The Swampland program in String Theory...WGC for axions Loophole: “spectator instantons” [Brown...
Transcript of The Swampland program in String Theory...WGC for axions Loophole: “spectator instantons” [Brown...
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The Swampland program in String Theory
Irene ValenzuelaHarvard University
Iberian Strings 2020, Santiago de Compostela, Jan 2020
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For a normal person…
For a string theorist…
For a phenomenologist…
New out-of-the-blue constraintsto take care of
What is swampland?
Whatever does not belong to string
theory
He believes he is the String Theory
Landscape
Stay in the Swampland
- QG
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Apparently consistent (anomaly-free) quantum effective field theories that cannot be UV embedded in quantum gravity
Swampland:
Not everything is possible in string theory/quantum gravity!!!
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Apparently consistent (anomaly-free) quantum effective field theories that cannot be UV embedded in quantum gravity
(they cannot arise from string theory)
Swampland:
Not everything is possible in string theory/quantum gravity!!!
(String)
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Landscape
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Landscape
Swampland[Vafa’06][Ooguri-Vafa’06]
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Landscape
Not consistent with quantum gravity
Consistent with quantum gravity
Swampland[Vafa’06][Ooguri-Vafa’06]
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What are the constraints that an effective theory must satisfy to be consistent with quantum gravity?
What distinguishes the landscape from the swampland?
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First guess: Anomalies
QFT of scalars and fermions
effective field theories
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First guess: Anomalies
Anomalous
Anomaly-free
QFT of scalars and fermions
QFT of scalars and fermions+ gauge fields
Anomaly constraints
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First guess: Anomalies
Anomalous
Anomaly-free
QFT of scalars and fermions
QFT of scalars and fermions+ gauge fields
Anomaly constraints
example. QFT of one fermion with SU(2) global symmetry
There is a Witten anomaly when coupling the theory to a gauge field!
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QFT of scalars and fermions
QFT of scalars and fermions+ gauge fields
QFT of scalars and fermions+ gauge fields
+ gravityAnomaly constraints
First guess: Anomalies
Anomalous
Swampland
Landscape
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QFT of scalars and fermions
QFT of scalars and fermions+ gauge fields
QFT of scalars and fermions+ gauge fields
+ gravityAnomaly constraints
First guess: Anomalies
Anomalous
Swampland
Landscape
Gravitational anomalies are not enough
Additional QG constraints!
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There are additional (swampland/QG) constraints that any effective QFT must satisfy to be consistent with quantum gravity
UV imprint of quantum gravity at low energies
Outstanding phenomenological implications!
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Proposals: Quantum Gravity Conjectures
Motivated by String Theory as well as Black Hole physics
(or Swampland Conjectures)
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Weak GravityConjecture
Non-susy AdS vacua are unstable
Cosmological constant and SM
neutrinos
No dual CFT
Large field inflation
Swampland DistanceConjecture
Cosmological relaxation
No global symmetries
No deSitter
Completeness hypothesis
evidence
+
-
No scale separation in AdS
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evidence
+
-
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Weak GravityConjecture
Large field inflationCosmological
relaxation
evidence
+
-
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Weak Gravity Conjecture
There exist at least a particle in which gravity acts weaker than the gauge force
[Arkani-Hamed,Motl,Nicolis,Vafa’06]
Q
m� 1 Q : charge
m : mass
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Weak Gravity Conjecture
Given an abelian gauge field, there must exist an electrically charged particle with
[Arkani-Hamed et al.’06]
in order to allow extremal black holes to decay.
Q
m� Q
m
����extremal
= 1
Electric version:
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Weak Gravity Conjecture
Given an abelian gauge field, there must exist an electrically charged particle with
[Arkani-Hamed et al.’06]
in order to allow extremal black holes to decay.
Q
m� Q
m
����extremal
= 1
Electric version:
Magnetic version:
The effective theory breaks down at a cut-off scale
which decreases as the gauge coupling goes to zero.
⇤ gYMMp
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Weak Gravity Conjecture
Given an abelian gauge field, there must exist an electrically charged particle with
[Arkani-Hamed et al.’06]
in order to allow extremal black holes to decay.
Q
m� Q
m
����extremal
= 1
Evidence:
- Plethora of examples in string theory (not known counter-example)
- Derivation from modular invariance of the 2d CFT
- Relation to entropy bounds, unitarity and causality
- Relation to cosmic censorship
[Heidenreich et al’16] [Montero et al’16]
[Cottrell et al’16]
[Crisford et al’17]
[Fisher et al’17][Cheung et al’18]
- Relation to thermodynamic arguments
[Hamada et al’18]
[Hod’17,] [Urbano’18]
[Montero’ 19]
- Derivation from higher derivative corrections to BH’s [Charles’19]
- Relation to entanglement entropy
[Andriolo et al’18]
[Jones et al’19]
Electric version:
[Cano et al’19]
[Lee et al’18-19][Grimm et al’18-19][Bonnefoy et al’18]
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WGC for axions
Given an axion, there must exist an electrically charged instanton with
S : action (mass)
decay constant (inverse gauge coupling)f :S Mp
f
V = Ae�Scos
✓�
f
◆Induce a scalar potential: +
X
n
Ae�nScos
✓n�
f
◆
[Rudelius, Heidenreich, Reece, Brown, Soler, Cottrell, Shiu, Bachlechner, Long, McAllister, Montero, I.V., Uranga,…]
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WGC for axions
Given an axion, there must exist an electrically charged instanton with
S : action (mass)
decay constant (inverse gauge coupling)f :S Mp
f
V = Ae�Scos
✓�
f
◆Induce a scalar potential:
Perturbative control + WGC f < MpS > 1
If instanton inducing the potential for inflation satisfies the WGC
[Arkani-Hamed et al.’06][Rudelius’15]
Transplanckian axions (for large field inflation)
are ruled out
+
X
n
Ae�nScos
✓n�
f
◆
[Rudelius, Heidenreich, Reece, Brown, Soler, Cottrell, Shiu, Bachlechner, Long, McAllister, Montero, I.V., Uranga,…]
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WGC for axions
Loophole: “spectator instantons” [Brown et al.’15] [Bachlechner et al’15]
Instantons satisfying the WGC are not the same than those generating the inflationary potential
Million dollar question! Who must satisfy the WGC? the lightes
t?
more than one?
small BH’s?
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WGC for axions
Loophole: “spectator instantons” [Brown et al.’15] [Bachlechner et al’15]
Instantons satisfying the WGC are not the same than those generating the inflationary potential
Million dollar question! Who must satisfy the WGC?
Different versions of the WGC (strong forms):[Heidenreich et al.’15]• (Sub)lattice WGC
• Tower WGCconsistency with dimensional reductionmodular invariance of CFTanalyticity and causality
Only instantons with small will contribute significantly to the potential
|Q|
S |Q|f
Mp
[Andriolo et al.’18][Montero et al.’15] [Heidenreich et al.’16]
the lightes
t?
more than one?
small BH’s?
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WGC for axions
Loophole: “spectator instantons”
Different versions of the WGC (strong forms):
Instantons satisfying the WGC are not the same than those generating the inflationary potential
Million dollar question! Who must satisfy the WGC?
• (Sub)lattice WGC• Tower WGC
Constraints on inflation depend on index n of sublatticen
[Heidenreich et al.’19]
[Brown et al.’15] [Bachlechner et al’15]
S |Q|f
Mp
[Heidenreich et al.’15]consistency with dimensional reductionmodular invariance of CFTanalyticity and causality [Andriolo et al.’18]
[Montero et al.’15] [Heidenreich et al.’16]
the lightes
t?
more than one?
small BH’s?
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Weak GravityConjecture
Large field inflationCosmological
relaxation
evidence
+
-
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Non-susy AdS vacua are unstable
Cosmological constant and SM
neutrinos
No dual CFT
Weak GravityConjecture
Large field inflationCosmological
relaxation
evidence
+
-
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Weak Gravity Conjecture
There exist at least a particle in which gravity acts weaker than the gauge force
[Arkani-Hamed,Motl,Nicolis,Vafa’06]
Q
m� 1 Q : charge
m : mass
only allowed if supersymmetric
q = m
[Ooguri-Vafa’17]
Sharpening of WGC:
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Weak Gravity Conjecture for fluxes
Brane (domain wall) with Bubble instability of the vacuum!T < Q
[Maldacena et al.’99]
AdS with less flux
AdS vacuum
There can be gauge fields propagating in the extra dimensions
4d space-time
Extra dimensions
f0 ⇠Z
⌃p
Fp (fluxes in 4d)
WGC applied to the fluxes (in a non-susy vacuum) implies: [Ooguri-Vafa’17]
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Weak Gravity Conjecture for fluxes
Brane (domain wall) with Bubble instability of the vacuum!T < Q
[Maldacena et al.’99]
AdS with less flux
AdS vacuum
There can be gauge fields propagating in the extra dimensions
4d space-time
Extra dimensions
f0 ⇠Z
⌃p
Fp (fluxes in 4d)
WGC applied to the fluxes (in a non-susy vacuum) implies: [Ooguri-Vafa’17]
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Non-susy vacua are at best metastable[Freivogel-Kleban’16]
[Ooguri-Vafa’16]
Non-susy stable AdS vacua are in the Swampland (inconsistent with Quantum Gravity)!
AdS Instability Conjecture
Implications:
Our universe must be metastable
Non-susy CFT cannot have an Einstein gravity AdS dual
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Non-susy vacua are at best metastable[Freivogel-Kleban’16]
[Ooguri-Vafa’16]
Non-susy stable AdS vacua are in the Swampland (inconsistent with Quantum Gravity)!
AdS Instability Conjecture
Implications:
Our universe must be metastable
Constraints on BSM from studying lower dimensional AdS vacua arising from compactifications of the SM
Non-susy CFT cannot have an Einstein gravity AdS dual
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Notice: Standard Model compactified to lower dimensions can yield non-SUSY AdS vacua
If stable, SM would be incompatible with quantum gravity!
Solution: Require absence of 3d AdS vacua
[Arkani-Hamed et al.’07]
(also [Hamada,Shiu’17])
[Ibanez,Martin-Lozano,IV’17]
Implications for Particle Physics
Constraints on light spectra of SM
[Arnold-Fornal-Wise’10],
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Notice: Standard Model compactified to lower dimensions can yield non-SUSY AdS vacua
If stable, SM would be incompatible with quantum gravity!
Solution: Require absence of 3d AdS vacua
[Arkani-Hamed et al.’07]
(also [Hamada,Shiu’17])
[Ibanez,Martin-Lozano,IV’17]
Implications for Particle Physics
Constraints on light spectra of SM
[Arnold-Fornal-Wise’10],
Lower bound on the cosmological constant in terms of the neutrino masses
Translated to upper bound on the EW scale:
Majorana neutrinos are ruled out unless new light BSM fermions
hHi . 1.6⇤1/4
Y⌫1
SM by itself ruled out MSSM survives [Gonzalo,Herraez,Ibanez’18]
[Ibanez,Martin-Lozano,IV’17]
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Naturalness?
Y = 10�14
hHi . 1.6⇤1/4
Y⌫1
Parameters leading to a higher EW scale do not yield theories consistent with quantum gravity
No EW hierarchy problem
Consistency with quantum gravity requires
New approach to fine-tuning/hierarchy problems?UV/IR mixing from quantum gravity?
Naturalness might not be a good principle, not everything goes!
(recall: sufficient but not necessary condition)
[Ibanez,Martin-Lozano,IV’17]
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Weak GravityConjecture
Non-susy AdS vacua are unstable
Cosmological constant and SM
neutrinos
No dual CFT
Large field inflationCosmological
relaxation
evidence
+
-
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Swampland DistanceConjecture
No global symmetries
Weak GravityConjecture
Non-susy AdS vacua are unstable
Cosmological constant and SM
neutrinos
No dual CFT
Large field inflationCosmological
relaxation
evidence
+
-
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Absence of global symmetries
Any global symmetry must be broken or gauged
Proof in AdS/CFTBlack Hole arguments
It does not constrain the IR effective theory
Evidence:[Harlow,Ooguri ’18]
[Banks-Dixon’88][Horowitz,Strominger,Seiberg…]
breaking can be very suppressed
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Absence of global symmetries
Any global symmetry must be broken or gauged
Proof in AdS/CFTBlack Hole arguments
It does not constrain the IR effective theory
Evidence:[Harlow,Ooguri ’18]
[Banks-Dixon’88][Horowitz,Strominger,Seiberg…]
breaking can be very suppressed
Exception:
to avoid global symmetry from (d-k-1)-dim defects
New swampland criterium ⌦QGk = 0
It implies all theories are connected by finite energy domain walls, and predicts the existence of new defects in string theory!
[McNamara,Vafa’19]
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What about approximate symmetries? How badly broken?
Absence of global symmetries
Any global symmetry must be broken or gauged
Proof in AdS/CFTBlack Hole arguments
It does not constrain the IR effective theory
It can constrain the IR effective theory!
WGC and SDC quantify how ‘approximate’ a global symmetry can be
Evidence:[Harlow,Ooguri ’18]
[Banks-Dixon’88][Horowitz,Strominger,Seiberg…]
breaking can be very suppressed
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Parameter space:
Assume some global symmetry can be restored in a continuous way at some special points of the parameter space
e.g. by sending gauge coupling gYM ! 0
Approximate global symmetries
we restore a U(1) global symmetry
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They can only be restored at infinite field distance (boundaries/singularities of the moduli space)
Global symmetries are not allowed in quantum gravity
Field space in String Theory
Parameter space:
=
Approximate global symmetries
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Asymptotic limits
Infinite distance loci: special limits where a weakly coupled description arises
(weakly coupled gauge theory, approximate global symmetries…)
Approximate global symmetries
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Asymptotic limits
but still, the EFT must break down when approaching the boundaryby quantum gravity effects
These limits seem under control from the point of view of QFT
Infinite distance loci: special limits where a weakly coupled description arises
(weakly coupled gauge theory, approximate global symmetries…)
Approximate global symmetries
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e.g. weak coupling limit: gYM ! 0
WGC acts as a Quantum Gravity obstruction to restore a global symmetry
Magnetic version of WGC:
⇤ gYMMpCut-off of effective theory
WGC and global symmetries
! 0
(EFT breaks down continuously in the global symmetry limit)
..⇤QGE
Mp
gYM ! 0
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e.g. global symmetry limit:
SDC acts as a Quantum Gravity obstruction to restore a global symmetry
Distance conjecture:
Cut-off of effective theory
Distance Conjecture and global symmetries
! 0
�� ! 1
⇤ . ⇤0 e����
due to the presence of an infinite tower of states becoming light(EFT breaks down continuously in the global symmetry limit)
m0
..
N
⇤QGE
Mp
global symmetry limit
infinitely many massless species=
�� ! 1
⇤QG =MppN
Species scale:[Dvali’07]
(scale at which QG effects become important)
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Asymptotic limits
New physicsEFT breaks down below a cut-off that vanishes in the limit
Constraints the EFT: yield no-go’s and universal patterns
Swampland Conjectures predict:
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Swampland Distance Conjecture
An effective theory is valid only for a finite scalar field variation because an infinite tower of states become exponentially light
when
��
�� ! 1
[Ooguri-Vafa’06]
L = gij(�)@�i@�j scalar manifold (moduli space)
P
Q
��
geodesic distance between P and Q
�� =
�1
�2 m(P ) . m(Q)e����
m ⇠ m0e����
This signals the breakdown of the effective theory:⇤
cut-o↵
⇠ ⇤
0
exp(����)
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Swampland Distance Conjecture
An effective theory is valid only for a finite scalar field variation ��
[Ooguri-Vafa’06]
This signals the breakdown of the effective theory:⇤
cut-o↵
⇠ ⇤
0
exp(����)
“Magnetic version”:
because an infinite tower of states become exponentially light
when �� ! 1m ⇠ m0e����
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Swampland Distance Conjecture
An effective theory is valid only for a finite scalar field variation ��
[Ooguri-Vafa’06]
This signals the breakdown of the effective theory:⇤
cut-o↵
⇠ ⇤
0
exp(����)
“Magnetic version”:
Given a scalar force, there must exist a particle with
‘Scalar WGC’Proposal:
m @�m
L � m2(�) h2 ! (m @�m)�h2
m ⇠ e��
“Electric version” ? [Palti’17]
because an infinite tower of states become exponentially light
when �� ! 1m ⇠ m0e����
[Gonzalo, Ibanez’19]
![Page 55: The Swampland program in String Theory...WGC for axions Loophole: “spectator instantons” [Brown et al.’15] [Bachlechner et al’15] Instantons satisfying the WGC are not the](https://reader036.fdocuments.in/reader036/viewer/2022062510/6130d9141ecc515869445bd8/html5/thumbnails/55.jpg)
H ⇤
�� 1
�log
Mp
H
If
Phenomenological implications
It gives an upper bound on the scalar field range that can be described by an effective field theory with finite cut-off
Cosmological relaxation of the EW scale
Large field inflation
�� . 1
�log
✓Mp
⇤
◆
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ΔφSDC ΔφLyth
0.00 0.05 0.10 0.15 0.20r
5
10
15
20Δφ
r 0.064<latexit sha1_base64="FRqNl3wvSYk4M4IbT6JZOCC5k2Y=">AAAB8nicdVDLSgMxFM3UV62vqks3wSK4Kpm+uyu6cVnB2sJ0KJk004ZmkjHJCKX0M9y4UMStX+POvzHTVlDRAyGHc+7l3nuCmDNtEPpwMmvrG5tb2e3czu7e/kH+8OhWy0QR2iGSS9ULsKacCdoxzHDaixXFUcBpN5hcpn73nirNpLgx05j6ER4JFjKCjZU81ef0DqIiqlUG+UL6V5tlZIUqcuvNZuqgWqNcgq4lKQpghfYg/94fSpJEVBjCsdaei2Ljz7AyjHA6z/UTTWNMJnhEPUsFjqj2Z4uV5/DMKkMYSmWfMHChfu+Y4UjraRTYygibsf7tpeJfnpeYsOHPmIgTQwVZDgoTDo2E6f1wyBQlhk8twUQxuyskY6wwMTalnA3h61L4P7ktFV1UdK8rhdbFKo4sOAGn4By4oA5a4Aq0QQcQIMEDeALPjnEenRfndVmacVY9x+AHnLdP5zaQWQ==</latexit><latexit sha1_base64="FRqNl3wvSYk4M4IbT6JZOCC5k2Y=">AAAB8nicdVDLSgMxFM3UV62vqks3wSK4Kpm+uyu6cVnB2sJ0KJk004ZmkjHJCKX0M9y4UMStX+POvzHTVlDRAyGHc+7l3nuCmDNtEPpwMmvrG5tb2e3czu7e/kH+8OhWy0QR2iGSS9ULsKacCdoxzHDaixXFUcBpN5hcpn73nirNpLgx05j6ER4JFjKCjZU81ef0DqIiqlUG+UL6V5tlZIUqcuvNZuqgWqNcgq4lKQpghfYg/94fSpJEVBjCsdaei2Ljz7AyjHA6z/UTTWNMJnhEPUsFjqj2Z4uV5/DMKkMYSmWfMHChfu+Y4UjraRTYygibsf7tpeJfnpeYsOHPmIgTQwVZDgoTDo2E6f1wyBQlhk8twUQxuyskY6wwMTalnA3h61L4P7ktFV1UdK8rhdbFKo4sOAGn4By4oA5a4Aq0QQcQIMEDeALPjnEenRfndVmacVY9x+AHnLdP5zaQWQ==</latexit><latexit sha1_base64="FRqNl3wvSYk4M4IbT6JZOCC5k2Y=">AAAB8nicdVDLSgMxFM3UV62vqks3wSK4Kpm+uyu6cVnB2sJ0KJk004ZmkjHJCKX0M9y4UMStX+POvzHTVlDRAyGHc+7l3nuCmDNtEPpwMmvrG5tb2e3czu7e/kH+8OhWy0QR2iGSS9ULsKacCdoxzHDaixXFUcBpN5hcpn73nirNpLgx05j6ER4JFjKCjZU81ef0DqIiqlUG+UL6V5tlZIUqcuvNZuqgWqNcgq4lKQpghfYg/94fSpJEVBjCsdaei2Ljz7AyjHA6z/UTTWNMJnhEPUsFjqj2Z4uV5/DMKkMYSmWfMHChfu+Y4UjraRTYygibsf7tpeJfnpeYsOHPmIgTQwVZDgoTDo2E6f1wyBQlhk8twUQxuyskY6wwMTalnA3h61L4P7ktFV1UdK8rhdbFKo4sOAGn4By4oA5a4Aq0QQcQIMEDeALPjnEenRfndVmacVY9x+AHnLdP5zaQWQ==</latexit><latexit sha1_base64="FRqNl3wvSYk4M4IbT6JZOCC5k2Y=">AAAB8nicdVDLSgMxFM3UV62vqks3wSK4Kpm+uyu6cVnB2sJ0KJk004ZmkjHJCKX0M9y4UMStX+POvzHTVlDRAyGHc+7l3nuCmDNtEPpwMmvrG5tb2e3czu7e/kH+8OhWy0QR2iGSS9ULsKacCdoxzHDaixXFUcBpN5hcpn73nirNpLgx05j6ER4JFjKCjZU81ef0DqIiqlUG+UL6V5tlZIUqcuvNZuqgWqNcgq4lKQpghfYg/94fSpJEVBjCsdaei2Ljz7AyjHA6z/UTTWNMJnhEPUsFjqj2Z4uV5/DMKkMYSmWfMHChfu+Y4UjraRTYygibsf7tpeJfnpeYsOHPmIgTQwVZDgoTDo2E6f1wyBQlhk8twUQxuyskY6wwMTalnA3h61L4P7ktFV1UdK8rhdbFKo4sOAGn4By4oA5a4Aq0QQcQIMEDeALPjnEenRfndVmacVY9x+AHnLdP5zaQWQ==</latexit>
H ⇤
�� 1
�log
Mp
H=
1
�log
r2
⇡2Asr
� = 1Planck constraints
Opposite scaling than Lyth bound!
[Scalisi,IV’18]
If
It gives an upper bound on the scalar field range that can be described by an effective field theory with finite cut-off
Cosmological relaxation of the EW scale
Large field inflation
Phenomenological implications
�� . 1
�log
✓Mp
⇤
◆
![Page 57: The Swampland program in String Theory...WGC for axions Loophole: “spectator instantons” [Brown et al.’15] [Bachlechner et al’15] Instantons satisfying the WGC are not the](https://reader036.fdocuments.in/reader036/viewer/2022062510/6130d9141ecc515869445bd8/html5/thumbnails/57.jpg)
�� . 1
�log
✓Mp
⇤
◆
Evidence: based on particular examples in string theory compactifications[Baume,Palti'16] [I.V.,’16] [Bielleman,Ibanez,Pedro,I.V.,Wieck’16] [Blumenhagen,I.V.,Wolf’17]
[Hebecker,Henkenjohann,Witkowski’17] [Cicoli,Ciupke,Mayhrofer,Shukla’18][Blumenhagen et al.’18][Ooguri,Vafa’06]
It gives an upper bound on the scalar field range that can be described by an effective field theory with finite cut-off
Million dollar question! What is � ? Refined SDC: � ⇠ O(1)
Phenomenological implications
Missing black hole argument: @�m
m� �
[Grimm, Palti, IV’18] [Corvilain, Grimm, Palti’18] [Lee,Lerche,Weigand’18]
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�� . 1
�log
✓Mp
⇤
◆It gives an upper bound on the scalar field range that can be described by an effective field theory with finite cut-off
Million dollar question! What is � ? Refined SDC: � ⇠ O(1)
is related to the properties of a discrete infinite symmetry generating the tower of states
�Proposal:
Phenomenological implications
Missing black hole argument: @�m
m� �
lower bounded for geodesics
[Grimm, Palti, IV’18]
In general, it can depend on the trajectory But….what type of trajectories and potentials are allowed by
Quantum Gravity?
![Page 59: The Swampland program in String Theory...WGC for axions Loophole: “spectator instantons” [Brown et al.’15] [Bachlechner et al’15] Instantons satisfying the WGC are not the](https://reader036.fdocuments.in/reader036/viewer/2022062510/6130d9141ecc515869445bd8/html5/thumbnails/59.jpg)
Evidence in String Theory
Complex structure moduli space of Type IIB Calabi-Yau threefold
4d N=2 theories:
Kahler moduli space of Type IIA Calabi-Yau threefold
Kahler moduli space of M-theory/F-theory Calabi-Yau threefold
5d/6d N=1 theories:
Infinite towers of BPS states (wrapping D3 branes)
Infinite towers of BPS states (wrapping D0-D2 branes)
Infinite towers of wrapping M2-branes/ tensionless strings
[Grimm, Palti, IV’18][Grimm,Palti,Li’18]
[Corvilain, Grimm, IV’18]
[Font,Herraez,Ibanez’19]
[Marchesano,Wiesner’19] [Grimm,van de Heisteeg’19]
Beyond particle excitations:
Towers of instantons (linked to WGC)
Membranes
[Lee,Lerche,Weigand’18-19] [Corvilain, Grimm, IV’18]
[Baume,Marchesano,Wiesner’19]
[Lee,Lerche,Weigand’18-19]
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We can identify an infinite tower of BPS states becoming exponentially massless at every infinite field distance point of any Calabi-Yau threefold
Limiting Mixed Hodge Structures and Nilpotent Orbit Theorem: to compute growth of field metric and central charge (mass) of BPS states
Walls of marginal stability: to show stability of the orbit of BPS states generated by the monodromy
transformation
[Grimm, Palti, IV’18]
Evidence in String Theory
(local universal expansion of the periods at infinite distance)
Tools:
[Grimm,Palti,Li’18] [Corvilain, Grimm, IV’18] [Font,Herraez,Ibanez’19] [Grimm,van de Heisteeg’19]Techniques later used in:
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We can identify an infinite tower of BPS states becoming exponentially massless at every infinite field distance point of any Calabi-Yau threefold
Monodromy of infinite orderInfinite distance
Infinite tower of massless BPS
states
Evidence in String Theory
Infinite distance singularity Finite distance
singularity
Infinite tower of massless BPS states
Finite number of massless BPS states
Ti
Tf
q0
..Tq0
Tnq0
stable
unstable..
n ⇠ ed�(P,Q)
n
[Grimm, Palti, IV’18]
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Proposal (Emergent string conjecture):
Types of asymptotic limits
Geometrical classification in terms of the properties of the monodromy transformations
- Decompactfication limit- Weakly coupled string theory limit (tensionless strings)
[Lee,Lerche,Weigand’ 19]
Any infinite distance limit is either:
[Lee,Lerche,Weigand’ 19][Grimm, Palti, IV’18] [Grimm,Palti,Li’18] [Corvilain, Grimm, IV’18] [Li, Grimm, IV’18]
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A lot of recent interest in configurations with both scalar + gauge fields
WGC with scalars: q2 � m2 + (@�m)2
gauge force gravity scalar force
(repulsive force conjecture)
q2 � �(�)m2
(superextremalitycondition)
=when??
If infinite distance limit is a weak coupling limit: SDC = Tower WGC
Gauge + Scalar fields
[Lee,Lerche,Weigand’18] [Heidenrecih,Reece,Rudelius’19][Palti’16]
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Weak GravityConjecture
Non-susy AdS vacua are unstable
Cosmological constant and SM
neutrinos
No dual CFT
Large field inflation
Swampland DistanceConjecture
Cosmological relaxation
No global symmetries
evidence
+
-
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No deSitter
Weak GravityConjecture
Non-susy AdS vacua are unstable
Cosmological constant and SM
neutrinos
No dual CFT
Large field inflation
Swampland DistanceConjecture
Cosmological relaxation
No global symmetries
evidence
+
-
![Page 66: The Swampland program in String Theory...WGC for axions Loophole: “spectator instantons” [Brown et al.’15] [Bachlechner et al’15] Instantons satisfying the WGC are not the](https://reader036.fdocuments.in/reader036/viewer/2022062510/6130d9141ecc515869445bd8/html5/thumbnails/66.jpg)
de Sitter conjecture
deSitter conjecture:
Consistent with known no-go’s for classical vacua in Type IIA
Evidence only based on particular examples…
|rV | � cV with c ⇠ O(1) [Obied,Ooguri,Spodyneik,Vafa’18]
Relation to the Swampland Distance Conjecture:
The infinite tower of states is responsible of
(implying that the deSitter conjecture should be valid at any infinite distance point)
|rV | � cV
[Ooguri,Palti,Shiu,Vafa ’18]
(not only large volume or string weak coupling)
[Hertzberg, Kachru, Taylor, Tegmark ’08]
[Wrase,Junghans,Andriot… ‘19][Wrase, Zagermann ’10] …
[Flauger,Paban,Robbin,Wrase ’09]
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deSitter conjecture: |rV | � cV with c ⇠ O(1) [Obied,Ooguri,Spodyneik,Vafa’18]
Dine-Seiberg problem for every scalar(every direction in field space)
V
�
at any asymptotic limit
(asymptotic)
de Sitter conjecture
We need to go beyond string weak coupling limit to check the conjecture
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Evidence in String Theory
saxions axions� :
kG`4k2sl(2) =
⇣s1
s2
⌘`1�4· · ·
⇣sn�1
sn
⌘`n�1�4(sn)`n�4 k⇢`(G4,�)k21
⇢(G4,�) ⌘ e�iNiG4
s :
VM =1
V34
⇣Z
Y4
G4 ^ ⇤G4 �Z
Y4
G4 ^G4
⌘M-theory on CY4
We can determine the asymptotic structure of flux-induced potential at any asymptotic limit of the complex structure moduli space of CY4
(including strong coupling limits)
via F-theory duality: 4d flux compactifications
integers determined by he the singularity type`i :
Using the same mathematical tools than for the SDC: [Li, Grimm, IV ’19]
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No-go theorem:
V ! 0
There is no dS vacua at parametric control near any two large field limit of a in the strict asymptotic approx if at the large field limitCY4
Evidence in String Theory
The potential satisfies the deSitter conjecture at any infinite distance limit in which an infinite tower of states can be identified
Linked to Distance conjecture
Future task: What about finite distance limits?
[Li, Grimm, IV ’19]
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Weak GravityConjecture
Non-susy AdS vacua are unstable
Cosmological constant and SM
neutrinos
No dual CFT
Large field inflation
Swampland DistanceConjecture
Cosmological relaxation
No global symmetries
No deSitter
evidence
+
-
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Weak GravityConjecture
Non-susy AdS vacua are unstable
Cosmological constant and SM
neutrinos
No dual CFT
Large field inflation
Swampland DistanceConjecture
Cosmological relaxation
No global symmetries
No deSitter
Completeness hypothesis
evidence
+
-
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Weak GravityConjecture
Non-susy AdS vacua are unstable
Cosmological constant and SM
neutrinos
No dual CFT
Large field inflation
Swampland DistanceConjecture
Cosmological relaxation
No global symmetries
No deSitter
Completeness hypothesis
evidence
+
-
No scale separation in AdS
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Why the conjectures should hold true in general?Underlying principle?
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Emergence proposal
The IR kinetic terms of all fields emerge from quantum corrections of integrating out an infinite tower of states
Infinite distance Infinite tower of statesSDC/WGC
Emergence(specific structure)
[Heidenreich,Reece,Rudelius’17-18]
[Grimm, Palti, IV ‘18]
Weak gauge coupling
Drop-off of the cut-off = Species scale
Increasing number of states as we approach the global symmetry limit:
[Harlow, Ooguri, ’18]
[Harlow ’15]
Runaway potential
(i.e. fields are not dynamical in UV, all kinetic terms vanish)
The swampland conjectures emerge from QFT renormalisation
⇤QG =MppN
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Summary
Network of conjectures (different faces of the same principle? )
Phenomenological implications for inflation and particle physics! To be more precise is necessary to clarify the specific definition of the conjectures first.
Significant new evidence in favour of the conjectures in the past years from different research areas.
Interesting relations with Mathematics (Mixed Hodge Structures, Modular forms…)
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The String Swampland and Quantum GravityConstraints on Effective Theories
KITP, Santa BarbaraFeb-Mar 2020
MITP, MainzAgo-Sept 2020
Mathematical Foundations of the Swampland Program
Swampland workshops
ESI, ViennaThe Landscape vs the Swampland
June 2021Thank you!
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back-up slides
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Weak Gravity Conjecture
Swampland Distance Conjecture
Global symmetry restored if
Spectra (“electric version”)
One? (Sub)Lattice? Tower? Infinite tower
Cut-off (“magnetic version”)
g ! 0 �� ! 1
Q
m� 1 gij
@�im@�jm
m2� O(1)(convex hull)
⇤ < gMp⇤ ⇠ Mp exp(����)
� ⇠ O(1) ?
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Weak Gravity Conjecture
Swampland Distance Conjecture
Global symmetry restored if
Spectra (“electric version”)
One? (Sub)Lattice? Tower? Infinite tower
Cut-off (“magnetic version”)
g ! 0 �� ! 1
Q
m� 1 gij
@�im@�jm
m2� O(1)(convex hull)
⇤ < gMp⇤ ⇠ Mp exp(����)
� ⇠ O(1) ?
global symmetry
infinite distance?
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Weak Gravity Conjecture
Swampland Distance Conjecture
Global symmetry restored if
Spectra (“electric version”)
One? (Sub)Lattice? Tower? Infinite tower
Cut-off (“magnetic version”)
g ! 0 �� ! 1
Q
m� 1 gij
@�im@�jm
m2� O(1)(convex hull)
⇤ < gMp⇤ ⇠ Mp exp(����)
� ⇠ O(1) ?Black hole argument missing
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Weak Gravity Conjecture
Swampland Distance Conjecture
Global symmetry restored if
Spectra (“electric version”)
One? (Sub)Lattice? Tower? Infinite tower
Cut-off (“magnetic version”)
g ! 0 �� ! 1
Q
m� 1 gij
@�im@�jm
m2� O(1)(convex hull)
⇤ < gMp⇤ ⇠ Mp exp(����)
� ⇠ O(1) ?
More than one U(1)? More than one scalar field?(different trajectories? mixing with axions?)
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Physics at infinite field distance
Einstein gravity, weak gauge theories, axions, large field ranges, approximate global symmetries…
Why interesting?
…come at a price
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Physics at infinite field distance
Einstein gravity, weak gauge theories, axions, large field ranges, approximate global symmetries…
Why interesting?
…come at a price
Geometrical tool Limiting Mixed Hodge Structure
Growth theorem: gives the leading asymptotic growth of hodge norm w.r.t moduli
(behaviour of field metric, gauge coupling, masses, flux potential…)
Model independent! Only depends on properties of infinite distance singularity
[Schmid,Cattani,Kaplan]
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Asymptotic limits
We can choose local coordinates so that the singularity occurs at:
ti = �i + isi
axion saxion
Ni = log Ti
monodromy transformation
N1 T1
Im(t1) ! 1
(complex codimension-one)singular locus
in the moduli space of a Calabi-Yau manifold
where
N2
N = N1 +N2
Im(t2) ! 1
(complex codimension-one)singular locus
(complex codimension-two)enhanced singularity
t1, t2 ! i1
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[Grimm,Li, IV’19][Grimm,Li, Zimmermann]
Classification of asymptotic limitsin a Calabi-Yau fourfold
Five main types of singularities: I, II, III, IV, Vinfinite distance
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H4p(Y4,R) =
M
`2EV` , ` = (`1, . . . , `n)
Finer splitting of the cohomology group adapted to the singularity type:
Asymptotic flux scalar potential
G4 =X
`2EG`
4Asymptotic flux splitting:
t1 , . . . , tn ! i1Consider the limit:
Given a growth sector we can determine:
,
1
ti = �i + isi
s1 � s2 � · · · � sn � 1
Z
CY4
G`4 ^G`0
4 = 0 unless `+ `0 = 8 ,
The flux splits into pairwise orthogonal components:
integer vector
[Cattani,Kaplan,Schmid]
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Asymptotic flux scalar potential
Asymptotic leading behaviour of hodge norm:
saxions axions
t1 , . . . , tn ! i1Consider the limit:
Given a growth sector
� :
[Cattani,Kaplan,Schmid]
ZG4 ^ ⇤G4 ⇠
X
`2EkG`
4k2sl(2)2
kG`4k2sl(2) =
⇣s1
s2
⌘`1�4· · ·
⇣sn�1
sn
⌘`n�1�4(sn)`n�4 k⇢`(G4,�)k21
we can determine:
, ti = �i + isi
s1 � s2 � · · · � sn � 1
Strict asymptotic approx.: it drops out terms of O(si+1/si)
⇢(G4,�) ⌘ e�iNiG4
s :
Natural interpretation in terms of the potential derived from Minkowski 3-form gauge fields:[Bielleman,Ibanez,IV,Carta,Marchesano,Staessens,Zoccarato,Farakos,Lanza,Martucci,Sorokin,Herraez,Quirant…’15-19]
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Two moduli limits
We compute leading behaviour of the flux induced scalar
potential for the 36 possible asymptotic limits
s, u ! 1
Classification of asymptotic flux-induced scalar potentials!
[Grimm,Li, IV’19]
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Two moduli limits
We compute leading behaviour of the flux induced scalar
potential for the 36 possible asymptotic limits
s, u ! 1
Classification of asymptotic flux-induced scalar potentials!
weak coupling + large volume limit in IIA
s ! 1 (type II): weak coupling
u ! 1 (type IV): large volume
VM
⇠ 1
V3
4
X
p=0,2,4,6
Afp
up�3s+
X
q=0,1,2,3
Ahqs
u3�2q�A
loc
!
[Grimm,Li, IV’19]
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Other results
There are AdS vacua at parametric control if we include:
Geometric origin of universal backreaction when displacing the axions
G4 = G4 +G04
unbounded massless fluxes:
hG4, G4i = 0 , hG4, G04i = 0
kG4k ! 0 s, u ! 1
Only scale separation at weak coupling/LCS point
V (�si,��i) ' �diV (si,�i)
@siV = 0 ! si = � �i + . . . Consistent with Refined SDC[Klaewer,Palti'16][Ooguri-Vafa’06]
as
[DeWolfe,Giryavets,Kachru,Taylor’05]
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Phenomenological implications
Upper bound on the scalar field range that can be described by an effective field theory with finite cut-off
�� . 1
�log
✓Mp
⇤
◆
is related to the properties of the discrete infinite symmetry generating the orbit of states
� =pd order one factor!
Multiple saxions:
Axionic trajectory:
� ", �� #� #, �� "
- One parameter moduli spaces: Nda0 6= 0 , Nd+1a0 = 0( )
�
- Beyond geodesics:
What is � ?
Cosmological relaxation of the EW scale
Large field inflation
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Phenomenological implications
Upper bound on the scalar field range that can be described by an effective field theory with finite cut-off
�� . 1
�log
✓Mp
⇤
◆
is related to the properties of the discrete infinite symmetry generating the orbit of states
� =pd order one factor!
Multiple saxions:
Axionic trajectory:
� ", �� #� #, �� "
- One parameter moduli spaces: Nda0 6= 0 , Nd+1a0 = 0( )
�
- Beyond geodesics:
What is � ?
What type of trajectories are allowed by the asymptotic scalar potential arising at infinite distance?
Cosmological relaxation of the EW scale
Large field inflation