We review what it means for a relativistic particle to be localized and argue that the most useful approach is through local measurement. This perspective ties localization directly to relativistic causality and measurable outcomes in spacetime. Strict localization in quantum field theory is formalized by states that give the same expectation value as vacuum for all local observables outside some spacetime region. With this formalism, single photons cannot be strictly localized, but coherent states can. The structure and interpretation of local observables and local operator algebras are discussed in connection with the Reeh-Schlieder theorem. Since probabilities of local measurement outcomes cannot vanish in vacuum, particle detection events must be phrased carefully. Key characteristics of strictly localized states are surveyed alongside concrete strategies for constructing them. The relationship between localization, causality, and on-demand sources is analyzed, finding that strictly localized states can represent localized, propagating information in quantum field theory. Explicit examples of localized photonic states are presented with an emphasis on quantum optics, including states that approximate single photons and (entangled) Bell states.
We connect three distinct lines of research that have recently explored extensions of the classical LOCAL model of distributed computing: A. distributed quantum computing and non-signaling distributions [e.g. STOC 2024], B. finitely-dependent processes [e.g. Forum Math. Pi 2016], and C. locality in online graph algorithms and dynamic graph algorithms [e.g. ICALP 2023]. We prove new results on the capabilities and limitations of all of these models of computing, for locally checkable labeling problems (LCLs). We show that all these settings can be sandwiched between the classical LOCAL model and what we call the randomized online-LOCAL model. Our work implies limitations on the quantum advantage in the distributed setting, and we also exhibit a new barrier for proving tighter bounds. Our main technical results are these: 1. All LCL problems solvable with locality
O(log⋆n) in the classical deterministic LOCAL model admit a finitely-dependent distribution with locality
O(1). This answers an open question by Holroyd [2024], and also presents a new barrier for proving bounds on distributed quantum advantage using causality-based arguments. 2. In rooted trees, if we can solve an LCL problem with locality
o(logloglogn) in the randomized online-LOCAL model (or any of the weaker models, such as quantum-LOCAL), we can solve it with locality
O(log⋆n) in the classical deterministic LOCAL model. One of many implications is that in rooted trees,
O(log⋆n) locality in quantum-LOCAL is not stronger than
O(log⋆n) locality in classical LOCAL.
In this thesis, I study how quantum computation and quantum communication can help large networks of computers to solve computational problems faster. I also connect the notion of locality between various models, including distributed quantum algorithms and online graph algorithms, and show that locality in online graph algorithms can be used to provide bounds for distributed quantum advantage. Towards proving distributed quantum advantage, I present the first family of LCL problems which shows a quantum advantage for distributed graph algorithms. Here LCLs, or Locally Checkable Labeling problems, are a family of graph problems described by a finite set of local constraints, and I mainly focus on them in this thesis. The models of distributed computing which this result separates are the classical LOCAL model and the quantum-LOCAL model. In both of these models, a network of computers exchanges messages in synchronous rounds, and the running time of the algorithm directly corresponds with locality, that is, how far the computers see in the network. In this thesis, I also introduce new models of computing that capture locality in stronger settings. Most notably, I introduce the online-LOCAL model which captures the locality of online graph algorithms, and show that it is, asymptotically, roughly as strong as the classical LOCAL model for solving LCL problems on rooted regular trees. I provide an online-LOCAL algorithm for finding a 3-coloring of a bipartite graph with lower locality than is possible in the classical LOCAL model, and show that the algorithm is tight. To draw things together, I show that quantum-LOCAL and online-LOCAL are indeed related to each other: any quantum-LOCAL algorithm can be simulated in the randomized online-LOCAL model. The converse does not hold in general, but an online-LOCAL algorithm solving an LCL problem in rooted, possibly non-regular, trees can be simulated in the classical LOCAL model—and thus in the quantum-LOCAL model—with an exponential cost in locality, putting indirectly a bound on the maximum possible attainable quantum advantage. Finally, I consider the sinkless orientation problem, which holds a central role in our understanding of the locality of LCL problems in the classical LOCAL model, and provide a simpler and more direct proof for its hardness using the supported LOCAL model. I also provide a simpler algorithm solving sinkless orientation in the SLOCAL model, which is a sequential version of the LOCAL model.