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Impact of Dark Matter
and Dark Energy on
Large Scale Structures
Carole-Anne Collins, Ruike Li, Joe Santrock, Rohan Srivastava, Carson West
Introduction to project
● Time evolving a Model Universe to show the impacts of dark energy and dark matter on
the evolution of large scale structures
○ Focussing specifically on the expansion rate of the universe
○ Comparing the Bulk Viscosity theory vs the Cosmological Constant Theory
● Simulation consists of 256³ (~16.7 million) bodies to lower the computational power
needed
● Simulation scale still allows the cosmological principle (>100 Mpc) to apply
○ Findings can be generalized to that of an entire universe
Why our topic is important/why we chose this
topic
● Understanding how large scale structures form
○ Cosmology has a basis in Relativity, which can draw support/proof from
simulations of how these structures form
○ The cause of the expansion of the universe is still largely unknown. Since we can’t
experiment with a universe, simulations are the next best tool
● Models can predict the age and position of astrophysical objects
● A manipulatable model gives the ability to answer “what ifs”
○ Gives a visual representation of how much contribution certain parameters have
on the universe’s motion
Observational Basis
● High-Z Supernova Search Team
○ Observations of Type 1a supernovae prove that these supernovae were moving away from each other, and at an
accelerating rate
○ Gave the first observational data that the universe was expanding
● Wilkinson Microwave Anisotropy Probe
○ Imaged the Cosmic Microwave Background
○ There must be some negative pressure or anti-gravity force in order for clusters we observe today to have
formed
○ Approximately flat universe (~Ω =1.002)
● Planck 2018
○ Measured parameters to greatest accuracy
Initial conditions
● Amplitude of the (linear) Power Spectrum on a scale of 8 h-1 Mpc
○ σ8 = 0.8159 ±0.0060
○ Power Spectrum:
● Scalar value tied to comoving distance and spatial curvature
○ ns= 0.9671±0.0038
● Spatial Curvature
○ κ ≈ 0
● Hubble Constant
○ H0 =
● Hubble Parameter
○ h = 0.6774 ± 0.0046
● Initial simulation size
○ L0 = 100 Mpc
● N-body mesh size
○ 256 x 256 x 256
Numerical Methods
Method Purpose Numerical methods used
ModelUniverse.simulate Simulates N-body system
with cosmological factors
FFT, Gaussian integration,
interpolation, parallel
computing
utils.scale_factor Solves first order ODEs to
find a(t)
ODE, integration, derivative
utils.animation Animates 3D scatter plots,
density plots, and scale
factor plots
Time evolved animations,
matplotlib
Simulated Universes
Theory Universe Parameters
Dark Energy Our Universe (Cosmological
Constant)
Ωr = 8.490*10^5, ΩM = 0.3103, ΩDE = 0.6897, ω = -1, κ = 0
Strong Dark Energy (Phantom
Energy)
Ωr = 8.490*10^5, ΩM = 0.3103 , ΩDE = 0.6897, ω = -1.5, κ = 0
Weak Dark Energy
(Quintessence)
Ωr = 8.490*10^5, ΩM = 0.3103, ΩDE = 0.6897, ω = -0.5, κ = 0
Bulk
Viscosity
Our Universe 𝜁0=4.389, 𝜁1=-2.166
No Big Bang 𝜁0=8.000, 𝜁1=2.000
Constant Pressure 𝜁0=1.000, 𝜁1=0
Logarithmic Expansion Ωr = 8.490*10^5, ΩM = 1 , ΩDE = 0, k= 0
Analytical
Models
Overdense Matter Ωr = 0, ΩM = 2, ΩDE = 0, κ = -1, 𝜁0=0.000, 𝜁1=0.000
de Sitter ΩDE = 1, ω = -1
Theory Universe Parameters
Dark Energy Our Universe (Cosmological
Constant)
Ωr = 8.490*10^-5, ΩM = 0.3103, ΩDE = 0.6897, ω = -1, κ = 0
Strong Dark Energy (Phantom
Energy)
Ωr = 8.490*10^-5, ΩM = 0.3103 , ΩDE = 0.6897, ω = -1.5, κ = 0
Weak Dark Energy
(Quintessence)
Ωr = 8.490*10^-5, ΩM = 0.3103, ΩDE = 0.6897, ω = -0.5, κ = 0
Bulk
Viscosity
Our Universe Ωr = 8.490*10^-5, ΩM = 1, 𝜁0=4.389, 𝜁1=-2.166
No Big Bang Ωr = 8.490*10^-5, ΩM = 1, 𝜁0=8.000, 𝜁1=2.000
Constant Pressure Ωr = 8.490*10^-5, ΩM = 1, 𝜁0=1.000, 𝜁1=0
Logarithmic Expansion Ωr = 8.490*10^5, ΩM = 1, 𝜁0<<0.000 and/or 𝜁1<<0.000
Analytical
Models
Overdense Matter Ωr = 0, ΩM = 2, ΩDE = 0, κ = -1, 𝜁0=0.000, 𝜁1=0.000
de Sitter ΩDE = 1, ωDE = -1
No Scale Factor: N-Body Animation
Math/Theory: Kinematics of Cosmology
● Relativistic, time independent radius:
Newtonian
Relativistic
● Fluid equation is a direct result of a thermodynamic system that is allowed to expand and
contract
● By taking the time derivative, and substituting the fluid equation, the acceleration equation
pops out
A sphere of radius Rs(t), and
mass Ms, expanding or
contracting under its own
gravity.
Rs(t) - Newtonian time
dependent
rs - Newtonian, time
independent
R0 - Relativistic, time
independent
Math/Theory: Kinematics of Cosmology
● Usually, a more useful form of the Friedmann equation is used where it is parameterized using density
parameters known as ‘ingredients’:
● Friedmann equation becomes
● Where index i sums over all ‘ingredients’ and exponent ki is the exponential dependence of that ingredient.
Here we also introduce the Hubble value H(a). It describes the relative expansion of the universe, where H(a0)
= H0
Math/Theory: Bulk
● A bulk viscous matter-dominated Universe
○ No dark energy, or cosmological constant
● Agrees with observations
● Scale factor dependence is known for ‘normal’ matter and
radiation. For BV, we solve fluid equation with pressure derived
from the conservation equation of a viscous fluid
Math/Theory: Bulk
● Solving the systems of equations of the fluid, acceleration, and
Friedmann equation yields a bulk viscosity scale factor dependence
● Using this in the parameterized version of the Friedmann equation
does not have an analytical solution
Math/Theory: Cosmological Constant
● One particularly interesting ingredient is dark energy
○ It explains the expansion we observe that no other ingredient does
● The general from of pressure is
○ Dark energy is a negative pressure ingredient where ⍵DE < 0
● Plugging this into the fluid equation and solving for energy density,
Cosmological Constant theory
● Now that we know the scale factor dependence, we can construct an ODE from the Friedmann
equation:
Simulated Universes Revisited
Theory Universe Parameters
Dark Energy Our Universe (Cosmological
Constant)
Ωr = 8.490*10^-5, ΩM = 0.3103, ΩDE = 0.6897, ω = -1, κ = 0
Strong Dark Energy (Phantom
Energy)
Ωr = 8.490*10^-5, ΩM = 0.3103 , ΩDE = 0.6897, ω = -1.5, κ = 0
Weak Dark Energy
(Quintessence)
Ωr = 8.490*10^-5, ΩM = 0.3103, ΩDE = 0.6897, ω = -0.5, κ = 0
Bulk
Viscosity
Our Universe Ωr = 8.490*10^-5, ΩM = 1, 𝜁0=4.389, 𝜁1=-2.166
No Big Bang Ωr = 8.490*10^-5, ΩM = 1, 𝜁0=8.000, 𝜁1=2.000
Constant Pressure Ωr = 8.490*10^-5, ΩM = 1, 𝜁0=1.000, 𝜁1=0
Logarithmic Expansion Ωr = 8.490*10^5, ΩM = 1, 𝜁0<<0.000 and/or 𝜁1<<0.000
Analytical
Models
Overdense Matter Ωr = 0, ΩM = 2, ΩDE = 0, κ = -1, 𝜁0=0.000, 𝜁1=0.000
de Sitter ΩDE = 1, ωDE = -1
● Scale factor vs time animation
○ 𝜁1 = 0
○ Evolving over the range: -5 < 𝜁0 < 5
● As 𝜁0 increases, the scale factor increases
more rapidly
○ 𝜁0 plays a big role in universes that
are not expanding quickly
● Increasing 𝜁0 increases the age of the
universe
○ Lower left corner of graph
Bulk Viscosity: Scale Factor Plot (𝜁0 )
● Scale factor vs time animation
○ 𝜁0 = -1
○ Evolving over the range: -5 < 𝜁1 < 5
● As 𝜁1 increases, the scale factor increases
more rapidly
○ As ȧ increases, 𝜁1 has a stronger
effect; thereby increasing ȧ even
more
● Increasing 𝜁1 increases the age of the
universe
○ Lower left corner of graph
Bulk Viscosity: Scale Factor Plot (𝜁1)
Method: death_of_universe
● Big Rip: da/dt > c
● Big Crunch da/dt << 0
● Heat/Big Freeze death: No thermodynamic processes can happen
○ Based on density fluctuations
○ Rate of expansion cannot exceed the speed of light, but it needs to be great
enough to break apart gravitationally bound systems
Method: death_of_universe (continued)
● If neither of the two aforementioned criteria are not
satisfied throughout the iteration, we check for a
possible Heat Death at the last time step
○ Calls on average_finder to determine average
spacing between bodies in our universe
■ Calls on simulate function to get
position arrays
○ Calculate expected average for an evenly
spaced universe
○ Compare these two values within a buffer of
2% to determine if the Model Universe is
showing signs of trending to an evenly spaced
universe
Bulk Viscosity: Death of Universe
Universe Theory Numerical
Result
Our Universe Big Rip Big Rip
No Big Bang Big Rip Big Rip
Constant Pressure Expand to infinity Expand to infinity
Logarithmic Expansion Heat/Big Freeze Expand to infinity
Overdense Matter Big Crunch Big Crunch
Overdense Matter (Big Crunch)
Bulk Viscosity: N-Body Animations
No Big Bang
Bulk Viscosity: N-Body and Density Animations
Our Universe Our Universe Heat Map
● Evolving -1.5 < ⍵DE < -0.5
● The smaller ⍵DE the stronger dark energy’s
effect is
● Stronger effects also slow expansion at early
times
Cosmological constant: scale factor plot
Cosmological Constant: Death of Universe
Universe Theory Numerical
Result
Our Universe (Cosmological Constant) Big Rip Big Rip
Strong Dark Energy (Phantom Energy) Big Rip Big Rip
Weak Dark Energy (Quintessence) Expand to infinity Expand to
infinity
de Sitter Big Rip Big Rip
de Sitter
Cosmological Constant: N-Body Animations
Quintessence
Cosmological Constant: N-Body and Density Animations
Our Universe Our Universe Heat Map
Conclusions
● Our code agrees to the theory at small scales (256^3 bodies), so generalizations to the entire universe
should be accurate.
● Similar to how Classical Mechanics models a pendulum, given a set of initial conditions, our code uses
Cosmology to model universes and agrees with other researcher’s results
●
● Youtube with all simulations: https://www.youtube.com/channel/UC55UoPo_8jY-iLoBns5QGPw
● Gitlab repository: https://gitlab.com/phys3266/darksim
Comparison to Millennium Simulation Project
Code Improvement
● ModelUniverse.simulate is not fully parallelized, though ~90% is using Tensorflow
○ Runtime for 256 mesh (~16.7 million bodies) ~4 minutes per time step
○ ~60% of the runtime is only using 1 CPU core (doing operations such as np.copy)
○ RAM usage peaks at 27 GB, with continuous usage at ~17 GB
● 3D animations are bulky
○ ~50 minutes to run
○ RAM usage peaks at ~16-30 GB
● Finish making it a package that is installable using pip (and documentation!)
● Larger Projects (CosmoFlow, ~134 million bodies)
○ More advanced usage of Tensorflow, namely 3D convolutional neural networks to cut down dataset size and calculation
time
○ Their goal was finding σ8, Ωm, and ns using 12,632 simulation boxes of 5123 particles (1.7 trillion total)
References
Aghanim, N. et al. “Cosmological parameters.” Planck Collaboration, vol. VI, no. ms, July 16, 2018, pp. 1-71. Astronomy &
Astrophysics, URL: https://www.cosmos.esa.int/documents/387566/387653/Planck_2018_results_L06.pdf/38659860-
210c-ffac-3921-e5eac3ae4101.
Avelino, Arturo, and Ulises Nucamendi. “Exploring a Matter-Dominated Model with Bulk Viscosity to Drive the Accelerated
Expansion of the Universe.” Journal of Cosmology and Astroparticle Physics, vol. 2010, no. 08, 2010, pp. 009–009.,
doi:10.1088/1475-7516/2010/08/009.
Barbara Sue Ryden.Introduction to cosmology. Cambridge University Press, 2017.
Bolotinet, Yu. L. al. “Cosmology In Terms Of The Deceleration Parameter. Part II.” arXiv, arXiv:1506.08918vl [gr-qc] 30 June 2015.
https://arxiv.org/pdf/1506.08918.pdf
Mathuriya, Amrita et al. “CosmoFlow: Using Deep Learning to Learn the Universe at Scale.” arXiv, Publisher, Publication Date,
arXiv:1808.04728v2 [astro-ph.CO] 9 Nov 2018. https://arxiv.org/pdf/1808.04728.pdf.
S Pfalzner, M B Davies, M Gounelle, A Hohansen, C M ̈unker, P Lacerda, S PortegiesZwart, L Testi, M Trieloff, D Veras, and et al.
The formation of the solar system. Royal Swedish Academy of Sciences, Apr 2015.
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The Dark Side of the Universe

  • 1. Impact of Dark Matter and Dark Energy on Large Scale Structures Carole-Anne Collins, Ruike Li, Joe Santrock, Rohan Srivastava, Carson West
  • 2. Introduction to project ● Time evolving a Model Universe to show the impacts of dark energy and dark matter on the evolution of large scale structures ○ Focussing specifically on the expansion rate of the universe ○ Comparing the Bulk Viscosity theory vs the Cosmological Constant Theory ● Simulation consists of 256³ (~16.7 million) bodies to lower the computational power needed ● Simulation scale still allows the cosmological principle (>100 Mpc) to apply ○ Findings can be generalized to that of an entire universe
  • 3. Why our topic is important/why we chose this topic ● Understanding how large scale structures form ○ Cosmology has a basis in Relativity, which can draw support/proof from simulations of how these structures form ○ The cause of the expansion of the universe is still largely unknown. Since we can’t experiment with a universe, simulations are the next best tool ● Models can predict the age and position of astrophysical objects ● A manipulatable model gives the ability to answer “what ifs” ○ Gives a visual representation of how much contribution certain parameters have on the universe’s motion
  • 4. Observational Basis ● High-Z Supernova Search Team ○ Observations of Type 1a supernovae prove that these supernovae were moving away from each other, and at an accelerating rate ○ Gave the first observational data that the universe was expanding ● Wilkinson Microwave Anisotropy Probe ○ Imaged the Cosmic Microwave Background ○ There must be some negative pressure or anti-gravity force in order for clusters we observe today to have formed ○ Approximately flat universe (~Ω =1.002) ● Planck 2018 ○ Measured parameters to greatest accuracy
  • 5. Initial conditions ● Amplitude of the (linear) Power Spectrum on a scale of 8 h-1 Mpc ○ σ8 = 0.8159 ±0.0060 ○ Power Spectrum: ● Scalar value tied to comoving distance and spatial curvature ○ ns= 0.9671±0.0038 ● Spatial Curvature ○ κ ≈ 0 ● Hubble Constant ○ H0 = ● Hubble Parameter ○ h = 0.6774 ± 0.0046 ● Initial simulation size ○ L0 = 100 Mpc ● N-body mesh size ○ 256 x 256 x 256
  • 6. Numerical Methods Method Purpose Numerical methods used ModelUniverse.simulate Simulates N-body system with cosmological factors FFT, Gaussian integration, interpolation, parallel computing utils.scale_factor Solves first order ODEs to find a(t) ODE, integration, derivative utils.animation Animates 3D scatter plots, density plots, and scale factor plots Time evolved animations, matplotlib
  • 7. Simulated Universes Theory Universe Parameters Dark Energy Our Universe (Cosmological Constant) Ωr = 8.490*10^5, ΩM = 0.3103, ΩDE = 0.6897, ω = -1, κ = 0 Strong Dark Energy (Phantom Energy) Ωr = 8.490*10^5, ΩM = 0.3103 , ΩDE = 0.6897, ω = -1.5, κ = 0 Weak Dark Energy (Quintessence) Ωr = 8.490*10^5, ΩM = 0.3103, ΩDE = 0.6897, ω = -0.5, κ = 0 Bulk Viscosity Our Universe 𝜁0=4.389, 𝜁1=-2.166 No Big Bang 𝜁0=8.000, 𝜁1=2.000 Constant Pressure 𝜁0=1.000, 𝜁1=0 Logarithmic Expansion Ωr = 8.490*10^5, ΩM = 1 , ΩDE = 0, k= 0 Analytical Models Overdense Matter Ωr = 0, ΩM = 2, ΩDE = 0, κ = -1, 𝜁0=0.000, 𝜁1=0.000 de Sitter ΩDE = 1, ω = -1 Theory Universe Parameters Dark Energy Our Universe (Cosmological Constant) Ωr = 8.490*10^-5, ΩM = 0.3103, ΩDE = 0.6897, ω = -1, κ = 0 Strong Dark Energy (Phantom Energy) Ωr = 8.490*10^-5, ΩM = 0.3103 , ΩDE = 0.6897, ω = -1.5, κ = 0 Weak Dark Energy (Quintessence) Ωr = 8.490*10^-5, ΩM = 0.3103, ΩDE = 0.6897, ω = -0.5, κ = 0 Bulk Viscosity Our Universe Ωr = 8.490*10^-5, ΩM = 1, 𝜁0=4.389, 𝜁1=-2.166 No Big Bang Ωr = 8.490*10^-5, ΩM = 1, 𝜁0=8.000, 𝜁1=2.000 Constant Pressure Ωr = 8.490*10^-5, ΩM = 1, 𝜁0=1.000, 𝜁1=0 Logarithmic Expansion Ωr = 8.490*10^5, ΩM = 1, 𝜁0<<0.000 and/or 𝜁1<<0.000 Analytical Models Overdense Matter Ωr = 0, ΩM = 2, ΩDE = 0, κ = -1, 𝜁0=0.000, 𝜁1=0.000 de Sitter ΩDE = 1, ωDE = -1
  • 8. No Scale Factor: N-Body Animation
  • 9. Math/Theory: Kinematics of Cosmology ● Relativistic, time independent radius: Newtonian Relativistic ● Fluid equation is a direct result of a thermodynamic system that is allowed to expand and contract ● By taking the time derivative, and substituting the fluid equation, the acceleration equation pops out A sphere of radius Rs(t), and mass Ms, expanding or contracting under its own gravity. Rs(t) - Newtonian time dependent rs - Newtonian, time independent R0 - Relativistic, time independent
  • 10. Math/Theory: Kinematics of Cosmology ● Usually, a more useful form of the Friedmann equation is used where it is parameterized using density parameters known as ‘ingredients’: ● Friedmann equation becomes ● Where index i sums over all ‘ingredients’ and exponent ki is the exponential dependence of that ingredient. Here we also introduce the Hubble value H(a). It describes the relative expansion of the universe, where H(a0) = H0
  • 11. Math/Theory: Bulk ● A bulk viscous matter-dominated Universe ○ No dark energy, or cosmological constant ● Agrees with observations ● Scale factor dependence is known for ‘normal’ matter and radiation. For BV, we solve fluid equation with pressure derived from the conservation equation of a viscous fluid
  • 12. Math/Theory: Bulk ● Solving the systems of equations of the fluid, acceleration, and Friedmann equation yields a bulk viscosity scale factor dependence ● Using this in the parameterized version of the Friedmann equation does not have an analytical solution
  • 13. Math/Theory: Cosmological Constant ● One particularly interesting ingredient is dark energy ○ It explains the expansion we observe that no other ingredient does ● The general from of pressure is ○ Dark energy is a negative pressure ingredient where ⍵DE < 0 ● Plugging this into the fluid equation and solving for energy density,
  • 14. Cosmological Constant theory ● Now that we know the scale factor dependence, we can construct an ODE from the Friedmann equation:
  • 15. Simulated Universes Revisited Theory Universe Parameters Dark Energy Our Universe (Cosmological Constant) Ωr = 8.490*10^-5, ΩM = 0.3103, ΩDE = 0.6897, ω = -1, κ = 0 Strong Dark Energy (Phantom Energy) Ωr = 8.490*10^-5, ΩM = 0.3103 , ΩDE = 0.6897, ω = -1.5, κ = 0 Weak Dark Energy (Quintessence) Ωr = 8.490*10^-5, ΩM = 0.3103, ΩDE = 0.6897, ω = -0.5, κ = 0 Bulk Viscosity Our Universe Ωr = 8.490*10^-5, ΩM = 1, 𝜁0=4.389, 𝜁1=-2.166 No Big Bang Ωr = 8.490*10^-5, ΩM = 1, 𝜁0=8.000, 𝜁1=2.000 Constant Pressure Ωr = 8.490*10^-5, ΩM = 1, 𝜁0=1.000, 𝜁1=0 Logarithmic Expansion Ωr = 8.490*10^5, ΩM = 1, 𝜁0<<0.000 and/or 𝜁1<<0.000 Analytical Models Overdense Matter Ωr = 0, ΩM = 2, ΩDE = 0, κ = -1, 𝜁0=0.000, 𝜁1=0.000 de Sitter ΩDE = 1, ωDE = -1
  • 16. ● Scale factor vs time animation ○ 𝜁1 = 0 ○ Evolving over the range: -5 < 𝜁0 < 5 ● As 𝜁0 increases, the scale factor increases more rapidly ○ 𝜁0 plays a big role in universes that are not expanding quickly ● Increasing 𝜁0 increases the age of the universe ○ Lower left corner of graph Bulk Viscosity: Scale Factor Plot (𝜁0 )
  • 17. ● Scale factor vs time animation ○ 𝜁0 = -1 ○ Evolving over the range: -5 < 𝜁1 < 5 ● As 𝜁1 increases, the scale factor increases more rapidly ○ As ȧ increases, 𝜁1 has a stronger effect; thereby increasing ȧ even more ● Increasing 𝜁1 increases the age of the universe ○ Lower left corner of graph Bulk Viscosity: Scale Factor Plot (𝜁1)
  • 18. Method: death_of_universe ● Big Rip: da/dt > c ● Big Crunch da/dt << 0 ● Heat/Big Freeze death: No thermodynamic processes can happen ○ Based on density fluctuations ○ Rate of expansion cannot exceed the speed of light, but it needs to be great enough to break apart gravitationally bound systems
  • 19. Method: death_of_universe (continued) ● If neither of the two aforementioned criteria are not satisfied throughout the iteration, we check for a possible Heat Death at the last time step ○ Calls on average_finder to determine average spacing between bodies in our universe ■ Calls on simulate function to get position arrays ○ Calculate expected average for an evenly spaced universe ○ Compare these two values within a buffer of 2% to determine if the Model Universe is showing signs of trending to an evenly spaced universe
  • 20. Bulk Viscosity: Death of Universe Universe Theory Numerical Result Our Universe Big Rip Big Rip No Big Bang Big Rip Big Rip Constant Pressure Expand to infinity Expand to infinity Logarithmic Expansion Heat/Big Freeze Expand to infinity Overdense Matter Big Crunch Big Crunch
  • 21. Overdense Matter (Big Crunch) Bulk Viscosity: N-Body Animations No Big Bang
  • 22. Bulk Viscosity: N-Body and Density Animations Our Universe Our Universe Heat Map
  • 23. ● Evolving -1.5 < ⍵DE < -0.5 ● The smaller ⍵DE the stronger dark energy’s effect is ● Stronger effects also slow expansion at early times Cosmological constant: scale factor plot
  • 24. Cosmological Constant: Death of Universe Universe Theory Numerical Result Our Universe (Cosmological Constant) Big Rip Big Rip Strong Dark Energy (Phantom Energy) Big Rip Big Rip Weak Dark Energy (Quintessence) Expand to infinity Expand to infinity de Sitter Big Rip Big Rip
  • 25. de Sitter Cosmological Constant: N-Body Animations Quintessence
  • 26. Cosmological Constant: N-Body and Density Animations Our Universe Our Universe Heat Map
  • 27. Conclusions ● Our code agrees to the theory at small scales (256^3 bodies), so generalizations to the entire universe should be accurate. ● Similar to how Classical Mechanics models a pendulum, given a set of initial conditions, our code uses Cosmology to model universes and agrees with other researcher’s results ● ● Youtube with all simulations: https://www.youtube.com/channel/UC55UoPo_8jY-iLoBns5QGPw ● Gitlab repository: https://gitlab.com/phys3266/darksim
  • 28. Comparison to Millennium Simulation Project
  • 29. Code Improvement ● ModelUniverse.simulate is not fully parallelized, though ~90% is using Tensorflow ○ Runtime for 256 mesh (~16.7 million bodies) ~4 minutes per time step ○ ~60% of the runtime is only using 1 CPU core (doing operations such as np.copy) ○ RAM usage peaks at 27 GB, with continuous usage at ~17 GB ● 3D animations are bulky ○ ~50 minutes to run ○ RAM usage peaks at ~16-30 GB ● Finish making it a package that is installable using pip (and documentation!) ● Larger Projects (CosmoFlow, ~134 million bodies) ○ More advanced usage of Tensorflow, namely 3D convolutional neural networks to cut down dataset size and calculation time ○ Their goal was finding σ8, Ωm, and ns using 12,632 simulation boxes of 5123 particles (1.7 trillion total)
  • 30. References Aghanim, N. et al. “Cosmological parameters.” Planck Collaboration, vol. VI, no. ms, July 16, 2018, pp. 1-71. Astronomy & Astrophysics, URL: https://www.cosmos.esa.int/documents/387566/387653/Planck_2018_results_L06.pdf/38659860- 210c-ffac-3921-e5eac3ae4101. Avelino, Arturo, and Ulises Nucamendi. “Exploring a Matter-Dominated Model with Bulk Viscosity to Drive the Accelerated Expansion of the Universe.” Journal of Cosmology and Astroparticle Physics, vol. 2010, no. 08, 2010, pp. 009–009., doi:10.1088/1475-7516/2010/08/009. Barbara Sue Ryden.Introduction to cosmology. Cambridge University Press, 2017. Bolotinet, Yu. L. al. “Cosmology In Terms Of The Deceleration Parameter. Part II.” arXiv, arXiv:1506.08918vl [gr-qc] 30 June 2015. https://arxiv.org/pdf/1506.08918.pdf Mathuriya, Amrita et al. “CosmoFlow: Using Deep Learning to Learn the Universe at Scale.” arXiv, Publisher, Publication Date, arXiv:1808.04728v2 [astro-ph.CO] 9 Nov 2018. https://arxiv.org/pdf/1808.04728.pdf. S Pfalzner, M B Davies, M Gounelle, A Hohansen, C M ̈unker, P Lacerda, S PortegiesZwart, L Testi, M Trieloff, D Veras, and et al. The formation of the solar system. Royal Swedish Academy of Sciences, Apr 2015.

Editor's Notes

  1. Presenter: Joe
  2. Presenter: Joe It helps us understand how large scale structures are formed. It also draws support and proof of how large scale structures are formed as cosmology has a basis in relativity. Tools like this can help explain why the universe acts this way since its expansion is still largely unknown It can also help us find the age and position of astrophysical objects as well as answer some what ifs we might have by showing the contribution of each parameter on the universe’s motion
  3. Presenter: Joe To explore this idea further, we can start by looking at observational data. In 1998, the High-Z Supernova Search Team and Supernova Cosmology Project indepen- dently found that the universe was expanding at an accelerating rate. They observed the relative movement of Type 1a supernovas by their brightness and found that they were not only moving away, but at an accelerating rate [1]. Another observation came from the Wilkinson Microwave Anisotropy Probe (WMAP) make key discoveries and con- firmed some existing ideas about our universe that dictate how it will end. Among other discoveries, they imaged the Cosmic Microwave Background (CMB) and saw that for large structures such as galaxy clusters there must be an negative pressure or anti-gravity force to have the current clusters we see today. They also observed the universe to be approximately flat [2, 3]. Flat universe means parallel lines remain parallel, 90deg is 90deg Explain what k is. K < 0 closed, k>0, open, k~1 flat universe Omega is sum of a set density parameters that describe the universe we will cover later
  4. Presenter: Carol-Anne Explain what each variable is/means. See: https://www.cosmos.esa.int/documents/387566/387653/Planck_2018_results_L06.pdf/38659860-210c-ffac-3921-e5eac3ae4101 Power spectrum: using the power spectrum you can see cosmic microwave background Using it bc it applies permutations to position and velocity Ns: has to do with when you take a slice of a comoving distance, we didn’t look too deep into this bc we just passed this to our model Kappa: universe is flat, it is an approximation we are making Hubble constant is the speed in km/s of a galaxy 1 parsec away. The hubble parameter sets the overall scale of the observed universe region.
  5. Presenter: Carol-Anne Why use the numerical methods for each computational method? Utils creates scale factor arrays Fast fourier transform Utils animation was used to show nbody expansion in our animations of the different simulated universes
  6. Presenter: Carole-Anne N-body scatter : 4 (dark energy our universe, einstein de sitter, bulk viscosity our universe, No scale factor) Heatmap: ~3 (No scale factor, dark energy our universe, (possibly bulk viscosity our universe) Explain what each parameter is
  7. Presenter: Carol-Anne
  8. Presenter: Carson
  9. Presenter: Carson Crit density: Density where universe expands forever, but asymptotically slows
  10. Presenter: Carson
  11. Presenter: Carson
  12. Presenter: Carson
  13. Presenter: Ruike
  14. Presenter: Carole-Anne N-body scatter : 4 (dark energy our universe, einstein de sitter, bulk viscosity our universe, No scale factor) Heatmap: ~3 (No scale factor, dark energy our universe, (possibly bulk viscosity our universe) Explain what each parameter is
  15. Presenter: Rohan Discuss how values of zeta0, zeta1 change the evolution of scale factor. What the most accurate values are. Explain full plot (dotted line is \Omega_m = 1), etc. Evolve over the range of zeta0 on left side Talk about how cyan line is a de sitter universe Weak dependencies of zeta0 (-5 to ~0) gives the result of little to no expansion. The expansion we do see is due to the “regular matter” and radiation. At zeta0 ~ 0, the universe takes the form of a regular omega_m = 0.3 and omega_r = 8.490e-5 (this has an analytical form we checked against)
  16. Presenter: Rohan Discuss how values of zeta0, zeta1 change the evolution of scale factor. What the most accurate values are. Explain full plot (dotted line is \Omega_m = 1), etc. Evolve over the range of zeta0 on left side
  17. Presenter: Rohan Takes in a time and scale factor array Scale factor array consists of the scale factor of our model universe at each time step present in the time array Iterates over the arrays to find each successive change in the scale factor with respect to time in order to compare this value with certain criteria that we have determined to lead to a respective death of a universe Exceeds speed of light: Big Rip Drops below a specified negative buffer: Big Crunch
  18. Presenter: Rohan Based on how the scale factor evolves with time we can do some calculations to find what the death of the universe will be Takes in a time and scale factor array Scale factor array consists of the scale factor of our model universe at each time step present in the time array Iterates over the arrays to find each successive change in the scale factor with respect to time in order to compare this value with certain criteria that we have determined to lead to a respective death of a universe
  19. Presenter: Rohan Insert scatter plot and heat map of universe with best fit values of zeta0 and zeta1
  20. Presenter: Rohan Insert scatter plot and heat map of universe with best fit values of zeta0 and zeta1
  21. Presenter: Ruike
  22. Presenter: Ruike
  23. Presenter: Rohan Insert scatter plot and heat map of universe with best fit values of zeta0 and zeta1
  24. Presenter: Rohan Insert scatter plot and heat map of universe with best fit values of zeta0 and zeta1
  25. Presenter: Carson
  26. Presenter: Carson
  27. Presenter: Carson
  28. Presenter: Carson