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The Indra Suite of Cosmological Simulations Bridget Falck (Johns Hopkins University) with Tamás Budavári (JHU), Shaun Cole (Durham), Daniel Crankshaw (JHU), László Dobos (Eötvös), Adrian Jenkins (Durham), Gerard Lemson (MPA), Mark Neyrinck (JHU), Alex Szalay (JHU), and Jie Wang (Durham)

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Page 1: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic

The Indra Suite of Cosmological

Simulations

Bridget Falck (Johns Hopkins University)

with Tamás Budavári (JHU), Shaun Cole (Durham), Daniel Crankshaw (JHU), László Dobos (Eötvös), Adrian Jenkins (Durham), Gerard Lemson (MPA), Mark Neyrinck

(JHU), Alex Szalay (JHU), and Jie Wang (Durham)

Page 2: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic

The Indra Simulations

Precise statistics of large-scale modes

512 different random instances, WMAP7 cosmology

each 1 Gpc/h-sided box

10243 particles per simulation

About 1 PB of data!

All data loaded into a SQL database

Particle data:

All particle positions and velocities for all 64 snapshots of each simulation run

Halo catalogs:

Standard FOF (and others) linked to particles

Fourier modes:

Density grid for 512 time steps of each run

Cosmology on the Beach, 2012 Bridget Falck 4

Page 3: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic

Indra-enabled Science

Covariance of the matter power spectrum

Baryon Acoustic Oscillations in real and redshift space

Cluster and void statistics

Large-scale structure morphology

Galaxy formation and evolution with halo catalogs and merger trees

Mock galaxy catalogs

Logarithmic density variable

Cosmology on the Beach, 2012 Bridget Falck 5

Page 4: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic

Indra-enabled Science

Covariance of the matter power spectrum

Baryon Acoustic Oscillations in real and redshift space

Cluster and void statistics

Large-scale structure morphology

Galaxy formation and evolution with halo catalogs and merger trees

Mock galaxy catalogs

Logarithmic density variable

Cosmology on the Beach, 2012 Bridget Falck 6

Page 5: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic

Logarithmic Power Spectrum

Neyrinck, Szapudi, & Szalay 2009

δ

ln(1+δ)

k (h/Mpc)

http://skysrv.pha.jhu.edu/~neyrinck/sonifylss.html

Page 6: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic

Density-Displacement Relation

• Continuity Equation:

• To linear order:

• Retain some higher-order terms to get logarithmic derivative:

)1ln(log

,0)1(1)1(

v

at

01

v

at

01)1(

)1(

1

v

at

linear

avwith

Falck, Neyrinck, Aragon-Calvo, Lavaux, & Szalay 2012, arXiv:1111.4466

Page 7: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic

Density-Displacement Relation

z= 7, 1.6 h-1Mpc cells:

both linear and log do well

Page 8: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic

z= 3, 1.6 h-1Mpc cells:

both linear and log do well

Density-Displacement Relation

Page 9: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic

Density-Displacement Relation

z= 1, 1.6 h-1Mpc cells:

log does much better

Page 10: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic

Density-Displacement Relation

z= 0, 1.6 h-1Mpc cells:

log does much better

Page 11: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic

Density-Displacement Relation

z= 0, 3.1 h-1Mpc cells:

both improve with larger cells

Page 12: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic

Density-Displacement Relation

z= 0, 6.3 h-1Mpc cells:

both improve with larger cells

Page 13: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic

Mock Catalogs with Indra

Large volume for mock surveys

512 simulations for many many mocks

Spatial indexing in the database

enables very fast on-the-fly light cones

Standard FOF catalog will be loaded (like Millennium DB) but new halo catalogs can be created from particle positions and velocities

Halo catalogs linked to particle tables

Cosmology on the Beach, 2012 Bridget Falck 15

Page 14: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic

ORIGAMI: Delineating Halos using Phase-Space Folds

Bridget Falck

with Mark Neyrinck and Alex Szalay

Johns Hopkins University

Cosmology on the Beach, 2012 16 Bridget Falck

Page 15: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic

The ORIGAMI method

• Halo particles have undergone shell-crossing along 3 orthogonal axes

• Filaments have crossed along 2, walls 1, and voids 0

In this 1D example,

particles flow toward an

initial overdensity at the

origin, eventually creating

a fold in phase-space

Cosmology on the Beach, 2012 17 Bridget Falck

Page 16: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic
Page 17: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic
Page 18: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic
Page 19: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic
Page 20: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic
Page 21: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic
Page 22: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic

Comparison to FOF

Cosmology on the Beach, 2012 24 Bridget Falck

• Mass functions similar; ORIGAMI halos larger

• Size difference due to definition of halo edge

• FOF may miss some collapsed particles (Anderhalden & Diemand 2011)

• (See also Knebe et al. 2011: Halo-Finder Comparison Project)

Page 23: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic

ORIGAMI Summary

• ORIGAMI gives a dynamical, geometric definition of the outer edge of a halo

• Identifies halo, filament, wall, and void particles by detecting shell-crossing

• Halos are larger and more diffuse than FOF halos but with similar total masses

• See our paper: Falck, Neyrinck, & Szalay 2012, arXiv:1201.2353

Cosmology on the Beach, 2012 Bridget Falck 25

Page 24: The Indra Suite of Cosmological Simulationsbccp.berkeley.edu/beach_program/presentations12/Falck.pdf · Indra-enabled Science Covariance of the matter power spectrum Baryon Acoustic

Conclusion

The log-density provides a better match to the divergence of the displacement on nonlinear scales

ORIGAMI identifies structures by detecting folds in phase-space

The Indra ensemble of Gpc/h simulations will produce ~ 1 PB of N-body data – stay tuned!

Cosmology on the Beach, 2012 Bridget Falck 26