# Schedule for: 18w5015 - Physics and Mathematics of Quantum Field Theory

Beginning on Sunday, July 29 and ending Friday August 3, 2018

All times in Banff, Alberta time, MDT (UTC-6).

Sunday, July 29 | |
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16:00 - 17:30 | Check-in begins at 16:00 on Sunday and is open 24 hours (Front Desk - Professional Development Centre) |

17:45 - 19:45 | Dinner (Vistas Dining Room) |

20:00 - 22:00 | Informal gathering (Corbett Hall Lounge (CH 2110)) |

Monday, July 30 | |
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07:00 - 08:50 | Breakfast (Vistas Dining Room) |

08:50 - 09:05 |
Introduction and Welcome by BIRS Staff ↓ A brief introduction to BIRS with important logistical information, technology instruction, and opportunity for participants to ask questions. (TCPL 201) |

09:05 - 10:00 |
Vincent Rivasseau: Holographic Tensors ↓ The theory of random tensors is expanding rapidly in scope. At the combinatorial (zero dimensional) level
the tensorial $1/N$ expansion has a much more complicated structure than 'tHooft $1/N$
expansion for matrices, but it is led by a simpler class of graphs, called melonic. Adding time to the
picture gives quantum mechanical tensor models which generalize in a promising way the Sachdev-Ye-Kitaev
model of near $AdS_2/CFT_1$ holographic correspondence. We shall review this fast growing topic. (TCPL 201) |

10:00 - 10:30 |
Daniel Siemssen: Feynman Propagators and the Self-Adjointness of the Klein–Gordon Operator ↓ The Feynman propagator is at the heart of quantum field theory. However, in quantum field
theory in curved spacetimes, no locally covariant notion of a distinguished Feynman propagator exists.
(TCPL 201) Instead, often a distinguished class of Feynman propagators is considered, which share a common parametrix. Nevertheless, certain classes of spacetimes possess distinguished Feynman propagators. First, I will give an in-depth introduction to propagators (Green functions) on curved spacetimes and their role in quantum field theory. In particular, I will highlight the importance of the so-called Hadamard states – an appropriate generalization of the Poincaré invariant vacuum state. Then, I will show that the free Klein–Gordon field on asymptotically static spacetimes comes equipped with a natural Feynman propagator (albeit globally constructed and generally not related to a state). Finally, I will argue that this Feynman propagator is closely related to the question of the self-adjointness of the Klein–Gordon operator on $L^2$(spacetime) and the boundary value of its resolvent. |

10:30 - 11:00 | Coffee Break (TCPL Foyer) |

11:00 - 11:55 |
Mathieu Lewin: Mean-field approximation of QED ↓ I will review several results obtained in collaboration with Philippe Gravejat, Christian
Hainzl and Eric Séré on a mean-field model in QED. I will particularly discuss charge renormalization
and the derivation of the Euler-Heisenberg effective Lagrangian. I will also mention the advantages and disadvantages of the model, as well as open problems. (TCPL 201) |

11:55 - 13:30 |
Lunch ↓ Lunch is served daily between 11:30am and 1:30pm in the Vistas Dining Room, the top floor of the Sally Borden Building. (Vistas Dining Room) |

13:55 - 14:25 |
Krzysztof Gawedzki: Heat waves in 1+1-dimensional Conformal Field Theory ↓ I shall discuss a class of nonequilibrium states
in CFT in one space dimension and how heat transport
in such states connects to the representation
theory of the group of circle diffeomorphisms. (TCPL 201) |

14:25 - 14:45 |
Group Photo ↓ Meet in foyer of TCPL to participate in the BIRS group photo. The photograph will be taken outdoors, so dress appropriately for the weather. Please don't be late, or you might not be in the official group photo! (TCPL 201) |

14:55 - 15:25 | Coffee Break (TCPL Foyer) |

15:25 - 16:20 |
Detlev Buchholz: The resolvent algebra of non-relativistic Bose fields: a C*-dynamical approach to interacting many body systems ↓ C*-dynamical systems are known to be a powerful tool in the analysis of infinite spin and
Fermionic systems. It has been argued that this approach cannot work for Bosons, however, where
singular states describing unrestrained accumulations of matter do appear. In this talk it is shown that
this fact does not constitute a mathematical obstruction if one deals with the (particle number
preserving) observables in the resolvent algebra generated by a Bose field.
(TCPL 201) For, in contrast to the Weyl algebra, this algebra contains ideals which vanish in singular states. A slight extension of this algebra thereby admits an automorphic action of dynamics for a large class of twobody interactions; it allows to proceed to corresponding C*-dynamical systems. If time permits, some standard problems in many body theory are also briefly addressed from this novel point of view. |

16:20 - 17:15 |
Abdelmalek Abdesselam: Space-dependent RG, anomalous dimensions in a hierarchical model for 3d CFT and connections to the AdS/CFT correspondence ↓ (Joint work with Ajay Chandra and Gianluca Guadagni)
(TCPL 201) An outstanding problem in the area of rigorous renormalization group theory is to develop a Wilsonian formalism which can handle space-dependent couplings in the Euclidean setting. I will present such a method in the simpler hierarchical model case and explain how this allowed us to prove a 46 years old prediction by Wilson regarding the anomalous scaling of the square/energy field in a hierarchical ferromagnet. The model we studied is a hierarchical version of a 3d ferromagnet with long-range interactions in a range of parameters which puts it slightly below the upper critical dimension. We constructed the scaling limit for the joint law of the elementary/spin field together with the square/energy field as well as all mixed correlation functions. The Euclidean version of this scaling limit is conjectured to be a conformal field theory in three dimensions according to recent work by physicists in the conformal bootstrap program. There is a natural analogue of conformal invariance in the hierarchical model which thus provides an ideal testing ground for renormalization group-based attempts at rigorously proving conformal invariance. The idea is to feed the space-dependent renormalization group space-dependent ultraviolet cutoffs. I will also mention emerging connections to the AdS/CFT correspondence. |

17:45 - 19:45 |
Dinner ↓ A buffet dinner is served daily between 5:30pm and 7:30pm in the Vistas Dining Room, the top floor of the Sally Borden Building. (Vistas Dining Room) |

Tuesday, July 31 | |
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07:00 - 08:50 | Breakfast (Vistas Dining Room) |

08:50 - 09:45 |
Wojciech Dybalski: Infrared problems in QED: Some topics of current research ↓ (Joint work with A. Pizzo)
(TCPL 201) I will discuss some recent progress on infrared problems in non-perturbative approaches to QED. First, I will explain the general distinction between the `infraparticle’ and `infravacuum’ picture of the electron which pertains to the existence resp. non-existence of the spacelike asymptotic flux of the electric field. On this basis the problem of electron-photon scattering will be discussed both in models of non-relativistic QED and in the setting of algebraic QED. On the infraparticle side, we will revisit the Faddeev-Kulish approach, theory of particle weights and the problem of velocity superselection. On the infravacuum side the talk will cover Kraus-Polley- Reents representations and the Buchholz-Roberts approach. If time allows, relations to a current trend in high-energy physics triggered by the works of A. Strominger et al. on the Weinberg's soft-photon theorems will be discussed. |

09:45 - 10:15 |
Alessandro Pizzo: From the infrared problems in non-relativistic QED to non-commutative recurrence ↓ (Joint work with W. Dybalski)
(TCPL 201) I plan to show an unexpected connection between infrared problems and the theory of noncommutative recurrence relations. This theory turns out to be a robust method to prove infrared regularity of physical quantities which suffer from superficial infrared divergencies even after implementation of multi-scale techniques. |

10:15 - 10:45 | Coffee Break (TCPL Foyer) |

10:45 - 11:15 |
Daniela Cadamuro: Construction of Haag-Kastler nets for factorizing S-matrices with poles. I ↓ (Part I of joint talk with Y. Tanimoto; joint work with H. Bostelmann)
(TCPL 201) A recent viewpoint in the construction of interacting quantum field theories in the operator algebraic setting considers observables localized in unbounded wedge-shaped regions rather than compact regions, allowing simpler expressions of certain observables. With this approach, we construct two-dimensional interacting massive scalar Haag-Kastler nets with factorizing S-matrices containing poles. We exhibit the concrete expression of certain observables in wedges, discuss their self-adjointness and prove the existence of observables in double cones. |

11:15 - 11:45 |
Yoh Tanimoto: Construction of Haag-Kastler nets for factorizing S-matrices with poles. II ↓ (Part II of joint talk with D. Cadamuro) (TCPL 201) |

11:45 - 13:30 | Lunch (Vistas Dining Room) |

13:30 - 14:25 |
Stefan Hollands: Renormalization of Yang-Mills theories ↓ The non-abelian Yang-Mills self-interaction is marginal in
four dimensions in the usual terminology of the renormalization group,
and thus requires renormalization to all orders in an expansion (in
either the coupling or a loop expansion). It is well-known in
principle how to reconcile UV-renormalization with local gauge
invariance, but a fully rigorous and satisfactory treatment taking
also into account the problems posed by the complicated IR-behavior of
the theory on non-compact manifolds has only been given relatively
recently. In this talk, I describe how a combination of the
Epstein-Glaser method/method of renormalization group flow equations
and cohomological techniques a la Batalin-Vilkovisky can be used to
establish the existence of correlation n-point functions of arbitrary
gauge invariant local operators to arbitrary orders in perturbation
theory. The second method of proof comes by construction with rather
refined bounds for these objects capturing their short and long
distance properties. Time permitting, I furthermore explain how the
operator product arises in this context. (TCPL 201) |

14:25 - 14:55 |
Markus B. Fröb: New results for the operator product expansion ↓ Originally conceived by Wilson in 1969, the operator product expansion (OPE) has found a
multitude of applications in high-energy physics, conformal field theory and condensed matter systems.
In the context of perturbative Euclidean quantum field theory, we review a couple of recent results
showing that the OPE is much better behaved than generally expected:
(TCPL 201) - instead of being just an asymptotic expansion, it converges for arbitrary finite separations of the operators, - the OPE coefficients factorise for suitable spacetime configurations, - there is an explicit formula for the recursive construction of the OPE coefficients, which is UV- and IR-finite. We also show how most of these results generalise to gauge theories, including suitable Ward identities for the OPE coefficients, and comment on how the above results could be used for a non-perturbative construction of quantum field theories. |

14:55 - 15:25 | Coffee Break (TCPL Foyer) |

15:25 - 16:20 |
Mikolaj Misiak: Perturbative calculations in QFT and the Laporta algorithm ↓ In searches for new phenomena in particle physics, we are often interested in observing tiny
deviations from the Standard Model (SM) predictions. In consequence, the SM predictions must be
known very precisely. This is often a challenge even in situations when purely perturbative calculations
are sufficient. At present, the most powerful methods amount to expressing the observables of interest
in terms of so-called Master Integrals (MIs). The MIs are not being evaluated directly but rather via
solving systems of differential equations. In the process of finding the MIs via the Laporta algorithm,
large numbers (often billions) of linear equations need to be generated and solved, with simplifications
of complicated rational functions at each step. In consequence, even the most powerful present-day
computer clusters are sometimes insufficient. The situation could radically improve if a clever
mathematical solution of the considered algebraic problem could be found in general.
(TCPL 201) hep-ph/0102033, arXiv:0804.3008, arXiv:1004.4199, arXiv:1412.2296. |

17:45 - 19:45 | Dinner (Vistas Dining Room) |

Wednesday, August 1 | |
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07:00 - 08:50 | Breakfast (Vistas Dining Room) |

09:00 - 12:30 |
Morning excursion ↓Proposal: Walk to the peak of Tunnel mountain, ca 3km one way, elevation gain 250m, no refreshments on the top, but rewarding views. Meeting: 9:00am in front of Corbett Hall. Appropriate footwear, water bottle, rain protection recommended.
Feel free to make your own plans! |

10:15 - 10:45 | Coffee Break (TCPL Foyer) |

11:40 - 13:30 | Lunch (Vistas Dining Room) |

14:00 - 14:55 |
Krzysztof Meissner: Conformal anomalies ↓ Conformal anomalies in quantum field theories of different spins coupled to gravity will be discussed. The contributions of spins 3/2 and 2 are gauge dependent and a criterion to fix this ambiguity will be presented. The arguments pointing to the necessity of the cancellation of the total contribution to the conformal anomaly and the existence of theories satisfying this requirement will be discussed. (TCPL 201) |

14:55 - 15:15 | Quick coffee break (TCPL 201) |

15:15 - 16:10 |
Scott Smith: Renormalized Stochastic PDE's ↓ The first half of this talk will survey recent progress on the stochastic
quantization of Phi4 models, emphasizing the fundamental work of Martin Hairer and
his theory of regularity structures. The second half will discuss some new
applications of this theory to parabolic stochastic PDE's of a quasi-linear nature. (TCPL 201) |

17:45 - 19:45 | Dinner (Vistas Dining Room) |

Thursday, August 2 | |
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07:00 - 08:50 | Breakfast (Vistas Dining Room) |

08:50 - 09:45 |
Christopher Fewster: Measurement schemes for quantum field theory in curved spacetimes ↓ (Joint work with R.Verch)
(TCPL 201) Algebraic quantum field theory is founded on the idea of algebras of observables associated with local regions of spacetime. However, not much attention has been given to how these observables can actually be measured. On the other hand, quantum measurement theory provides an operational understanding of measurement schemes, in which a probe system is used to measure a quantum observable of the system of interest. However these discussions are not usually framed in a spacetime context. This talk will describe a generally covariant formalism of measurement schemes adapted to quantum field theory in curved spacetimes, illustrated by a specific model that can be analysed in detail. |

09:45 - 10:15 |
Kasia Rejzner: BV quantization in perturbative algebraic quantum field theory: gauge theories and effective quantum gravity ↓ I will give an overview of how the Batalin-Vilkovisky (BV) formalism can be incorporated
into perturbative algebraic quantum field theory in full generality and I will discuss two examples:
gauge theories and effective quantum gravity. In the latter case, there is an additional difficulty in
constructing gauge-invariant observables. I will explain how this is addressed in our approach. (TCPL 201) |

10:15 - 10:45 | Coffee Break (TCPL Foyer) |

10:45 - 11:40 |
Michał Wrochna: Propagators and distinguished states on curved spacetimes ↓ (Joint work with Ch. Gerard)
(TCPL 201) In QFT on curved spacetimes, a central difficulty is how to reconcile local properties of states (short-distance behaviour of N-point functions) with global ones (positivity, spacetime or gauge symmetries, asymptotic convergence to vacuum or thermal state, boundary conditions, etc.). In the last few years, these difficulties have been overcome in a wide range of situations, leading in particular to rigorous descriptions of thermal effects on black hole spacetimes. The aim of the talk will be to present the new state-of-the-art and discuss the main conjectures, with a particular focus on: - distinguished states on black hole spacetimes and their thermal properties - Hadamard states and (generalized) Feynman propagators in scattering situations - the Reeh-Schlieder property - states with good holographic properties on AdS spacetimes |

11:40 - 13:30 | Lunch (Vistas Dining Room) |

13:30 - 14:25 |
Nicola Pinamonti: Thermal states in perturbative algebraic quantum field theory: stability, relative entropy and entropy production ↓ We analyze some properties shown by extremal KMS states for interacting massive scalar
fields propagating over Minkowski spacetime. These states have been recently constructed in the
framework of perturbative algebraic quantum field theories by Fredenhagen and Lindner. In particular,
we discuss the validity of the return to equilibrium property when the interaction Lagrangian has
compact spatial support. If the adiabatic limit is considered, the return to equilibrium is in general not
valid. This implies that an equilibrium state under the adiabatic limit for a perturbative interacting
theory evolved with the free dynamics does not converge to the free equilibrium state. Actually, we
show that the ergodic mean of this state converges to a non-equilibrium steady state (NESS) for the free
theory. We thus compute the relative entropy among equilibrium states for different evolutions showing
that such an extent is compatible with perturbation theory. We then analyze the entropy production in
the NESS discussed above to estimate how far from equilibrium is this state. (TCPL 201) |

14:25 - 14:55 |
Paweł Duch: Infrared problem and adiabatic limit in perturbative quantum field theory ↓ I will discuss different types of the adiabatic limit in perturbative quantum field theory in the
Minkowski space in the Epstein-Glaser approach: the algebraic adiabatic limit, the weak adiabatic limit
and the strong adiabatic limit.
(TCPL 201) (1) The algebraic adiabatic limit is the construction of the net of local algebras of interacting fields and interacting observables. This construction is well-understood even in the case of models with gauge symmetries and is applicable also to theories defined on curved spacetime. (2) The weak adiabatic limit allows to construct the Wightman and Green functions. I will present the recent results about its existence in most physically relevant models of quantum field theory and show that these results can be used to define a Poincaré-invariant state on the algebra of interacting fields in the algebraic adiabatic limit. The state obtained in this way can be interpreted as an interacting vacuum state. (3) The strong adiabatic limit is used to define the scattering matrix and the interacting fields as operators acting on a Hilbert space. This limit is under control only in the case of purely massive models. Because of the infrared problem it does not exist in most models with massless particles. The notable example is quantum electrodynamics for which even the first order correction to the scattering matrix is ill-defined. Based on the ideas of Dollard, Kulish and Faddeev, I will propose a definition of a modified scattering matrix and modified interacting fields in a model with the infrared problem and show the existence of the strong adiabatic limit in the modified sense in low orders of perturbation theory. |

14:55 - 15:25 | Coffee Break (TCPL Foyer) |

15:25 - 15:55 |
Joseph C. Várilly: Wigner's "continuous-spin" representations reconsidered ↓ Starting with proposals by Schuster and Toro (2013), the massless "continuous-spin" or
"infinite-helicity" irreducible representations of the Poincaré group have been the subject of
several recent investigations. Their status as string-localizable particles was shown in principle by
Mund, Schroer and Yngvason (2006). From the viewpoint of Wigner's equations of motion for such (as
yet unobserved) particles, we endeavour to give a first-quantized approach to them, based on a
background of classical elementary systems. (TCPL 201) |

17:45 - 19:45 | Dinner (Vistas Dining Room) |

19:45 - 20:15 |
Henning Bostelmann (adhoc talk): "Backflow: A tale of potentials in quantum mechanics with potential for public impact" ↓ One of the unintuitive features of quantum mechanics is "quantum
backflow": Particles can, in certain circumstances, move in the
direction opposite to their momentum. More technically, for a
one-dimensional particle with positive momentum, the (averaged)
probability flux operator may have negative expectation values, although
to a limited amount. This effect has been known for quite some time for
free particles. We recently verified that the effect is stable under
interaction in the sense of scattering theory: particles with
*asymptotically* positive momentum can exhibit a limited amount of
negative probability flux in the interaction region. This mathematical
result, somewhat unexpectedly for us, resulted in a brief flurry of
coverage in the international press. (TCPL 201) |

Friday, August 3 | |
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07:00 - 08:50 | Breakfast (Vistas Dining Room) |

08:50 - 09:45 |
David Simmons-Duffin: The conformal bootstrap in d>2 dimensions ↓ The conformal bootstrap seeks to use conformal symmetry,
associativity of the operator product expansion, and other physical
consistency conditions to constrain nontrivial conformal field
theories (CFTs). I will review recent progress in the conformal
bootstrap, including Rattazzi, Rychkov, Tonni, and Vichi's algorithm
for deriving bounds on CFT data, bounds on the 3d critical Ising
model, and some analytic results about the bootstrap equations. (TCPL 201) |

09:45 - 10:15 |
Christian Jaekel: The Haag-Kastler Axioms for the $P (\varphi)_2$ Model on the De Sitter Space ↓ (Joint work with Jens Mund)
(TCPL 201) We establish the Haag-Kastler axioms for a class of interacting quantum field theories on the twodimensional de Sitter space, which satisfy finite speed of light. The $P (\varphi)_2$ model constructed by Barata, Jäkel & Mund, describing massive scalar bosons with polynomial interactions, provides an example. |

10:15 - 10:45 | Coffee Break (TCPL Foyer) |

10:45 - 11:40 |
Sebastiano Carpi: AQFT and VOAs ↓ We have two different axiomatic approaches to chiral conformal field theory (CFT). The
conformal net approach is based on the theory of operator algebras on Hilbert spaces (C^*-algebras and
von Neumann algebras) and it is the chiral CFT version of algebraic quantum field theory (AQFT). On
the other hand, the vertex operator algebra (VOA) approach is based on an algebraic reformulation of
the relevant properties of conformal invariant quantum fields on the circle.
(TCPL 201) I will give an overview of the present status of understanding in relation to the connections between these two approaches. |

11:40 - 12:10 |
Checkout by Noon ↓ 5-day workshop participants are welcome to use BIRS facilities (BIRS Coffee Lounge, TCPL and Reading Room) until 3 pm on Friday, although participants are still required to checkout of the guest rooms by 12 noon. (Front Desk - Professional Development Centre) |

12:10 - 13:30 | Lunch (Vistas Dining Room) |