covariant eft of gravity and dark energygies/conf/sift2015/codello.pdf · •the theory of small...
TRANSCRIPT
Alessandro Codello
Covariant EFT of Gravityand Dark Energy
in collaboration with Rajeev K. JainarXiv:1507.06308arXiv:1507.07829
Jena6 Nov 2015
• Covariant EFT of gravity
• LO quantum corrections
• Curvature expansion
• Cosmological effective action
• Effective Friedmann equations
• Early times: Inflation
• Late times: Dark energy
Outline of the talk
• The theory of small fluctuations of the metric
• Planck’s scale is the characteristic scale of gravity
• Classical theory (CT) is successful over many orders of magnitude
EFT of Gravity
gµν → gµν +√16πGhµν = gµν +
1
Mhµν
M ≡ 1√16πG
=MPlanck√
16π
MPlanck =1√G
= 1.2× 1019 GeV
gµν
1
Mhµν
Seff [g] = M2
I1[g] +
1
M2I2[g] +
1
M4I3[g] + ...
I1[g] =
d4x
√gM2c0 − c1R
I2[g] =
d4x
√gc2,1R
2 + c2,2Ric2 + c2,3Riem
2
I3[g] =
d4x
√gc3,1RR+ c3,2RµνRµν + c3,3R
3 + ...
Derivative expansion of the UV action
EFT of Gravity
UV action contains all couplings expressed in terms of the scale M
EFT: saddle point expansion in 1
M2
e−Γ[g] =
1PI
Dhµν e−Seff [g+
1M h]
=
1PI
Dhµν e−M2I1[g+ 1
M h]+ 1M2 I2[g+ 1
M h]+...
Γ[g] = I1[g]
+1
M2
I2[g] +
1
2Tr log I(2)1 [g]
+1
M4
I3[g] +
1
2Tr
I(2)1 [g]
−1I(2)2 [g]
+ 2-loops with I1[g]
+ . . .
Covariant EFT of Gravity
Covariant EFT of Gravity
=Γ
+1
2+
1
M2
+
1
2− 1
12+
1
8+
1
M4
+ . . .
LO
NLO
CT
NNLO
I1
I2
I3
Covariant EFT of Gravity
=Γ
+1
2+
1
M2
+
1
2− 1
12+
1
8+
1
M4
+ . . .
LO
NLO
CT
NNLO
1) the general lagrangian of order is to be used both at tree level and in loop diagrams
2) the general lagrangian of order is to be used at tree level and as an insertion in loop diagrams
3) the renormalization program is carried out order by order
E2
En≥4
The EFT recipe in three lines
I1
I2
I3
Covariant EFT of Gravity
=Γ
+1
2+
1
M2
+
1
2− 1
12+
1
8+
1
M4
+ . . .
LO
NLO
CT
NNLO
LOQG: the only QG we will ever observe!
Even if we have a fundamental theory its is generally difficult to compute phenomenological parameters...
Renormalization
=1
2
1
(4π)2
d4x
√g
Λ4UV − 10Λ2
UV m2 + 5m4 log
Λ2UV
m2
+
−23
3Λ2UV +
13
3m2 log
Λ2UV
m2
R
+
7
20C2 +
1
4R2 +
149
180E − 19
15R
log
Λ2UV
m2
Cutoff regularization
measured+ phenomenological
parameters
Renormalization
=1
2
1
(4π)2
d4x
√g
Λ4UV − 10Λ2
UV m2 + 5m4 log
Λ2UV
m2
+
−23
3Λ2UV +
13
3m2 log
Λ2UV
m2
R
+
7
20C2 +
1
4R2 +
149
180E − 19
15R
log
Λ2UV
m2
Cutoff regularization
Dimensional regularization
logΛ2UV → 1
Λ2UV → 0 Λ4
UV → 0
measured+ phenomenological
parameters
Renormalization
=1
2
1
(4π)2
d4x
√g
Λ4UV − 10Λ2
UV m2 + 5m4 log
Λ2UV
m2
+
−23
3Λ2UV +
13
3m2 log
Λ2UV
m2
R
+
7
20C2 +
1
4R2 +
149
180E − 19
15R
log
Λ2UV
m2
Cutoff regularization
m2 = −2Λ
G runs if there is a mass scale involved alsoin dimensional regularization
measured+ phenomenological
parameters
Dimensional regularization
logΛ2UV → 1
Λ2UV → 0 Λ4
UV → 0
+1
2= − 1
2(4π)d/2
ddx
√g trR γi
−m2
R+ ...
Curvature expansion
The finite physical part of the effective action is covariantly encoded in the structure functionswhich can be computed using the non-local heat kernel expansion
Non-local heat kernel structure functions
Non-local heat kernelA. O. Barvinsky and G. A. Vilkovisky, Nucl. Phys. B 282 (1987) 163I. G. Avramidi, Lect. Notes Phys. M 64 (2000) 1A. Codello and O. Zanusso, J. Math. Phys. 54 (2013) 013513
γi
X
m2
≡ lim
ΛUV →∞
∞
1/Λ2UV
ds
ss−d/2+2 [fi(sX)− fi(0)]e
−sm2
= − 1
2(4π)2
d4x
√g tr
1RµνγRic
−m2
Rµν +
1
120RγR
−m2
R
−1
6RγRU
−m2
U+
1
2UγU
−m2
U+
1
12ΩµνγΩ
−m2
Ωµν
+
1
2
Curvature expansion
γRic(u) =1
40+
1
12u− 1
2
1
0dξ
1
u+ ξ(1− ξ)
2log [1 + u ξ(1− ξ)]
γR(u) = − 23
960− 1
96u+
1
32
1
0dξ
2
u2+
4
u[1 + ξ(1− ξ)]
− 1 + 2ξ(2− ξ)(1− ξ2)log [1 + u ξ(1− ξ)]
γRU (u) =1
12− 1
2
1
0dξ
1
u− 1
2+ ξ(1− ξ)
log [1 + u ξ(1− ξ)]
γU (u) = −1
2
1
0dξ log [1 + u ξ(1− ξ)]
γΩ(u) =1
12− 1
2
1
0dξ
1
u+ ξ(1− ξ)
log [1 + u ξ(1− ξ)]
Explicit form for the structure functions
u ≡ −m2
Curvature expansion
γRic(u) = − u
840+
u2
15120− u3
166320+O(u4)
γR(u) = − u
336+
11u2
30240− 19u3
332640+O(u4)
γRU (u) =u
30− u2
280+
u3
1890+O(u4)
γU (u) = − u
12+
u2
120− u3
840+O(u4)
γΩ(u) = − u
120+
u2
1680− u3
15120+O(u4)
= − 1
2(4π)2
d4x
√g tr
1RµνγRic
−m2
Rµν +
1
120RγR
−m2
R
−1
6RγRU
−m2
U+
1
2UγU
−m2
U+
1
12ΩµνγΩ
−m2
Ωµν
+
1
2
u ≡ −m2
High energy expansion u 1
Curvature expansion
γRic(u) =23
450− 1
60log u+
5
18u− log u
6u+
1
4u2− log u
2u2+O
1
u3
γR(u) =1
1800− 1
120log u− 2
9u+
log u
12u+
1
8u2+
log u
4u2+O
1
u3
γRU (u) = − 5
18+
1
6log u+
1
u− 1
2u2− log u
u2+O
1
u3
γU (u) = 1− 1
2log u− 1
u− log u
u− 1
2u2+
log u
u2+O
1
u3
γΩ(u) =2
9− 1
12log u+
1
2u− log u
2u− 3
4u2− log u
2u2+O
1
u3
= − 1
2(4π)2
d4x
√g tr
1RµνγRic
−m2
Rµν +
1
120RγR
−m2
R
−1
6RγRU
−m2
U+
1
2UγU
−m2
U+
1
12ΩµνγΩ
−m2
Ωµν
+
1
2
Low energy expansion u 1
u ≡ −m2
LO effective action to R2
Γ[g] =1
16πG
d4x√g (2Λ−R) +
1
2λ
d4x√g C
2 +1
ξ
d4x√g R
2
+
d4x√g Cµναβ G
−m2
C
µναβ +
d4x√g RF
−m2
R+O(R3)
G2(u) = − 1
2(4π)2
5γRic(u) + 3γU (u)− 12γΩ(u)
− 4γRic(u)− γU (u) + 4γΩ(u)
F2(u) = − 1
2(4π)2
10
3γRic(u) + 10γR(u) + 6γRU (u) + 4γU (u)− 2γΩ(u)
−8
3γRic(u)− 8γR(u) + 2γRU (u)−
2
3γU (u) +
2
3γΩ(u)
G0(u),F0(u),G1/2(u),F1/2(u),G1(u),F1(u)
Matter contributions:
Graviton contributions:
LO effective action to R2
Γ[g] =1
16πG
d4x√g (2Λ−R) +
1
2λ
d4x√g C
2 +1
ξ
d4x√g R
2
+
d4x√g Cµναβ G
−m2
C
µναβ +
d4x√g RF
−m2
R+O(R3)
0.01 0.1 1 10 100 10000.002
0.001
0.000
0.001
0.002
u
0.01 0.1 1 10 100 10000.04
0.02
0.00
0.02
0.04
u
u ≡ −m2
Adding matter
LO
NLO
CT=Γ
+1
2+
1
M2
+
+
1
2
+ . . .
Integrating out matter
= −1
2
1
(4π)2
n= d2+1
1
m2n−dB2n
1
2
Matter induced effective action:expandable in inverse powers of the (lightest) particle mass
Integrating out matter
= −1
2
1
(4π)21
m2B6 + ...
1
2
As in QED when we integrate out electrons
Integrating out matter
= −1
2
1
(4π)21
m2
d4x
√g
1
336RR+
1
840RµνRµν
+1
1296R3 − 1
1080RRµνR
µν − 4
2835Rν
µRανR
µα
+1
945RµνRαβR
µανβ +1
1080RRµναβR
µναβ +1
7560RµνR
µαβγRναβγ
+17
45360R αβ
µν R γδαβ R µν
γδ − 1
1620Rα β
µ νRµ νγ δR
γ δα β
+ . . .
1
2
1
M4→ 1
m2M2
Changes how cubic terms are suppressed
Corrections to Newton’s potential
iκ
2
Pαβ,γδ
kµkν + (k − q)µ(k − q)ν + qµqν − 3
2ηµνq2
+2qλqσIλσ,αβI
µν,γδ + Iλσ,γδI
µν,αβ − Iλµ,αβI
σν,γδ − Iσν,αβI
λµ,γδ
+qλq
µηαβI
λν,γδ + ηγδI
λν,αβ
+ qλq
νηαβI
λµ,γδ + ηγδI
λµ,αβ
−q2ηαβI
µν,γδ + ηγδI
µν,αβ
− ηµνqλqσ (ηαβIγδ,λσ + ηγδIαβ,λσ)
+2qλ
Iσν,αβIγδ,λσ(k − q)µ + Iσµ,αβIγδ,λσ(k − q)ν
−Iσν,γδIαβ,λσkµ − Iσµ,γδIαβ,λσk
ν
+q2Iσµ,αβI
νγδ,σ + I ν
αβ,σ Iσµ,αδ
+ ηµνqλqσ
Iαβ,λρI
ρσ,γδ + Iγδ,λρI
ρσ,αβ
+
k2 + (k − q)2
Iσµ,αβI
νγδ,σ + Iσν,αβI
µγδ,σ − 1
2ηµνPαβ,γδ
−k2ηγδI
µν,αβ + (k − q)2ηαβI
µν,γδ
=
the truth behind Feynman diagrams...
Corrections to Newton’s interaction
Leading quantum corrections to Newton’s potentialJ.F. Donoghue, Phys. Rev. Lett. 72, 2996 (1994)
V = −GMm
r
1 + 3
G(M +m)
c2r+
41
10π
Gc3r2
+ · · ·
Corrections to Newton’s interaction
GM⊙c2r⊙
∼ 10−6
Gc3r2⊙
∼ 10−88
Leading quantum corrections to Newton’s law are incredibly small!
sun
Corrections to Newton’s interaction
Look for physical situations whereLO corrections are enhanced
Can we ever observequantum gravity effects?
Cosmological effective action
Γ[g] =1
16πG
d4x
√−g (R− 2Λ) + ξ
d4x
√−g R2 +
d4x
√−g RF ()R
ds2 = −dt2 + a2(t)dx2
Cαβγδ = 0
FRW metric
Weyl tensor vanishes
Euclidean to Lorentzian
A predictive framework for cosmology
Phenomenological parameters
Cavendish 1797 (1% off best value!)
G = 6.67428× 10−11m3kg−1s−2
Phenomenological parameters
Supernova Cosmology Project
Λ = 10−47 GeV4
Planck mission
Phenomenological parameters
ξ(k∗) ∼ 109 k∗ ≡ 0.05Mpc−1 ∼ 10−40GeVξ ≡ cR2
Cosmological effective action
Γ[g] =1
16πG
d4x
√−g (R− 2Λ) + ξ
d4x
√−g R2 +
d4x
√−g RF ()R
Cαβγδ = 0
Cosmological effective action
Γ[g] =1
16πG
d4x
√−g (R− 2Λ) + ξ
d4x
√−g R2 +
d4x
√−g RF ()R
F () = α log−m2
+ βm2
−
+ γm2
− log−m2
+ δm4
(−)2
+ ...
α, β, γ, δ
are calculable constants
depending on effective gravitons
and matter content
Cαβγδ = 0
Cosmological effective action
Γ[g] =1
16πG
d4x
√−g (R− 2Λ) + ξ
d4x
√−g R2 +
d4x
√−g RF ()R
Leading logsJ. F. Donoghue and B. K. El-Menoufi, Phys. Rev. D 89, 104062 (2014)
Non-local cosmologyS. Deser and R. P. Woodard, Phys. Rev. Lett. 99, 111301 (2007)
Non-local gravity and dark energyM. Maggiore and M. Mancarella, Phys. Rev. D 90, 023005 (2014).
F () = α log−m2
+ βm2
−
+ γm2
− log−m2
+ δm4
(−)2
+ ...
Cαβγδ = 0
α, β, γ, δ
are calculable constants
depending on effective gravitons
and matter content
Effective non-local cosmologyA. C. and K. J. Jain
Effective Friedmann equations (local)
H2 + 96πξG
2HH + 6H2
H − H2=
1
3Λ+
8πG
3ρ
Gµν +∆Gµν = 8πGTµν
− ξ
16πG∆Gµν = 2
Rµν − 1
4gµνR
R− 2 (∇µ∇ν − gµν)RR2
Modified Einstein’s equations
Local correction (covariant form)
Local correction (FRW form)
Effective Friedmann equations (local)
Pure Starobinsky gravity is exactly solvable
2HH + 6H2H − H
2 = 0
t+ C2 =
dH
C1
√H − 2H2
H =1
2t
H = 0 inflation
radiation
H2 + 96πξG
2HH + 6H2
H − H2=
1
3Λ+
8πG
3ρ
R R2 Λ ρ
Jordan frame Starobinsky gravity
Early times: Inflation
R+R2 = Λ
R+R2 = 0
Early times: Inflation
R+R2 = ργ
Early times: Inflation
R+R2 = ργ + ρm
Early times: Inflation
Effective Friedmann equations (non-local)
H2 − 16πGβm2
1
6U
2 − 2HU − 2H2U
=
8πG
3ρ
U + 3HU = 62H2 + H
1
16πGβm2∆G
R 1−R
µν = −2GµνU + 2gµνR+ 2∇µ∇νU +∇µU∇νU
− 1
2gµν∇αU∇αU
−U = R
Gµν +∆Gµν = 8πGTµν
Modified Einstein’s equations
Non local correction (covariant form)
Non local correction (FRW form)
Effective Friedmann equations (non-local)
H2 − 32πGδm4
2H2
S +HS +1
2HS − 1
6U S
=
8πG
3ρ
U + 3HU = 62H2 + H
S + 3HS = U
1
16πGδm4∆G
R 12 R
µν = − 2GµνS + 2gµνU + 2∇µ∇νS
+ 2∇µU∇νS − gµν∇αU∇αS +1
2gµνU
2
−U = R
−S = U .
Effective Friedmann equations (non-local)
H2 − 32πGδm4
2H2
S +HS +1
2HS − 1
6U S
=
8πG
3ρ
U + 3HU = 62H2 + H
S + 3HS = U
1
16πGδm4∆G
R 12 R
µν = − 2GµνS + 2gµνU + 2∇µ∇νS
+ 2∇µU∇νS − gµν∇αU∇αS +1
2gµνU
2
−U = R
−S = U .
H2 =
8πG
3(ρ+ ρDE )
0.001 0.1 10 1000 1051.0
0.8
0.6
0.4
0.2
0.0
0.2
Τ
w
R1
−R
R1
2R
Λ
matter
radiation
ρtot + 3H(1 + w)ρtot = 0 w = −1− 1
3H
ρtotρtot
Late times: Dark energy
0.001 0.1 10 1000 1051056
1046
1036
1026
1016
106
Τ
Ρ
ρr
ρm
ρde
R+R1
2R = ρr + ρm
Late times: Dark energy
Ωde
Ωm
Ωr
0.001 0.1 10 10000.0
0.2
0.4
0.6
0.8
1.0
Τ
Late times: Dark energy
Conclusions and Outlook
• Consistent cosmological history
• Compute all LO terms
• The role of the Conformal anomaly
• Apply to stars/black holes
• Connection with high energy quantum gravity
• Falsify!
Thank you