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Storyline P=ωρ The Dark Energy

Student in anthropology at McGill University in Montreal, Etienne and Eloise associate has a team of paranormal investigators to unravel the mystery surrounding the death of a student of the same court, 10 years ago. Their research will combine science and paranormal while we will follow the court their visit to Quebec three places known for their haunting phenomena. Faced with the horror and death, they will face their own demons in order to survive their nightmare.

Movie details

Title : P=ωρ The Dark Energy
Release : 2015-10-13
Genre : Horror
Runtime : 90
Company :
Rating :
out of 10 From Users

Homepage : Homepage Movie
Trailer : Video Trailer
Casts of P=ωρ The Dark Energy
Leonardo Fuica, Isabelle Blais, Marc-André Boulanger, Pierre-Luc Brillant,


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P=ωρ The Dark Energy (2015) User Score. Overview. Student in anthropology at McGill University in Montreal, Etienne and Eloise associate has a team of paranormal investigators to unravel the mystery surrounding the death of a student of the same court, 10 years ago. Their research will combine science and paranormal while we will follow the ...

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In the equation of state p = ωρ, a >.. 0 corresponds to the range of values ω < −1/3, referred to as quintessence dark energy. The case ω = −1 is equivalent to assuming Einstein’s cosmological constant. It has been forcefully argued by Bousso [6] that the cosmological constant is the best model for dark energy.

Evolution of Universe as a Homogeneous System: Changes of Scale Factors with Different Dark Energy Equation of States PromilaBiswas∗1 andRitabrataBiswas†2 Department of Mathematics, The University of Burdwan, Golapbag Academic Complex, City : Burdwan-713104, ... ii It reduces to p = ωρ in the limit that the Chaplygin parameter A → 0 .

p = ωρ, (2) where p is the pressure, ρ is the energy density and ω a constant parameterwhich may be positive (white energy) and negative (dark energy). The cases ω = 1/3, 1, and −1 characterizes, respectively, the blackbody radiation, a stiff-fluid and the vacuum state while ω < −1 stands to a phantomlike behavior.

so that we obtain the holographic dark energy (HDE) density ρΛ = 3c2M2 pL −2, (1) where c is a free dimensionless O(1) parameter that can be determined by observations. Taking L as the Hubble radius H = H−1 0 this ρΛ is comparable to the observed dark energy density, but gives wrong EoS for the dark energy [14].

tion of state p =ωρ to describe the hypothesized dark energy. While ω<−13 is sufficient to yield an accelerated expansion, it concluded that is ω=−1 is the only value allows our solution to remain close enough to which Einstein gravity to be consistent with observation.

J. S. Farnes : A unifying theory of dark energy and dark matter Fig. 3. N-body simulations showing the formation of a non-cuspy dark matter halo from an initially motionless particle distribution ...

energy, i.e., not dark energy. In this context we could have the dark energy sustaining the collapse of the standard energy, while the standard matter would trap the dark energy. In our model the mass function is a natural consequence of the Einstein’s field equations and the energy density as well as the pressure decreases with the radial ...

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