Theoretical Physics

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Within the research of theoretical physics we try to answer the most fundamental questions of nature. The main direction of the research is investigation of different issues of Quantum Field Theory and String Theory. The main goal of this research is to improve our understanding of how different quantum field theories and string theory works.

In the future this should help us to solve many fundamental problems in the description of nature, such as quantum theory of gravity and physics of strongly coupled and strongly correlated systems. Below you can find a list of topics covered by our research with links to the short descriptions, useful references and lists of our division members conducting research in corresponding topic.

Publications

Research in Theoretical Physics

In theoretical physics we use mathematics to describe Nature, often creating new mathematical structures during our research, just like Newton did when he invented calculus to formulate his “Laws of Motion” describing the motion of planets, stars or even swinging weights.

Later on, in the 19th century calculus evolved into classical field theory and physicists were able to successfully describe electromagnetism. But with the discovery of the electron, there was suddenly some new physics to understand and particle physics was born. Using the new framework of quantum mechanics and experimental observation, the scientific community gained an understanding of the fundamental particles and their division into two classes: bosons and fermions, particles that transmit forces and make up matter, respectively.

At the same time, increasing observational evidence showed that light travelled at one fixed speed according to any observer. This fact, together with new mathematics that Einstein developed to describe it gave birth to the special theory of Relativity. During the 20th century physicists worked hard and were able to merge this together with quantum mechanics, which gave origin to the relativistic quantum field theory. This theory is the foundation of our understanding of subatomic particle physics in the form of the Standard Model, which has so successfully described the phenomena occurring at the LHC.

However, Einstein continued his work and improved Newton's theory of gravitation. Bringing the new concepts of differential geometry into physics, he created the General Theory of Relativity. This theory has been proven to be a great description of Nature. Nevertheless, some of its features that have been observed, such as black holes and an expanding universe, have led the scientific community to believe that our knowledge is still somehow incomplete.

On one hand, quantum field theory describes elementary particles extremely well, but it neglects gravitational effects, and on the other hand we have general relativity which gives great insight into gravitational effects but ignores quantum effects. This is where String Theory comes in, since we believe that it is the theory that closes this gap.

It is well known that a good quantum theory of gravity must include a massless particle that carries the gravitational force and has two units of spin, the graviton. In string theory, particles arise from excitation modes of the string (just like the string of a stringed instrument can vibrate to produce several harmonics), and the graviton is one of those excitations.

This is however not enough for us to say that we have a good theory of quantum gravity, since the graviton could also have been added to quantum field theory by hand, but that was shown to produce disastrous behaviour at small distances because the particles were point-like. In string theory this problem is solved since the fundamental objects have a non-zero length which leads to a nice behaviour at small distances.

If we want our string theory to include fermions, then we have to add a special kind of symmetry called supersymmetry, which means that for every boson there must be a corresponding fermion. Supersymmetric partners to known particles have not yet been found, but theorists believe this is because those particles would be too heavy to be detected with the technology that we have today. There is however a chance that the new improvements at LHC might be enough to find supersymmetry which would be compelling evidence that string theory is the theory of quantum gravity.

Another surprising revelation was that superstring theories include more structures than the fundamental strings. There are also higher dimensional objects called D-branes, which are membranes where the ends of open strings are localized and correspond to a collective excitation of strings.

Finally, one has also to remember that superstring theories are only consistent if the number of space-time dimensions is ten. This means that to give a good description of nature one has to compactify the unwanted spacetime dimensions, which makes the number of possible string theories grow quite a lot since there are many possible ways to make six dimensions much smaller than the other four. This compactification procedure is very interesting on its own and gives rise to very nice mathematical structures.

Depending on how supersymmetry works and whether or not the strings are required to be closed loops, there are five different string theories in ten dimensions. In spite of that, one can also say that this number is shrinking, since string theorists have discovered that what they thought were five totally distinct theories seem in fact to be related to each other through dualities and are all special limits of a more fundamental theory, which they call M theory.

Before string theory won the full attention of the theoretical physics community, the most popular unified theory was an eleven dimensional theory of supergravity, which is supersymmetry combined with gravity. Technically speaking, M theory is the unknown eleven-dimensional theory whose low energy limit is that supergravity theory in eleven dimensions and from which the known superstring theories emerge as special limits.

We still do not know much about the fundamental M theory, but a lot has been learned about how it relates to superstrings in ten spacetime dimensions and judging from all these relationships, it is certainly a very interesting and rich theory.

Cosmological observations have shown that most of the mass in the universe occurs in the form of dark matter. One leading candidate for the composition of dark matter is the WIMP (Weakly Interacting Massive Particle), and many people believe the WIMP to be a spin 1/2 fermion called neutralino which is the supersymmetric partner of gauge bosons and Higgs particles. They are very heavy, interact very weakly with other particles which makes them excellent candidates to explain dark matter.

Supersymmetry needs to be broken in some way because there is no exact match between fermions and bosons, but one can break supersymmetry without losing all the advantages of having it. One example of such mechanism is how the Higgs boson gives mass to the other particles. One of the reasons that string theorists originally liked supersymmetry was that the vacuum energy of bosons and fermions cancelled each other. However, when supersymmetry in string theory is broken that cancellation does not occur anymore, which might explain the cosmological constant behind the expansion of the Universe. String theory also provides us with new scalar fields that could in principle have driven the inflationary phase of our Universe, even though this is still an active area of research.

String theory also provides an excellent framework to study black holes. When it was discovered that black holes can decay by quantum processes, it was also discovered that black holes seem to have the thermodynamic properties of temperature and entropy. Entropy is a quantity that measures the number of allowed quantum states. One of the great successes of string theory was to show precisely how the counting of quantum states for a system of D-branes relates with the entropy as the area of the black hole horizon which appears in the D-brane setup.

Finally another great contribution from string theory has come in the form of the so called AdS/CFT duality, a powerful realization of the holographic principle which states that the description of gravity in some space is encoded in its boundary. AdS/CFT relates some string theories with highly symmetric quantum field theories and the most studied case corresponds to a string theory in five dimensions which is dual to a quantum field theory in four dimensions. This correspondence has the striking property that when the gravitational theory is difficult to solve, the computations in the corresponding quantum field theory become trivial and vice-versa. This duality then gives great insights into quantum gravity, as it provides a non-perturbative formulation of string theory, and at the same time it provides a powerful toolkit for studying strongly coupled quantum field theories, as is the case of QCD, the theory describing the strong force which keeps atoms together.

Binary Kerr black-hole scattering at 2PM from quantum higher-spin Compton

Authors: Lara Bohnenblust, Lucile Cangemi, Henrik Johansson, Paolo Pichini

Preprint number: UUITP-31/24

Abstract: Quantum higher-spin theory applied to Compton amplitudes has proven to be surprisingly useful for elucidating Kerr black hole dynamics. Here we apply the framework to compute scattering amplitudes and observables for a binary system of two rotating black holes, at second post-Minkowskian order, and to all orders in the spin-multipole expansion for certain quantities. Starting from the established three-point and conjectured Compton quantum amplitudes, the infinite-spin limit gives classical amplitudes that serves as building block that we feed into the unitarity method to construct the 2-to-2 one-loop amplitude. We give scalar box, vector box, and scalar triangle coefficients to all orders in spin, where the latter are expressed in terms of Bessel-like functions. Using the Kosower-Maybee-O’Connell formalism, the classical 2PM impulse is computed, and in parallel we work out the scattering angle and eikonal phase. We give novel all-orders-in-spin formulae for certain contributions, and the remaining ones are given up to O(S11). Since Kerr 2PM dynamics beyond O(S≥5) is as of yet not completely settled, this work serves as a useful reference for future studies.

Pinching rules in the chiral-splitting description of one-loop string amplitudes

Authors: Filippo Maria Balli, Alex Edison, Oliver Schlotterer

Preprint number: UUITP-30/24

Abstract: Loop amplitudes in string theories reduce to those of gauge theories and (super)gravity in their worldline description as the inverse string tension α' tends to zero. The appearance of reducible diagrams in these α' → 0 limits is determined through so-called pinching rules in the worldline literature. In this work, we extend these pinching rules to the chiral-splitting description of one-loop superstring amplitudes where left- and right-moving degrees of freedom decouple at fixed loop momentum. Starting from six points, the Kronecker-Eisenstein integrands of chiral amplitudes introduce subtleties into the pinching rules and integration-by-parts simplifications. Resolutions of these subtleties are presented and applied to produce a new superspace representation of the six-point one-loop amplitude of type IIA/B supergravity. The worldline computations and their subtleties are compared with the ambitwistor-string approach to one-loop field-theory amplitudes where integration-by-parts manipulations are shown to be more flexible. Throughout this work, the homology invariance of loop-momentum dependent correlation functions on the torus is highlighted as a consistency condition of α' → 0 limits and their comparison with ambitwistor methods.

The Equivariant B model

Authors: Guido Festuccia, Roman Mauch, Maxim Zabzine

Preprint number: UUITP-29/24

Abstract: In this work, we introduce an equivariant deformation of the B model on the sphere with a U(1)-action. We present the deformed supersymmetry transformations and corresponding Lagrangians and study observables in the supercharge cohomology. The inclusion of equivariance allows for the introduction of novel, position-dependent observables on the sphere, which have no counterparts in the conventional B model. Two specific cases we explore in detail are position-dependent superpotentials and complex structure deformations. In both instances, the theory exhibits notable differences from the standard B model, revealing intriguing new features.

Exploring Defects with Degrees of Freedom in Free Scalar CFTs

Authors: Vladimir Bashmakov, Jacopo Sisti

Preprint number: UUITP-28/24

Abstract: Defects in conformal field theories are interesting objects to study from both formal and applied points of view. In this paper, we construct conformal defects in free scalar field CFTs in diverse dimensions. After discussing the possible quadratic defects, we explore interacting setups. These are realized by coupling the bulk free scalar to lower-dimensional theories, including the unitary family of minimal models M(p, p + 1). Another example involves coupling to a two-dimensional free scalar field, from which we construct surface defects for the bulk dimensions three and five. Additionally, we consider monodromy defects associated with a global U(1) flavour symmetry. In these theories, we study both self-defect interactions and couplings to Minimal Models, finding new IR defect fixed points. For all our examples, we provide results for correlation functions, such as those involving the bulk stress tensor and the displacement operator, and for the defect central charges.

Off-shell color-kinematics duality from codifferentials

Authors: Maor Ben-Shahar, Francesco Bonechi, Maxim Zabzine

Preprint number: UUITP-27/24

Abstract: We examine the color-kinematics duality within the BV formalism, highlighting its emergence as a feature of specific gauge-fixed actions. Our goal is to establish a general framework for studying the duality while investigating straightforward examples of off-shell color-kinematics duality. In this context, we revisit Chern-Simons theory as well as introduce new examples, including BF theory and 2D Yang-Mills theory, which are shown to exhibit the duality off-shell. We emphasize that the geometric structures responsible for flat-space color-kinematics duality appear for general curved spaces as well.

Infinite-Length Limit of Spectral Curves and Inverse Scattering

Authors: Niklas Beisert, Kunal Gupta

Preprint number: UUITP-26/24

Abstract: Integrability equips models of theoretical physics with efficient methods for the exact construction of useful states and their evolution. Relevant tools for classical integrable field models in one spatial dimensional are spectral curves in the case of periodic fields and inverse scattering for asymptotic boundary conditions. Even though the two methods are quite different in many ways, they ought to be related by taking the periodicity length of closed boundary conditions to infinity. Using the Korteweg-de Vries equation and the continuous Heisenberg magnet as prototypical classical integrable field models, we discuss and illustrate how data for spectral curves transforms into asymptotic scattering data. In order to gain intuition and also for concreteness, we review how the elliptic states of these models degenerate into solitons at infinite length.

Weak G2-manifolds and scale separation in M-theory from type IIA backgrounds

Authors: Vincent Van Hemelryck

Preprint number: UUITP-25/24

Abstract: This work provides evidence for the existence of supersymmetric and scale-separated AdS4 vacua in M-theory of the Freund-Rubin type. The internal space has weak G2-holonomy, which is obtained from the lift of AdS vacua in massless type IIA on a specific SU(3)-structure with O6-planes. Such lifts require a local treatment of the O6-planes, therefore going beyond the usual smeared approximation. The setup is analysed by solving the pure spinor equations and the Bianchi identities perturbatively in a small backreaction parameter, preserving supersymmetry manifestly and therefore extending on previous work. This approach is applicable to lifts of other type IIA vacua on half-flat SU(3)-structures, including those with D6-brane sources. The resulting 7d manifold presented here exhibits singularities originating from the O6-planes loci in type IIA theory. Additionally, scale separation in M-theory arises from a decoupling between the Ricci curvature and
the first eigenvalue of the Laplacian of the proposed 7d manifold, thereby challenging certain conjectures in the swampland program.

Gauging generalised symmetries in linear gravity

Authors: Chris Hull, Maxwell L Hutt, Ulf Lindström

Preprint number: UUITP-24/24

Abstract: The theory of a free spin-2 field on Minkowski spacetime has 1-form and (d − 3)-form symmetries associated with conserved currents formed by contractions of the linearised Riemann tensor with conformal Killing-Yano 2-forms. We show that a subset of these can be interpreted as Noether currents for specific shift symmetries of the graviton that involve a Killing vector and a closed 1-form parameter. We give a systematic method to gauge these 1-form symmetries by coupling the currents to background gauge fields and introducing a particular set of counter-terms involving the background fields. The simultaneous gauging of certain pairs of 1-form and (d − 3)-form symmetries is obstructed by the presence of mixed ’t Hooft anomalies. The anomalous pairs of symmetries are those which are related by gravitational duality. The implications of these anomaliesare discussed.

Generalised symmetries in linear gravity

Authors: Chris Hull, Maxwell L Hutt, Ulf Lindström

Preprint number: UUITP-23/24

Abstract: Linearised gravity has a global symmetry under which the graviton is shifted by a symmetric tensor satisfying a certain flatness condition. There is also a dual symmetry that can be associated with a global shift symmetry of the dual graviton theory. The corresponding conserved charges are shown to satisfy a centrally-extended algebra. We discuss the gauging of these global symmetries, finding an obstruction to the simultaneous gauging of both symmetries which we interpret as a mixed ’t Hooft anomaly for the ungauged theory. We discuss the implications of this, analogous to those resulting from a similar structure in Maxwell theory, and interpret the graviton and dual graviton as Nambu-Goldstone modes for these shift symmetries.

Symplectic cuts and open/closed strings II

Authors: Luca Cassia, Pietro Longhi, Maxim Zabzine

Preprint number: UUITP-22/24

Abstract: In arXiv:2306.07329 we established a connection between symplectic cuts of Calabi-Yau threefolds and open topological strings, and used this to introduce an equivariant deformation of the disk potential of toric branes. In this paper we establish a connection to higher-dimensional Calabi-Yau geometries by showing that the equivariant disk potential arises as an equivariant period of certain Calabi-Yau fourfolds and fivefolds, which encode moduli spaces of one and two symplectic cuts (the maximal case) by a construction of Braverman arXiv:alg-geom/9712024. Extended Picard-Fuchs equations for toric branes, capturing dependence on both open and closed string moduli, are derived from a suitable limit of the equivariant quantum cohomology rings of the higher Calabi-Yau geometries.

Learning Group Invariant Calabi-Yau Metrics by Fundamental Domain Projections

Authors: Yacoub Hendi, Magdalena Larfors, Moritz Walden

Preprint number: UUITP-21/24

Abstract: We present new invariant machine learning models that approximate the Ricci-flat metric on Calabi-Yau (CY) manifolds with discrete symmetries. We accomplish this by combining the φ-model of the cymetric package with non-trainable, G-invariant, canonicalization layers that project the φ-model’s input data (i.e. points sampled from the CY geometry) to the fundamental domain of a given symmetry group G. These G-invariant layers are easy to concatenate, provided one compatibility condition is fulfilled, and combine well with spectral φ-models. Through experiments on different CY geometries, we find that, for fixed point sample size and training time, canonicalized models give slightly more accurate metric approximations than the standard φ-model. The method may also be used to compute Ricci-flat metric on smooth CY quotients. We demonstrate this aspect by experiments on a smooth Z52 quotient of a 5-parameter quintic CY manifold.

Vortices on Cylinders and Warped Exponential Networks

Authors: Kunal Gupta, Pietro Longhi

Preprint number: UUITP-20/24

Abstract: We study 3d N = 2 U(1) Chern-Simons-matter QFT on a cylinder C × R. The topology of C gives rise to BPS sectors of low-energy solitons known as kinky vortices, which interpolate between (possibly) different vacua at the ends of the cylinder and at the same time carry magnetic flux. We compute the spectrum of BPS vortices on the cylinder in an isolated Higgs vacuum, through the framework of warped exponential networks, which we introduce. We then conjecture a relation between these and standard vortices on R2, which are related to genus-zero open Gromov-Witten invariants of toric branes. More specifically, we show that in the limit of large Fayet-Iliopoulos coupling, the spectrum of kinky vortices on C undergoes an infinite sequence of wall-crossing transitions, and eventually stabilizes. We then propose an exact relation between a generating series of stabilized CFIV indices and the Gromov-Witten disk potential, and discuss its consequences for the structure of moduli spaces of vortices.

The worldsheet skein D-module and basic curves on Lagrangian fillings of the Hopf link conormal

Authors: Tobias Ekholm, Pietro Longhi, Lukas Nakamura

Preprint number: UUITP-19/24

Abstract: HOMFLYPT polynomials of knots in the 3-sphere in symmetric representations satisfy recursion relations. Their geometric origin is holomorphic curves at infinity on knot conormals that determine a D-module with characteristic variety the Legendrian knot conormal augmention variety and with the recursion relations as operator polynomial generators [arXiv:1304.5778, arXiv:1803.04011]. We consider skein lifts of recursions and D-modules corresponding to skein valued open curve counts [arXiv:1901.08027] that encode HOMFLYPT polynomials colored by arbitrary partitions. We define a worldsheet skein module which is the universal target for skein curve counts and a corresponding D-module. We then consider the concrete example of the Legendrian conormal of the Hopf link. We show that the worldsheet skein D-module for the Hopf link conormal is generated by three operator polynomials that annihilate the skein valued partition function for any choice of Lagrangian filling and recursively determine it uniquely. We find Lagrangian fillings for any point in the augmentation variety and show that their skein valued partition functions admit quiver-like expansions where all holomorphic curves are generated by a small number of basic holomorphic disks and annuli and their multiple covers.

Generalized Nahm Sums

Authors: Kaiwen Sun

Preprint number: UUITP-18/24

Abstract: TBA

Fay identities for polylogarithms on higher-genus Riemann surfaces

Authors: Eric D’Hoker, Oliver Schlotterer

Preprint number: UUITP-17/24

Abstract: A recent construction of polylogarithms on Riemann surfaces of arbitrary genus in arXiv:2306.08644 is based on a flat connection assembled from single-valued non-holomorphic integration kernels that depend on two points on the Riemann surface. In this work, we construct and prove infinite families of bilinear relations among these integration kernels that are necessary for the closure of the space of higher-genus polylogarithms under integration over the points on the surface. Our bilinear relations generalize the Fay identities among the genus-one Kronecker-Eisenstein kernels to arbitrary genus. The multiple-valued meromorphic kernels in the flat connection of Enriquez are conjectured to obey higher-genus Fay identities of exactly the same form as their single-valued non-holomorphic counterparts. We initiate the applications of Fay identities to derive functional relations among higher-genus polylogarithms involving either single-valued or meromorphic integration kernels.

Canonicalizing zeta generators: genus zero and genus one

Authors: Daniele Dorigoni, Mehregan Doroudiani, Joshua Drewitt, Martijn Hidding, Axel Kleinschmidt, Oliver Schlotterer, Leila Schneps, Bram Verbeek

Preprint number: UUITP-16/24

Abstract: Zeta generators are derivations associated with odd Riemann zeta values that act freely on the Lie algebra of the fundamental group of Riemann surfaces with marked points. The genus-zero incarnation of zeta generators are Ihara derivations of certain Lie polynomials in two generators that can be obtained from the Drinfeld associator. We characterize a canonical choice of these polynomials, together with their non-Lie counterparts at even degrees w ≥ 2, through the action of the dual space of formal and motivic multizeta values. Based on these canonical polynomials, we propose a canonical isomorphism that maps motivic multizeta values into the f-alphabet. The canonical Lie polynomials from the genus-zero setup determine canonical zeta generators in genus one that act on the two generators of Enriquez’ elliptic associators. Up to a single contribution at fixed degree, the zeta generators in genus one are systematically expanded in terms of Tsunogai’s geometric derivations dual to holomorphic Eisenstein series, leading to a wealth of explicit high-order computations. Earlier ambiguities in defining the non-geometric part of genus-one zeta generators are resolved by imposing a new representation-theoretic condition. The tight interplay between zeta generators in genus zero and genus one unravelled in this work connects the construction of single-valued multiple polylogarithms on the sphere with iterated-Eisenstein-integral representations of modular graph forms.

Minimal W-algebras with non-admissible levels and intermediate Lie algebras

Authors: Kaiwen Sun

Preprint number: UUITP-15/24

Abstract: In [Kawasetsu:2018irs], Kawasetsu proved that the simple W-algebra associated with a minimal nilpotent element W k(g, fθ) is rational and C2-cofinite for g = D4, E6, E7, E8 with non-admissible level k = −h/6. In this paper, we study W k(g, fθ) algebra for g = E6, E7, E8 with non-admissible level k = −h/6 + 1. We determine all irreducible (Ramond twisted) modules, compute their characters and find coset constructions and Hecke operator interpretations. These W-algebras are closely related to intermediate Lie algebras and intermediate vertex subalgebras.

Monodromies of Second Order q-difference Equations from the WKB Approximation

Authors: Fabrizio Del Monte, Pietro Longhi

Preprint number: UUITP-14/24

Abstract: This paper studies the space of monodromy data of second order q-difference equations through the framework of WKB analysis. We compute connection matrices for Stokes phenomena of WKB wavefunctions and develop a general formalism to parameterize monodromies of the q-difference equation. Computations of monodromies are illustrated with explicit examples, including the q-Mathieu equation and its degenerations. In all examples we show that the monodromy around C* admits an expansion in terms of quantum periods with integer coefficients. Physically these monodromies correspond to expectation values of Wilson line operators in five dimensional quantum field theories with minimal supersymmetry. We confirm these expectations against predictions from work on cluster integrable systems.

Charged Nariai black holes on the dark bubble

Authors: Ulf Danielsson and Vincent Van Hemelryck

Preprint number: UUITP-13/24

Abstract: In this paper, we realise the charged Nariai black hole on a braneworld from a nucleated bubble in AdS5, known as the dark bubble model.

Geometrically, the black hole takes the form of a cylindrical spacetime pulling on the dark bubble. This is realised by a brane embedding in an AdS5 black string background. Identifying the brane with a D3-brane in string theory allows us to determine a relation between the fine structure constant and the string coupling, αEM = 3/2 gs, which was previously obtained for a microscopic black hole. We also speculate on the consequences for the Festina Lente bound and neutrino masses.

Exploring Black Hole Mimickers: Electromagnetic and Gravitational Signatures of AdS Black Shells 

Authors: Suvendu Giri, Ulf Danielsson, Luis Lehner, Frans Pretorius

Preprint number: UUITP-12/24

Abstract: We study electromagnetic and gravitational properties of AdS black shells (also referred to as AdS black bubbles) – a class of quantum gravity motivated black hole mimickers, that in the classical limit are described as ultra compact shells of matter. We find that their electromagnetic properties are remarkably similar to black holes. We then discuss the extent to which these objects are distinguishable from black holes, both for its intrinsic interest within the black shell model, but also as a guide for similar efforts in other sub-classes of ECOs. We study photon rings and lensing band characteristics, relevant for very large baseline inteferometry (VLBI) experiments, as well as gravitational wave observables – quasinormal modes in the eikonal limit and the static tidal Love number for non-spinning shells – relevant for ongoing and upcoming gravitational wave experiments.

Gauge-Invariant Magnetic Charges in Linearised Gravity

Authors: Chris Hull, Maxwell L. Hutt, Ulf Lindström

Preprint number: UUITP-11/24

Abstract: Linearised gravity has magnetic charges carried by (linearised) Kaluza-Klein monopoles. A gauge-invariant expression is found for these charges that is similar to Penrose's gauge-invariant expression for the ADM charges. A systematic search is made for other gauge-invariant charges.

Super Yang-Mills on Branched Covers and Weighted Projective Spaces 

Authors: Roman Mauch and Lorenzo Ruggeri

Preprint number: UUITP-10/24

Abstract: In this work we conjecture the Coulomb branch partition function, including flux and instanton contributions, for the N = 2 vector multiplet on weighted projective space CP2N for equivariant Donaldson Witten and “Pestun-like” theories. More precisely, we claim that this partition function agrees with the one computed on a certain branched cover of CP2 upon matching conical deficit angles with corresponding branch indices. Our conjecture is substantiated by checking that similar partition functions on spindles agree with their equivalent on certain branched covers of CP1. We compute the one-loop determinant on the branched cover of CP2 for all flux sectors via dimensional reduction from the N = 1 vector multiplet on a branched five-sphere along a free S1 action. Our work paves the way for obtaining partition functions on more generic symplectic toric orbifolds.

Non-holomorphic modular forms from zeta generators

Authors: Daniele Dorigoni, Mehregan Doroudiani, Joshua Drewitt, Martijn Hidding, Axel Kleinschmidt, Oliver Schlotterer, Leila Schneps and Bram Verbeek

Preprint number: UUITP-09/24

Abstract: We study non-holomorphic modular forms built from iterated integrals of holomorphic modular forms for SL(2,Z) known as equivariant iterated Eisenstein integrals. A special subclass of them furnishes an equivalent description of the modular graph forms appearing in the low-energy expansion of string amplitudes at genus one. Notably the Fourier expansion of modular graph forms contains single-valued multiple zeta values. We deduce the appearance of products and higher-depth instances of multiple zeta values in equivariant iterated Eisenstein integrals, and ultimately modular graph forms, from the coefficients of simpler odd Riemann zeta values. This analysis relies on so-called zeta generators which act on certain non commutative variables in the generating series of the iterated integrals. From an extension of these non-commutative variables we incorporate iterated integrals involving holomorphic cusp forms into our setup and use them to construct the modular completion of triple Eisenstein integrals. Our work represents a fully explicit realisation of the modular graph forms within Brown's framework of equivariant iterated Eisenstein integrals and reveals structural analogies between single-valued period functions appearing in genus zero and one string amplitudes.

Effective interactions of the open bosonic string via field theory

Authors: Lucia M. Garozzo, Alfredo Guevara

Preprint number: UUITP-08/24

Abstract: We describe a method to extract an effective Lagrangian description for open bosonic strings, at zero transcendentality. The method relies on a particular formulation of its scattering amplitudes derived from color-kinematics duality. More precisely, starting from a (DF)2 + YM quantum field theory, we integrate out all the massive degrees of freedom to generate an expansion in the inverse string tension α′. We explicitly compute the Lagrangian terms through O(α′4), and target the sector of operators proportional to F4 to all orders in α′.

T-duality between 6d (2,0) and (1,1) Little String Theories with Twist

Authors: Hee-Cheol Kim, Kimyeong Lee, Kaiwen Sun, Xin Wang

Preprint number: UUITP-07/24

On Intermediate Exceptional Series

Authors: Kimyeong Lee, Kaiwen Sun, Haowu Wang

Preprint number: UUITP-06/24

Abstract: The Freudenthal–Tits magic square m(A1,A2) for A=R,C,H,O of semi-simple Lie algebras can be extended by including the sextonions S. A series of non-reductive Lie algebras naturally appear in the new row associated with the sextonions, which we will call the intermediate exceptional series, with the largest one as the intermediate Lie algebra E7+1/2 constructed by Landsberg–Manivel. We study various aspects of the intermediate vertex operator (super)algebras associated with the intermediate exceptional series, including rationality, coset constructions, irreducible modules, (super)characters and modular linear differential equations. For all gI belonging to the intermediate exceptional series, the intermediate VOA L1(gI) has characters of irreducible modules coinciding with those of the simple rational C2-cofinite W-algebra W-h∨/6(g,fθ) studied by Kawasetsu, with g belonging to the Cvitanović–Deligne exceptional series. We propose some new intermediate VOA Lk(gI) with integer level k and investigate their properties. For example, for the intermediate Lie algebra D6+1/2 between D6 and E7 in the subexceptional series and also in Vogel's projective plane, we find that the intermediate VOA L2(D6+1/2) has a simple current extension to a SVOA with four irreducible Neveu–Schwarz modules. We also provide some (super) coset constructions such as L2(E7)/L2(D6+1/2) and L1(D6+1/2)⊗2/L2(D6+1/2). In the end, we find that the theta blocks associated with the intermediate exceptional series produce some new holomorphic Jacobi forms of critical weight and lattice index.

N=(2,2) superfields and geometry revisited

Authors: Chris Hull and Maxim Zabzine

Preprint number: UUITP-05/24

Charges and topology in linearised gravity

Authors: Chris Hull, Maxwell L. Hutt and Ulf Lindström

Preprint number: UUITP-04/24

Abstract: Covariant conserved 2-form currents for linearised gravity are constructed by contracting the linearised curvature with conformal Killing–Yano tensors. The corresponding conserved charges were originally introduced by Penrose and have recently been interpreted as the generators of generalised symmetries of the graviton. We introduce an off-shell refinement of these charges and find the relation between these improved Penrose charges and the linearised version of the ADM momentum and angular momentum. If the graviton field is globally well-defined on a background Minkowski space then some of the Penrose charges give the momentum and angular momentum while the remainder vanish. We consider the generalisation in which the graviton has Dirac string singularities or is defined locally in patches, in which case the conventional ADM expressions are not invariant under the graviton gauge symmetry in general. We modify these expressions to render them gauge-invariant and show that the Penrose charges give these modified charges plus certain magnetic gravitational charges. We discuss properties of the Penrose charges, generalise to toroidal Kaluza–Klein compactifications and check our results in a number of examples.

The soaring kite: a tale of two punctured tori

Authors: Mathieu Giroux, Andrzej Pokraka, Franziska Porkert, Yoann Sohnle

Preprint number: UUITP-03/24

Abstract: We consider the 5-mass kite family of Feynman integrals and present a systematic approach for constructing an ε-form basis, along with its differential equation pulled back onto the moduli space of two tori. Each torus is associated with one of the two distinct elliptic curves this family depends on. We demonstrate how the relevant punctures, which are required to parametrize the full image of the kinematic space onto this moduli space, can be obtained from integrals over maximal cuts. Given an appropriate boundary value, the differential equation is systematically solved in terms of iterated integrals over Kronecker-Eisenstein g-kernels and modular forms. Then, the numerical evaluation of the master integrals is discussed, and important challenges in that regard are emphasized. In an appendix, we introduce new relations between g-kernels.

What can abelian gauge theories teach us about kinematic algebras? 

Authors: Kymani Armstrong-Williams, Silvia Nagy, Chris D. White, Sam Wikeley

Preprint number: UUITP–02/24

Abstract: The phenomenon of BCJ duality implies that gauge theories possess an abstract kinematic algebra, mirroring the non-abelian Lie algebra underlying the colour information. Although the nature of the kinematic algebra is known in certain cases, a full understanding is missing for arbitrary non-abelian gauge theories, such that one typically works outwards from well-known examples. In this paper, we pursue an orthogonal approach, and argue that simpler abelian gauge theories can be used as a testing ground for clarifying our understanding of kinematic algebras. We first describe how classes of abelian gauge fields are associated with well-defined subgroups of the diffeomorphism algebra. By considering certain special subgroups, we show that one may construct interacting theories, whose kinematic algebras are inherited from those already appearing in a related abelian theory. Known properties of (anti-)self-dual Yang–Mills theory arise in this way, but so do new generalisations, including self-dual electromagnetism coupled to scalar matter. Furthermore, a recently obtained non-abelian generalisation of the Navier–Stokes equation fits into a similar scheme, as does Chern–Simons theory. Our results provide useful input to further conceptual studies of kinematic algebras.

Plücker Coordinates and the Rosenfeld Planes

Authors: Jian Qiu

Preprint number: UUITP-01/24

Abstract: The exceptional compact hermitian symmetric space EIII is the quotient E6/SO(10)×Z4 U(1). We introduce the Plücker coordinates which give an embedding of EIII into CP26 as a projective subvariety. The subvariety is cut out by 27 Plücker relations. We show that, using Clifford algebra, one can solve this over-determined system of relations, giving local coordinate charts to the space. Our motivation is to understand EIII as the complex projective octonion plane (C⊗O)P2, which is a piece of folklore scattered across literature. We will see that the EIII has an atlas whose transition functions have clear octonion interpretations, apart from those covering a sub-variety of dimension 10 denoted X. This subvariety is itself a hermitian symmetric space known as DIII, with no apparent octonion interpretation. We give detailed analysis of the geometry in the neighbourhood of X. We further decompose X into F4-orbits: X=Y0∪Y, where Y is an open F4-orbit and is the complexified octonion projective plane and Y has co-dimension 1, and is needed to complete Y into a projective variety. This decomposition appears in the classification of equivariant completion of homogeneous algebraic varieties by Ahiezer.

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