154 The Quantum Structure of Space and Time
n n n n n A n
Ql Q2 Q3 Q4 Q5 a6 Q7 a8 Q9
Fig. 4.1 Dynkjn diagram of elo.
However, it is known that, generically, they grow exponentially as a2 4 -00, like
the number of massive string states. In order to get a handle at least on low-lying
generators, one analyzes el0 w.r.t. certain finite-dimensional regular subalgebras
by means of a level decomposition: pick one special node ao, and write a given
root as Q = Cjrnjaj +~QO with aj E subalgebra, and where t is the ‘level’. For
instance, decomposing w.r.t. the subalgebra Ag = 5110 (i.e. QO = ale) we obtain
the following table for t 5 3:
A9 module Tensor
[000000 1001
l0100000011 EUl ... us la9
[OOO 100000] Eal ... a6
These tensors correspond to the bosonic fields of D = 11 supergravity and their
‘magnetic’ duals. Similar low level decompositions of el0 w.r.t. its other distin-
guished rank-9 subalgebras Dg -- sa(9,9) and As @ A1 = 5Ig @ 512 yield the correct
bosonic multiplets, again with ‘magnetic’ duals, of (massive) type IIA and type
IIB supergravity, respectively. Furthermore, for the Dg decomposition, one finds
that the (Neveu-Schwarz)2 states (at even levels) and the (Ramond)2 states (at
odd levels), respectively, belong to tensorial and spinorial representations of the T-
duality group SO(9,9), and that the truncation to even levels contains the rank-10
hyperbolic Kac-Moody algebra DElo, corresponding to type-I supergravity, as a
subalgebra.
Dynamics (cf. [2, 3, 51): The equations of motion are derived from the following
(essentially unique) ‘geodesic’ a-model over Elo/K(Elo):
where P := PV-’ -w(PV-~) is the ‘velocity’, (.I.) is the standard invariant bilinear
form, and n(t) a one-dimensional ‘lapse’ needed to ensure (time) reparametrisation
invariance. When truncated to levels 5 3, the corresponding equations of motion
coincide with the appropriately truncated bosonic supergravity equations of motion,
where only first order spatial gradients are retained [2]. Analogous results hold for