REVIEW
Tests of the Gravitational Inverse-Square Law below the Dark-Energy Length Scale
High Energy Physics - Phenomenology · Submitted 14 Nov 2006 · 17 references
Pith's verdict: A genuine hundredfold improvement in short-range gravity bounds, with one ambiguity — whether the detector-bow correction is measured or fitted — that a careful reader should press on.
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Referee report
The paper
The paper claims
A torsion balance finds no deviation from Newtonian gravity at separations down to 55 micrometers, so any gravitational-strength Yukawa force must have a range shorter than 56 micrometers and any single compact extra dimension must be no 44
The reading
What carries the argument
The instrument is a ``missing mass'' torsion balance: a molybdenum detector ring with 42 machined holes in two 21-fold-symmetric circles hangs above an attractor built from a thin molybdenum disc with 42 holes atop a thicker tantalum disc with 21 holes, and the gravitational coupling between the holes produces a torque that oscillates 21 times per attractor revolution. The lower attractor holes are offset by $360/42$ degrees so that, if the inverse-square law holds, the $21ω$ torque nearly cancels, while a short-range Yukawa interaction with $λ$ below the 1 mm disc thickness is not cancelled. Running with the lower disc at two thicknesses (differing by 0.140 mm) makes a genuine short-range force flip sign between experiments while a systematic error would not, and a separate three-sphere gravitational octupole driven by a turntable provides a continuous absolute calibration of the torque scale.
Extended reading notes
Core claim
The authors claim that Newtonian gravity, augmented by nothing, fits their measured torques across three separate experiments spanning 9.53 mm to 55 µm. Parameterizing a deviation as $V(r) = -G m_1 m_2 [1 + α e^{-r/λ}]/r$, they find at 95% confidence that $|α| ≤ 1$ requires $λ ≤ 56~$µm, so no gravitational-strength Yukawa force with a range above that value survives. Translated into extra dimensions, the same data exclude a single compact dimension larger than $R ≤ 44~$µm, and for the two-large-extra-dimension scenario they require a $2σ$ lower limit on the unification mass $M_* ≥ 3.2$ TeV/$c^2$. The combined Newtonian fit gives $χ^2 = 407$ for 421 degrees of freedom, and adding a Yukawa term improves the fit by only $Δχ^2 = 3.5$, at $α = -0.0037$, $λ = 2$ mm, with no $2σ$ effect at any range.
Load-bearing premise
The 95% confidence bound depends on the modeled bow of the detector ring, which the authors invoke to explain the marginally significant excess attraction seen at the smallest separations in Experiments I and III.
Editorial extensions
If this is right
- Any gravitational-strength Yukawa force mediating a new long-range interaction must have a range below 56 µm, which removes a wide band of parameter space for light scalar or vector mediators coupled to mass.
- A single compact extra dimension must be smaller than 44 µm, and in the two-large-extra-dimension picture the unification mass must exceed 3.2 TeV/$c^2$ at $2σ$.
- Scenarios in which gravity weakens for separations below the dark-energy length scale, such as a graviton with a size near 85 µm, are pushed to sizes below the experiment's reach.
- The techniques demonstrated here — patterned nulled torques, multiple attractor thicknesses, and in-situ autocollimator linearity mapping — set a template for pushing torsion-balance tests to smaller separations.
Reading between the lines
- The bound is set by the smallest separation achieved, so the natural next step is engineering: a flatter, more rigid detector and a thinner membrane would move the 56 µm limit toward the 20 µm scale where thermal and electrostatic backgrounds begin to dominate.
- Because the same data can be recast as a bound on any power-law or finite-range modification once the geometry integral is redone, the exclusion is broader than the single Yukawa curve shown; the authors say as much by deferring other functional forms to a separate publication.
- The persistent excess torque noise at the smallest separations, roughly four times thermal, is the practical ceiling on this generation of the experiment; if it is instrumental rather than statistical, better vibration and patch-potential control would tighten the limit more than extra data at large separation.
- A laboratory bound at the dark-energy length scale invites the reverse question: if no new force appears exactly where cosmic acceleration suggests one might, the coincidence between $\lambda_d$ and the reachable laboratory range becomes a constraint on model building rather than a hint.
Original abstract
We conducted three torsion-balance experiments to test the gravitational inverse-square law at separations between 9.53 mm and 55 micrometers, probing distances less than the dark-energy length scale $\lambda_{\rm d}=\sqrt[4]{\hbar c/\rho_{\rm d}}\approx 85 \mu$m. We find with 95% confidence that the inverse-square law holds ($|\alpha| \leq 1$) down to a length scale $\lambda = 56 \mu$m and that an extra dimension must have a size $R \leq 44 \mu$m.
The compiled record
The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
The abstract, sentence by sentence
We conducted three torsion-balance experiments to test the gravitational inverse-square law at separations between 9.53 mm and 55 micrometers, probing distances less than the dark-energy length scale $\lambda_{\rm d}=\sqrt[4]{\hbar c/\rho_{\rm d}}\approx 85 \mu$m. We find with 95% confidence that the inverse-square law holds ($|\alpha| \leq 1$) down to a length scale $\lambda = 56 \mu$m and that an extra dimension must have a size $R \leq 44 \mu$m.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We conducted three torsion-balance experiments to test the gravitational inverse-square law at separations between 9.53 mm and 55 micrometers, probing distances less than the dark-energy length scale $\lambda_{\rm d}=\sqrt[4]{\hbar c/\rho_{\rm d}}\approx 85 \mu$m. | method 0.59 | 0.97 | 0.06 | asserted 0.92 |
| s1 | We find with 95% confidence that the inverse-square law holds ($|\alpha| \leq 1$) down to a length scale $\lambda = 56 \mu$m and that an extra dimension must have a size $R \leq 44 \mu$m. | result 0.99 | 0.97 | 0.93 | asserted 1.00 |
What was examined, and what was not
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Figures
Showing 5 of the paper's 6 figures. See all figures in the PDF ↗ Figures reproduced from arXiv:hep-ph/0611184 by the authors.
References
How later papers used it
259 later papers cite it
19 later papers by other authors are listed below: 19 used its data or values.
Uses its data or values 19 of 65 papers with this label
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Obtained its datapoints from Figs. 3, 4 and 5 of this paper using plot-digitizer software and showed them in its Table II.
Sub-millimeter Spatial Oscillations of Newton's Constant: Theoretical Models and Laboratory Tests (2016) · 1.00 · paraphrased: the licence does not allow quoting
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Used the limit yielded by the Eöt-Wash experiment of this paper, a ≲10^-10 m^2, for its specific model.
On the 1/c Expansion of f(R) Gravity (2010) · 1.00 · paraphrased: the licence does not allow quoting
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Took the upper limits for λ given by Figure 6 of this paper for two values of α.
Non-relativistic limit of multidimensional gravity: exact solutions and applications (2009) · 1.00 · paraphrased: the licence does not allow quoting
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Cited this paper for the current upper bound of 0.01 cm on the size of such extra dimensions.
A scale at 10 MeV, gravitational topological vacuum, and large extra dimensions (2017) · 1.00 · paraphrased: the licence does not allow quoting
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Used the absence of modifications to the inverse-square law down to 56 μm reached in this paper to correspond to a probe at ξ = 6·10^-24 m^-2.
Asymptotic safety casts its shadow (2019) · 1.00 · paraphrased: the licence does not allow quoting
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Cited this paper for the current bound of R < 37 μm for two extra dimensions of the same size.
2009 TASI Lecture -- Introduction to Extra Dimensions (2010) · 0.99 · paraphrased: the licence does not allow quoting
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Cited this paper for the bound L ≲ 44 μm = 2.2×10^14 TeV^-1.
Production of tidal-charged black holes at the Large Hadron Collider (2010) · 0.99 · paraphrased: the licence does not allow quoting
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Interpreted the current limit from the Eöt-Wash experiment of this paper to imply that kr > 1 at the scale 0.04 mm, and derived bounds on k, M_5 and the brane tension.
Braneworld Cosmology (2007) · 0.99 · paraphrased: the licence does not allow quoting
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Used this paper's current limit R < 37 μm for k = 2 to infer M_* > 1.4 TeV.
Compactified Spacelike Extra Dimension & Brane-Higgs Field (2020) · 0.99 · paraphrased: the licence does not allow quoting
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Combined experimental bounds on the coupling α of the Weyl-squared term from another work, obtained from torsion-balance experiments of this paper, to estimate an upper bound on the horizon area.
Rotating near-horizon extreme geometries in quadratic gravity (2026) · 0.98 · paraphrased: the licence does not allow quoting
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Took L ≈ 50 μm and ρ_m ≈ 10^-12 g cm^-3 for this paper's Cavendish-type experiment to obtain a sufficient condition n ≥ 1.
Disappearing cosmological constant in f(R) gravity (2007) · 0.98 · paraphrased: the licence does not allow quoting
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Took R ≈ 44 μm, the largest flat extra dimension allowed according to data from torsion-balance experiments of this paper, as its compactification scale.
Kaluza-Klein Towers in the Early Universe: Phase Transitions, Relic Abundances, and Applications to Axion Cosmology (2016) · 0.98 · paraphrased: the licence does not allow quoting
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Post-Cavendish experiments put an upper limit of [ref] $ℓ_0 ≤45 μm$.
Modified gravity approaches to the cosmological constant problem (2022) · Supersymmetric large extra dimensions · 0.97
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Setting the largest value of $Λ_c$ to be equal to $𝒪(10μ m$), thus saturating bounds from table-top experiments [ref] , and solving for $α_i$, we find
Gravitational-Wave Tests of General Relativity with Ground-Based Detectors and Pulsar-Timing Arrays (2024) · Modified quadratic gravity · 0.96
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Used the laboratory bound from the Eöt-Wash experiment of this paper to give F''(0) ≤ 2×10^-6 cm^2.
Born - Infeld-like modified gravity (2012) · 0.95 · paraphrased: the licence does not allow quoting
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Used this paper's prediction that an extra dimension must have a size R ≤ 44 μm to rule out δ = 2.
Associated production of graviton with $e^+e^-$ pair via photon-photon collisions at a linear collider (2007) · 0.82 · paraphrased: the licence does not allow quoting
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Took the upper limit on the Yukawa characteristic length λ ≲ 10^-3 cm from this paper for its estimate α_1 ≲ 1.
Weak field limit of higher dimensional massive Brans-Dicke gravity: Observational constraints (2019) · 0.80 · paraphrased: the licence does not allow quoting
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Cited this paper for the upper limit λ ≲ 10^-3 cm when |Ω| ∼ O(1).
Exact and asymptotic black branes with spherical compactification (2012) · 0.82 · paraphrased: the licence does not allow quoting
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Restricted the range of M_UV to above 10^8 GeV to comply with this paper's bound on deviations from Newton's inverse-square law.
Aspects of the Dark Dimension in Cosmology (2022) · 0.81 · paraphrased: the licence does not allow quoting
How the literature uses it
205 arXiv papers cite this in 288 sentences
Papers citing it · 188 sentences without a confident label
Builds on it 1 paper
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In the next section we extend the analysis of the Washington group [ref] using a oscillating parametrization in addition to the Yukawa one in an attempt to search for oscillating signatures or constraints in the data.
Sub-millimeter Spatial Oscillations of Newton's Constant: Theoretical Models and Laboratory Tests · Observational viability of spatial oscillations of Newton constant · 0.97
Uses its method or tool 1 paper
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The goal of this article is to use torsion pendulum experiments such as [ref] to constrain fifth forces from chameleon dark energy models [ref] .
Dark energy fifth forces in torsion pendulum experiments · Introduction · 0.88
Uses its data or values 60 papers
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Then, if we take the natural value $ω∼O(1)$, we get an estimate $α_1 ≲1$ and, consequently, the upper limit on the Yukawa characteristic length of interaction leading to $λ=1/m ≲10^-3$cm [ref] .
Weak field limit of higher dimensional massive Brans-Dicke gravity: Observational constraints · Massive scalar field · 0.80
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A total of 87 residual points were shown along with three predicted residual curves [ref] that would arise in the context of Yukawa type deviations (eq.
Sub-millimeter Spatial Oscillations of Newton's Constant: Theoretical Models and Laboratory Tests · Maximum Likelihood Analysis · 0.94
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Based on these differences, 95% c.l. upper limits were set on possible Yukawa interactions [ref] .
Model Comparison tests of modified gravity from the E\"ot-Wash experiment · Summary of results and P19 · 0.90
Compares with it 6 papers
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For $α=1$ the line intersects the $2σ$ contours at $m=m'≃20 mm^-1$ (for the 'all data' plot) thus leading to a $2σ$ constraint $m20 mm^-1$ which is almost identical with the constraint of Ref. [ref] .
Sub-millimeter Spatial Oscillations of Newton's Constant: Theoretical Models and Laboratory Tests · Maximum Likelihood Analysis · 0.97
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The deviations of the oscillation frequency [ref] with respect to the gravity-free oscillation frequency $2ω_0$ are shown for the particle numbers $N=10^9$ (the second panel) and $N=10^12$ (the fourth panel) with respect to the current exclusion limits [ref] .
Testing weakest force with coldest spot · Yukawa interaction · 0.84
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It should be noticed that this result agrees with the $σ$-value inferred from Newtonian potential experiments designed to measure the Newtonian coupling parameter [ref] .
Degravitation, Orbital Dynamics and the Effective Barycentre · The perihelion precession of Mercury: · 0.95
Cites it as support 2 papers
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However, such fifth-force effects are ruled out by the very same experiments that test gravity at the sub-millimeter scale [ref] (measuring the Eddington parameter in the post-Newtonian expansion).
The $F$-term Problem and other Challenges of Stringy Quintessence · Preliminaries and Requirements · 0.97
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GR is well tested to $μm$ scales in the laboratory [ref] , in the weak-field setting in the solar system [ref] , the Milky Way [ref] , and at extragalactic scales [ref] .
$\Lambda$CDM Tensions: Localising Missing Physics through Consistency Checks · Cosmological Bedrock: GR + FLRW · 0.97
Cites it as background 17 papers
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A wide range of experiments has focused on this range of scales [ref] and constraints have been imposed on particular parametrizations of extensions of Newton's gravitational potential.
Sub-millimeter Spatial Oscillations of Newton's Constant: Theoretical Models and Laboratory Tests · Introduction · 0.80
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Experimental searches for Yukawa interactions have been actively pursued using torsion balances, atom interferometry, and precision force measurements [ref] , placing strong constraints over a broad range of $(α_Y,λ)$ parameter space.
Probing Yukawa Gravity with Modulated Newtonian Cancellation in the CHRONOS Detector · Introduction · 0.93
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They include torsion balance experiments [ref] , Casimir force experiments [ref] , levitating microsphere experiments [ref] , atomic interferometry [ref] etc.
Constraints on Spatially Oscillating Sub-mm Forces from the Stanford Levitated Microsphere Experiment Data · Introduction · 0.97
Discussion
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