| Ofer
 Aharony  (Weizmann Institute) | Tuesday 
20th July 09:45 | 
| Strongly coupled field theories in anti-de Sitter
 space | 
| I will discuss work in progress on strongly coupled
  field theories on anti-de Sitter space. These are interesting in
  their own right, as the anti-de Sitter space provides a natural IR
  cutoff. They are also interesting in the context of the AdS/CFT
  correspondence, in two directions. Strongly coupled field theories on
  D dimensional AdS space can have (D+1) dimensional gravitational
  duals. And, if such theories appear as part of a gravitational
  background, they could be dual to conformal field theories in (D-1)
  dimensions. I will focus on two main examples, the d=4 N=4 SYM theory
  on AdS4, and confining field theories on AdS space. | 
| 
 | 
| Richard
 Battye  (University of Manchester) | Friday
 23rd July 17:15 | 
| Evolution charged domain wall networks | 
| The standard lore of domain wall evolution is that 
they scaling with the number of walls being inversely proportional to 
time. We will show how this can be very different is the domain wall 
forming field is coupled to the an unbroken U(1) field which generates a
 Noether current. The natural propensity of loops of wall to collapse 
under their own tension is resisted by the current leading to the 
possibility of glass-like configurations of walls. | 
| 
 | 
| Niklas
 Beisert  (AEI Potsdam) | Tuesday 20th July
 11:00 | 
| Integrability for scattering amplitudes in planar
 N=4 super Yang-Mills | 
| Tremendous progress in computing perturbative 
scattering amplitudes in N=4 supersymmetric gauge theory has been made 
over the past few years. Importantly the planar amplitudes appear to 
display a dual conformal invariance next to the usual conformal 
symmetry. Altogether the symmetry enlarges to a Yangian algebra known 
from the context of integrable models. This infinite-dimensional 
symmetry might have the power to completely fix the S-matrix by 
algebraic means.
In this talk we review the above developments. We then discuss conformal
 symmetry for tree and loop scattering amplitudes. It turns out that the
 free conformal symmetry generators are anomalous which calls for 
certain deformations to make the symmetries exact. These relate 
amplitude with different numbers of legs, and thus they contribute 
substantially to a complete algebraic determination. | 
| 
 | 
| Andreas
 Brandhuber  (Queen Mary University of London) | Wednesday 21st July 09:45 | 
| Surprises in the Wilson loop/Amplitude Duality | 
| MHV Amplitudes in planar N=4 super Yang-Mills are 
conjectured to be equal to lightlike polygonal Wilson loops at all 
orders in perturbation theory. In this talk we discuss recent progress 
and results at two-loop order and at weak coupling. Usually the duality 
is expressed in terms of four-dimensional quantities. We demonstrate the
 completely unanticipated fact that the equality continues to hold at 
two loops through order epsilon in dimensional regularization for the 
four- and five-particle amplitudes. | 
| 
 | 
| Nick
 Dorey  (University of Cambridge ) | Wednesday
 21st July 11:00 | 
| Wall Crossing and Instantons in Compactified 
Gauge Theory | 
|  | 
| 
 | 
| Jerome
 Gauntlett  (Imperial College London) | Thursday
 22nd July 09:00 | 
| AdS/CMT and Consistent KK Truncations | 
|  | 
| 
 | 
| Rajesh
 Gopakumar  (Harish-Chandra Research Institute) | Monday 19th July 09:45 | 
| Unravelling the String Dual to the Gaussian 
Matrix Model | 
| I will give a concrete description of how the string
 dual
  to the simplest large N theory - the Gaussian matrix integral -
  emerges from its Feynman graphs. | 
| 
 | 
| Nicolay
 Gromov  (King's College) | Wednesday 21st 
July 11:45 | 
| Y-system for AdS/CFT: News, Tests and Tools | 
|  | 
| 
 | 
| Amihay
 Hanany  (Imperial College London) | Monday
 19th July 17:15 | 
| Chiral Operators on the Moduli space of 
Instantons | 
| The moduli space of instantons has been a subject of
 many research problems. In this talk we will see some new results on 
this moduli space, by taking a look at chiral operators. | 
| 
 | 
| Derek
 Harland  (Durham University) | Friday 23rd
 July 11:00 | 
| Instantons in dimensions greater than 4 | 
| Generalisations of the 4-dimensional anti-self-dual 
Yang-Mills equation to dimensions up to and including 8 have been known 
since the early eighties.  These equations have subsequently found 
applications in string compactifications, in Donaldson-Thomas theory, 
and in Kapustin-Witten's work on the geometric Langlands program.  In 
flux compactifications, one is particularly interested in manifolds with
 torsionful G-structures: I will discuss examples of solutions on such 
manifolds.  For certain kinds of torsion, the instanton equations have 
interpretation as gradient and Hamiltonian flows. | 
| 
 | 
| Roman
 Jackiw  (Massachusetts Institute of Technolog) | Friday 23rd July 09:00 | 
| The physics of zero energy modes: Fractional 
Charge | 
| (Joint work with So-Young Pi) A "Dirac" - type equation, i.e. a matrix equation with first-order 
derivatives, usually possesses positive- and negative- energy 
eigenvalues. In the vacuum  the former are empty and the latter are 
filled.  However it may happen that when the "Dirac" equation is 
considered in a topologically non-trivial background, it possesses 
zero-energy eigenvalues. The question then arises whether in the vacuum 
these zero-energy states are empty or filled. Analysis of this question 
results in the conclusion that the charge- or the number- eigenvalue 
becomes fractional.
 | 
| 
 | 
| Romuald
 Janik  (Jagiellonian University) | Tuesday
 20th July 17:15 | 
| Far from equilibrium plasma and AdS/CFT | 
| I would like to describe the application of the 
AdS/CFT correspondence to
study the dynamics of far from equilibrium plasma. | 
| 
 | 
| Andreas
 Karch  (University of Washington ) | Thursday
 22nd July 16:30 | 
| A particle physicist's perspective on topological
 insulators. | 
| The theory of topological insulators will be 
reviewed in terms familiar to particle theorists. These tools will be 
used to describe a novel state of matter that could be thought 
experimentally, a fractional topological insulator. | 
| 
 | 
| David
 A. Kosower  (Institut de Physique Théorique, CEA-Saclay) | Monday 19th July 11:45 | 
| A Basis for Two-Loop Integrals | 
| I discuss the construction of an integral basis at 
two loops, both to 
all orders in the dimensional regulator eps, and for integrals truncated
to O(eps). I also discuss a new approach for organizing 
integration-by-parts equations needed in the construction of such bases. | 
| 
 | 
| Prem
 Kumar  (Swansea University) | Monday 19th 
July 11:00 | 
| Quantum Phases of k-strings | 
| I will describe aspects of confining k-strings in 
mass deformed N=4 theory, 
and in particular, the quantum dynamics on their moduli space. | 
| 
 | 
| David
 Kutasov  (University of Chicago) | Tuesday
 20th July 09:00 | 
| a-Maximization, Global Symmetries and RG Flows | 
| I will describe a generalization of the construction
 of the a-function of
hep-th/0312098, which is defined along RG flows and coincides with the 
central charge a at fixed points, to general F-term perturbations of an 
arbitrary 3+1 dimensional N=1 SCFT. This construction will be used to 
argue 
that the central charge a always decreases along the corresponding
RG flows, and for some other applications. | 
| 
 | 
| Kimyeong
 Lee  (Korea Institute for Advanced Study) | Thursday 22nd July 17:15 | 
| Supersymmetric Theories on M2 Branes | 
| I review Nge 5 Superconformal Field Theories in 2+1 
dimensional spacetime,
and cover our recent works on ABJM model. | 
| 
 | 
| Nick
 Manton  (University of Cambridge) | Friday
 23rd July 09:45 | 
| Vortices and complex geometry | 
| I will discuss the interplay of the physics and 
mathematics of abelian Higgs vortices on a compact Riemann surface. When
 the surface is large, the vortices behave like particles. When the 
surface is small, and can only just accommodate the vortices (the 
Bradlow limit), the vortices reduce to divisors on the Riemann surface, 
and their fields can be described using classical, holomorphic concepts 
like abelian differentials. The metric on the 1-vortex moduli space can 
be computed in both limits. | 
| 
 | 
| Michel
 Peyrard  (ENS Lyon) | Saturday 24th July 
09:00 | 
| Talk: Nonlinear excitations as tools to analyze 
DNA thermodynamics and dynamics. | 
| 
DNA is not the static object that structural images show. It is a highly
dynamical molecule. The base pairs, which encode the genetic 
information,
fluctuate widely. The lifetime of a base pair, i.e. the time during 
which it
stays closed, is only of the order of a few milliseconds. At high 
temperature
some parts of the double helix open locally and form the so called 
'denaturation bubbles', which play a role in biological function.
When it is viewed at the scale of base pairs, DNA appears as a nonlinear
lattice. There are certainly no solitons in DNA but nonlinear localized
excitations are nevertheless very helpful to analyze its properties.
 
Computing the free energy of the 'domain walls', which separate open and
closed regions, we can predict the temperature at which the two strands 
fully
separate due to thermal fluctuations (the 'melting' transition of DNA) 
with
a much better accuracy than with the standard methods of statistical 
physics.
 
The local fluctuations of the double helix can be described in terms of
localized modes (discrete breathers) but establishing a satisfactory 
model is
a challenge because the accurate experiments which can be performed on 
this
molecule impose severe constraints on the models. The analysis of
the time scales of the fluctuations led us to a model that sustains a 
new
class of discrete breathers.
 
References:
 
[1] M. Peyrard,
 Nonlinear dynamics and statistical physics of DNA.
Nonlinearity 17, R1-R40 (2004)
 
[2] T. Dauxois, N. Theodorakopoulos and M. Peyrard,
Thermodynamic instabilities in one dimension: correlations, scaling and 
solitons.
J. Stat. Phys. 107,  869-891, (2002)
 
[3] N. Theodorakopoulos, M. Peyrard and R.S. MacKay,
Nonlinear structures and thermodynamic instabilities in a 
one-dimensional lattice system.
Phys. Rev. Lett. 93, 258101-1-4 (2004)
 
[4]  M. Peyrard, S. Cuesta Lopez and G. James,
Modelling DNA at the mesoscale: a challenge for nonlinear science?
Nonlinearity 21, T91-T100 (2008)
 | 
| 
 | 
| Mikhail
 Polikarpov  (Institute for Theoretical and Experimental Physics) | Saturday 24th July 11:00 | 
| Talk: Effects of strong magnetic field in lattice
 QCD | 
| In the non-central heavy ion collisions a very 
strong magnetic field can be generated and the interference of strong 
and electromagnetic interactions produce various physical effects. We 
use the chirally invariant lattice Dirac operator to study gluodynamics 
in the strong magnetic field. The observed effects are: the enhancement 
of the chiral condensate, magnetization of the vacuum (spins of the 
virtual quarks turn parallel to the external field), the local 
generation of the anomalous quark electric dipole moment along the 
magnetic field, the chiral magnetic effect (a CP-odd generation of the 
electric current of quarks directed along the magnetic field), existence
 of nonzero electric conductivity along the direction of the field (the 
vacuum becomes an anisotropic conductor). | 
| 
 | 
| Mukund
 Rangamani  (Durham University) | Thursday 
22nd July 11:00 | 
| Quantum fields in curved spacetime: The strong 
coupling story | 
|  | 
| 
 | 
| Simon
 Ross  (Durham University) | Wednesday 21st
 July 09:00 | 
| Holography for non-relativistic CFTs | 
|  | 
| 
 | 
| Edward
 Shuryak  (Stony Brook University ) | Saturday
 24th July 11:45 | 
| QCD topology and RHIC experiments | 
| The first half of the talk is related with 
confinement problem and its relation to instantons/dyons/monopoles: one 
new element is lattice study of the monopole clustering 
which provides clear evidence of their Bose condensation exactly at Tc. 
The second tells about
several topology-related issues of the RHIC program.
QCD sphalerons and RHIC experiment aimed at observing them directly in 
double-diffractive pp
collisions. The so called Magnetic Chiral Effect looks for CP-odd 
domains inside the QGP produced
in heavy ion collisions. Finally, there are evidences of flux tubes 
preserved in hot matter, confirming
a view that near-Tc matter is basically a plasma of magnetic objects. | 
| 
 | 
| Jacob
 Sonnenschein  (Tel Aviv University) | Thursday
 22nd July 09:45 | 
| Non-perturbative field theory- from 2d CFT to QCD
 in     four dimensions | 
|  | 
| 
 | 
| Mikhail
 Stephanov  (University of Illinois, Chicago) | Thursday 22nd July 11:45 | 
| AdS/QCD and Charmonium at Finite Temperature | 
| I shall discuss holographic approach to charmonium 
and its
  spectral function at finite temperature in terms of the position and
  the strength of the complex singularities (quasinormal modes). Within
  the model, the 'melting' of the J/psi spectral peak occurs at a
  temperature T~540 MeV, in agreement with lattice results. | 
| 
 | 
| Paul
 Sutcliffe  (Durham University) | Friday 
23rd July 11:45 | 
| Skyrmions, instantons and holography | 
| I will describe how the holonomy of Yang-Mills 
instantons yields exact solutions of a BPS Skyrme model, in which the 
Skyrme field is coupled to a tower of vector mesons. | 
| 
 | 
| Arkady
   Tseytlin  (Imperial College London) | Tuesday
 20th July 16:30 | 
| Superstrings in AdS5 × S5:  some perturbative 
results | 
| I will review some recent results of perturbative 
computations for superstrings in AdS5 × S5  and their correspondence 
with Bethe ansatz results for the spectrum. I will also discuss 
semiclassical approximation for 2-point correlators of string vertex 
operators. | 
| 
 | 
| Dmytro
 Volin  (Penn State University) | Tuesday 
20th July 11:45 | 
| Y-systems and spin chains | 
| There is an intriguing fact that transfer matrices 
of
  integrable spin chains and T-functions that follow from the
  thermodynamic Bethe Ansatz obey the same Hirota equations. It is
  therefore natural to ask the question if these two originally
  different objects coincide. We will consider two different examples
  trying to answer this question. For one case the answer is "yes". For
  another one the answer is not clear, and there are arguments that
  favor the negative answer. | 
| 
 | 
| Erick
 Weinberg  (Columbia University) | Friday 
23rd July 16:30 | 
| Massless magnetic monopoles | 
|  | 
| 
 | 
| Laurence
 Yaffe  (University of Washington) | Saturday
 24th July 09:45 | 
| Large N volume independence in conformal and 
confining gauge theories | 
| In the large N limit, gauge theories compactified on
 Rd-k × (S1)k are independent of the S1
 radii provided the theory has unbroken center symmetry. This implies that a large N gauge theory which, on Rd, flows 
to an IR fixed point retains the infinite correlation length and other 
scale invariant properties even when toroidally compactified. Numerical 
studies to determine the conformal window boundary may, in the large N 
limit, be performed on one-site lattice models.  Large N QCD with 
massive adjoint fermions, when toroidally compactified, has a rich phase
 structure with infinitely many phase transitions coalescing in the zero
 radius limit.
 | 
| 
 | 
| Piljin
 Yi  (Korea Institute for Advanced Study) | Monday
 19th July 16:30 | 
| Holographic Baryons and a Matrix Model | 
|  |