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The Consequences of a Dynamical Dark Energy Density on the Evolution of the Universe. By Christopher Limbach, Alexander Luce, and Amanda Stiteler. Background image: Andrey Kravtsov., University of Chicago, 2003. Presentation Overview. Image by Martin Altmann, Observatory Hoher List, 1997.
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The Consequences of a Dynamical Dark Energy Density on the Evolution of the Universe By Christopher Limbach, Alexander Luce, and Amanda Stiteler Background image: Andrey Kravtsov., University of Chicago, 2003.
Presentation Overview Image by Martin Altmann, Observatory Hoher List, 1997. • Amanda Stiteler • Introduction • Theory • Chris Limbach • Assumptions • Verification of Methods • Alex Luce • Results • Conclusion
Einstein’s Cosmological Model Rij = Ricci tensor R = curvature scalar gij= space-time metric tensor G = Newton’s gravitational constant Tij = stress-energy tensor Λ = cosmological constant
The Friedmann Equation a = dimensionless scale factor ρR = relativistic matter density ρM = non-relativistic matter density ρΛ = dark energy density k = curvature of the universe c = speed of light l0 = present distance between two galaxies
Quintessence • Equation relating the scalar field, , and its potential, : • Energy density of the scalar field: • Evolution of the scalar field:
Free Parameters and • Parameters which characterize potential • Chosen such that V(φ) mimics nearly constant Λ at present
Purpose of this Project • Compare the evolution of a universe with constant dark energy density to one with variable dark energy density • Determine restrictions of the constants κ and α Image by NASA., 2006.
Assumptions • Homogeneous, Isotropic Universe • (from WMAP) • Total Density = Critical Density • Initial Conditions for ΩR, ΩM, ΩΛfrom WMAP • No Spatial Curvature
Method • 4th Order Runge-Kutta • Equations Solved:
Numeric Solutions “Time of Big Bang” 0.01 Scale Factor a 1 t 0 Time Relative to Present [Gyrs]
h = 0.01 h= 0.02 h = 0.005 Solution error δh Verification Scale Factor a 1 h= time step t Time From Present [Gyrs]
Simulation Results Constant Dark Energy vs. Time Dependent Dark Energy? Restrictions on Free Parameters of Model
Dark Energy: Constant Radiation Plays Large role at early times Matter Increases as radiation dies off Dominated by Dark Energy at later times
Dark Energy: Time Dependent Dominated by Dark Energy at early times Again dominated by Dark Energy at later times Kappa and Alpha were chosen to agree w/ observations Amount of radiation is relatively lower
Scale Factor Represents relative expansion of universe Independent of Free Parameters which characterize expansion
Power Law Model of Time Dependent dark energy: Possible Free Parameters do not influence Dynamical behaviour WMAP findings: Universe is >13.7 billion years old
Acknowledgments Dimitrios Psaltis Chi Kwan Chan Drew Milsom
Sources Cited Kravtsov, Andrey. “Computer-generated image of the distribution of dark matter.” Image from “Cosmologists to plot strategy for dark energy research campaign at Chicago workshop Sept. 17-20.” 3 Sept 2003. 29 April 2007. <http://www-news.uchicago.edu/ releases/03/030903.darkmatter.shtml>. Limbach, Christopher, Alexander Luce, and Amanda Stiteler. “The Consequences of a Dynamical Dark Energy Density on the Evolution of the Universe.” 5 Dec 2006. 29 April 2007. <http://www.physics.arizona.edu/~dpsaltis/Phys205/limbach_luce_stiteler.pdf >. NASA. “WMAP picture of the infant universe.” Image from “Ringside Seat to the Universe’s First Split Second.” 20 March 2006. 30 April 2007. <http://imagine.gsfc.nasa.gov/docs/ features/news/20mar06.html>. National Taiwan Science Education Center. “The origin and the evolution of the Universe.” Image from “The Emergence of the Cosmos.” 29 April 2007. <http://www.ntsec.gov.tw/ space/EN/show.asp?XH36>. WMAP. “Geometry of the Universe.” “Image from “Sachs-Wolfe Effect.” 2 May 2007. <http://zebu.uoregon.edu/2004/a321/lec15.html>.