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Searching for primordial features from CMB and LSS surveys Bin Hu Lorentz Institute, Leiden University The primordial Universe after Planck, IAP, Paris, Dec. 2014 collab. with A. Achucarro, V. Atal, P. Ortiz, J. Torrado See also J.Torrado Poster [PRD 89 (2014) 103006] [PRD 90 (2014) 023511] [arXiv:1410.4804]
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See also J.Torrado Poster Searching for primordial features from … · 2021. 2. 16. · See also J.Torrado Poster [PRD 89 (2014) 103006] [PRD 90 (2014) 023511] [arXiv:1410.4804]

Mar 15, 2021

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Page 1: See also J.Torrado Poster Searching for primordial features from … · 2021. 2. 16. · See also J.Torrado Poster [PRD 89 (2014) 103006] [PRD 90 (2014) 023511] [arXiv:1410.4804]

Searching for primordial features from CMB and LSS surveys

Bin HuLorentz Institute, Leiden University

The primordial Universe after Planck, IAP, Paris, Dec. 2014

collab. with A. Achucarro, V. Atal, P. Ortiz, J. Torrado

See also J.Torrado Poster

[PRD 89 (2014) 103006] [PRD 90 (2014) 023511]

[arXiv:1410.4804]

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Outline

1. Observational hints of oscillatory features

2. Models with a transient reduction of the speed of sound

3. Search with CMB map

4. Search with LSS survey

5. Conclusion

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Planck-2013: Great success of base-LCDM & single-field slow-roll inflationary model

[Planck-2013: XVI]

[Planck-2013: XXII]

[Planck-2013: XXIV]

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1. Observational hints of oscillatory features

TT spectrum residual from best-fit LCDM model

[Planck-2013: XXII]

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l ∈(500,1200)

Appears in all channels

Spectrum residual from best-fit LCDM model

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2. CMB bispectrum

Observational hints of oscillatory features

The best-fit template to the reconstructed CMB bisp

~ detection3σ

[Planck-2013: XXIV]

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1. A transient reduction of sound speed generically gives primordial oscillatory features.

2. It could produce sizeable and distinguishable features in CMB spectrum, bispectrum and matter spectrum.

3. Planck-2013 and WiggleZ data shows a coincidence in the best-fit mode.

4. The statistical significance is not big enough to claim a detection.

5. Based on our best-fit mode from power spectra, we have a specific prediction on the bispectrum, and we are waiting for Planck-2014(5) test.

Main results

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2. Models with a transient reduction of the speed of sound

Assumption: 1 light & 1 heavy fields

Time

cs2

Two field model:

[C. Cheung et. al. JHEP 0803 (2008) 014] [S. Weinberg Phys.Rev. D77 (2008) 123541] [A. Achucarro et. al. JHEP 1205 (2012) 066]

EFT for inflation:

light adiabatic heavy isocurvature

derivative coupling, e.g. => a turn

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After Integrating out heavy field

effective action for light field: slow roll sound speed

Primordial sprectrum: sub-leading

Primordial bispectrum: leading

Do NOT interrupt slow roll condition!

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Oscillatory features in the transient sound speed reduction models— Power spectrum

keep slow roll condition

[A.Achucarro et. al. PRD 89 (2014) 103006]Gaussian reduction in e-folds

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~ 10% effect

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2. Primordial Bispectrum (leading order)

removing 1k13k2

3 +1

k13k3

3 +1

k23k3

3K = 0.19 K = 0.21

[Miranda et al. Phys.Rev. D86 (2012)], [Park et al. Phys.Rev. D85 (2012)]Step in sound speed:

[Adshead et al. PhysRevD.84.043519], [Bartolo et al. JCAP 1310 (2013) 038]

[Adshead et al. PhysRevD.84.043519], [Nakashima et al. Prog.Theor.Phys. 125 (2011)][Bean et al. JCAP 0803 (2008) 026], [Cannone et al. Phys.Rev. D89 (2014)]

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squeezedl1 = 4,l3 = l 2+4

-2.5

-2

-1.5

-1

-0.5

0

0.5

1

0 100 200 300 400 500 600 700 800 900 1000

l 24 b4,l 2,l 2+4×10

8 [µK3 ]

l2

ISWLlocal (fNL=10)Sound speed model (|B|=0.1, log(-τ0)=5.55, log(β)=7.15)

sin model (fNL=106, kc=0.01, φ=0)

single field slow roll: fNL

local ~ 0.01

preliminary

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equilateral

-15

-10

-5

0

5

10

15

20

25

0 100 200 300 400 500 600 700 800 900 1000

l4b l,l,l×10

3 [µK3 ]

l

local (fNL=1)Sound speed model (|B|=0.1, log(-τ0)=5.55, log(β)=7.15)

sin model (fNL=103, kc=0.01, φ=0)

l1 = l2 = l3

preliminary

Also see Munchmeyer’s & Van Tent’s talks

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Fergusson et al. 1410.5114

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A

B

C

D

3. Search with CMB map—TT spectrum

degeneracy of featured and

vanilla parameters is

negligible

Planck+WP

profile likelihood

Also see Meerburg’s talk

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800

900

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4. Search with LSS survey—WiggleZ

features shows around k~(0.1,0.2)

Search up to k=0.2

10

100

1000

10000

100000

0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5

P(k)

[h-3

Mpc

3 ]

k [h/Mpc]

|B|=0.1, log(-τ0)=5.55, log(β)=7.15

z=0z=0.5z=1z=1.5z=2

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Independent search with different data

Planck+WP WiggleZ

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Planck+WP WiggleZ

Independent search with different data

Two coincident modes including the best-fit mode

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Combine Planck and WiggleZ

get better constrained in Planck+WiggleZ

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Bayesian Evidence

posterior evidenceBeyesian

ratio

Jeffreys’s criterion (1<R<3): Barely worth mentioning!

Evidence:

: Sound speed modelM1M 0 : Base-LCDM model

R>1: data faver M1R<1: data faver M0

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1. A transient reduction of the speed of sound generically gives primordial oscillatory features.

2. It could produce sizeable and distinguishable features in CMB spectrum, bispectrum and matter spectrum.

3. Planck-2013 and WiggleZ data shows a coincidence in the best-fit mode.

4. The statistical significance is not big enough to claim a detection.

5. Based on our best-fit mode from power spectra, we have specific prediction on the bispectrum, and we are waiting for Planck-2014(5) test.

Conclusion-2.5

-2

-1.5

-1

-0.5

0

0.5

1

0 100 200 300 400 500 600 700 800 900 1000

l 24 b4,l 2,l 2+4×10

8 [µK3]

l2

ISWLlocal (fNL=10)Sound speed model (|B|=0.1, log(-τ0)=5.55, log(β)=7.15)

sin model (fNL=106, kc=0.01, φ=0)

-15

-10

-5

0

5

10

15

20

25

0 100 200 300 400 500 600 700 800 900 1000

l4b l,l,l×10

3 [µK3]

l

local (fNL=1)Sound speed model (|B|=0.1, log(-τ0)=5.55, log(β)=7.15)

sin model (fNL=103, kc=0.01, φ=0)

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Thanks for your attention! Merry Xmas to Planck!

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bonus slide

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Log(β ) = 7.2

Two mode with the same frequency but with different location (red) (green)

Log(−τ 0 ) = 5.5Log(β ) = 6.3 Log(β ) = 7.2

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1.9e-09

1.95e-09

2e-09

2.05e-09

2.1e-09

2.15e-09

2.2e-09

2.25e-09

2.3e-09

2.35e-09

2.4e-09

0.01 0.1

Log tau0=5.5, Log beta=6.3Log tau0=5.5, Log beta=7.2

Primordial power spectrum

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0

5e+06

1e+07

1.5e+07

2e+07

2.5e+07

1e-06 1e-05 0.0001 0.001 0.01 0.1 1 10

’./test_cs_transfer_out.dat’ u 1:7

Transfer function

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After convolving with transfer function they looks similar, due to the damping effect on small scale

0

5e-10

1e-09

1.5e-09

2e-09

2.5e-09

0.01 0.1

Log tau0=5.5, Log beta=6.3/before filteringLog tau0=5.5, Log beta=7.2/before filtering

Log tau0=5.5, Log beta=6.3/after filteringLog tau0=5.5, Log beta=7.2/after filtering

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A

B

C

D

3. Search with CMB map—TT spectrum

degeneracy with vanilla

parameter is negligible

Planck+WPprofile likelihood

CoV Mat

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Search with CMB map—Zoom in best-fit

Need to consider look-elsewhere effect!

Enlarge the parameter space

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2. Models with a transient reduction of the speed of sound

integrating out heavy field

Time

cs2

turn

sound speed reduced

A.Achucarro et. al. JHEP 1205 (2012) 066 light adiabatic heavy isocurvature

effective action:

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4. Search with LSS survey—WiggleZ

1

10

100

1000

10000

100000

0.0001 0.001 0.01 0.1 1

P(k)

[h-3

Mpc

3 ]

k [h/Mpc]

|B|=0.1, log(-τ0)=5.55, log(β)=7.15

z=0z=0.5z=1z=1.5z=2

features shows around k~(0.1,0.2)

Search up to k=0.2