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On gravity localization in scalar braneworlds with a super-exponential warp factor

High Energy Physics - Theory · Submitted 1 Oct 2012

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim We show that within tachyonic braneworld models,"super-exponential" warp factors of the form $e^{-2f} \sim e^{-2c_1e^{c_2 |\sigma|}}$ are problematic when dealing with both the finiteness of the effective four-dimensional (4d) Planck mass and the localization of 4d gravity, which can be stated by the requirement that $\int e^{-2f(\sigma)}d\sigma < \infty$, because this condition necessarily implies that c_1 and c_2 should be positive.

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arXiv ID1210.0597 (version 3)
Pith ID56B6E66T, Pith's permanent record of this paper and its review
CitationAlfredo Herrera-Aguilar, Dagoberto Malagon-Morejon, Gabriel German, Mariana Carrillo-Gonzalez. "On gravity localization in scalar braneworlds with a super-exponential warp factor." arXiv:1210.0597 (2012). https://pith.science/paper/56B6E66T
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What the abstract itself states, as probabilities: claims first 0.04 · states limitation 0.67 · human participants 0.01 · controlled comparison 0.15 · randomized assignment 0.01 · states quantitative result 0.11 · compares with prior results 0.58 · mentions code or data availability 0.02.

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arXiv listing abstract v3. Results and the main claim are underlined; .

We show that within tachyonic braneworld models,"super-exponential" warp factors of the form $e^{-2f} \sim e^{-2c_1e^{c_2 |\sigma|}}$ are problematic when dealing with both the finiteness of the effective four-dimensional (4d) Planck mass and the localization of 4d gravity, which can be stated by the requirement that $\int e^{-2f(\sigma)}d\sigma < \infty$, because this condition necessarily implies that c_1 and c_2 should be positive. As a consequence of this fact the tachyonic field $T$ turns out to be complex in contradiction with the real nature of the starting action for the tachyonic braneworld. Conversely if one requires to have a real tachyon field, 4d gravity will not be localized and the effective gravitational coupling will be infinite. We present several typical examples where this problem occurs: we have analysed this situation for thin as well as thick tachyonic braneworlds with 4d Poincare symmetry, for the case when a bulk cosmological constant is present, and even for a brane with an induced spatially flat 4d cosmological background, and shown that in all cases the tachyon field T comes out to be inconsistently complex when imposing localization of 4d gravity. On the other hand, when dealing with a further reduction of the hierarchy problem one should carefully consider the sign of the constants c_1 and c_2 to avoid inconsistencies in the tachyonic braneworld model. We also present a similar discusion involving a canonical scalar field in the bulk where none of these problems arise and hence, the mass hierarchy and 4d gravity localization problems can be successfully addressed at once. Finally, the stability analysis of this scalar tensor braneworld model with a super-exponential warp factor is performed.

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What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 We show that within tachyonic braneworld models,"super-exponential" warp factors of the form $e^{-2f} \sim e^{-2c_1e^{c_2 |\sigma|}}$ are problematic when dealing with both the finiteness of the effective four-dimensional (4d) Planck mass and the localization of 4d gravity, which can be stated by the requirement that $\int e^{-2f(\sigma)}d\sigma < \infty$, because this condition necessarily implies that c_1 and c_2 should be positive. result 0.87 0.87 0.47 asserted 1.00
s1 As a consequence of this fact the tachyonic field $T$ turns out to be complex in contradiction with the real nature of the starting action for the tachyonic braneworld. result 0.84 0.90 0.24 asserted 1.00
s2 Conversely if one requires to have a real tachyon field, 4d gravity will not be localized and the effective gravitational coupling will be infinite. result 0.93 0.83 0.31 asserted 1.00
s3 We present several typical examples where this problem occurs: we have analysed this situation for thin as well as thick tachyonic braneworlds with 4d Poincare symmetry, for the case when a bulk cosmological constant is present, and even for a brane with an induced spatially flat 4d cosmological background, and shown that in all cases the tachyon field T comes out to be inconsistently complex when imposing localization of 4d gravity. contribution 0.72 0.95 0.23 asserted 1.00
s4 On the other hand, when dealing with a further reduction of the hierarchy problem one should carefully consider the sign of the constants c_1 and c_2 to avoid inconsistencies in the tachyonic braneworld model. interpretation 0.83 0.37 0.14 hedged possibility 0.61
s5 We also present a similar discusion involving a canonical scalar field in the bulk where none of these problems arise and hence, the mass hierarchy and 4d gravity localization problems can be successfully addressed at once. contribution 0.60 0.89 0.17 asserted 0.99
s6 Finally, the stability analysis of this scalar tensor braneworld model with a super-exponential warp factor is performed. contribution 0.94 0.93 0.06 asserted 0.94

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The paper
Original abstract

We show that within tachyonic braneworld models,"super-exponential" warp factors of the form $e^{-2f} \sim e^{-2c_1e^{c_2 |\sigma|}}$ are problematic when dealing with both the finiteness of the effective four-dimensional (4d) Planck mass and the localization of 4d gravity, which can be stated by the requirement that $\int e^{-2f(\sigma)}d\sigma < \infty$, because this condition necessarily implies that c_1 and c_2 should be positive. As a consequence of this fact the tachyonic field $T$ turns out to be complex in contradiction with the real nature of the starting action for the tachyonic braneworld. Conversely if one requires to have a real tachyon field, 4d gravity will not be localized and the effective gravitational coupling will be infinite. We present several typical examples where this problem occurs: we have analysed this situation for thin as well as thick tachyonic braneworlds with 4d Poincare symmetry, for the case when a bulk cosmological constant is present, and even for a brane with an induced spatially flat 4d cosmological background, and shown that in all cases the tachyon field T comes out to be inconsistently complex when imposing localization of 4d gravity. On the other hand, when dealing with a further reduction of the hierarchy problem one should carefully consider the sign of the constants c_1 and c_2 to avoid inconsistencies in the tachyonic braneworld model. We also present a similar discusion involving a canonical scalar field in the bulk where none of these problems arise and hence, the mass hierarchy and 4d gravity localization problems can be successfully addressed at once. Finally, the stability analysis of this scalar tensor braneworld model with a super-exponential warp factor is performed.

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4 arXiv papers cite this in 12 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 9 sentences without a confident label

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  • We shall analyze the localization of 4d gravity in our braneworld field configuration following the work presented in [ref] , where a generalization of the Bardeen formalism for metric fluctuations of higher–dimensional backgrounds with non–compact extra dimensions was accomplished (see also [ref] and [ref] for similar approaches); moreover, the master equations for the coupled system of metric and scalar perturbations were also derived in a gauge–invariant form.

    Stability of Scalar Fields in Warped Extra Dimensions · Tensor perturbations and localization of 4d gravity · 0.99

Cites as background 3 papers
  • Several authors have chosen a tachyonic scalar field in the bulk and address issues like the hierarchy problem, and localization of gravity and matter fields [ref] – [ref] .

    A de Sitter tachyon thick braneworld · Introduction · 0.97

  • It has also become a matter of interest to find smooth braneworld solutions (for interesting reviews on these issues see e.g., [ref] – [ref] ).

    Thick brane solutions · Introduction · 1.00

  • It has also become a matter of interest to find smooth braneworld solutions (for interesting reviews on these issues see e.g., [ref] – [ref] ).

    Brane-World Gravity · Introduction · 1.00

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