisms on the membrane worldvolume by SU(N)-matrices and the resulting equivalence of the quantization of the membrane to the BFSS matrix model of D0-branes is reviewed and further dicussed in the following articles:
Hermann Nicolai, Robert Helling, Supermembranes and M(atrix) Theory, In Trieste 1998, Nonperturbative aspects of strings, branes and supersymmetry 29-74 (arXiv:hep-th/9809103, spire:476366)
Arundhati Dasgupta, Hermann Nicolai, Jan Plefka, An Introduction to the Quantum Supermembrane, Grav.Cosmol.8:1,2002; Rev.Mex.Fis.49S1:1-10, 2003 (arXiv:hep-th/0201182)
Gijs van den Oord, On Matrix Regularisation of Supermembranes, 2006 (pdf)
The back membrane solution of 11-dimensional supergravity was found in
Its regularity throughout the event horizon is due to
Further discussion of such Freund-Rubin compactifications:
The Horava-Witten-orientifold of the black M2, supposedly yielding the black heterotic string is discussed in
Zygmunt Lalak, André Lukas, Burt Ovrut, Soliton Solutions of M-theory on an Orbifold, Phys. Lett. B425 (1998) 59-70 (arXiv:hep-th/9709214)
Ken Kashima, The M2-brane Solution of Heterotic M-theory with the Gauss-Bonnet $R^2$ terms, Prog.Theor.Phys. 105 (2001) 301-321 (arXiv:hep-th/0010286)
Meanwhile AdS-CFT duality was recognized in
where a dual description of the worldvolume theory of M2-brane appears in section 3.2. More on this is in
An account of the history as of 1999 is in
More recent review is in
A detailed discussion of this black brane-realization of the M2 and its relation to AdS-CFT is in
The generalization of this to $\geq 1/2$ BPS sugra solutions of the form $AdS_4 \times X_7$ is due to
Paul de Medeiros, José Figueroa-O'Farrill, Sunil Gadhia, Elena Méndez-Escobar, Half-BPS quotients in M-theory: ADE with a twist, JHEP 0910:038,2009 (arXiv:0909.0163, pdf slides)
Paul de Medeiros, José Figueroa-O'Farrill, Half-BPS M2-brane orbifolds, Adv. Theor. Math. Phys. Volume 16, Number 5 (2012), 1349-1408. (arXiv:1007.4761, Euclid)
Discussion of the history includes
Other recent developments are discussed in
Paul Howe, Ergin Sezgin, The supermembrane revisited, (arXiv:hep-th/0412245)
Igor Bandos, Paul Townsend, SDiff Gauge Theory and the M2 Condensate (arXiv:0808.1583)
Jonathan Bagger, Neil Lambert, Sunil Mukhi, Constantinos Papageorgakis, Multiple Membranes in M-theory, Physics Reports, Volume 527, Issue 1, 1 June 2013, Pages 1-100 (arXiv:1203.3546, doi:10.1016/j.physrep.2013.01.006)
Nathan Berkovits, Towards Covariant Quantization of the Supermembrane (arXiv:hep-th/0201151)
Formulations of multiple M2-branes on top of each other are given by the BLG model and the ABJM model. See there for more pointers. The relation of these to the above is discussed in section 3 of
Discusson of boundary conditions in the ABJM model (for M2-branes ending on M5-branes) is in
A kind of double dimensional reduction of the ABJM model to something related to type II superstrings and D1-branes is discussed in
Discussion of the ABJM model in Horava-Witten theory and reducing to heterotic strings is in
Discussion of general phenomena of M-branes in higher geometry and generalized cohomology is in
Discussion of $G7$-charge quantization in the fluxed case:
Domenico Fiorenza, Hisham Sati, Urs Schreiber, Prop. 4.31 of: Twisted Cohomotopy implies M-theory anomaly cancellation (arXiv:1904.10207)
The role of and the relation to duality in string theory of the membrane is discussed in the following articles.
Relation to T-duality is discussed in:
J.G. Russo, T-duality in M-theory and supermembranes (arXiv:hep-th/9701188)
M.P. Garcia del Moral, J.M. Pena, A. Restuccia, T-duality Invariance of the Supermembrane (arXiv:1211.2434)
Relation to U-duality is discussed in:
Martin Cederwall, M-branes on U-folds (arXiv:0712.4287)
M.P. Garcia del Moral, Dualities as symmetries of the Supermembrane Theory (arXiv)
Discussion from the point of view of E11-U-duality and current algebra is in
Hirotaka Sugawara, Current Algebra Formulation of M-theory based on E11 Kac-Moody Algebra, International Journal of Modern Physics A, Volume 32, Issue 05, 20 February 2017 (arXiv:1701.06894)
Shotaro Shiba, Hirotaka Sugawara, M2- and M5-branes in E11 Current Algebra Formulation of M-theory (arXiv:1709.07169)
Discussion of M2-M5 brane bound states, i.e. dyonic$\,$black M2-branes (M5-branes wrapped on a 3-manifold, see also at NS5-branes – D2/D4/NS5-bound states):
J.M. Izquierdo, Neil Lambert, George Papadopoulos, Paul Townsend, Dyonic Membranes, Nucl. Phys. B460:560-578, 1996 (arXiv:hep-th/9508177)
Michael Green, Neil Lambert, George Papadopoulos, Paul Townsend, Dyonic $p$-branes from self-dual $(p+1)$-branes, Phys.Lett.B384:86-92, 1996 (arXiv:hep-th/9605146)
Troels Harmark, Section 3.1 of Open Branes in Space-Time Non-Commutative Little String Theory, Nucl.Phys. B593 (2001) 76-98 (arXiv:hep-th/0007147)
Troels Harmark, N.A. Obers, Section 5.1 of Phase Structure of Non-Commutative Field Theories and Spinning Brane Bound States, JHEP 0003 (2000) 024 (arXiv:hep-th/9911169)
George Papadopoulos, Dimitrios Tsimpis, The holonomy of the supercovariant connection and Killing spinors, JHEP 0307:018, 2003 (arXiv:hep-th/0306117)
Nicolò Petri, slide 14 of Surface defects in massive IIA, talk at Recent Trends in String Theory and Related Topics 2018 (pdf)
Domenico Fiorenza, Hisham Sati, Urs Schreiber, Section 4 of Twisted Cohomotopy implies M-theory anomaly cancellation (arXiv:1904.10207)
Jay Armas, Vasilis Niarchos, Niels A. Obers, Thermal transitions of metastable M-branes (arXiv:1904.13283)
Further bound states of M2/M5-branes to giant gravitons:
Last revised on November 13, 2019 at 15:04:57. See the history of this page for a list of all contributions to it.