Imagine two friends performing a quantum experiment. One measures an electron's spin and records the result. The other, standing outside the lab, describes the same electron as still being in superposition until she opens the door. Both descriptions are simultaneously correct. Neither is more fundamental than the other. This is not a puzzle to be solved but the actual structure of reality according to one of the most radical interpretations of quantum mechanics.
The relational interpretation, developed primarily by Carlo Rovelli in the mid-1990s, proposes something startling: quantum states are not properties that systems possess in isolation. They are relations between systems. There is no absolute quantum state of the universe, no God's-eye view from which the true wavefunction can be read. Every physical description is a description relative to something else.
This move dissolves the measurement problem that has haunted quantum mechanics since its birth. But it does so at a considerable cost: we must abandon the intuition that there exists a single, shared reality independent of the relations between physical systems. What replaces it is stranger and, perhaps, more honest about what our best theory has been telling us all along.
No View from Nowhere
The classical worldview inherits from Galileo and Newton a powerful assumption: reality consists of objects with definite properties, and observers merely record what is already there. Quantum mechanics fractured this picture, but most interpretations attempt to repair it. Many-worlds preserves objectivity by multiplying universes. Bohmian mechanics preserves it through hidden variables. Copenhagen preserves it by drawing a mysterious line between quantum and classical realms.
Rovelli's relational interpretation takes a different path. It refuses to reconstruct any absolute reality behind the equations. Instead, it insists that the wavefunction always describes the state of a system relative to another system. When we write ψ for an electron, we are implicitly writing ψ relative to some reference frame, some measuring apparatus, some other physical system that will interact with it.
Crucially, no observer is privileged. A photon can serve as an observer for an atom, just as a physicist serves as an observer for a laboratory. Consciousness plays no special role. What matters is only that two systems interact and thereby become correlated. The interaction itself is the measurement, and the measurement is always relative to one of the interacting parties.
This is a radical extension of Einstein's relativity. Special relativity taught us that simultaneity is relative to a reference frame. General relativity made the geometry of spacetime itself relational. Relational quantum mechanics completes this trajectory by making the very facts of the world relational. There is no fact of the matter about whether the electron has spin up, only facts about spin up relative to specific systems.
The philosophical resonance with Leibniz is unmistakable. Leibniz argued against Newton that space and time were not absolute containers but systems of relations. Three centuries later, quantum mechanics may be vindicating him in a domain he could not have imagined.
TakeawayPhysical properties are not intrinsic possessions of objects but arise from their interactions with other systems. To ask what something 'really is' apart from all relations may be to ask a question with no physical content.
Measurement Naturalized
The infamous measurement problem asks why quantum systems evolve smoothly according to the Schrödinger equation until someone measures them, at which point they mysteriously collapse into a definite state. This apparent dualism—unitary evolution versus discontinuous collapse—has generated nearly a century of interpretive controversy. Where exactly does the collapse occur? What counts as a measurement? Does consciousness matter?
In the relational framework, these questions dissolve rather than resolve. There is no collapse in any absolute sense. When system A interacts with system B, the quantum state of A relative to B updates in accordance with the interaction. But relative to a third system C that has not yet interacted with either A or B, the composite AB remains in superposition. Both descriptions are complete, correct, and irreducible.
The measurement is thus stripped of its metaphysical weight. It becomes just another physical interaction, no different in kind from an electron scattering off a proton. What we call 'measurement' is simply the specific class of interactions where a system becomes correlated with a macroscopic apparatus. The apparatus is not epistemically special—it is merely large enough that decoherence quickly stabilizes the correlation.
This naturalization preserves every empirical prediction of standard quantum mechanics. The Born rule still applies, expectation values are unchanged, and the mathematics is identical. What changes is the ontology: we no longer need a mysterious mechanism that promotes possibilities into actualities. Actualities are always for some system, and the shift from possibility to actuality is just the establishment of a correlation.
One might object that this makes quantum mechanics unhelpfully perspectival, but Rovelli argues the opposite. The theory becomes more consistent, more parsimonious, and more compatible with special relativity, which has no place for instantaneous collapse events happening across space.
TakeawayThe measurement problem may not be a problem to solve but a symptom of insisting on an observer-independent reality that quantum mechanics has never actually described.
The Consistency Challenge
If every observer has their own set of relative facts, how do we ever agree on anything? When two physicists compare notes about an experiment, why do their accounts cohere so seamlessly? This is the consistency challenge, and it is where the relational interpretation faces its most serious tests.
The standard response is that when observers compare results, they are themselves engaging in a physical interaction. Observer B's records about the electron become correlated with observer A through their communication. The quantum formalism guarantees that these correlations will be consistent: if A saw spin up relative to their apparatus, then A's report to B will be a report of spin up relative to B. Agreement emerges from the structure of the interactions, not from access to a shared underlying reality.
But recent thought experiments, particularly the Frauchiger-Renner paradox and Wigner's friend scenarios extended by Brukner and others, have complicated this picture. These setups suggest that observers who each apply quantum mechanics consistently to their situations can arrive at contradictory conclusions about the same events. The relational interpretation must argue that no genuine contradiction arises because the facts belong to different relational contexts.
This response is coherent but philosophically demanding. It requires accepting that there is no meta-perspective from which all relational facts can be assembled into a single narrative. Reality is genuinely fragmented into a web of pairwise relations, and any attempt to unify them into one story imports an assumption the theory rejects.
Debates continue over whether this fragmentation is a feature or a bug. Some philosophers argue it renders science incoherent; others see it as the appropriate humility demanded by a genuinely quantum world. The empirical predictions remain unchanged, so the disagreement is about what we should accept as the price of understanding.
TakeawayConsistency between observers may be an emergent property of physical correlations rather than evidence of a shared underlying reality. Agreement is achieved through interaction, not discovered through common access to facts.
The relational interpretation asks us to give up something we have always taken for granted: the notion that reality has properties independent of relations. In return, it offers a quantum mechanics without observers, without collapse, and without the dualism that has troubled the theory since its inception.
Whether this trade is worth making remains contested. But the interpretation reminds us that our discomfort with quantum mechanics may reflect not defects in the theory but the persistence of pre-quantum intuitions we have never fully surrendered. Perhaps the theory has been telling us all along that the world is not made of things but of relations.
Heisenberg once suggested that atoms are not things but tendencies. Rovelli extends this insight to its logical endpoint: the entire quantum world is not a collection of entities with properties but a network of interactions in which properties arise only when systems meet.