L3

In 1977, Cline Parshall, Scott and van der Kallen wrote a seminal paper `Rational and generic cohomology' which exhibited a connection between the cohomology for algebraic groups and the cohomology for finite groups of Lie type, showing that in many cases one can conclude that there is an isomorphism of cohomology through restriction from the algebraic to the finite group.

One unfortunate problem with their result is that there remain infinitely many modules for which their theory---for good reason---tells us nothing. The main result of this talk (recent work with Parshall and Scott) is to show that almost all the time, one can manipulate the simple modules for finite groups of Lie type in such a way as to recover an isomorphism of its cohomology with that of the algebraic group.

To any complex smooth variety Y with an action of a finite group G, Etingof associates a global Cherednik algebra. The usual rational Cherednik algebra corresponds to the case of Y= C^n and a finite Coxeter group G

The question of estimating the length of short conjugators in between
elements in a group could be described as an effective version of the
conjugacy problem. Given a finitely generated group $G$ with word metric
$d$, one can ask whether there is a function $f$ such that two elements
$u,v$ in $G$ are conjugate if and only if there exists a conjugator $g$ such
that $d(1,g) \leq f(d(1,u)+d(1,v))$. We investigate this problem in free
solvable groups, showing that f may be cubic. To do this we use the Magnus
embedding, which allows us to see a free solvable group as a subgroup of a
particular wreath product. This makes it helpful to understand conjugacy
length in wreath products as well as metric properties of the Magnus
embedding.

Consider a diagram of the unknot with c crossings. There is a

sequence of Reidemeister

moves taking this to the trivial diagram. But how many moves are required?

In my talk, I will give

an overview of my recent proof that there is there is an upper bound on the

number of moves, which

is a polynomial function of c.

We will discuss the origin of the conjectured colour-kinematics

duality in perturbative gauge theory, according to which there is a

symmetry between the colour dependence and the kinematic dependence of the

S-matrix. Based on this duality, there is a prescription to obtain gravity

amplitudes as the "double copy" of gauge theory amplitudes. We will first

consider tree-level amplitudes, where a diffeomorphism algebra underlies

the structure of MHV amplitudes, mirroring the colour algebra. We will

then draw on the progress at tree-level to consider one-loop amplitudes.