Abstract

It has been conjectured that in theories consistent with quantum gravity infinite distances in field space coincide with an infinite tower of states becoming massless exponentially fast in the proper field distance. The complex-structure moduli space of Calabi-Yau manifolds is a good testing ground for this conjecture since it is known to encode quantum gravity physics. We study infinite distances in this setting and present new evidence for the above conjecture. Points in moduli space which are at infinite proper distance along any path are characterised by an infinite order monodromy matrix. We utilise the nilpotent orbit theorem to show that for a large class of such points the monodromy matrix generates an infinite orbit within the spectrum of BPS states. We identify an infinite tower of states with this orbit. Further, the theorem gives the local metric on the moduli space which can be used to show that the mass of the states decreases exponentially fast upon approaching the point. We also propose a reason for why infinite distances are related to infinite towers of states. Specifically, we present evidence that the infinite distance itself is an emergent quantum phenomenon induced by integrating out at one-loop the states that become massless. Concretely, we show that the behaviour of the field space metric upon approaching infinite distance can be recovered from integrating out the BPS states. Similarly, at infinite distance the gauge couplings of closed-string Abelian gauge symmetries vanish in a way which can be matched onto integrating out the infinite tower of charged BPS states. This presents evidence towards the idea that also the gauge theory weak-coupling limit can be thought of as emergent.

Highlights

  • Quantum field theory and gravity are notoriously difficult to combine at high energy scales close to the Planck mass Mp

  • At infinite distance the gauge couplings of closed-string Abelian gauge symmetries vanish in a way which can be matched onto integrating out the infinite tower of charged BPS states

  • We explicitly identified an infinite tower of BPS states which become massless exponentially fast in the proper distance upon approaching any infinite distance d = 3 locus on Calabi-Yau threefolds

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Summary

Introduction

We will consider the tower to be formed of BPS states, which in type IIB are D3-branes wrapping special Lagrangian three-cycles Once this tower is identified, we will show that the exponential mass behaviour of the Swampland Distance Conjecture can be proven in generality due to a powerful mathematical theorem, termed the Nilpotent Orbit Theorem [14], which, among other things, gives a general expression for the asymptotic infinite distance form of the field space metric. Introduce the technology of Mixed Hodge Structures and their utilisation in the Sl2-orbit theorem of Schimd [14] This will allow us to study when an infinite monodromy orbit through massless BPS states exists and to identify it quite precisely.

Infinite distance divisors in Calabi-Yau moduli space
Complex structure moduli space and monodromy
The local Kahler potential and a necessary condition for infinite distance
Infinite distance paths in one-parameter degenerations
Massless BPS states
Monodromy orbits and massless states
The monodromy orbit and BPS states
The exponential mass behaviour
Microscopic physics for BPS stability
Infinite monodromy orbits and mixed Hodge structures
A coarse introduction to the refined Hodge structure
Mathematical machinery of mixed Hodge structures
Polarized pure Hodge structures
Monodromy weight filtrations and mixed Hodge structures
Deligne splitting
Properties of a0
Growth of the Hodge norm
Infinite monodromy orbits at singular loci
Monodromy intersection loci
Infinite distances from integrating out states
Field space corrections from integrating out states
Application to the monodromy loci
Relation to the Scalar WGC and to global symmetries
The gauge kinetic function and the Weak Gravity Conjecture
Behaviour of the gauge kinetic function
Gauge kinetic function from integrating out states
Summary
A Non-mutually stable BPS states
B Some simple examples and classification results

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