Inflation, geometry and stochasticity
Sébastien Renaux-PetelCNRS - Institut d’Astrophysique de Paris
IHP Trimestre Analytics, Inference, and Computation in Cosmology: Advanced methods
18th September 2018
Based on Pinol, RP, Tada, 1806.10126, and in preparation
1. Introduction
2. Geometrical destabilization of inflation
3. Ito vs Stratonovich in single-field slow-roll inflation
4. Multifield inflation, and ‘derivation’
5. Stochastic diffusion in curved field space
Outline
Renaux-Petel, IAP
Planck all sky map
l(l+1)C
l/2�
[µK
2]
Quantum fluctuations stretched to
cosmological scales
QFT and GR!
Cosmological inflation provides seeds of CMB anisotropies and LSS
Renaux-Petel, IAP
- conceptually not satisfactory
background + fluctuations
Classical Quantum
�
��V (�)
�
- breaks down for very light scalar fields
Stochastic formalism
Conventional formulation
Renaux-Petel, IAP
time
physical scale
H�1
�k =a
kBackground
super-Hubble modes
Classical stochastic effective theory for
coarse-grained fields
d�
dN= �V 0(�)
3H2+
H
2⇡⇠
Continuous flow of initially sub-Hubble (UV) modes joining the super-Hubble (IR) sector
Open quantum system
normalized Gaussian white noise
Stochastic formalism
⇠
IR modes
Renaux-Petel, IAP
Starobinsky, 86
cf C. Burgess’s talk
- reproduce non-trivial results from QFT in curved spacetime
- recover conventional perturbation theory in suitable classical limit
Success
Open questions
- EFT: delineate regime of validity
- non-Gaussianity of noise, non-white, non-Markovian, phase-space analysis,
curved field-space and covariance
- Eternal inflation and multiverse- Primordial Black Holes production Scope
- Geometrical destabilization of inflation
Stochastic formalism
Starobinsky, Woodard et al
Vennin, Starobinsky
1. Introduction
2. Geometrical destabilization of inflation
3. Ito vs Stratonovich in single-field slow-roll inflation
4. Multifield inflation, and ‘derivation’
5. Stochastic diffusion in curved field space
Outline
Renaux-Petel, IAP
Realistic inflationary models have fields which live in an internal space with curved geometry.
This effect applies during inflation, it easily overcomes the effect of the potential, and can destabilize inflationary trajectories.
Initially neighboring geodesics tend to fall away from each other in the presence of negative curvature.
Geometrical destabilization of inflation
V (�1,�2)
�1
�2
Basic mechanism
Effective single-field dynamics
Light inflaton+
Extra heavy fields
Simplest ‘realistic’ models (hope):
(valley with steep walls)
RP, Turzynski, 1510.01281, PRL Editors’ Highlight
Renaux-Petel, IAP
V (�1,�2)
�1
�2
More realistic:
Geometrical instability
Light inflaton+
Extra heavy fields+
Curved field space
Basic mechanism
m2e↵ � ✏H2RM2
Pl
RP, Turzynski, 1510.01281, PRL Editors’ Highlight
Like eta-problem but no symmetry to help
L = �1
2(@�)2
✓1 + 2
�2
M2
◆� V (�)� 1
2(@�)2 � 1
2m2
h�2
Single-field slow-roll
Sidetracked inflation
m2e↵ = m2
h � 4✏H2M2Pl
M2
Fate of the instability?
Toy-model:
Backreaction of fluctuations on effective background?
?
Renaux-Petel, IAP
- Universal bound on curvature scale
- Modified ranking of inflationary models
Second phase of inflation: sidetracked inflationPremature end of inflation
Inhomogeneities dominate
Fate of the instability?
Inhomogeneities are shut off
RP, Turzynski, Vennin 1706.01835
RP, Turzynski, 1510.01281 Garcia-Saenz, RP, Ronayne, 1804.11279
OR
- Rich phenomenology
- EFT with imaginary sound speed
Garcia-Saenz, RP 1805.12563
Renaux-Petel, IAP
1. Introduction
2. Geometrical destabilization of inflation
3. Ito vs Stratonovich in single-field slow-roll inflation
4. Multifield inflation, and ‘derivation’
5. Stochastic diffusion in curved field space
Outline
Renaux-Petel, IAP
Stochastic calculus
NiN
BrownianW(N) ∆Wi : Gaussian (0, ∆N2)
h⇠(N)⇠(N 0)i = �(N �N 0)
N�i � [Ni, Ni+1]
Langevin equation:
Continuous limit of discrete process:
X’s properties depend on choice of
dX
dN= h(X) + g(X) ⇠
�Xi = h(X(N⇤i ))�Ni + g (X(N⇤
i ))�Wi
N⇤i
Renaux-Petel, IAP
Ito StratonovichN⇤
i = Ni N⇤i =
1
2(Ni +Ni+1)
dX = h dN + g dW dX = h dN + g � dW
df(X) = fXdX +1
2fXXg2dN df(X) = fXdX
Ito’s lemma: standard chain rule
Stochastic calculus
Renaux-Petel, IAP
Ito StratonovichN⇤
i = Ni N⇤i =
1
2(Ni +Ni+1)
dX = h dN + g dW dX = h dN + g � dW
df(X) = fXdX +1
2fXXg2dN df(X) = fXdX
Ito’s lemma: standard chain rule
Stochastic calculus
P (X,N): pdf of X at time NFokker-Planck equation for
drift diffusion
@P
@N= LFP · P = � @
@X(D(X)P ) +
1
2
@2
@X2
�g2(X)P
�
Renaux-Petel, IAP
Ito StratonovichN⇤
i = Ni N⇤i =
1
2(Ni +Ni+1)
dX = h dN + g dW dX = h dN + g � dW
df(X) = fXdX +1
2fXXg2dN df(X) = fXdX
Ito’s lemma: standard chain rule
Stochastic calculus
P (X,N): pdf of X at time NFokker-Planck equation for
@P
@N= LFP · P = � @
@X(D(X)P ) +
1
2
@2
@X2
�g2(X)P
�
DI = h DS = h+1
2g@g
@Xnoise-induced
drift
Ito ‘to respect causality’
• Stratonovich: white noises are idealizations of colored noises
• Discrepancy exceeds the accuracy of stochastic formalism
Ito versus Stratonovich for inflation
• Many papers: (not good reason)
Vilenkin 1999, Fujita, Kawasaki, Tada 2014, Tokuda & Tanaka 2017, …
Mezhlumian & Starobinsky 1994UV
UVIR
Mezhlumian & Starobinsky 1994
Vennin & Starobinsky 2015
smooth splitting between UV and IR modes
• Us: new perpective with requirement of covariance Renaux-Petel, IAP
3H2(�)M2Pl = V (�)
Single-field slow-roll
d�
dN= �V 0(�)
3H2+
H
2⇡⇠
Test scalar fields (e.g. in de Sitter)H(�) unambiguous
Inflaton:Ito versus Stratonovich ambiguity
of multiplicative noises
number of e-folds of inflation realized starting from �
stochastic quantity, directly related to observable curvature perturbation
⇣ = �N = N � hN i
N (�) :
cf. V. Vennin’s talk
Renaux-Petel, IAP
L†FP(�)�N (!,�) = �i! �N (!,�)
1
M2Pl
L†FP,I = v
@2
@�2� v0
v
@
@�
1
M2Pl
L†FP,S = v
@2
@�2� v0
v
⇣1� v
2
⌘ @
@�
v ⌘ V
24⇡2M4Pl
�N (!,�) ⌘ hei!N (�)i
In regime of validity of stochastic inflation v ⌧ 1
No difference between Ito and Stratonovich, in classical or stochastic regimes
All information in characteristic function
Single-field slow-roll
versus
v2v′�′�v′�2
> 1
Strato
Ito
sad
cl
10-8 10-5 0.01 1010-9
10-5
0.1
1000.0
107
φ
�ζ
Strato
Ito
sad
cl
10-8 10-5 0.01 100
1000
2000
3000
4000
5000
φ
⟨N⟩
V = Λ4 (1 − φ2
μ2 ), Λ = 10−2MPl, μ = 20MPl
No Ito-Stratonovich difference even in highly stochastic case
Single-field slow-roll: example
v2v′�′�v′�2
> 1
Renaux-Petel, IAP
1. Introduction
2. Geometrical destabilization of inflation
3. Ito vs Stratonovich in single-field slow-roll inflation
4. Multifield inflation, and ‘derivation’
5. Stochastic diffusion in curved field space
Outline
Renaux-Petel, IAP
Multivariate calculus
dXa
dN= ha(X) + ga↵(X) ⇠↵
h⇠↵(N)⇠�(N 0)i = �↵��(N �N 0)
Langevin equations
Renaux-Petel, IAP
Multivariate calculus
dXa
dN= ha(X) + ga↵(X) ⇠↵
h⇠↵(N)⇠�(N 0)i = �↵��(N �N 0)
DaI = ha
DaS = ha +
1
2gb↵
@ga↵@Xb
drift vectordiffusion matrixDab = ga↵g
b↵
Langevin equations
Fokker-Planck equation
@P
@N= LFP(X
a) · P
with LFP(Xa) = � @
@XaDa +
1
2
@2
@Xa@XbDab
Renaux-Petel, IAP
L = �1
2GIJ@µ�
I@µ�J � V
d�I
dN= � GIJV,J
3H2(�I)+ ⌅I
h⌅I(N)⌅J(N 0)i =✓H
2⇡
◆2
GIJ �(N �N 0)
⌅I = gI↵ ⇠↵ gI↵ =H
2⇡eI↵
Multifield generalization?
Not yet stochastic differential equations
and set of vielbeins eI↵eJ↵ = GIJ
with noise correlations
with
Renaux-Petel, IAP
Slow-roll, overdamped limit
Arbitrary choice of vielbeins:
no impact on Ito FP equation
matters for Stratonovich!
ga↵ ! ⌦ �↵ (X)ga�
• Vielbeins can a priori differ by arbitrary field-dependent rotations
Multifield generalization
Renaux-Petel, IAP
Arbitrary choice of vielbeins:
no impact on Ito FP equation
matters for Stratonovich!
• Field space covariance
Physical quantities should not depend on field redefinitions
ga↵ ! ⌦ �↵ (X)ga�
• Vielbeins can a priori differ by arbitrary field-dependent rotations
Covariance is respected only in Stratonovich interpretation!
(Ito lemma vs standard chain rule)
Multifield generalization
Renaux-Petel, IAP
Ps(�I) =
P (�I)pdet(GIJ)
should be a scalar under field redefinitions
Multifield generalization
Renaux-Petel, IAP
Ps(�I) =
P (�I)pdet(GIJ)
@Ps
@N= rI
✓V ,I
3H2Ps
◆+
1
2rI
✓H
2⇡rI
✓H
2⇡Ps
◆◆
+1
2rI
✓H
2⇡
◆2
eI↵(rJeJ↵)Ps
!
should be a scalar under field redefinitions
Multifield generalization
Stratonovich: manifestly covariant FP equation
Renaux-Petel, IAP
Ps(�I) =
P (�I)pdet(GIJ)
@Ps
@N= rI
✓V ,I
3H2Ps
◆+
1
2rI
✓H
2⇡rI
✓H
2⇡Ps
◆◆
+1
2rI
✓H
2⇡
◆2
eI↵(rJeJ↵)Ps
!
should be a scalar under field redefinitions
Stratonovich: manifestly covariant FP equation
covariant derivatives
Multifield generalization
Renaux-Petel, IAP
Ps(�I) =
P (�I)pdet(GIJ)
@Ps
@N= rI
✓V ,I
3H2Ps
◆+
1
2rI
✓H
2⇡rI
✓H
2⇡Ps
◆◆
+1
2rI
✓H
2⇡
◆2
eI↵(rJeJ↵)Ps
!
should be a scalar under field redefinitions
covariant derivatives Spurious dependence on
the arbitrary choice of vielbeins, in curved or flat field space
Multifield generalization
but…
Stratonovich: manifestly covariant FP equation
Renaux-Petel, IAP
Ps(�I) =
P (�I)pdet(GIJ)
@Ps
@N= rI
✓V ,I
3H2Ps
◆+
1
2rI
✓H
2⇡rI
✓H
2⇡Ps
◆◆
+1
2rI
✓H
2⇡
◆2
eI↵(rJeJ↵)Ps
!
should be a scalar under field redefinitions
New light on single-field slow-roll: field redefinition innocuous
only in Stratonovich
Multifield generalization
Stratonovich: manifestly covariant FP equation
Renaux-Petel, IAP
• More rigorous approach:
• Heuristic approach:
�IR �UV+� =
classical equations of motion + time-dependence of coarse graining scale
Schwinger-Keldysh formalism (time-dependence) + Gaussian action for UV modes + phase space (effective Hamiltonian action)
integrate out UV modes at level of action
Derivation?
• Splitting
Renaux-Petel, IAP
W
DN⇡I = ⇡0I � �K
IJ�J0⇡K
3H2M2Pl = V (�I) +
1
2GIJ⇡I⇡J
First principles
Hamiltonian constraint
�I0 =GIJ⇡J
H+ ⇠IQ
DN⇡I = �3⇡I �VI
H+ ⇠P I
Langevin type equations in phase space
Correlation matrix of noises: power spectra of UV modes in IR background
Renaux-Petel, IAP
DN⇡I = ⇡0I � �K
IJ�J0⇡K
3H2M2Pl = V (�I) +
1
2GIJ⇡I⇡J
Correlation matrix of noises: power spectra of UV modes in IR background
First principles
Hamiltonian constraint
�I0 =GIJ⇡J
H+ ⇠IQ
DN⇡I = �3⇡I �VI
H+ ⇠P I
Langevin type equations in phase space
Complex!Non-Markovian
(noise depends on its past history)
Non-Gaussian and non-white noises (smooth splitting between UV and IR modes)
Renaux-Petel, IAP
Covariance
Even under simplifying assumptions of Markovian, Gaussian white noises, issue of covariance
Phase-space pdf should be proper scalarP (�I ,⇡I , N)
Need to introduce arbitrary `square-roots' of the correlation matrix of the noises (gIQ↵, gP I↵)
covariance, but spurious ‘frame’ dependence
drops out but not covariant
Ito Stratonovich
Renaux-Petel, IAP
Stratonovich covariant Fokker-Planck equation:
@P
@N= �⇡I
HD�IP +
✓V,I
H+ 3⇡I
◆@⇡IP + 3nP
First line: neat Boltzmann-like reformulation
of deterministic evolution
Covariance
+1
2
�D�I
⇥gIQ↵·
⇤+ @⇡I [gP I↵·]
� �D�J (gJQ↵P ) + @⇡J (gP I↵P )
�
D�I = r�I + �KIJ⇡K@⇡J
phase-space covariant derivative
Second line: ’frame’ dependence…
Renaux-Petel, IAP
1. Introduction
2. Geometrical destabilization of inflation
3. Ito vs Stratonovich in single-field slow-roll inflation
4. Multifield inflation, and ‘derivation’
5. Stochastic diffusion in curved field space
Outline
Renaux-Petel, IAP
Stochastic diffusion in curved field space
Assuming inflationary stochastic anomaly is an artefact
And for test fields in dS space (simplicity)
@Ps
@N=
1
3H20
rI
�V ,IPs
�+
1
2
✓H0
2⇡
◆2
rIrIPs
Covariant equation for diffusion of light scalar fields in curved field space in overdamped limit.
Simplest multifield covariantization: no curvature invariants for effectively light fields
(like adding suitable noise-induced drift)
Renaux-Petel, IAP
(@�)2 + e2b(�)(@ )2
h�ni0 = � n
3H20
h�n�1V,�i
+1
2
✓H0
2⇡
◆2 ⇥n(n� 1)h�n�2i+ nh�n�1b,�i
⇤.
For sum-separable potentials, only depends on �
Stochastic diffusion in curved field space
Field space geometry
Easily solvable for polynomial V and b
Renaux-Petel, IAP
Case study: phi4 in hyperbolic geometry
Z2 symmetry of potential broken by geometry
b(�) = ��/MV (�) = ��4/4 R = �2/M2
Renaux-Petel, IAP
Case study: phi4 in hyperbolic geometry
h�(N)i = � H20N
8⇡2M
1� �N2
12⇡2� �H2
0N3
768⇡4M2+ . . .
�
h�2(N)i = H20N
4⇡2
1 +
H20N
16⇡2M2� �N2
6⇡2� 7�H2
0N3
384⇡4M2+ . . .
�
Starting from �(�)
Double expansion in �
⇡2N2 H2
0
⇡2M2Nand
Z2 symmetry of potential broken by geometry
Benchmark for QFT computations
b(�) = ��/MV (�) = ��4/4 R = �2/M2
Renaux-Petel, IAP
h�ni0 = � n
3H20
h�n�1V,�i
+1
2
✓H0
2⇡
◆2 ⇥n(n� 1)h�n�2i+ nh�n�1b,�i
⇤.
Resummation at late times?
Case study: phi4 in hyperbolic geometry
Renaux-Petel, IAP
Ve↵(�) = V (�)� 3H40/(8⇡
2) b(�)
Peq / e�8⇡2/(3H40 )Veff (�)
h�ni0 = � n
3H20
h�n�1V,�i
+1
2
✓H0
2⇡
◆2 ⇥n(n� 1)h�n�2i+ nh�n�1b,�i
⇤.
Resummation at late times?
Mapping to single-field model with effective potential:
Case study: phi4 in hyperbolic geometry
e.g.Renaux-Petel, IAP
Conclusion
• New light on Ito vs Stratonovich dilemma with criterion of general covariance
• Manifestly covariant in Stratonovich only, at expense of frame-dependences: inflationary stochastic anomaly
• Single-field slow-roll: no practical difference, but Stratonovich is unambiguous
• Ambiguity in full phase space, or w. multiple fields
• Stochastic diffusion in curved field space: mapping to single-field models and benchmark model
Renaux-Petel, IAP
Open questions
• Fate of instability in geometrical destabilization of inflation, and general implications for inflation
• Scrutinize foundations of stochastic inflation: non-Gaussianity of noise, non-white, non-Markovian, phase-space analysis, curved field-space, covariance
• Inflationary stochastic anomaly: stochastic counterparts of notoriously difficult problem of maintaining general covariance in quantum theories
Renaux-Petel, IAP
Postdoc opportunity next Fall: ERC group at IAP
Thank you for your attention
Renaux-Petel, IAP