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Constraining the Ultra-Large Scale Structure ofthe Universe
Jonathan Braden
University College London
ICG Portsmouth, May 25, 2016
w/ Hiranya Peiris, Matthew Johnson and Anthony Aguirre
based on arXiv:1604.04001 and in progress
Inhomogeneous Nonlinear Ultra-Large Scale Cosmology
... A Mosaic of Interesting Dynamics
I Strongly inhomogeneous and nonlinear cosmologicalinitial conditions (this talk) [JB, Peiris, Johnson, Aguirre]
I Isocurvature mode conversion into intermittent densityperturbations [JB, Bond, Frolov, Huang]
I Caustic formation in chaotic long wavelength dynamicsI Generalised form of local nonGaussianity
I First order phase transitions [JB, Bond, Mersini-Houghton]
I Entropy production in highly inhomogeneous nonlinear fieldtheories [JB, Bond]
Spatially intermittent dynamics, fundamental issues in QFT, noveland poorly constrained observables
Numerical Approach is Essential [JB, in preparation]
Hybrid MPI/OpenMP Lattice Code
I Solve field equation (e.g.)
φi + 3a
aφi −
∇2φia2
+ V ′(~φ) = 0
I 10th order Gauss-Legendreintegration (general) or 8th orderYoshida (nonlinear sigma models)
I Finite-difference (fully parallel) orPseudospectral (OpenMP)
I Optional absorbing boundaries
I Quantum fluctuations →realization of random field
I Energy conservationO(10−9 − 10−14)
Numerical Approach is Essential [JB, in preparation]
Hybrid MPI/OpenMP Lattice Code
I Solve field equation (e.g.)
φi + 3a
aφi −
∇2φia2
+ V ′(~φ) = 0
I 10th order Gauss-Legendreintegration (general) or 8th orderYoshida (nonlinear sigma models)
I Finite-difference (fully parallel) orPseudospectral (OpenMP)
I Optional absorbing boundaries
I Quantum fluctuations →realization of random field
I Energy conservationO(10−9 − 10−14)
Dawn of Numerical Relativity in Cosmology
I Bentivegna, Bruni
I Mertens, Giblin, Starkman
I Kleban, Linde, Senatore, West
I Peiris, Johnson, Feeney, Aguirre, Wainwright (symmetryreduced bubbles)
I Adamek, Daverio, Durrer, Kunz (weak field subhorizon)
Connection of Initial Conditions with Observables
I Requires Monte Carlo sampling of Initial Conditions
I Highly accurate integrators to achieve machine precision
Dawn of Numerical Relativity in Cosmology
I Bentivegna, Bruni
I Mertens, Giblin, Starkman
I Kleban, Linde, Senatore, West
I Peiris, Johnson, Feeney, Aguirre, Wainwright (symmetryreduced bubbles)
I Adamek, Daverio, Durrer, Kunz (weak field subhorizon)
Connection of Initial Conditions with Observables
I Requires Monte Carlo sampling of Initial Conditions
I Highly accurate integrators to achieve machine precision
Outline
I Brief Review of Cosmology and Role of Inflation
I Inflationary Models and Initial Conditions
I Choice of Initial Conditions
I Planar Symmetric Dynamics
I Projection of Dynamics into Observations (CMB quadrupole)
I Semi-analytic Approximation (work in progress)
History of the Universe
Model Choices
V (φ) = V0
(1− e
−√
23α
φMP
)2
I α� 1→ small-field model
I α = 1→ Starobinski
I α� 1→ m2φ2/2
Model Choices
V (φ) = V0
(1− e
−√
23α
φMP
)2
0 1 2 3 4 5 6
φ/MP
0.0
0.2
0.4
0.6
0.8
1.0
1.2
V(φ
)
×10−11
α = 0.1
I α� 1→ small-field model
I α = 1→ Starobinski
I α� 1→ m2φ2/2
Model Choices
V (φ) = V0
(1− e
−√
23α
φMP
)2
0 2 4 6 8 10 12
φ/MP
0.0
0.2
0.4
0.6
0.8
1.0
V(φ
)
×10−10
α = 1.0
I α� 1→ small-field model
I α = 1→ Starobinski
I α� 1→ m2φ2/2
Model Choices
V (φ) = V0
(1− e
−√
23α
φMP
)2
0 5 10 15 20 25 30
φ/MP
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
4.0
V(φ
)
×10−9
α = 100.0
I α� 1→ small-field model
I α = 1→ Starobinski
I α� 1→ m2φ2/2
Model Choices
V (φ) = V0
(1− e
−√
23α
φMP
)2
0 5 10 15 20 25 30 35
φ/MP
0.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
V(φ
)
×10−8
α = 100000.0
I α� 1→ small-field model
I α = 1→ Starobinski
I α� 1→ m2φ2/2
CMB Parameter Predictions
10−5 10−3 10−1 101 103 105 107 109
α
−0.050
−0.045
−0.040
−0.035
−0.030
−0.025
ns−
1
∆ ln a60
50
40
35 40 45 50 55 60
∆ ln a
−0.060
−0.055
−0.050
−0.045
−0.040
−0.035
−0.030
−0.025
ns−
1
α0.01
1.0
100.0
10000.0
1000000.0
10−510−410−310−210−1100 101 102 103 104 105 106 107
α
10−810−710−610−510−410−310−210−1100101102103104105
r
∆ ln a = 60
∆ ln a = 50
∆ ln a = 40
35 40 45 50 55 60
∆ ln a
10−5
10−4
10−3
10−2
10−1
100
r
α = 0.01
α = 0.1
α = 1.0
α = 100.0
α = 10000.0
Ultra-Large Scale Structure
Local Remnants of Ultra-Large Scale Structure?
I Structure present at start of inflation
I Conversion of structure during or after inflation
Ultra-Large Scale Structure
Local Remnants of Ultra-Large Scale Structure?
I Structure present at start of inflation
I Conversion of structure during or after inflation
Ultra-Large Scale Structure
Local Remnants of Ultra-Large Scale Structure?
I Structure present at start of inflation
I Conversion of structure during or after inflation
Dimensional Reduction: Planar Symmetry
Synchronous Gauge
ds2 = −dτ2 + a2‖(x , τ)dx2 + a2
⊥(x , τ)(dy2 + dz2)
Residual gauge freedom : a‖(x , τ = 0), a⊥(x , τ = 0)
Isotropised Expansion
a ≡ det(γij)1/6 =
(a‖a
2⊥)1/3
H ≡ −1
3γ ijKij = −1
3(K x
x + 2K yy )
Initial Conditions: Field
Work in Spatially Flat Gauge a‖(τ = 0) = 1 = a⊥(τ = 0)
φ(x) = φ+ δφ
φ gives desired N e-folds of inflation in homogeneous limit3H2
I ≡ V (φ)
Field Fluctuations
δφ(xi ) = Aφ∑
n=1
G e iknxi√P(kn) G =
√−2 ln βe2πiα
P(k) = Θ(kmax − k) H−1I kmax = 2π
√3
Initial Conditions: Field
Work in Spatially Flat Gauge a‖(τ = 0) = 1 = a⊥(τ = 0)
φ(x) = φ+ δφ
φ gives desired N e-folds of inflation in homogeneous limit3H2
I ≡ V (φ)
Field Fluctuations
δφ(xi ) = Aφ∑
n=1
G e iknxi√P(kn) G =
√−2 ln βe2πiα
P(k) = Θ(kmax − k) H−1I kmax = 2π
√3
Initial Conditions: Metric
Work in Spatially Flat Gauge a‖(τ = 0) = 1 = a⊥(τ = 0)
Momentum Constraint Sews Neighbouring Grid Sites Together
0 = P = K yy′ − a′⊥
a⊥(K x
x − K yy )− φ′Πφ
2a‖M2P
Hamiltonian Constraint Enforces Energy Conservation
0 = H =2a⊥a
′‖a′⊥ − a‖a
′2⊥ − 2a‖a⊥a
′′⊥
a3‖a
2⊥
+ 2K xxK
yy + K y
y2
−M−2P
(φ′2 + Π2
φ
2a2‖
+ V
)= 0
Distribution of Initial Conditions
0 50 100 150 200
HIx/√
3
0.934
0.936
0.938
0.940
0.942
0.944
0.946
φ/M
P
0 50 100 150 200
HIx/√
3
−6
−5
−4
−3
−2
Kxx
×10−5 − 5.7728×10−1
0 50 100 150 200
HIx/√
3
−0.61
−0.60
−0.59
−0.58
−0.57
−0.56
−0.55
−0.54
Kyy
What’s the response in the curvature perturbation?
Time Evolution
a‖ = −a‖K xx , ˙a⊥ = −a⊥K y
y ,
˙K xx =
a′2⊥a2⊥a
2‖
+ K xx
2 − K yy
2 +
(Π2φ − φ′2
)
2a2‖M
2P
,
˙K yy = − a′2⊥
2a2⊥a
2‖
+3
2K y
y2 − V (φ)
2M2P
+
(Π2φ + φ′2
)
4a2‖M
2P
,
Πφ = 2K yyΠφ +
1
a‖φ′′ +
(2a′⊥a‖a⊥
−a′‖
a2⊥
)φ′ − a⊥∂φV (φ),
φ =Πφ
a‖
Numerical Approach
Machine precision accuracy
I Gauss-Legendre time-integrator (O(dt10), symplectic)
I Fourier pseudospectral discretisation (exponentialconvergence)
Fast to allow sampling
I Adaptive time-stepping
I Adaptive grid spacing
O(1− 10)s to evolve through 60 e-folds of inflation
Convergence Testing : Dynamical Variables
Vary grid spacing dx at fixed dx/dt
0 50 100 150 200 250
HIτ/√
3
10−16
10−15
10−14
10−13
10−12
10−11
‖Hdx−Hdx/2‖
0 50 100 150 200 250
HIτ/√
3
10−16
10−15
10−14
10−13
10−12
10−11
‖ln
(a) dx−
ln(a
) dx/2‖
Vary time-step dt at fixed dx
0 50 100 150 200 250
HIτ/√
3
10−1610−1510−1410−1310−1210−1110−1010−910−810−710−610−510−4
‖Hdx−Hdx/2‖
0 50 100 150 200 250
HIτ/√
3
10−1510−1410−1310−1210−1110−1010−910−810−710−610−510−410−310−2
‖ln
(a) dx−
ln(a
) dx/2‖
Convergence Testing : Constraint Preservation
Vary grid spacing dx at fixed dx/dt
0 50 100 150 200 250
HIτ/√
3
10−16
10−15
10−14
10−13
10−12
10−11
10−10
10−9
‖H‖
0 50 100 150 200 250
HIτ/√
3
10−1410−1310−1210−1110−1010−910−810−710−610−510−410−310−210−1
100
‖P‖
Vary time-step dt at fixed dx
0 50 100 150 200 250
HIτ/√
3
10−1610−1510−1410−1310−1210−1110−1010−910−810−710−610−510−410−3
‖H‖
0 50 100 150 200 250
HIτ/√
3
10−1510−1410−1310−1210−1110−1010−910−810−710−610−510−410−310−210−1
100‖P‖
Self-Gravitating Dynamics: Isotropisation of Expansion
0 10 20 30 40 50 60 70
ln a
−0.5
0.0
0.5
1.0
1.5
2.0Kxx/Kyy−
1×10−5
Expansion quickly isotropises itself
Self-Gravitating Dynamics: Attractor Behaviour
−0.2 0.0 0.2 0.4 0.6 0.8 1.0
φ
−1.5
−1.0
−0.5
0.0
0.5
1.0
1.5
φ
Self-Gravitating Dynamics: Geometry Attractor
−0.1 0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7
H
−0.5
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5ε H
Individual Lattice Sites Evolve Along AttractorFixed H, εH are equivalent
Self-Gravitating Dynamics: Spatially Dependent ExpansionHistory
0 10 20 30 40 50 60 7016 ln det(g)
0.0
0.1
0.2
0.3
0.4
0.5
0.6
−1 3K
i i
Observations: Relation to Local Multipoles
ζ(H) ≡ δ ln a|Ha‖=1=a⊥
Large-scale perturbations →evaluate ζ on last-scattering surface around a point x0
Expand for Large-Scale Fluctuations
ζ(x0+rls) ≈ ζ(x0)+(HI rls)∂ζ
∂(HI xp)(x0)+
(HI rls)2
2
∂2ζ
∂(HI xp)2(x0)+. . .
Matches onto Multipoles
a(UL)20 ≈ F (LobsHI)
2∂2xpζ ' F (LobsHI)
2 1
a‖∂x
[∂xζ
a‖
]
Required Evolution
0 50 100 150 200
HIx/√
3
−0.06
−0.04
−0.02
0.00
0.02
0.04
0.06
lna
0 50 100 150 200
HIx/√
3
0.934
0.936
0.938
0.940
0.942
0.944
0.946
φ/M
P
0 50 100 150 200
HIx/√
3
0.000000
0.000002
0.000004
0.000006
0.000008
0.000010
0.000012
0.000014
H
+5.773×10−1
Initial Conditions (τ = 0)
Required Evolution
0 50 100 150 200
HIx
59.560.060.561.061.562.062.563.063.564.0
lna
0 50 100 150 200
HIx/√
3
0.112
0.114
0.116
0.118
0.120
0.122
0.124
0.126
φ/M
P
0 50 100 150 200
HIx/√
3
0.375
0.380
0.385
0.390
0.395
0.400
0.405
0.410
0.415
0.420
H
End of Inflation (εH = −d lnH/d ln a = 1)
Freeze-in of Superhorizon Perturbations
0 100 200 300 400 500 600
H0x/√
3
2.0
1.5
1.0
0.5
0.0
0.5
1.0
1.5
2.0δζ
H/HI
0. 98
0. 95
0. 75
0. 50
0. 05
Initial transient modifies result from separate universeapproximation
Weighting of Observers
Distribution of Superhorizon a20
−2 −1 0 1 2
a(UL)20 /σ(UL)
0
1
2
3
4P( a
(UL
)20
/σ
(UL
)|Aφ,...)
α = 2300
Aφ
1× 10−5
3× 10−5
6× 10−5
Statistical Framework
Pr(Aφ, Lobs|C obs2 ) ∝ L(Aφ, Lobs, . . . )Pr(Aφ, Lobs, . . . )
L(Aφ, Lobs) = Pr(C obs2 |Aφ, Lobs, . . . )
Planck high-` “theory” and low-` “observed”
C obs2 = 253.6µK2 C theory
2 = 1124.1µK2
Distribution of CMB quadrupole
C2 =1
5
(a
(UL)20 + a
(Q)20
)2+
2∑
m=−2, m 6=0
(a
(Q)2m
)2
0 1500 3000 4500
C2 [µK2]
0.0
0.2
0.4
0.6
0.8
P( C
2|A
φ,
σ(UL)
σ(Q
),.
..)
×10−3
σ(UL)
σ(Q) = 4
Aφ
1 × 10−5
3 × 10−5
6 × 10−5
χ2dof=5
Relative RMS of superhorizon contribution depends of distance tolast-scattering surface
a(UL)20 ≈ F (LobsHI)
2∂2xpζ ' F (LobsHI)
2 1
a‖∂x
[∂xζ
a‖
]
Constraints from the CMB Quadrupole
−5 −4 −3 −2 −1 0
log10(HILobs)
−6
−5
−4
−3lo
g10(A
φ)
α = 2300
0
2
4
6
8
P(log
10A
φ,l
og10H
ILobs|C
obs
2)×10−4
Strong Modification from Gaussian Ansatz at Large Aφ
Marginalised Constraints
−6.0 −5.5 −5.0 −4.5 −4.0 −3.5 −3.0
log10(Aφ)
0.00
0.02
0.04
0.06
0.08
0.10P( lo
g10(A
φ)|C
obs
2
)
α = 2300
Numerical GR
Gaussian
Constraint of Aφ as we marginalise over Lobs
Marginalised Constraints
−5 −4 −3 −2 −1 0
log10(HILobs)
0.000
0.002
0.004
0.006
0.008
0.010
0.012
0.014
0.016
0.018P( lo
g10(H
ILobs)|C
obs
2
)
α = 2300
Numerical GR
Gaussian
Constraint of Lobs as we marginalise over Aφ
Heuristic Picture of Large Amplitude Effects
Heuristic Picture of Large Amplitude Effects
Modelling With Toy Distributions
Model behaviour with Johnson distribution
Removing Inhomogeneous Expansion
−4 −3 −2 −1 0 1 2 3 4
a2‖a20/
√〈a4‖a
220〉
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8P( (a
2 ‖a20/√〈a
4 ‖a2 20〉)
Statistics of ζ
ζ and comoving derivatives nearly Gaussian
−4 −3 −2 −1 0 1 2 3 4
ζ/σζ
0.00
0.05
0.10
0.15
0.20
0.25
0.30
0.35
0.40
P(ζ/σζ)
−4 −3 −2 −1 0 1 2 3 4
ζ ′′/σζ′′
0.00
0.05
0.10
0.15
0.20
0.25
0.30
0.35
0.40
0.45
P(ζ′′ /σζ′′)
40 50 60 70 80 90
ζ
40
50
60
70
80
90
ζ ‖
−0.006−0.005−0.004−0.003−0.002−0.0010.000 0.001
ζ − ζ‖
0
500
1000
1500
2000
2500
3000
3500
4000
P(ζ−ζ ‖
)Aφ = 10−3
Analytical Modelling
ζ(H, xcom) ∼ GRF
Large-Scale Approximation for a20
a20(x0) ≈ Ae−2ζ‖(x0)(ζ ′′(x0)− ζ ′‖(x0)ζ ′(x0)
)
ζ, ζ ′, ζ ′′ are correlated Gaussian random deviates, with covariance
Cζ =
σ20 0 −σ2
1
0 σ21 0
−σ21 0 σ2
2
σi =∫dkk2i
⟨∣∣∣ζk∣∣∣2⟩
Analytical Modelling
ζ(H, xcom) ∼ GRF
Large-Scale Approximation for a20
a20(x0) ≈ Ae−2ζ(x0)(ζ ′′(x0)− ζ ′(x0)2
)
ζ, ζ ′, ζ ′′ are correlated Gaussian random deviates, with covariance
Cζ =
σ20 0 −σ2
1
0 σ21 0
−σ21 0 σ2
2
σi =∫dkk2i
⟨∣∣∣ζk∣∣∣2⟩
Anaytic a20 Distributions
−1.5 −1.0 −0.5 0.0 0.5 1.0 1.5
a20/σζ
0.0
0.5
1.0
1.5
2.0
2.5
3.0P
(a20/σζ)
Vary σζ at fixed σζ(p)/σζ
Anaytic a20 Distributions
−1.5 −1.0 −0.5 0.0 0.5 1.0 1.5
a20/σζ
0.0
0.5
1.0
1.5
2.0P
(a20/σζ)
Vary σζ′/σζ at fixed σζ and σζ′′/σζ
Future Steps
I Three-dimensional simulations (in progress)
I Multi-field models (additional isocurvature modes,non-attractor, etc.)
I Inclusion of stochastic effects from subhorizon fluctuations(technical challenge)
I Correlated anomalies
Conclusions
I Fully relativistic treatment of highly inhomogeneous initialconditions for inflation
I Constraints obtained from CMB quadrupole based on fullBayesian analysis
I Gravitational nonlinearities extremely important indetermining final distributions of observables
I Very large amplitude initial inhomogeneities more poorlyconstrained than intermediate amplitudes
I Comoving curvature perturbation ζ approximately GRF inappropriate coordinate system