1. Relativity and Abstract State Machines Edel Sherratt Aberystwyth University Aberystwyth, Wales, UK

2. Content Abstract State Machines rock Global Time doesn’t We’ve been here before Some analogies A small step towards admissible transformations between ASMs’ frames of reference

3. ASMs are Powerful and Versatile Every kind of algorithm (Blass, Gurevich) Conway's game of life, ambiguous grammars, lift control, Internet telephony, database recovery … (Börger, Stärk) Asynchronous communication (Glässer, Gurevich, Veanes) SDL semantics (Glässer, Gotzhein, Prinz)

4. Basic ASM States are first order structures (base set with functions) Vocabulary, terms, locations Moves update the values of locations

5. Distributed ASM ASM with multiple threads of control Each associated with an agent Each agent interprets its ASM program according to its partial view of the state This gives an update set

6. Distributed ASM

7. A run is a partially ordered set of moves (M,<) such that – each move has finitely many predecessors – the moves performed by a given agent are linearly ordered by < – for every finite initial segment X of (M, <), and every maximal move m  X, there is a unique state  X) that results from performing m in the state  X\{m})

8. Distributed ASM Freedom to schedule a run Moves can be carried out – In parallel, unless they conflict – Interleaved – According to an explicit schedule Coherence condition; more restrictive than serializability in e.g. database scheduling

9. ASMs with Time (Graf, Prinz) Focus on moves rather than states Moves are events (contrast with spacetime events) Moves are timed so that the partial ordering on moves is reflected in a compatible order on time Time allows measurement of distance between (some) events

10. Global Time Implicit in the basic ASM Is it present in the case of a distributed ASM? – Confluence of rule applications suggests that it is – In any run, moves are ordered in global time, though some occur at the same global time – Local timestamps set by reading the monitored function ‘now’, which gives a global time

11. What’s wrong with global time? Server with clients; online ticketing system A distributed ASM, but clients have distinct, usually conflicting, goals Server determines which requests succeed and which fail Global time is determined by the server

12. What’s wrong with global time? A new client for a running service Abstract Communicator (Glässer et al.) acts as intermediary Communicator is part of client’s environment Global time is determined by communicator Communicator determines global time for all clients And resolves clients’ times with server’s time

13. What’s wrong with global time? Suppose client uses multiple services Global time is determined by more than one communicator Which takes precedence?

14. We’ve been here before

15. Galileo (and Newton) Absolute space Inertial frame is in uniform motion relative to absolute space Universal absolute time shared by all inertial frames Galilean transformation: x’=x-vt, t’=t, y’=y, z’=z

16. Fitzgerald, Lorentz, Einstein Inertial frames do not accelerate wrt each other Lorentz transformation preserves laws of electrodynamics So no preference for any frame

17. Relevance to ASMs? Analogy Space is defined by the vocabulary of an ASM Time progresses through a run Event is a combination of state (values at locations) and time (contrast with event as move) ASMs communicate only through mutually accessible locations

18. Where the analogy breaks down ASMs need not operate in the same space In general, shared locations represent minor points of overlap ASM spacetime is not continuous Nonetheless, differences between states can be computed as can distances in time

19. Aim Identify transformations analogous to the Galilean and Lorentz transformations that preserve required properties of abstract state machines

20. Observing an event Two ASMs, A and B Can B observe a location as A sees it? Only mutually accessible location(s) can be observed Terms of A map to terms of B iff the terms refer to the same location

21. Time of an event (state) Local clocks can only be synchronized if mutually accessible locations have the same values Otherwise each ASM sees the state of the other as being in its own past or future

22. Private state Updates are applied instantaneously But computing the update set is not necessarily instantaneous Shareable locations should not be used for scratch work

23. Conserving History Suppose S A precedes S A ’ in the history of A, and suppose B observes those states as S B and S B ’ That is, mutually accessible locations are mapped from A’s terms and A’s time to B’s terms and B’s time Then S B must also precede S B ’ in B’s frame of reference

24. Summary Some initial requirements that must be fulfilled by any transformation of observations from the state and time of one ASM to those of another have been identified Much remains to be done to achieve the aim of identifying useful transformations