Testing Gravity in the Cosmic Web Bridget Falck Institute of - - PowerPoint PPT Presentation

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Testing Gravity in the Cosmic Web Bridget Falck Institute of - - PowerPoint PPT Presentation

Testing Gravity in the Cosmic Web Bridget Falck Institute of Cosmology and Gravitation University of Portsmouth, UK Modifying General Relativity What caused the late-time acceleration? If it is a cosmological constant, it is very small


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Testing Gravity in the Cosmic Web

Bridget Falck

Institute of Cosmology and Gravitation University of Portsmouth, UK

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Modifying General Relativity

π»πœˆπœ‰ = π‘†πœˆπœ‰ βˆ’ 1 2 π‘•πœˆπœ‰π‘† +? = 8πœŒπ»π‘ˆ

πœˆπœ‰ βˆ’Ξ›π‘•πœˆπœ‰?

May 19, 2015 Bridget Falck 2

What caused the late-time acceleration? If it is a cosmological constant, it is very small compared to the scale of gravity: Ξ› β‰ˆ 10βˆ’120π‘π‘žπ‘š

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Change: geometry – β€œmodified gravity”, matter – β€œdark energy”

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Screening the Fifth Force

  • GR well-tested on small scales but not cosmological scales

– Chameleon: in f(R) gravity, make mass of scalar field large in high density environments – Symmetron: change scalar field coupling to matter – Vainshtein: in massive gravity, galileon, and braneworld (DGP) models, derivative self-interactions hide fifth force, depending on dimensionality of the system (see Bloomfield,

Burrage, & Davis 2014)

  • I will look at the cosmic web and environmental

dependence of chameleon and Vainshtein screening

– (BF+ 2014, 1404.2206; BF+ 2015, 1503.06673)

Bridget Falck 3 May 19, 2015

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Simulations

  • Models: nDGP (for Vainshtein), Hu-Sawicki f(R) (for

chameleon), and LCDM

– ECOSMOG (Li et al. 2012, 1110.1379; Li et al. 2013, 1303.0008) – 64 Mpc/h, 2563 particles

  • 3 model parameters: tuned rc in nDGP such that

simulations have same Οƒ8 as f(R) chameleon model

– Allows direct comparison of Vainshtein and chameleon screening

  • Cosmic web of dark matter particles identified with

ORIGAMI (BF+ 2012, 1201.2353)

Bridget Falck 4 May 19, 2015

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The ORIGAMI Cosmic Web

Halos collapse along 3 axes, Filaments 2, Walls 1, and Voids 0 Find the phase-space folds by looking for simulation particles that are out of order along

  • rthogonal axes

(Falck, Neyrinck, & Szalay 2012, 1201.2353)

May 19, 2015 Bridget Falck 5

single- stream multi- stream single- stream

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Halo Filament Wall Void

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Halo Filament Wall Void

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Halo Filament Wall Void

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Bridget Falck 9 May 19, 2015

Vainshtein Screening of Dark Matter Particles

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Bridget Falck 10 May 19, 2015

Vainshtein Screening of Dark Matter Particles

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Bridget Falck 11 May 19, 2015

Vainshtein Screening of Dark Matter Particles

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screened screened unscreened unscreened

Vainshtein Chameleon

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Vainshtein Screening Profile

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Fifth Force / Gravitational Force

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Screening vs. Halo Mass

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Vainshtein Chameleon

Linear (unscreened) Δ𝑁 = 0.2 (red), 0.11 (purple), 0.03 (blue) Linear (unscreened) Δ𝑁 = 0.33

(see also Schmidt 2010, 1003.0409)

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Chameleon Screening Profiles

May 19, 2015 Bridget Falck 15

Fifth Force / Gravitational Force

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Vainshtein Chameleon

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Screening vs. Environmental Density

May 19, 2015 Bridget Falck 17

Vainshtein Chameleon

Linear (unscreened) Δ𝑁 = 0.2 (red), 0.11 (purple), 0.03 (blue) Linear (unscreened) Δ𝑁 = 0.33

(see also Zhao et al. 2011, 1105.0922)

dense env’t. sparse envβ€˜t. dense env’t. sparse env’t.

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What about voids?

But single-stream regions not surrounded on all sides by walls & filaments – single-stream voids percolate

(Falck & Neyrinck 2015, 1410.4751)

May 19, 2015 Bridget Falck 18

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Summary

  • ORIGAMI identifies cosmic web by finding folds in phase space

– (Falck, Neyrinck, & Szalay 2012, 1201.2353)

  • The Vainshtein mechanism depends on cosmic web morphology of

dark matter particles, not mass or environment

– (Falck, Koyama, Zhao, & Li 2014, 1404.2206)

  • The chameleon mechanism depends on mass and environment, not

cosmic web

– (Falck, Koyama, & Zhao 2015, 1503.06673)

  • Single-stream regions (voids) percolate, not surrounded by walls

– (Falck & Neyrinck 2015, 1410.4751)

May 19, 2015 Bridget Falck 19