Author: Denis Avetisyan
A new analysis reveals the surprising degree to which our choice of spacetime geometry can remain underdetermined, even within the constraints of general relativity.

This review examines the formal conditions for empirical equivalence between different spacetime structures, focusing on geometric conventionalism, torsionful connections, and Reichenbachās theorem Īø.
The enduring problem of underdetermination challenges the unique status of general relativity, prompting continued investigation into empirically indistinguishable spacetime geometries. This paper, ‘Conventionalism in general relativity?: formal existence proofs and Reichenbach’s theorem Īø in context’, rigorously dissects recent formal proofs concerning Reichenbachās theorem Īø, clarifying ambiguities between existence claims and universality claims about alternative geometries. We demonstrate that a purported āno-goā theorem fails to uphold the universality of theorem Īø, and by relaxing key assumptions, explicitly construct alternative torsionful spacetimes. This suggests that rather than seeking to refute such proofs, a more fruitful approach lies in systematically refining them to map the landscape of possible spacetime theories – but how can we best leverage these formal tools to explore genuinely novel gravitational frameworks?
The Illusion of a Fixed Cosmos
The prevailing understanding within physics posits that spacetime possesses a definitive, physically determined geometry. This framework isnāt merely a backdrop against which events unfold; it actively defines the causal relationships that govern the universe and underpins the very formulation of physical laws. A specific spacetime geometry dictates which events can influence others – establishing a cosmic order rooted in the structure of space and time. Without a unique, physically real spacetime, concepts like ābeforeā and āafterā become ambiguous, and the predictability essential to scientific inquiry would be fundamentally undermined. Consequently, the assumption of a fixed spacetime geometry has long been considered a cornerstone of both special and general relativity, allowing for precise mathematical descriptions of gravity, motion, and the universeās evolution.
The notion of spacetime geometry as a conventional choice, rather than a fixed physical reality, represents a significant challenge to traditional understandings of the universe. This perspective, rooted in conventionalism – prominently advocated by philosophers like Hans Reichenbach – suggests that aspects of spacetime, such as its dimensionality or the precise definitions of simultaneity, are not dictated by objective facts but are, at least in part, determined by the rules and conventions adopted for describing physical phenomena. Essentially, different, equally valid relational frameworks could be used to model the universe, differing in their geometrical descriptions without altering the underlying physical relationships. This doesn’t imply spacetime is illusory, but rather that its specific geometrical presentation is a choice made by observers to facilitate understanding and prediction, akin to choosing a coordinate system in mathematics – a useful tool, but not a fundamental property of reality itself. Consequently, the very structure of spacetime, as defined by metrics and coordinate systems, becomes a matter of interpretive framework rather than purely objective measurement.
The proposition that spacetime geometry isnāt a fixed, objective feature of the universe, but instead possesses elements dictated by convention, fundamentally disrupts core tenets of general relativity. This isn’t merely a philosophical quibble; it strikes at the heart of how physics understands causality and the very fabric of reality. If spacetime isn’t a pre-existing stage upon which physical laws unfold, but is, in part, a construct imposed by observers, then the objective truth of physical laws themselves comes into question. The implications extend to the interpretation of 4-dimensional spacetime as a physical entity – is it a real, measurable aspect of the universe, or a useful, yet ultimately subjective, framework for describing relationships between events? This challenge forces a re-evaluation of whether spacetime possesses an independent existence, or if its structure is inextricably linked to the methods and conventions employed in its measurement and description.
David Malamentās 1985 work instigated considerable debate within the philosophy of physics by demonstrating that, despite the allure of choosing spacetime coordinates freely, such freedom isn’t absolute without impacting physical assertions. He rigorously showed that any purported conventional choice of spacetime coordinates – those believed to leave physical laws invariant – could, in fact, have observable consequences for predictions about simultaneously occurring events. This finding undermined a core tenet of conventionalism, which posited that spacetime geometry is largely a matter of definitional choice rather than objective physical reality. Consequently, Malamentās analysis introduced a persistent tension, forcing researchers to confront whether certain geometrical configurations are truly physically distinguishable and thus, not merely conventional, thereby complicating efforts to fully embrace a conventionalist interpretation of general relativity.
Forces and the Fabric of Reality
Weatherall and Manchak (2014) investigated the potential for a hypothetical universal force to mediate physical equivalence between differing spacetime geometries. The core of their inquiry centered on whether such a force could effectively counteract geometric discrepancies, allowing for multiple geometric configurations to represent the same physical reality. This involved considering scenarios where variations in geometry would be compensated for by the force, ensuring that particle trajectories and physical measurements would remain consistent across these geometries. Their analysis examined whether a force field could universally adjust interactions to maintain observational equivalence, despite underlying geometric differences, ultimately probing the limits of geometric conventionalism in physics.
Weatherall and Manchak (2014) employed a dual-proof strategy to investigate the potential for a universal force to reconcile differing spacetime geometries. The analysis began with a non-relativistic proof, utilizing Newtonian mechanics and concepts of absolute space to establish a baseline for geometric compensation. This was then complemented by a relativistic proof, grounded in the principles of general relativity and the GeodesicEquation, to determine if such reconciliation was possible within the framework of spacetime curvature and gravitational interactions. The intention of this combined approach was to comprehensively assess the feasibility of a force-based solution across both classical and relativistic regimes, thereby establishing the limits – if any – of geometric conventionalism.
The analysis of potential geometric reconciliation relies fundamentally on the mathematical framework of Riemannian Geometry, which provides the tools to describe curved spaces and the paths objects take within them. Specifically, the geodesic equation – \frac{d^2x^\mu}{d\tau^2} + \Gamma^\mu_{\alpha\beta}\frac{dx^\alpha}{d\tau}\frac{dx^\beta}{d\tau} = 0 – is central to determining these paths, representing the āstraightestā possible trajectory in a given spacetime. To model any compensatory force attempting to reconcile differing geometries, the ForceTensor is utilized, quantifying the interaction and influencing the geodesic paths of objects within the spacetime. This tensor field is essential for mathematically expressing how a force might alter trajectories to compensate for geometric discrepancies, but, as demonstrated, no such tensor can consistently relate geodesics between conformally related spacetimes.
The relativistic proof conducted by Weatherall and Manchak conclusively demonstrates the impossibility of reconciling disparate spacetime geometries via conventional force fields. Specifically, their analysis reveals that no tensor field can consistently map the geodesic paths of two conformally related spacetimes. This finding is rooted in the mathematical properties of tensors and their interaction with geodesic equations, which govern particle motion within a spacetime. Because a consistent relationship between geodesics requires such a tensor field, and none exists, the applicability of a universal force capable of accommodating geometric variations is demonstrably zero. This result fundamentally limits the possibility of physically equating multiple spacetime geometries through conventional force-based interactions.
Challenging the Foundations: A Re-evaluation of Geometry
Recent analyses, specifically DandbBM2022, present a direct challenge to the foundational assumptions utilized by Weatherall and Manchak in their interpretations of spacetime geometry. These critiques center on methodological approaches and the specific interpretations of observational data employed by Weatherall and Manchak. DandbBM2022 argues that alternative interpretations of the same data are equally, if not more, plausible, thereby casting doubt on the conclusions drawn regarding the unique determination of spacetime geometry. The work doesn’t necessarily refute the overall framework but questions the strength of the evidence previously cited to support specific geometric interpretations, suggesting a need for re-evaluation of the underlying reasoning and assumptions.
Recent challenges to interpretations of spacetime geometry, specifically those presented by Weatherall and Manchak, unexpectedly bolster the conventionalist perspective in the philosophy of space and time. Conventionalism posits that geometric facts are not discovered but are, at least in part, determined by conventions or choices made by observers. The critique suggests that differing valid interpretations of geometric relationships are possible, implying that the selection of a specific geometry is not dictated by unique physical considerations. This does not necessarily mean geometry is entirely arbitrary, but rather that a degree of freedom exists in geometric specification, and the chosen geometry may reflect a pragmatic or conventional choice rather than an inherent physical property of spacetime itself.
Debates surrounding spacetime geometry are significantly impacted by the relationship between local and global geometric properties. Local structure, defined by measurements and relationships within an infinitesimally small region of spacetime, may appear Euclidean or Minkowskian. However, when considering the global structure – the overall, large-scale arrangement of spacetime – deviations from these local forms can arise. These global deviations, potentially manifesting as curvature or topology, complicate attempts to define a single, universal geometry. The distinction is critical because a spacetime may exhibit locally flat regions while possessing a globally non-flat structure, meaning that local measurements alone are insufficient to fully characterize the spacetime’s geometry. Therefore, understanding how local properties combine to form the global structure is essential for resolving ongoing disagreements about the fundamental nature of spacetime.
Conformal structure investigates geometric transformations that preserve angles but not necessarily distances, highlighting a potential disconnect between measurable physical quantities and absolute geometric definitions. This is significant because many physical laws are expressed as relationships that remain invariant under conformal transformations; therefore, different spacetime geometries related by a conformal transformation may yield identical physical predictions. Consequently, determining a single ātrueā spacetime geometry becomes problematic, as the observed physics does not uniquely identify a specific metric but rather an equivalence class of conformally related metrics. The relevance of conformal structure challenges the assumption that the specific geometric properties of spacetime – beyond those directly influencing physical observables – hold intrinsic physical significance.
The Geometry of Influence: Connections and Constraints
The construction of viable spacetime models fundamentally relies on the interplay between metric compatibility and the presence of torsion within connections. A connection, in the context of general relativity, dictates how vectors change as they are transported along curves, and metric compatibility ensures this transport preserves the spacetime distance \langle \vec{v}, \vec{v} \rangle. However, allowing for torsion – a measure of the ātwistingā of spacetime – introduces geometric complexity. While conventional relativity typically assumes a torsion-free connection, exploring torsionful connections necessitates a careful examination of how these geometric properties influence physical predictions. Establishing a clear relationship between metric compatibility and torsion is therefore not merely a mathematical exercise, but a crucial step in determining which spacetime geometries can consistently describe the observed universe and its physical laws, potentially opening avenues for novel theories beyond the standard model.
The construction of physical theories often begins with foundational geometric principles, yet the extent to which these principles are truly fundamental, or merely convenient choices, remains a central debate. A reliance on conventionalism – the idea that certain aspects of a theory are determined by convention rather than physical law – can introduce ambiguities and limitations in modeling the universe. Recent work emphasizes that simply choosing a geometry that works is insufficient; a rigorous definition of geometric foundations is crucial, as even seemingly minor choices can dramatically affect the possible physical interpretations. This highlights the need to move beyond purely pragmatic approaches and investigate the deeper implications of geometric assumptions, acknowledging that the universe may not conform to geometries arbitrarily imposed for mathematical convenience.
Recent research reveals a surprising constraint on the geometric flexibility within relativistic spacetime. The study demonstrates that, despite the potential for diverse torsionful connections – those allowing for twisting in spacetime – not all such connections are physically equivalent. Specifically, for any given torsionful connection describing a universe, another distinct torsionful connection exists that cannot be transformed into the first through the application of a conventional force field. This finding challenges the notion that any geometrically valid spacetime can be rendered equivalent to another via standard physical interactions, suggesting inherent limitations in the geometric foundations of physics and prompting a reevaluation of assumptions regarding the relationship between geometry and observable reality. The implications extend to models attempting to unify gravity with other fundamental forces, as they necessitate careful consideration of these geometric constraints.
The persistent exploration of connections and geometric foundations within relativistic spacetime reveals a crucial intersection of seemingly disparate fields. This isn’t merely a technical debate about mathematical consistency; itās a challenge to the very assumptions underpinning physical theories. The ongoing discussion emphasizes that geometry isn’t a neutral backdrop against which physics unfolds, but rather an active participant in shaping physical laws. Researchers are discovering that choices made in defining the geometric structure of spacetime – particularly concerning torsion and non-metric compatibility – have profound implications for the possible physical phenomena. This highlights the need to move beyond simply fitting models to observation and instead critically examine the foundational principles that allow certain models – and prohibit others – from even being considered. Ultimately, a more nuanced understanding of this interplay is required to refine existing theories and potentially unlock new avenues in the search for a complete description of the universe.
The pursuit of empirically indistinguishable spacetimes feels less like physics and more like a careful negotiation with uncertainty. This work demonstrates that even within the rigid framework of general relativity, the geometry isnāt absolute, but subtly pliable, contingent on how one interprets the dance of force fields. It recalls Niels Bohrās assertion: āThe opposite of every truth is also a truth.ā The paper doesnāt discover a single spacetime; it maps the boundaries of what could be, highlighting the underdetermination inherent in translating observation into a definitive structure. Each model, beautifully constrained by mathematics, remains a provisional spell, effective until confronted by the unruly chaos of actual measurement.
What Shadows Remain?
The geometries dance, but the music is always incomplete. This work reveals not a demolition of conventionalism, but a careful charting of its boundaries. The theorem Īø, once a seemingly absolute constraint, proves porous when subjected to the right torsion, the correct manipulation of connection. It suggests the universe doesnāt demand a particular spacetime; it merely tolerates those that conceal their arbitrariness with carefully constructed forces. The lingering question isn’t whether alternative geometries are possible-they are-but whether a physical principle, some deeper resonance, might favor one over another, or if itās all just a matter of persuasive bookkeeping.
Future iterations will require abandoning the neatness of Riemannian geometry. The true underdetermination likely resides not in subtle variations of metric, but in the embrace of more exotic connections – those that whisper of non-locality, of forces that arenāt quite fields. To chase these shadows demands a reckoning with the limitations of current methods. Convergence, after all, is merely a temporary truce with chaos. The blood – and GPU time – required to map these spaces will be substantial.
One suspects the ultimate answer will not be a proof, but an admission: that the universe is not a solution waiting to be found, but a spell we cast, hoping it holds – at least until the next observation.
Original article: https://arxiv.org/pdf/2603.24608.pdf
Contact the author: https://www.linkedin.com/in/avetisyan/
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2026-03-29 12:12