We review the postulates of quantum mechanics with respect to the representation of physical states and measurable quantities, their time evolution, and the interpretation of measurements. We first formulate the postulates in terms of wave functions and differential operators, and then reformulate them in the abstract Hilbert space of state vectors, using Dirac’s notations. Improper states subject to Dirac’s delta normalization are introduced, and the space of physical states is extended to include them. The postulates are rationalized by associating each Hermitian linear operator with a complete orthonormal system of its eigenvectors, where measurement probabilities depend on the projections of these eigenvectors on the system’s state vector. Particularly, wave functions are identified as projections of state vectors on the position operator eigenstates. State vectors representing multidimensional systems are formulated as tensor products of vectors in their subspaces. Finally, we address the general uncertainty relations in simultaneous measurements of different observables.
The relationship between physical notions and the structures expressing them is an issue of primary importance the history and philosophy of pre-modern natural philosophy and of modern science. Historical evidence suggests that, when investigating the relationship between physics and mathematics, one should pay attention to the material, sensually perceivable forms mediating it: spoken or written words, drawings, artefacts, descriptions of experimental set-ups or, as the case discussed the present paper, symbolic notation. The reason for this is that, historically, physical notions and their expressions have very often been developed as one, and only distinguished from each other at a later stage. This was for example the case with what we today regard as mathematical and classical mechanics, which were developed the course of the eighteenth century as the discipline of the analysis of motion. When considered from a later point of view, both the physical notions and the concepts involved historical developments appear as being in flux, vague, and, as far as the side is concerned, non-rigorous. In such cases, verbal description, mechanical artefacts or symbols do not simply mediate between physical notions and structures, as might be the case at a later stage, but represent both of them one, allowing the historical actors to construct and manipulate physical-mathematical meaning by following, at times, their physical reasoning and, at times, their criteria of rigour. The history of quantum mechanics offers many examples of how new physics and new mathematics can emerge as one, with symbolic notation playing a central role shaping both. Among the many creators of quantum theory, Paul Dirac was particularly sensitive to questions of notation:
W Pauli pointed out that the existence of a self-adjoint time operator is incompatible with the semi-bounded character of the Hamiltonian spectrum. As a result, there has been much argument about the time–energy uncertainty relation and other related issues. In this paper, we show a way to overcome Pauli's argument. In order to define a time operator, by treating time and space on an equal footing and extending the usual Hamiltonian Ĥ to the generalized Hamiltonian Ĥ μ (with Ĥ 0 = Ĥ), we reconstruct the analytical mechanics and the corresponding quantum (field) theories, which are equivalent to the traditional ones. The generalized Schrödinger equation i∂ μ ψ = Ĥ μ ψ and Heisenberg equation d /d x μ = ∂ μ + i[Ĥ μ , ] are obtained, from which we have: (1) t is to Ĥ 0 as x j is to Ĥ j ( j = 1, 2, 3); likewise, t is to i∂ 0 as x j is to i∂ j ; (2) the proposed time operator is canonically conjugate to i∂ 0 rather than to Ĥ 0 , therefore Pauli's theorem no longer applies; (3) two types of uncertainty relations, the usual Δ x μ Δ p μ ≥ 1/2 and the Mandelstam–Tamm treatment Δ x μ Δ H μ ≥ 1/2, have been formulated.
Foundations of physics · For the general reader The Relational Architecture of Time Emergent temporal order, delayed-choice photon experiments, and the thermodynamic arrow — a complete mathematical account, explained from the ground up János Gábor Melegh The Relational Architecture of TimeEmergent temporal order, delayed-choice photon experiments, and the thermodynamic arrow. Copyright © 2026 János Gábor Melegh. All rights reserved. No part of this book may be reproduced in any form without written permission from the author, except for brief quotations in reviews and scholarly works. This book unifies and expands two research manuscripts by the author: Time as an Emergent Relational Structure (2026) and Relational Time Structure in Delayed-Choice Photon Experiments (axiomatically extended version, 2026). Every definition, theorem, proof, and derivation of those works is reproduced here in full and without abridgement; the surrounding prose has been substantially expanded so that a motivated reader without formal training in physics or mathematics can follow the entire argument. First English edition, 2026. Preface How to Read This Book This is a book about a deceptively simple question: what is time, physically? Not what a clock reads, and not how time feels, but what structure in the physical world earns the name "time" at all. The answer defended here can be stated in one sentence: time is not a fundamental ingredient of the universe but an emergent, relational structure — an ordering that arises when physical descriptions defined through interaction fit together consistently, with its familiar one-way direction supplied separately by thermodynamics. That single sentence carries a lot of machinery, and this book unpacks all of it. The book makes an unusual promise, and it is worth stating explicitly: The promise of this book Nothing has been simplified away. Every equation, every definition, every theorem, and every proof from the underlying research papers appears here in full. What has been added — greatly — is explanation: before and after each formal step you will find plain-language accounts of what the symbols say, why the step matters, and what would go wrong without it. If you skip the equations entirely, the prose still tells a complete story. If you read the equations, the prose tells you exactly how to read them. Throughout the book you will meet a small family of recurring boxes, each with a fixed job: In plain language (copper boxes) — the intuition. What a formal statement means in everyday terms, often with an analogy. Definitions (blue boxes) — precise introductions of new mathematical objects. These are the vocabulary of the theory. Theorems (framed boxes) — the claims that are actually proved, followed by their proofs in full. A proof ends with the traditional square symbol □. Warnings and scope limits (red boxes) — the places where the theory deliberately stops claiming things. These boxes are part of the scientific content, not decoration: a theory earns trust partly by declaring its own boundaries. A five-minute notation primer Readers who have never used the notation of quantum mechanics need only a handful of symbols, all introduced properly when they first appear. As a preview:
∣ψ⟩ — a "ket," the standard label for a quantum state. Think of it as the complete catalogue of what quantum theory says about a system.
ρ — a density operator, the more general bookkeeping device for quantum states, including states known only statistically.
Tr — the trace, a summing-up operation.
TrB ("partial trace over
B") means: average away everything about subsystem
B and keep the rest.
P(x∣b) — the probability of outcome
x given setting
b. Ordinary conditional probability.
e1≺e2 — event
e1 causally precedes event
e2; it can influence it.
∑ — a sum;
sup and
inf — the least upper bound and greatest lower bound of a set of numbers, close cousins of "maximum" and "minimum." Everything else — beam splitters, POVMs, quantum channels, entropy, modular flow — is built up step by step in the chapters where it is needed, and Appendix A collects every symbol in one table. The shape of the argument Part I poses the problem of time and develops the conceptual core: relational description, the principle of relational consistency, the removal of subjective experience from the foundations, and the division of labor between relational ordering and thermodynamic direction. Part II takes the framework into the laboratory. It builds the full mathematical toolkit from scratch and then works through the two most notorious "time-bending" experiments of quantum optics — Wheeler's delayed choice and the delayed-choice quantum eraser — with complete derivations, showing that nothing in them requires the future to reach back into the past. Part III formalizes relational consistency exactly, explains what a physical record is, de-mystifies the "observer" (including a careful treatment of the Wigner's-friend and Frauchiger–Renner thought experiments), and shows the correct use of causal event graphs. Part IV separates order from direction, develops the thermodynamic arrow, connects the framework to thermal time and to neighboring research programs. Part V asks the hardest questions of any theory — what does it mean, and how could it be wrong? — and closes with a complete empirical research program and conclusions. What this book does not claim This book does not announce a new physical force, a new dynamical law, or an experimental result that contradicts standard quantum mechanics. Its framework is deliberately, provably empirically equivalent to standard quantum theory in every laboratory situation treated here. Its contribution is a rigorously constrained conceptual and mathematical reconstruction: an account of what time is, and of what delayed-choice experiments do and do not show, that is causally clean, fully formalized, and — crucially — falsifiable in the precise, limited sense worked out in Chapter 22. Readers deserve to know which statements are established mathematics, which are structural proposals, and which are open questions; this book labels all three throughout. Contents Table of Contents Preface: How to Read This Book Part I — The Problem of Time 1. Why Time Is a Problem 2. Relational Descriptions in Contemporary Physics 3. Relational Consistency as a Structural Principle 4. Time Without Experience 5. Relational Ordering and Thermodynamic Asymmetry 6. Ontological Implications and Open Questions Part II — The Laboratory of Time 7. Aim and Scientific Status 8. The Experimental Foundation 9. The Mathematical Toolkit 10. Postulates of the Relational-Time Delayed-Choice Model 11. Wheeler's Delayed Choice: The Complete Two-Path Derivation 12. The Delayed-Choice Quantum Eraser: A Density-Matrix Derivation 13. The General No-Signalling Theorem Part III — Consistency, Records, and the Event Graph 14. Relational Consistency: Exact and Experimental Formalization 15. Physical Records, Decoherence, and the Observer De-Mystified 16. Relational Time and the Correct Use of the Event Graph Part IV — The Arrow and the Landscape 17. Relational Order and the Thermodynamic Direction of Time 18. Distinctions from Related Approaches 19. A Formal Bridge: Consistent Quantum Histories 20. Separating Temporal Consistency from Quantum Coherence Part V — Meaning and Testability 21. What Does "Determined Later" Mean, Mathematically? 22. Empirical Content, Falsifiability, and a Research Program 23. Conclusions Back Matter Appendix A — Notation and Conceptual Correspondence Appendix B — The Logical Core in a Single Chain of Formulas Appendix C — Claim–Assumption Matrix References Part I The Problem of Time In which time is neither denied nor assumed, but asked to explain itself — and the concepts of relational description, relational consistency, and the thermodynamic arrow are assembled. Chapter 1 Why Time Is a Problem The conceptual status of time remains deeply problematic in contemporary physics. Relativity eliminates absolute simultaneity; quantum theory challenges the notion of observer-independent states; and neither framework explains how temporal structure itself arises. Ask a physicist of the nineteenth century what time is, and the answer would have been serene: time is a universal, externally given parameter. Every event in the universe happens at some moment of a single cosmic clock, and physics describes how things change as that clock ticks. Newton wrote it into the foundations: absolute time "flows equably without regard to anything external." This picture is intuitive, it matches everyday experience, and it is built into the very grammar of classical mechanics, where every equation of motion says how a quantity changes with respect to
t — a
t that is simply assumed to be there, the same for everyone, everywhere. Modern physics profoundly destabilized this picture — twice, from two independent directions. The first blow came from special relativity. Einstein's 1905 analysis showed that there is no such thing as absolute simultaneity: whether two distant events happen "at the same time" depends on the observer's state of motion. Time intervals themselves are frame-dependent. This is not a limitation of our measuring devices; it is a structural feature of spacetime. There is no privileged universal "now" slicing the universe into past and future — no preferred foliation, in the technical vocabulary — that all observers could agree on. What relativity leaves behind is a network of relations: which events can influence which, encoded in the invariant light-cone structure. The second blow came from quantum theory, which undermines something even more basic: the idea that a physical system simply has a defin
The problem of quantum time and evolution of quantum systems, where time is not a parameter, is considered. In our model, following some earlier works, time is represented by a quantum operator. In this paper, similarly to the position operators in the Schrödinger representation of quantum mechanics, this operator is a multiplication-type operator. It can be also represented by an appropriate positive operator-valued measure (POVM) which together with the 3D position operators/measures provide a quantum observable giving a position in the quantum spacetime. The quantum evolution itself is a stochastic process based on Lüder’s projection postulate. In fact, it is a generalization of the unitary evolution. This allows to treat time and generally the spacetime position as a quantum observable, in a consistent and observer-independent way.