1988
DOI: 10.1088/0305-4470/21/17/012
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Semiclassical investigation of a charged relativistic membrane model

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Cited by 19 publications
(32 citation statements)
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“…To this end, we can choose alternative parametrizations for equation (6) (see for example [28] for a detailed variety of embeddings) which requires analogue developments. At this stage, we mention only that depending on the parametrization chosen, the momenta π t and π a acquire a different form but, however, they pleasantly lead to an unaltered form for the energy conservation law (see (20) below). Hereafter, the three possible geometries for the universe will be considered in the successive equations through the parameter k, (k = −1, 0, 1) and the use of the cosmic gauge, N = 1.…”
Section: Inclusion Of Mattermentioning
confidence: 99%
See 1 more Smart Citation
“…To this end, we can choose alternative parametrizations for equation (6) (see for example [28] for a detailed variety of embeddings) which requires analogue developments. At this stage, we mention only that depending on the parametrization chosen, the momenta π t and π a acquire a different form but, however, they pleasantly lead to an unaltered form for the energy conservation law (see (20) below). Hereafter, the three possible geometries for the universe will be considered in the successive equations through the parameter k, (k = −1, 0, 1) and the use of the cosmic gauge, N = 1.…”
Section: Inclusion Of Mattermentioning
confidence: 99%
“…Now, by defining X :=ṫ/[a(Λ +ρ) 1/2 ] = (ȧ 2 + k) 1/2 /[a(Λ +ρ) 1/2 ] we are able to rewrite the energy equation (20) as X 3 + 3 β * X 2 − X + 2 E * a −4 = 0 where we have introduced the notation, β * (a) =β/(Λ +ρ)…”
Section: Friedmann Type Equationmentioning
confidence: 99%
“…We have absorbed a global constant in (5) and (6) in order to avoid the density character of the momenta and we have defined the quantity N = √ṫ 2 −ȧ 2 , where the dot stands for derivation with respect to τ. The three possible geometries for the Universe will be consider in the successive equations through the parameter k, (k = −1, 0, 1) and the use of the cosmic gauge, N = 1.…”
Section: Modified Geodetic Branelike Cosmologymentioning
confidence: 99%
“…This correction term was also considered in the bending and shape determination of phospholipid membranes [5]. In the relativistic context, these kind of terms appear in the improvement for the earlier attempt by Dirac to depict the electron as a bubble [6,7], or in a general expansion for a local action describing extended objects embedded in a codimension one bulk spacetime taking into account the widht [8]. More recently, it has been discovered that this geometrical term belongs to a finite set of effective 4−dimensional field theories known as Galileons pursuing possible applications to particle physics and cosmology [9,10,11].…”
Section: Introductionmentioning
confidence: 99%
“…Long time ago, this framework has been considered by Chen to accomodate a non-vanishing mean curvature in the study of hypersurfaces in differential geometry [3]. In a physical context, in the improvement of Dirac to draw the electron as a bubble, the proposal of include the mean curvature to the Dirac's electron came in by Onder and Tucker [4,5]. Thus, this type of correction fits accordingly in the brane cosmological context when we consider our Universe as a hypersurface floating in a 5-dimensional Minkowski spacetime.…”
Section: Introductionmentioning
confidence: 99%