-
11
-
-
0031558143
-
-
M. Aganagic, J. Park, C. Popescu, and J. H. Schwarz, Nucl. Phys. B496, 191 (1997);
-
(1997)
Nucl. Phys. B
, vol.496
, pp. 191
-
-
Aganagic, M.1
Park, J.2
Popescu, C.3
Schwarz, J.H.4
-
13
-
-
33847357145
-
-
note
-
Due to the self-duality condition we avoid mentioning the action and focus on the equations of motion only.
-
-
-
-
14
-
-
0000749413
-
-
E. Bergshoeff, D. S. Berman, J. P. van der Schaar, and P. Sundell, Nucl. Phys. B590, 173 (2000);
-
(2000)
Nucl. Phys.
, vol.B590
, pp. 173
-
-
Bergshoeff, E.1
Berman, D.S.2
Van Der Schaar, J.P.3
Sundell, P.4
-
15
-
-
0034718888
-
-
Phys. Lett. B 492, 193 (2000).
-
(2000)
Phys. Lett. B
, vol.492
, pp. 193
-
-
-
18
-
-
33847413851
-
-
J. Park, hep-th/0012141
-
J. Park, hep-th/0012141;
-
-
-
-
19
-
-
33847373134
-
-
C. M. Hofman and W. K. Ma, hep-th/0102201
-
C. M. Hofman and W. K. Ma, hep-th/0102201.
-
-
-
-
23
-
-
0042055973
-
-
N.Y.
-
Ann. Phys. (N.Y.) 185, 330 (1988).
-
(1988)
Ann. Phys.
, vol.185
, pp. 330
-
-
-
27
-
-
33847353108
-
-
note
-
Membranes could also end on Horava-Witten nine-branes or on one-dimensional defects (see, e.g., [3]).
-
-
-
-
28
-
-
7044228100
-
-
R. Gopakumar, S. Minwalla, N. Seiberg, and A. Strominger, J. High Energy Phys. 08, 008 (2000).
-
(2000)
J. High Energy Phys.
, vol.8
, pp. 008
-
-
Gopakumar, R.1
Minwalla, S.2
Seiberg, N.3
Strominger, A.4
-
31
-
-
33847380409
-
-
M. Berkooz, hep-th/0010158.
-
M. Berkooz, hep-th/0010158.
-
-
-
-
33
-
-
33847340863
-
-
P. Etingof, D. Kazhdan, and A. Polishchuk, math.AG/0003009
-
P. Etingof, D. Kazhdan, and A. Polishchuk, math.AG/0003009.
-
-
-
-
35
-
-
33744925186
-
-
B. Pioline, H. Nicolai, J. Plefka, and A. Waldron, J. High Energy Phys. 03, 036 (2001).
-
(2001)
J. High Energy Phys.
, vol.3
, pp. 036
-
-
Pioline, B.1
Nicolai, H.2
Plefka, J.3
Waldron, A.4
-
36
-
-
85107712671
-
-
note
-
k is a very natural gauge-fixing function, and it would be interesting to study the field configurations onto which it localizes.
-
-
-
-
39
-
-
0000318076
-
-
2 made by Regge and Lund [20] does not seem adequate for the membrane case at hand; however it does lead to interesting soliton solutions [A. Zee, Nucl. Phys. B4211, 111 (1994)].
-
(1994)
Nucl. Phys.
, vol.B4211
, pp. 111
-
-
Zee, A.1
-
40
-
-
85107712382
-
-
private communication
-
2 - g(σ), which yields the commutation rules for SU(2) currents at level 0 [S. Minwalla (private communication)].
-
-
-
Minwalla, S.1
-
45
-
-
85107712429
-
-
note
-
i after using the symmetry under spatial diffeomorphisms.
-
-
-
-
48
-
-
0010158573
-
-
H. Awata, M. Li, D. Minie, and T. Yoneya, J. High Energy Phys. 02, 013 (2001).
-
(2001)
J. High Energy Phys.
, vol.2
, pp. 013
-
-
Awata, H.1
Li, M.2
Minie, D.3
Yoneya, T.4
-
49
-
-
0031541570
-
-
G. Dito, M. Flato, D. Sternheimer, and L. Takhtajan, Commun. Math. Phys. 183, 1 (1997).
-
(1997)
Commun. Math. Phys.
, vol.183
, pp. 1
-
-
Dito, G.1
Flato, M.2
Sternheimer, D.3
Takhtajan, L.4
-
50
-
-
33847390074
-
-
R. Jackiw, physics/0010042
-
R. Jackiw, physics/0010042.
-
-
-
-
52
-
-
33744708804
-
-
A somewhat similar equivalence to SU(2) WZW model with the topological term only has been produced in I. Rudychev, J. High Energy Phys. 04, 015 (2001).
-
(2001)
J. High Energy Phys.
, vol.4
, pp. 015
-
-
Rudychev, I.1
-
54
-
-
33847341405
-
-
L. Susskind, hep-th/0101029
-
L. Susskind, hep-th/0101029.
-
-
-
-
55
-
-
0000534116
-
-
It should be noted that this deformation is different from the Freedman-Townsend vertex Tr(b∧[*d6,*db]), which still yields an Abelian gauge symmetry on-shell [D. Z. Freedman and P. K. Townsend, Nucl. Phys. B177, 282 (1981)].
-
(1981)
Nucl. Phys.
, vol.B177
, pp. 282
-
-
Freedman, D.Z.1
Townsend, P.K.2
|