Biocentrism: How Life and Consciousness are the Keys to by Robert Lanza, Bob Berman

By Robert Lanza, Bob Berman

Robert Lanza is without doubt one of the most useful scientists within the world—a US information & global Report hide tale referred to as him a “genius” and a “renegade thinker,” even likening him to Einstein. Lanza has teamed with Bob Berman, the main largely learn astronomer on the earth, to supply Biocentrism, a innovative new view of the universe.

Every every now and then an easy but radical notion shakes the very foundations of data. The startling discovery that the realm used to be now not flat challenged and eventually replaced the best way humans perceived themselves and their dating with the area. for many people of the fifteenth century, the inspiration of Earth as ball of rock used to be nonsense. the total of Western, normal philosophy is present process a sea swap back, more and more being pressured upon us by means of the experimental findings of quantum thought, and whilst, in the direction of doubt and uncertainty within the actual reasons of the universe’s genesis and constitution. Biocentrism completes this shift in worldview, turning the planet the wrong way up back with the progressive view that lifestyles creates the universe rather than the opposite direction around.

In this paradigm, existence isn't an unintended byproduct of the legislation of physics. Biocentrism takes the reader on a probably inconceivable yet finally inescapable trip via a international universe—our own—from the viewpoints of an acclaimed biologist and a number one astronomer. Switching standpoint from physics to biology unlocks the cages during which Western technological know-how has unwittingly controlled to restrict itself. Biocentrism will shatter the reader’s rules of life—time and area, or even demise. even as it's going to unlock us from the uninteresting worldview of lifestyles being only the task of an admixture of carbon and some different parts; it indicates the exhilarating danger that lifestyles is essentially immortal.

The twenty first century is expected to be the Century of Biology, a shift from the former century ruled by way of physics. it kind of feels becoming, then, to start the century via turning the universe outside-in and unifying the rules of technological know-how with an easy concept came across by means of one of many top life-scientists of our age. Biocentrism awakens in readers a brand new experience of chance, and is filled with such a lot of surprising new views that the reader won't ever see fact an identical approach back.

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In both the cases, −1 < w < 1, though it is possible to construct more complicated scalar field Lagrangians with even w < −1. ) Since the quintessence field (or the tachyonic field) has an undetermined free function V (φ), it is possible to choose this function in order to produce a given H(a). ) and ρφ (a) is due to a scalar field. When w(a) is given, one can determine the V (φ) using either (47) or (52). For quintessence, (47) along with (43) gives 3H 2(a) φ˙ 2 (a) = ρ(1 + w) = (1 − Q)(1 + w); 8πG 41 2V (a) = ρ(1 − w) = 3H 2 (a) (1 − Q)(1 − w) 8πG (53) For tachyonic scalar field, (52) along with (43) gives φ˙ 2 (a) = (1 + w); V (a) = ρ(−w)1/2 = 3H 2 (a) (1 − Q)(−w)1/2 8πG (54) Given Q(a), w(a) these equations implicitly determine V (φ).

This means that clusters will be comparatively rare at high redshifts in a ΩNR = 1 universe compared to models with cosmological constant. 5 in a universe with cosmological constant[212,213,214,215,75]. ) Hence the evolution of cluster population as a function of redshift can be used to discriminate between these models. An indirect way of measuring this abundance is through the lensing effect of a cluster of galaxy on extended background sources. Typically, the foreground clusters shears the light distribution of the background object and leads to giant arcs.

The resulting equation is valid in the linear regime and hence will be satisfied by each of the Fourier modes δk (t) obtained by Fourier transforming δ(t, x) with respect to x. Taking δ(t, x) = D(t)f (x), the D(t) satisfies the equation ¨ + 2 a˙ D˙ = 4πGρb D D a (66) The power spectra P (k, t) =< |δk (t)|2 > at two different redshifts in the linear regime are related by P (k, zf ) = T 2 (k, zf , zi , bg)P (k, zi) (67) where T (called transfer function) depends only on the parameters of the background universe (denoted by ‘bg’) but not on the initial power spectrum and can be computed by solving (66).

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