lt;10^{-5}$). ### Gate 1: The z-Dependent Baryonic Tully-Fisher Relation $v_{\text{flat}}^4 = GM_b \cdot a_0(z) \propto M_b \cdot H(z)$ At $z = 2$, galaxies of fixed baryonic mass must show $\sim$31% higher asymptotic rotation velocity and $\sim$42% inward-shifted transition radius. The Radial Acceleration Relation must shift from the local curve ($a_0 = 1.04 \times 10^{-10}$, $n = 1.25$) to a distinct curve ($a_0 = 3.1 \times 10^{-10}$, $n = 2.34$). **Test:** JWST and ALMA resolved kinematics of high-$z$ disk galaxies. **Kill condition:** If early galaxies exhibit a static $a_0$, the theory is dead. ### Gate 2: Wide Binary Parity The low-acceleration anomaly in local stellar systems must break at exactly: $a_0 = \frac{cH_0}{2\pi} \approx 1.04 \times 10^{-10} \text{ m/s}^2$ with interpolation sharpness $n_0 = 1.25$. **Test:** Gaia DR3/DR4 wide binary orbital statistics. **Kill condition:** If the anomaly appears at a significantly different threshold, or does not appear at all, the $a_0$-$H$ link is broken. ### Gate 3: Dimensionless Ratio Drift Dimensionless couplings — specifically the fine-structure constant $\alpha$ — are predicted to exhibit a small drift tied to the noise floor evolution: $\frac{\Delta\alpha}{\alpha} = \kappa \cdot \frac{\Delta H}{H}$ The drift coefficient $\kappa$ is **derived** as the derivative of the $L^n$-norm volume with respect to the expansion rate: $\kappa = \partial\ln(V_{L^n})/\partial\ln(H)$ ([[Substrate Eigenvalues]]). The EM noise floor $E_0 \propto H(z)$ gives $\Delta\alpha/\alpha \sim (E_0/E_\text{typical})^n \cdot \Delta H/H$. See [[RST Four-Force Bridge]]. Existing constraints require $\kappa < 5 \times 10^{-6}$. Gate 3 is a strict numerical prediction for quasar spectroscopy (Many-Multiplet method). **Test:** High-resolution quasar absorption spectroscopy. **Status:** $\kappa$ **derived** as $\kappa = \partial\ln(V_{L^n})/\partial\ln(H)$ ([[Substrate Eigenvalues]]). Gate 3 is a strict numerical prediction. --- ## Part VII-B: The Relational Adjustment Protocol Standard physics formalisms — PPN, gravitational wave propagation, CMB perturbation theory — are derived under the assumption that the background spacetime is either a perfect vacuum (Minkowski) or a perfectly homogeneous expansion (FLRW). RST violates both assumptions: the substrate is never empty ($\theta \neq 0$ everywhere), the workload field $q$ is always active (even when saturated at $\mu \to 1$), and the effective gravitational constant $G_\text{eff}$ is not identical to the bare $G$ in the action. Before applying any standard constraint to RST, the following three adjustments must be performed. Failure to apply them will produce incorrect bounds and potentially false falsifications. ### Adjustment 1: Bare vs. Measured $G$ The $G$ appearing in the RST action (Part III) is a bare parameter. The gravitational constant measured in a Cavendish experiment or inferred from planetary orbits is an effective quantity that absorbs contributions from the aether energy density and the workload field's saturation state: $G_\text{measured} = \frac{G_\text{bare}}{1 - c_{14}/2} \cdot \left(1 + \delta_q\right)$ where $c_{14} = c_1 + c_4$ is the standard Einstein-Aether renormalization, and $\delta_q$ is the workload correction from the saturated AQUAL field. In the deep Newtonian regime ($g \gg a_0$), $\delta_q \sim \mathcal{O}(a_0/g)$ is small but nonzero. Any PPN calculation must use $G_\text{measured}$, not $G_\text{bare}$, when comparing to Solar System data. ### Adjustment 2: The Local Expansion Scalar $\theta$ Standard PPN expands the metric around flat Minkowski space ($\theta = 0$). In RST, the correct background is **cosmological Minkowski**: the metric is locally flat, but the aether field carries the cosmological expansion scalar $\bar{\theta} = 3H_0 \neq 0$. Inside gravitationally bound systems (Solar System, galaxy), $\theta$ is not the global Hubble value. The system has decoupled from the Hubble flow, and the local $\theta$ is determined by the boundary conditions at the edge of the bound region. This is the gravitational analogue of the **External Field Effect** (EFE) in MOND: the relevant $a_0$ inside the Solar System is set by the cosmological $\theta$ at the boundary, not by the local gravitational field of the Sun. The perturbation must be performed as: $\theta(r) = \bar{\theta}_\text{boundary} + \delta\theta(r)$ where $\delta\theta(r)$ encodes the Sun's distortion of the aether field. The PPN parameters $\gamma$ and $\beta$ receive corrections from $\delta\theta$ that are absent in standard Einstein-Aether theory. ### Adjustment 3: Deep-Newtonian Residuals When $g_N \gg a_0$ ($y \to \infty$ in the action), the interpolation function saturates at $\mu \to 1$ and the workload field locks to the Newtonian potential: $q \to \Phi_N$. Standard MOND treatments assume the scalar field "turns off" here. In RST, it does not — the locked field carries an energy density: $\varepsilon_q = \frac{a_0^2}{8\pi G}\,\mathcal{F}(y \to \infty,\, n)$ This residual acts as a tiny effective mass distribution around the central body. For the Sun, the correction to orbital dynamics scales as $a_0/g_N \sim 10^{-10}/10^{-3} \sim 10^{-7}$ at 1 AU — below the current Cassini bound ($2.3 \times 10^{-5}$) but potentially relevant for future missions (LISA Pathfinder, lunar laser ranging improvements). ### The GW Speed Exception Tensor perturbations (gravitational waves) are spin-2 modes. On an isotropic background, spin-2 modes do not mix with spin-0 modes ($q$, $\delta\theta$) at linear order. Therefore, the GW speed constraint from GW170817 ($|c_\text{GW} - c|/c < 10^{-15}$) applies directly without relational corrections. The standard Einstein-Aether result holds: RST requires $c_1 + c_3 = 0$ (or the equivalent relation for its specific $\mathcal{K}$ structure). ### Summary Rule > **The Relational Adjustment Rule:** No standard-physics bound may be applied to RST without first (1) identifying whether it assumes $\theta = 0$, (2) re-deriving the relevant observable with $\bar{\theta} \neq 0$, and (3) using $G_\text{measured}$, not $G_\text{bare}$. Tensor-mode constraints (GW speed) are exempt. Scalar-mode and vector-mode constraints (PPN, CMB, perihelion precession) are not. --- ## Part VIII: Empirical Calibration — The SPARC Evaluation ### VIII.1 Dataset and Method RST has been evaluated against the **SPARC database** (Lelli, McGaugh & Schombert 2016, AJ 152, 157; [arXiv:1606.09251](https://arxiv.org/abs/1606.09251)); [download](http://astroweb.cwru.edu/SPARC/): 175 nearby galaxies with surface photometry at 3.6 $\mu$m and rotation curves from HI/H$\alpha$. **Verification:** [[SPARC Evaluation Verification]]; method: [[about systems/expanded theory/sparc evaluation/SPARC evaluation - Code]]; results: [[python calculations results]]. For each galaxy, the Newtonian acceleration $g_N(r)$ was computed from the observed gas, disk, and bulge velocity contributions. The RST field equation $\mu(q'/a_0,\, n)\, q' = g_N$ was solved to predict the total rotation curve $v(r) = \sqrt{r \cdot q'}$, using the cosmologically fixed threshold $a_0 = cH_0/(2\pi) = 1.04 \times 10^{-10}$ m/s$^2$. The only free parameter per galaxy is the stellar disk mass-to-light ratio $\Upsilon_{\text{disk}}$, fitted by minimising reduced $\chi^2$ against the observed rotation curve. No dark matter halo parameters (mass, concentration, core radius) are used. ### VIII.2 Fixed-$n$ Results | Metric | $n = 1$ | $n = 2$ | |:---|:---|:---| | Galaxies fitted | 171 | 171 | | Median $\Upsilon_{\text{disk}}$ | 0.44 | 0.62 | | Median $\chi^2_{\text{red}}$ | 1.63 | 1.59 | | $\chi^2 < 2$ | 57% | 57% | | $\chi^2 < 5$ | 79% | 80% | | $\chi^2 < 10$ | 85% | 87% | Head-to-head, $n = 2$ produces better fits for 61% of galaxies, but pushes $\Upsilon_{\text{disk}}$ above the stellar population synthesis (SPS) expectation of $0.5 \pm 0.1$. ### VIII.3 Floating-$n$ Results and the Calibrated Baseline Allowing $n$ to float as a second free parameter alongside $\Upsilon_{\text{disk}}$ for each galaxy: | Metric | Value | |:---|:---| | Galaxies fitted | 171 | | Median $\Upsilon_{\text{disk}}$ | **0.491** | | Median $\chi^2_{\text{red}}$ | **1.40** | | $\chi^2 < 2$ | 61% | | $\chi^2 < 5$ | 81% | | $\chi^2 < 10$ | 86% | The raw $n$ distribution was bimodal, with a pile-up at the optimizer boundary ($n = 5$) caused by deep-MOND dwarf galaxies where the asymptotic velocity $v_f^4 = GMa_0$ is independent of $n$ — the interpolation shape has no leverage when the galaxy never enters the transition zone. **The Filtered Sample:** Restricting to galaxies that actually constrain $n$ (51 transition-zone galaxies with $v_{\text{max}} > 100$ km/s, $\max(g_N) > 0.5\,a_0$, and $n$ not pinned to optimizer bounds): | Parameter | Value | |:---|:---| | $n_0$ (median) | **1.255** | | $n_0$ (IQR) | [0.97, 1.95] | | $\Upsilon_{\text{disk}}$ (median) | **0.491** | ### VIII.4 Physical Interpretation 1. **The $a_0$ anchor is validated.** The cosmologically derived threshold $a_0 = cH_0/(2\pi)$ produces exactly the correct amount of "missing gravity" across 171 galaxies spanning three orders of magnitude in baryonic mass. The fitted $\Upsilon_{\text{disk}} = 0.49$ matches the independent Spitzer 3.6 $\mu$m SPS prediction ($0.5 \pm 0.1$) to within rounding error. If $a_0$ were systematically wrong, $\Upsilon$ would have been forced to unphysical values. 2. **The transition sharpness is approximately universal at $z = 0$.** In the clean, filtered sample, $n$ scatters around $n_0 = 1.25$ with no statistically significant dependence on galaxy mass, surface brightness, or maximum velocity ($p > 0.3$ for all Spearman tests). The scatter (IQR $\approx$ 1 unit) is consistent with observational systematics: distance uncertainties, inclination errors, non-circular motions, and the spherical approximation of the AQUAL field equation. 3. **The remaining $\sim$12% of failures are geometric, not gravitational.** The worst-fit galaxies are massive, high surface brightness spirals where the algebraic shortcut ($\mu q' = g_N$, assuming spherical symmetry) breaks down. The true 2D AQUAL Poisson solution for a thin disk is known to resolve these intermediate-radius overshoots. 4. **$n$ and $\Upsilon$ are independent.** The Spearman correlation between best-fit $n$ and best-fit $\Upsilon$ is $\rho = -0.008$ ($p = 0.92$) in the full sample. The optimizer extracts genuinely distinct information from each parameter. ### VIII.5 The $z > 0$ Prediction With the $z = 0$ anchor now empirically locked, the high-redshift RAR prediction becomes strictly computable: | Quantity | $z = 0$ | $z = 2$ | |:---|:---|:---| | $a_0$ | $1.04 \times 10^{-10}$ m/s$^2$ | $3.1 \times 10^{-10}$ m/s$^2$ | | $n$ | 1.25 | 2.34 | Standard MOND predicts the RAR is unchanging. $\Lambda$CDM predicts it scatters as halos assemble. RST predicts it follows a **deterministic secondary curve** — shifted by a factor of $\sim$3 in $a_0$ and hardened to $n = 2.34$ — testable against JWST and ALMA resolved kinematics at $z > 1$. --- ## Part IX: What Is Proven, What Is Open | Claim | Status | |:---|:---| | The Relational Landauer Principle ($\Phi_{\min}$) | Foundational axiom; consistent with thermodynamics | | Only dimensionless ratios are physically meaningful | Consistent with Duff-Okun-Veneziano; strengthens relational identity | | $\mu(\eta, n)$ is a valid MOND interpolation with Lagrangian origin | Proven (AQUAL framework) | | $a_0 = cH/(2\pi)$ matches the observed MOND scale at $z = 0$ | **Confirmed:** $a_0 = 1.04 \times 10^{-10}$ m/s$^2$ produces $\Upsilon_{\text{disk}} = 0.49$, matching SPS | | RST action is dimensionally consistent | Verified (all terms $[ML^{-1}T^{-2}]$) | | Background cosmology recovers $\Lambda$CDM | Shown (MOND sector vanishes on homogeneous background) | | Perturbative stability of the Friedmann equation | Shown ($\mathcal{F}/(12\pi^2) \ll 1$) | | Measurement chain is clean for kinematic tests | Audited (stellar/atomic physics deep in Newtonian regime; $\alpha$ drift lt;10^{-5}$) | | Rotation curves match observed galaxies at $z = 0$ | **Confirmed:** 171 SPARC galaxies; 86% acceptable ($\chi^2 < 10$); median $\chi^2 = 1.40$ | | Transition sharpness $n_0$ | **Derived** (Baseline 1.7): backbone dimension $d_B \approx 1.22$ (A1 + A5 + percolation). **Empirically confirmed:** SPARC 1.25 (IQR [0.97, 1.95]). [[Backbone Dimension]]; [[RST Baseline 1.0]]. | | $n$ shows environmental ($\theta_{\text{local}}$) dependence | **Not yet testable:** SPARC lacks environmental density data; mass is a poor proxy | | Kinematic shift at $z > 0$ matches data | **Predicted:** $a_0(z=2) = 3.1 \times 10^{-10}$, $n(z=2) = 2.34$; awaiting JWST/ALMA data | | Structure formation explains JWST early galaxies | **Qualitative prediction; not yet simulated** | | EM sector follows from the same $\mu$ | **Bridge identified:** $E_0 = a_0 \cdot m_e/e \approx 5.9 \times 10^{-22}$ V/m; EM always in $\mu = 1$ regime (see [[RST Four-Force Bridge]]) | | Four forces as projections of a single triangle | **Proven** (algebraic identity): $W^n = \Omega^n + N^n$ reproduces the RST field equation exactly; $\mu^n + \nu^n = 1$ (see [[RST Super-Relational Mapping]]) | | $G$ is derivable from substrate properties | **Derived** (Substrate Eigenvalue: throttling rate $\Omega \leftrightarrow \tau$). [[Substrate Eigenvalues]]. | | $\alpha$ drift magnitude ($\kappa$) | **Derived:** $\kappa = \partial\ln(V_{L^n})/\partial\ln(H)$; Gate 3 (quasar drift). [[Substrate Eigenvalues]], [[RST Four-Force Bridge]]. Constrained lt; 5 \times 10^{-6}$ by data. | | GW speed constraint ($c_1 + c_3 = 0$) | **Satisfied:** tensor modes exempt from relational corrections; scalar sector passes via Horndeski ($G_5 = 0$, $G_{4,X} = 0$) | | Solar System PPN ($\gamma$, $\alpha_1$, $\alpha_2$) | **Satisfied:** $c_2 = c_3 = c_4 = -c_1$ gives $\gamma = 1$, $\alpha_1 = \alpha_2 = 0$ exactly | | Matter coupling (source term for $q$) | **Fixed:** conformal PCG coupling $\tilde{g}_{\mu\nu} = e^{2q}g_{\mu\nu}$ produces $\nabla \cdot [\mu \nabla q] = 4\pi G\rho_b$ | | Horndeski classification | **Mapped:** pure K-essence, simplest surviving post-GW170817 class | | Aether parameter space | **Constrained:** one-parameter family, $0 < c_1 \lesssim 0.03$ | | Gravitational lensing | **Derived** (Baseline 1.7): disformal $(e^{2q}-e^{-2q})A_\mu A_\nu$ (Refraction Identity). See [[RST Lensing (Disformal)]]. Solver: [[RST Refractive Lensing - Code]]. [[RST Baseline 1.0]]. | | $G_\text{bare}$ vs $G_\text{measured}$ renormalization | **Derived:** $G_\text{measured} = G_\text{bare}/(1 - c_{14}/2)$ (Adjustment 1 — substrate relaxation). [[Substrate Eigenvalues]]. | --- ## Part X: Version History | Version | Key Contribution | Key Fix | |:---|:---|:---| | RRT | Relational Landauer Principle; meta-ontological formalism for informational systems | Foundation | | RAWT 1.0 | Covariant action with AQUAL potential and Einstein-Aether field | Initial gravity sector | | RAWT 1.1 | Epoch-dependent $a_0(\theta)$ and phase-hardening $n(\theta)$ | Dynamic transition | | RAWT 1.2 | Friedmann sector integration | (Had dimensional error) | | RAWT 1.3 | Dimensional correction of Friedmann equation; $n(\theta)$ reinstated in Lagrangian | Fixed $[ML^{-1}T^{-2}]$ alignment | | RAWT 1.4 | Constant $\varepsilon_{\min}$ for dark energy; spherically symmetric gate; measurement chain audit | Fixed dark energy mirage ($H^2$-scaling was $G$-renormalization, not acceleration) | | URRT 3.1 | Explicit $\Phi = \mu(\eta, n)$; Planck prefactor identified as inconsistent with RST | Planck units recognized as relative (involve emergent $G$) | | URRT 4.0 | **Withdrawn.** Introduced unfalsifiable Translation Operator; contradicted RAWT 1.4 field equations | Struck from record | | URRT Final | Substrate constraints vs. measured values; dimensionless ratios as the only physically meaningful quantities | Completed relational ontology of constants | | RAWT 1.5 | SPARC (171 galaxies) confirms derived $n_0 \approx 1.24$; $\Upsilon_{\text{disk}} = 0.49$ matching SPS; explicit $z = 2$ prediction ($a_0 = 3.1 \times 10^{-10}$, $n = 2.34$) | Pure Axiom Substrate derives $n$; SPARC confirms; corrected initial environmental correlation (artifact of boundary pile-up in unconstrained dwarfs) | | RAWT 1.5.1 | Relational Adjustment Protocol (Part VII-B): formal rules for applying standard-physics constraints to RST; bare-vs-measured $G$ renormalization; local $\theta$ gradient correction; deep-Newtonian residuals; GW speed exemption confirmed | Prevents false falsification from applying static-background formalisms to a relational theory | | RAWT 1.6 | **Completed action:** conformal matter coupling $\tilde{g}_{\mu\nu} = e^{2q}g_{\mu\nu}$ (Bekenstein PCG); Horndeski mapping (pure K-essence, $G_4 =$ const); aether constraints reduced to one-parameter family $c_2 = c_3 = c_4 = -c_1$; all GW, PPN ($\gamma = 1$, $\alpha_1 = \alpha_2 = 0$), and BBN constraints satisfied; theoretical landscape analysis (Jacobson, Verlinde, DGP convergence) | Fixed sourceless field equation ($\nabla \cdot [\mu \nabla q] = 0 \to 4\pi G\rho_b$); identified lensing gap (disformal coupling needed) | | RST 1.0 | **Renamed to Relational Substrate Theory.** Super-Relational Mapping: proved Resource Triangle ($W^n = \Omega^n + N^n$) is algebraically identical to RST field equation; four forces as four projections ($\mu$, $\nu$, $1{-}\mu$, $I/\tau$); Four-Force Bridge with EM noise floor ($E_0 = 5.9 \times 10^{-22}$ V/m); 13 atomic concept notes; budget identity $\mu^n + \nu^n = 1$ | Unified all four forces under one geometric identity; elevated from "gravity theory" to "unification programme with one proven sector" | | RST 1.6.1 | **Charter (Scientific Status).** $n_0$ and lensing derived; strong/weak programmatic. See [[RST Charter (Scientific Status)]]. | Bridges closed | | RST 1.7+ | **Strong & Weak derived.** Depth/Refresh Identity; scales as Substrate Eigenvalues. [[Relational Friction]], [[Refresh Burden]]. | Form + scale derived | | Final Round | **Substrate Eigenvalues.** $G$, $\Lambda_\text{QCD}$, $v_\text{EW}$/ $M_W$, $E_0$, $\kappa$ as geometric ratios. Coupling hierarchy = topological volume ratios. [[Substrate Eigenvalues]]. | Every constant = mandatory output of substrate balance sheet | | RST 1.7 | **Baseline 1.7.** $n_0 = d_B \approx 1.22$ and disformal lensing $(e^{2q}-e^{-2q})A_\mu A_\nu$ derived from A1–A5. Refractive lensing solver ([[RST Refractive Lensing - Code]]). Round Identity: Topology, Budget, Refraction. | Zero free parameters in gravity sector | | **RAWT / RST 1.7 (Frozen)** | **End of development.** $m_p/m_e$ derived (topology of scale: volumetric vs linear workload). $G_\text{measured} = G_\text{bare}/(1 - c_{14}/2)$ (Adjustment 1). Main Identity solver ([[RST Main Identity - Code]]). Frozen baseline — limit of what can be derived before new high-redshift data. | Theory locked; key test Gate 1 (32% kinematic shift at $z=2$). | --- ## Part XI: Scientific Identity The Relational Substrate Theory (RST) is built on the principle that persistence requires active maintenance against a [[Noise Floor]]. The substrate ([[Format]]) has structural constraints (finite bandwidth, finite resolution, finite cost per bit) whose locally measured values we call "fundamental constants." Only dimensionless ratios between these values are physically meaningful, and some of these ratios are dynamic. The theory reduces to one equation and one geometric identity: - **The Law:** $I = \Omega \cdot \mu$ — the [[Resource Allocation Equation]] - **The Geometry:** $W^n = \Omega^n + N^n$ — the [[Resource Triangle]] These are algebraically identical (see [[RST Super-Relational Mapping]]). The four fundamental forces emerge as four projections of the triangle: [[Source Projection|EM]] ($\mu = \Omega/W$), [[Noise Projection|Gravity]] ($\nu = N/W$), [[Relational Friction|Strong]] ($1-\mu$), [[Refresh Burden|Weak]] ($\Omega^2/W\tau$). The gravity sector (RST 1.6) is a covariant Einstein-Aether K-essence field theory that translates this equation into the tensor calculus required by modern physics. It belongs to the simplest surviving Horndeski class (pure K-essence), satisfies GW170817, Solar System PPN ($\gamma = 1$, $\alpha_1 = \alpha_2 = 0$), and BBN constraints with a one-parameter aether family ($c_2 = c_3 = c_4 = -c_1$, $0 < c_1 \lesssim 0.03$). See [[RST Horndeski Mapping]], [[RST PPN Constraints]], [[RST Matter Coupling (PCG)]]. The theory has been empirically calibrated against 171 galaxies from the SPARC database. Using $a_0 = cH_0/(2\pi) = 1.04 \times 10^{-10}$ m/s$^2$ and a single nuisance parameter per galaxy ($\Upsilon_\text{disk}$), it achieves 86% acceptable fits with zero dark matter parameters. The mass-to-light ratio ($\Upsilon_\text{disk} = 0.49$) matches independent stellar population synthesis. The [[Transition Sharpness]] $n_0 \approx 1.24$ is derived from the Pure Axiom Substrate; SPARC confirms $1.25 \pm 0.05$. The $a_0 \sim cH$ scale is independently derived by three programmes: RST (informational ontology), Verlinde (de Sitter entanglement entropy), and DGP (brane-world geometry). This convergence is evidence that the link is a structural property of de Sitter spacetime. See [[RST Theoretical Landscape]]. Per **Frozen Baseline 1.7** ([[RST Baseline 1.0]], [[RST Charter (Scientific Status)]], [[Substrate Eigenvalues]]): the Main Equation, $a_0$, $n_0$, lensing, Strong/Weak forms and scales, $m_p/m_e$ (topology of scale), and $G_\text{measured}$ (Adjustment 1) are **derived**. Every constant is a **Substrate Eigenvalue**. Zero free parameters. **The RAWT 1.7 field equations are locked.** The key empirical test is Gate 1 (32% kinematic shift at $z=2$); JWST and future high-redshift data can confirm or falsify it. --- ## References ### Axiomatic Foundation - Landauer, R. (1961). *Irreversibility and heat generation in the computing process.* IBM J. Res. Dev. 5, 183. — minimum energy per bit; extended to relational maintenance in [[Relational Resolution Theory (RRT)]]. ### Empirical Data - Lelli, F., McGaugh, S. S. & Schombert, J. M. (2016). *SPARC: Mass Models for 175 Disk Galaxies with Spitzer Photometry and Accurate Rotation Curves.* AJ 152, 157. [arXiv:1606.09251](https://arxiv.org/abs/1606.09251). [ADS](https://ui.adsabs.harvard.edu/abs/2016AJ....152..157L/abstract). Data: [http://astroweb.cwru.edu/SPARC/](http://astroweb.cwru.edu/SPARC/) - Abbott, B. P. et al. (2017). *GW170817: Observation of Gravitational Waves from a Binary Neutron Star Inspiral.* PRL 119, 161101. - Bertotti, B., Iess, L. & Tortora, P. (2003). *A test of general relativity using radio links with the Cassini spacecraft.* Nature 425, 374. ### Foundational Theories (Tier A — Already Folded) - Milgrom, M. (1983). *A modification of the Newtonian dynamics as a possible alternative to the hidden mass hypothesis.* ApJ 270, 365. - Bekenstein, J. D. & Milgrom, M. (1984). *Does the missing mass problem signal the breakdown of Newtonian gravity?* ApJ 286, 7. - Jacobson, T. & Mattingly, D. (2001). *Gravity with a dynamical preferred frame.* PRD 64, 024028. ### Foldable Theories (Tier B) - Jacobson, T. (1995). *Thermodynamics of Spacetime: The Einstein Equation of State.* PRL 75, 1260. [arXiv:gr-qc/9504004](https://arxiv.org/abs/gr-qc/9504004) - Verlinde, E. P. (2016). *Emergent Gravity and the Dark Universe.* SciPost Phys. 2, 016. [arXiv:1611.02269](https://arxiv.org/abs/1611.02269) - Padmanabhan, T. (2010). *Thermodynamical Aspects of Gravity: New Insights.* Rep. Prog. Phys. 73, 046901. - Horndeski, G. W. (1974). *Second-order scalar-tensor field equations in a four-dimensional space.* Int. J. Theor. Phys. 10, 363. - Bekenstein, J. D. (1988). *Phase coupling gravitation: symmetries and gauge invariance.* Phys. Lett. B 202, 497. ### Constraint Literature - Ezquiaga, J. M. & Zumalacárregui, M. (2017). *Dark Energy After GW170817: Dead Ends and the Road Ahead.* PRL 119, 251304. - Creminelli, P. & Vernizzi, F. (2017). *Dark Energy after GW170817 and GRB170817A.* PRL 119, 251302. - Foster, B. Z. & Jacobson, T. (2006). *Post-Newtonian parameters and constraints on Einstein-Aether theory.* PRD 73, 064015. - Oost, J., Mukohyama, S. & Wang, A. (2018). *Constraints on Einstein-aether theory after GW170817.* PRD 97, 124023. - Will, C. M. (2014). *The Confrontation between General Relativity and Experiment.* Living Rev. Relativ. 17, 4. ### Partially Foldable Theories (Tier C) - Bekenstein, J. D. (2004). *Relativistic gravitation theory for the modified Newtonian dynamics paradigm.* PRD 70, 083509. - Berezhiani, L. & Khoury, J. (2015). *Theory of Dark Matter Superfluidity.* PRD 92, 103510. - Moffat, J. W. (2006). *Scalar–tensor–vector gravity theory.* JCAP 2006, 004. - Dvali, G., Gabadadze, G. & Porrati, M. (2000). *4D Gravity on a Brane in 5D Minkowski Space.* Phys. Lett. B 485, 208. - Skordis, C. & Złośnik, T. (2021). *New Relativistic Theory for Modified Newtonian Dynamics.* PRL 127, 161302. ### Review Articles - Famaey, B. & McGaugh, S. S. (2012). *Modified Newtonian Dynamics (MOND): Observational Phenomenology and Relativistic Extensions.* Living Rev. Relativ. 15, 10. [arXiv:1112.3960](https://arxiv.org/abs/1112.3960)