
1 Introduction
Symmetries spanned by infinite-dimensional Lie algebras tightly constrain the possibilities
to devise theories or computing amplitudes, among others. Along these lines, consistent
nonlinear maps between the generators of infinite-dimensional linear algebras can also be
very useful, but since they are just sporadically found, the systematic study of this kind
of mappings turns out to be uncharted territory either in physics or mathematics (for
a recent related discussion see [1]). A time-honored example of this sort is the Sugawara
construction [2], which is known to play a very relevant role in the context of conformal field
theories (CFT’s) in two-dimensional spacetimes. In this class of mapping, the generators
of the Virasoro algebra are obtained from a precise quadratic combination of those of an
affine Kac-Moody algebra (see e.g. [3,4]). Similar quadratic Sugawara-like relationships,
realized in a variety of setups, are also known to exist for the ultra/non-relativistic limit
of the conformal algebra in 2D (CCA2≈GCA2≈BMS3)) [5–9], and its supersymmetric
extensions [10–15] whose generators also emerge from different quadratic combinations of
current algebras.
Another type of nonlinear mappings of the class under discussion is naturally formu-
lated in the context of integrable systems. Indeed, since the Virasoro algebra describes
one of the Poisson structures of the KdV hierarchy (see e.g., [16–18]), their generators are
also nonlinearly related to the infinite-dimensional Abelian algebra of conserved charges,
spanned by the subset of commuting generators of the enveloping algebra. A similar non-
linear relationship of this kind is also known to hold for the generators of the BMS3algebra
[19].
A different kind of nonlinear map that requires going beyond the enveloping algebra has
been recently introduced in [20], which relates the generators of the classical (nonanoma-
lous) conformal algebra in 2D (Diff(S1)⊕Diff(S1)) with those of the BMS3algebra. Under
this mapping, the Hamiltonian of a generic CFT2, with chiral (holomorphic) conformal gen-
erators given by Tand ¯
T, acquires a finite marginal non-analytic deformation determined
by √T¯
T, so that the deformed theory it is no longer a CFT2, but a conformal Carrollian
field theory instead, because its energy and momentum densities fulfill the BMS3algebra1.
Remarkably, no limiting process is involved in the nonlinear map between the conformal
algebra and its ultra/non-relativistic version. This map, and its corresponding deformation
were then shown to be recovered through a class of “infinite boosts” spanned by certain
degenerate (non-invertible) linear transformations acting on the coordinates [31]. Further
recent interesting results about continuous √T¯
Tdeformations have also been addressed for
field theories in 2D along different approaches and points of view in [32], [33], [34] (see also
[35], [36]), and for the deformation of two free harmonic oscillators in classical mechanics
[37].
One of the main purposes of our work is showing that the conformal algebra in 2D
admits a “nonlinear SO(1,1) automorphism” that maps the algebra to itself, which once
1These marginal deformations are clearly different from the well-known irrelevant T¯
Tones [21–23], whose
diverse properties have been studied in e.g., [24–29] (for a review and further references see also [30]).
–2–