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Collider Signals of Gravitational Fixed Points
High Energy Physics - Phenomenology · Submitted 21 Jul 2007
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We find significant effects in the processes of Kaluza-Klein (KK) graviton exchange or resonant KK graviton production in both the Drell-Yan reaction as well as in $e^+e^-\to f\bar f$.
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The abstract, sentence by sentence
Recent studies have shown that the poor perturbative behavior of General Relativity in the ultraviolet regime may be ameliorated by the existence of a non-Gaussian fixed point which renders the theory asymptotically safe and possibly non-perturbatively renormalizable. This results in a running of the (effective) gravitational coupling such that gravity becomes weaker at high energies. We parameterize this effective coupling with a form factor and study its consequences at the LHC and ILC in models with large extra dimensions or warped extra dimensions. We find significant effects in the processes of Kaluza-Klein (KK) graviton exchange or resonant KK graviton production in both the Drell-Yan reaction as well as in $e^+e^-\to f\bar f$. On the otherhand, processes leading to KK graviton emission show qualitatively less sensitivity to the presence of a form factor. In addition, we examine tree-level perturbative unitarity in $2\to 2$ gravity-mediated scattering and find that this form factor produces a far better behaved amplitude at large center of mass energies.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Recent studies have shown that the poor perturbative behavior of General Relativity in the ultraviolet regime may be ameliorated by the existence of a non-Gaussian fixed point which renders the theory asymptotically safe and possibly non-perturbatively renormalizable. | background 1.00 | 0.04 | 0.07 | hedged possibility 0.95 |
| s1 | This results in a running of the (effective) gravitational coupling such that gravity becomes weaker at high energies. | background 0.73 | 0.15 | 0.08 | asserted 1.00 |
| s2 | We parameterize this effective coupling with a form factor and study its consequences at the LHC and ILC in models with large extra dimensions or warped extra dimensions. | method 0.70 | 0.92 | 0.05 | asserted 0.90 |
| s3 | We find significant effects in the processes of Kaluza-Klein (KK) graviton exchange or resonant KK graviton production in both the Drell-Yan reaction as well as in $e^+e^-\to f\bar f$. | result 1.00 | 0.96 | 0.43 | asserted 1.00 |
| s4 | On the otherhand, processes leading to KK graviton emission show qualitatively less sensitivity to the presence of a form factor. | result 1.00 | 0.86 | 0.09 | asserted 1.00 |
| s5 | In addition, we examine tree-level perturbative unitarity in $2\to 2$ gravity-mediated scattering and find that this form factor produces a far better behaved amplitude at large center of mass energies. | result 0.99 | 0.96 | 0.23 | asserted 1.00 |
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The paper
Original abstract
Recent studies have shown that the poor perturbative behavior of General Relativity in the ultraviolet regime may be ameliorated by the existence of a non-Gaussian fixed point which renders the theory asymptotically safe and possibly non-perturbatively renormalizable. This results in a running of the (effective) gravitational coupling such that gravity becomes weaker at high energies. We parameterize this effective coupling with a form factor and study its consequences at the LHC and ILC in models with large extra dimensions or warped extra dimensions. We find significant effects in the processes of Kaluza-Klein (KK) graviton exchange or resonant KK graviton production in both the Drell-Yan reaction as well as in $e^+e^-\to f\bar f$. On the otherhand, processes leading to KK graviton emission show qualitatively less sensitivity to the presence of a form factor. In addition, we examine tree-level perturbative unitarity in $2\to 2$ gravity-mediated scattering and find that this form factor produces a far better behaved amplitude at large center of mass energies.
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References
How the literature uses it
26 arXiv papers cite this in 35 sentences
Papers citing it · 22 sentences without a confident label
Compares with it 2 papers
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We also compare our results, and in particular the $m_μμ$-dependence, with those from effective field theory [ref] , the form-factor approximation [ref] , and the Standard Model background.
Asymptotic safety and Kaluza-Klein gravitons at the LHC · Phenomenology · 1.00
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Note that a similar proposal has been made to solve problems with unitarity in models with large extra-dimensions [ref] .
Asymptotically safe weak interactions · Introduction · 0.89
Cites it as background 10 papers
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Experimental signatures for asymptotic safety within low-scale quantum gravity are discussed in [ref] .
Asymptotic safety and Kaluza-Klein gravitons at the LHC · Introduction · 0.80
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This scenario was dubbed “asymptotic safety” by Weinberg [ref] and is reviewed e.g. in [ref] (for a recent attempt in this direction see e.g. [ref] ).
A pedagogical explanation for the non-renormalizability of gravity · Asymptotic Safety? · 0.99
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(3) As for possible physics implications of the RG flow predicted by QEG, ideas from particle physics, in particular the “RG improvement”, have been employed in order to study the leading quantum gravity effects in black holes [ref] , cosmological space-times [ref] or possible observable signatures from Asymptotic Safety at the LHC [ref] .
Asymptotic Safety, Fractals, and Cosmology · Introduction · 0.86
What it cites · 22 sentences without a confident label
Uses the method or tool of 1 paper
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Following Bonanno and Reuter [ref] , the relevant RGE corresponding to the action above is found to be
Spacetime Structure of an Evaporating Black Hole in Quantum Gravity · Background Formalism · 0.92
Uses data or values from 2 papers
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At the $√(s)=500$ GeV ILC, the search reach for the cutoff $Λ_H$ in the conventional ADD model is approximately 5 TeV [ref] , independent of the value of $δ$, assuming an integrated luminosity of 500 $fb^-1$ and $80%$ electron beam polarization.
TESLA Technical Design Report Part III: Physics at an e+e- Linear Collider · Large Extra Dimensions · 0.91
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At the $√(s)=500$ GeV ILC, the search reach for the cutoff $Λ_H$ in the conventional ADD model is approximately 5 TeV [ref] , independent of the value of $δ$, assuming an integrated luminosity of 500 $fb^-1$ and $80%$ electron beam polarization.
Indirect Collider Signals for Extra Dimensions · Large Extra Dimensions · 0.91
Cites as background 10 papers
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The operator for this transition takes the generic form [ref] [equation] where the scale $Λ_H$ represents a naive cutoff that regulates the integral over the sum of KK graviton propagators weighted by the density of KK states. $Λ_H$ is of order the fundamental scale $M$, with the exact relationship between the two being governed by the full UV theory.
Indirect Collider Signals for Extra Dimensions · Large Extra Dimensions · 0.85
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The operator for this transition takes the generic form [ref] [equation] where the scale $Λ_H$ represents a naive cutoff that regulates the integral over the sum of KK graviton propagators weighted by the density of KK states. $Λ_H$ is of order the fundamental scale $M$, with the exact relationship between the two being governed by the full UV theory.
Quantum Gravity and Extra Dimensions at High-Energy Colliders · Large Extra Dimensions · 0.85
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In the RS model [ref] , the $S^1/Z_2$ orbifolded, slice of 5-dimensional space bounded by two branes is described by a non-factorizable metric
A Large Mass Hierarchy from a Small Extra Dimension · Warped Extra Dimensions · 0.99
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