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<article xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>On Existence of Global-in-Time Tra jectories of Non-deterministic Markovian Systems</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Ievgen Ivanov</string-name>
          <email>ivanov.eugen@gmail.com</email>
          <xref ref-type="aff" rid="aff0">0</xref>
          <xref ref-type="aff" rid="aff1">1</xref>
          <xref ref-type="aff" rid="aff2">2</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Key Terms. Mathematical Model</institution>
          ,
          <addr-line>Specification Process, Verification Process</addr-line>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>Paul Sabatier University</institution>
          ,
          <addr-line>Toulouse</addr-line>
          ,
          <country country="FR">France</country>
        </aff>
        <aff id="aff2">
          <label>2</label>
          <institution>Taras Shevchenko National University of Kyiv</institution>
          ,
          <country country="UA">Ukraine</country>
        </aff>
      </contrib-group>
      <fpage>312</fpage>
      <lpage>320</lpage>
      <abstract>
        <p>We consider the following question: given a continuous-time non-deterministic (not necessarily time-invariant) dynamical system, is it true that for each initial condition there exists a global-in-time trajectory. We study this question for a large class of systems, namely the class of complete non-deterministic Markovian systems. We show that for this class of systems, the question can be answered using analysis of existence of locally defined trajectories in a neighborhood of each time.</p>
      </abstract>
      <kwd-group>
        <kwd />
        <kwd>dynamical systems</kwd>
        <kwd>non-deterministic systems</kwd>
        <kwd>Markovian systems</kwd>
        <kwd>global-in-time trajectories</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>-</title>
      <p>In this paper we consider the following question: given a continuous-time
nondeterministic (not necessarily time-invariant) dynamical system Σ, is it true
that for any time moment t0 and initial state x0 there exists a global-in-time
trajectory t 7→ s(t) such that s(t0) = x0.</p>
      <p>
        Some related problems, e.g. global existence of solutions of initial value
problems for various classes of diferential equations [
        <xref ref-type="bibr" rid="ref2 ref3 ref7">2, 3, 7</xref>
        ] and inclusions [
        <xref ref-type="bibr" rid="ref4 ref5 ref6">4–6</xref>
        ],
existence of non-Zeno global-in-time executions of hybrid automata [
        <xref ref-type="bibr" rid="ref10 ref8 ref9">8–10</xref>
        ] are well
known. However, they have mostly been studied in the context of
deterministic systems (diferential equations with unique solutions, deterministic hybrid
automata, etc.). Diferential inclusions [
        <xref ref-type="bibr" rid="ref5">5</xref>
        ] are in principle non-deterministic
systems, but for them a more common question is whether any (instead of some)
solution for each initial condition exists into future [
        <xref ref-type="bibr" rid="ref4 ref6">4, 6</xref>
        ].
      </p>
      <p>For deterministic systems the existence of a global trajectory for each initial
condition implies that each partial trajectory (e.g. defined on a proper open
interval of the real time scale) can be extended to a global trajectory. But this is
not necessary for non-deterministic systems. For example, for each initial
condition x(t0) = x0 the diferential inclusion ddxt ∈ [0, x2] has both a globally defined
constant trajectory x(t) = x0 and a trajectory of the equation ddxt = x2 which
escapes to infinity in finite time. Thus it is not true that any (locally defined)
solution extends infinitely into future.</p>
      <p>We will study our existence question for a large class of systems, namely the
class of complete non-deterministic Markovian systems. We will show that for
this class of systems, the question can be answered using analysis of existence
of locally defined trajectories in a neighborhood of each time.</p>
      <p>Note that in this paper we use the term Markovian in the context of purely
non-deterministic (i.e. non-stochastic) systems. The formal definition will be
given below. Also note that many well-known classes of continuous-time systems
either belong to this class of can be represented by systems of this class. We will
give examples later in the paper.
2</p>
      <p>
        Non-deterministic Complete Markovian Systems
The notions of a Markov process or system [
        <xref ref-type="bibr" rid="ref12">12</xref>
        ] are usually defined and studied in
the context of probability theory. However, they also make sense in a purely
nondeterministic setting, where no quantitative information is attached to events
(trajectories, transitions, etc.), i.e. each event is either possible or impossible.
      </p>
      <p>
        General definitions of continuous-time Markovian systems of such kind have
appeared in the literature [
        <xref ref-type="bibr" rid="ref1">1</xref>
        ]. They give a large class of (not necessarily
deterministic) systems which can have both continuous and discontinuous (jump-like)
trajectories. Essentially, the notion of a non-deterministic Markovian system
captures the idea that only the system’s current state (but not its past) determines
the set of its possible futures.
      </p>
      <p>
        Below we define the notion of a non-deterministic (complete) Markovian
system in spirit of, but not exactly as in [
        <xref ref-type="bibr" rid="ref1">1</xref>
        ]. The main reasons for this are that
we would like to include non-time-invariant systems in the definition and focus
on partial trajectories, i.e. trajectories defined on a subset of the time scale.
      </p>
      <p>We will use the following notation: N = {1, 2, 3, ...}, N0 = N ∪ {0}, f : A → B
is a total function from A to B, f : A →˜B is a partial function from A to B,
f |X is the restriction of a function f to a set X, 2A is the power set of a set A.
The notation f (x) ↓ (f (x) ↑) means that f (x) is defined (resp. undefined) on
the argument x, dom(f ) = {x | f (x) ↓}. Also, ¬, ∨, ∧, ⇒, ⇔ denote the logical
operations of negation, disjunction, conjunction, implication and equivalence
correspondingly. Let us denote:
– T = [0, +∞) is the (real) time scale. We assume that T is equipped with a
topology induced by the standard topology on R
– T is the set of all connected subsets of T with cardinality greater than one.</p>
      <p>For the purpose of this paper, we will use the following definition of a
dynamical system on the time scale T .</p>
      <p>Definition 1. A dynamical system on T is as an abstract object M (a
mathematical model; in applications this may be an equation, inclusion, switched
system, etc.) together with the associated time scale T (this scale will be the same
throughout the paper), the set of states Q, and the set of (partial) trajectories T r.
A trajectory is a function s : A → Q, where A ∈ T (note that trivial trajectories
defined on singleton or empty time sets are excluded). The set T r satisfies the
property: if s : A → Q ∈ T r, B ∈ T, and B ⊆ A, then s|B ∈ T r. We will refer
to this property as ”Tr is closed under proper restrictions (CPR)”.</p>
      <p>We will say that a trajectory s1 ∈ T r is a subtrajectory of s2 ∈ T r (denoted
as s1 v s2), if s1 = s2|A for some A ∈ T. The trajectories s1 and s2 are
incomparable, if s1 is not a subtrajectory of s2 and vice versa.</p>
      <p>According to the definition given above, for a time t0 ∈ T and q0 ∈ Q there
may exist multiple incomparable trajectories s such that s(t0) = q0 (as well as
one or none). In this sense a dynamical system can be non-deterministic.</p>
      <p>It is easy to see that (T r, v) is a partially ordered set (poset).</p>
      <p>Definition 2.</p>
      <p>A set T r (which is CPR) is
s2(t), t ∈ dom(B)</p>
      <p>.</p>
      <p>s(t) =
– complete, if (T r, v) is a chain-complete poset (every chain has a supremum)
– Markovian, if s ∈ T r for each s1, s2 ∈ T r and t ∈ T such that t =
sup dom(s1) = inf dom(s2), s1(t) ↓, s2(t) ↓, and s1(t) = s2(t), where
(s1(t), t ∈ dom(A)</p>
      <p>Note that because T r is closed under restrictions to sets A ∈ T, the supremum
of a chain c in poset (T r, v) exists if s∗ ∈ T r, where s∗ : Ss∈c dom(s) → Q is
defined as follows: s∗(t) = s(t), if s ∈ c and t ∈ dom(s) (this definition is correct,
because c is a chain with respect to subtrajectory relation).</p>
      <p>The notions of complete and Markovian sets of trajectories are illustrated in
Fig. 1 and 2.</p>
      <p>The following proposition gives some examples of sets of trajectories.
Proposition 1. Let Q = R. Consider the following sets of trajectories:
– T rall is the set of all functions s : A → Q, A ∈ T.
– T rcont is the set of all continuous functions s ∈ T rall (on their domains)
– T rdiff is the set of all diferentiable functions s ∈ T rall (on their domains)
– T rbnd is the set of all bounded functions s ∈ T rall (on their domains).</p>
    </sec>
    <sec id="sec-2">
      <title>Then the following holds:</title>
      <p>(1) ∅, T rall, T rcont, T rdiff , T rbnd, T rdiff ∩ T rbnd are CPR
(2) ∅, T rall, T rcont are complete and Markovian
(3) T rdiff is complete, but is not Markovian
(4) T rbnd is Markovian, but is not complete
(5) T rdiff ∩ T rbnd is neither complete, nor Markovian.</p>
      <p>Definition 3. A non-deterministic complete Markovian system (NCMS) is
dynamical system is (M, T, Q, T r) such that T r is complete and Markovian.</p>
      <p>The following propositions 2-4 give some examples of NCMS.</p>
      <p>Proposition 2. Let Q = Rd (d ∈ N) and M be a diferential equation ddyt =
f (t, y), where f : R × Rd → Rd is a given total function. Let T r be the set of all
functions s : A → Q, A ∈ T such that s is diferentiable on A and satisfies M
on A. Then (M, T, Q, T r) is a NCMS.</p>
      <p>Proposition 3. Let M be a diferential inclusion ddyt = F (t, y), where F : R ×
Rd → 2Rd is a given (total) function. This is not necessarily a NCMS, but it
can be converted to a NCMS as follows. Let M 0 be the system
y ∈ F (t, x)
where x is a new variable. Let Q = Rd × Rd and T r be the set of all s : A → Q,
A ∈ T such that s is locally absolutely continuous on A and satisfies M 0 almost
everywhere on A (w.r.t. Lebesgue’s measure). Then (M, T, Q, T r) is a NCMS.
( ddyt = x
Proposition 4. Let Q be a set equipped with discrete topology. Let r ⊆ Q × Q be
(y(t+) = y(t),
a relation on Q. Let M be a system t ∈/ N0 , where y denotes
(y(t), y(t+)) ∈ r, t ∈ N0
an unknown function, y(t+) denotes the right limit at t. Let T r be the set of all
piecewise-constant left-continuous functions s : A → Q (w.r.t. discrete topology
on Q) which satisfy M on A (see Fig. 3). Then (M, T, Q, T r) is a NCMS.</p>
      <p>A predicate p : ST (Q) → Bool (Bool = {true, f alse}) is called
.
– left-local, if p(s1, t) ⇔ p(s2, t) whenever (s1, t), (s2, t) ∈ ST (Q) and s1 =t−
s2, and moreover, p(s, t) whenever t is the least element of dom(s) .
– right-local, if p(s1, t) ⇔ p(s2, t) whenever (s1, t), (s2, t) ∈ ST (Q), s1 =t+ s2,
and moreover, p(s, t) whenever t is the greatest element of dom(s)
– left-stable, if whenever t is not the least element of dom(s), p(s, t) implies
that there exists t0 ∈ [0, t) such that p(s, τ ) for all t0 ∈ [t0, t] ∩ dom(s)
– right-stable, if whenever t is not the greatest element of dom(s), p(s, t)
implies that there exists t0 &gt; t such that p(s, τ ) for all τ ∈ [t, t0] ∩ dom(s).</p>
      <p>The theorems given below show how left- and right-local predicates can be
used to specify/represent a complete Markovian set of trajectories (or system).
Theorem 1. Let l : ST (Q) → Bool be a left-local predicate and r : ST (Q) →
Bool be a right-local predicate. Then the set</p>
      <p>T r = {s : A → Q | A ∈ T ∧ (∀t ∈ A l(s, t) ∧ r(s, t))}.
is CPR, complete, and Markovian.</p>
      <p>Theorem 2. Let T r be a CPR complete Markovian set of trajectories which take
values in the set of states Q. Then there exist unique predicates l, r : ST (Q) →
Bool such that l is left-local and left-sable, r is right-local and right-stable, and</p>
      <p>T r = {s : A → Q | A ∈ T ∧ (∀t ∈ A l(s, t) ∧ r(s, t))}.</p>
      <p>Let us consider an example which illustrates these theorems. Let Q = Rd and
T r be the set of all functions s : A → Q, A ∈ T such that s is diferentiable on
A and satisfies a diferential equation ddyt = f (t, y) on A, where f : R × Rd → Rd
is a given function. Then T r is complete and Markovian by Proposition 2.</p>
      <p>Let us show how T r can be represented using left- and right-local predicates.
Let l, r : ST (Q) → Bool be predicates such that
– l(s, t) if either t is the least element of dom(s), or ∂−s(t) ↓= f (t, s(t)),
– r(s, t) if either t is the greatest element of dom(s), or ∂+s(t) ↓= f (t, s(t)),
where ∂−s(t) and ∂+s(t) denote the left- and right- derivative of s at t (the
symbol ↓ indicates that the left hand side of the equality is defined). It is not dificult
to check that l is left-local, r is right-local, and T r = {s : A → Q | A ∈ T ∧ (∀t ∈
A l(s, t) ∧ r(s, t))}. In general case, l and r are not necessarily (respectively)
leftand right-stable. But we can define another predicates l∗, r∗ on ST (Q) such that
– l∗(s, t) if either t is the least element of dom(s), or there exists t0 &lt; t such
that s is diferentiable on ( t0, t] and satisfies diferential equation ddyt = f (t, y)
on (t0, t] (at the time t the derivative is understood as left-derivative).
– r∗(s, t) if either t is the greatest element of dom(s), or there exists t0 &gt; t
such that s is diferentiable on [ t, t0) and satisfies ddyt = f (t, y) on [t, t0).
Then it is not dificult to see that l∗ is left-local and left-stable, and r∗ is
rightlocal and right-stable, and T r = {s : A → Q | A ∈ T ∧ (∀t ∈ A l(s, t) ∧ r(s, t))}.</p>
      <p>Existence of Global-in-Time Trajectories
Let us recall our original question about global-in-time trajectories and formulate
it for non-deterministic complete Markovian systems.</p>
      <p>Let (M, T, Q, T r) be a NCMS. Our question (let us denote it as Q0) is
whether it is true that for each t0 ∈ T , q0 ∈ Q there exists a trajectory s : T → Q
(i.e. global-in-time) such that s(t0) = q0.</p>
      <p>Note that we ask about existence of a trajectory defined in both time
directions relative to t0. The case when we are interested in existence of a trajectory
defined in one direction (e.g s : [t0, +∞) → Q) is not considered in this paper,
but can be studied analogously.</p>
      <p>
        Let us decompose Q0 into the following two questions:
Q1: Is it true that for each t0 ∈ T , q0 ∈ Q there exists a (partial) trajectory
s : A → Q such that t0 is an interior point of A (relative to the topology on
T , e.g. 0 is considered an interior point of [
        <xref ref-type="bibr" rid="ref1">0, 1</xref>
        ]) and s(t0) = q0 ?
Q2: Is it true that for each partial trajectory s : A → Q such that A is a
compact segment there exists a trajectory s0 : T → Q such that s = s0|A ?
Proposition 5. The answer to the question Q0 is positive if the answers to
Q1 and Q2 are positive.
      </p>
      <p>The question Q1 is about existence of a local-in-time trajectories. We will not
study it in this paper and assume that it can be answered using domain-specific
methods. Our aim is to answer Q2 using only information about existence of
locally defined trajectories in the neighborhood of each time moment.</p>
      <p>Let us introduce several definitions. Let Σ = (M, T, Q, T r) be a fixed NCMS.
Definition 6. – A right dead-end path (in Σ) is a trajectory s : A → Q such
that A has a form [a, b), where a, b ∈ T . and there is no s0 : [a, b] → Q ∈ T r
such that s = s0|dom(s) (i.e. s cannot be extended to a trajectory on [a, b]).</p>
      <p>The value b is called the end of this path.
– A left dead-end path (in Σ) is a trajectory s : A → Q such that A has a
form (a, b], where a, b ∈ T . and there is no s0 : [a, b] → Q ∈ T r such that
s = s0|dom(s). The value a is called the end of this path.
– A dead-end path is either a right dead-end path, or a left dead-end path.</p>
      <p>Let f : [0, +∞) → [0, +∞) be a positive-definite (i.e. f (0) = 0, f (x) &gt; 0 when
x &gt; 0), monotonously non-decreasing, and continuous function (e.g. f (x) = x).
Definition 7. – A right dead-end path s : [a, b) → Q is called f -Ob-escapable,
where Ob is a connected neighborhood of b, if there exists c ∈ (a, b) ∩ Ob,
d ∈ [b + f (b − c), +∞), and a trajectory s0 : [c, d] ∩ Ob → Q such that
s(c) = s0(c).
– A left dead-end path s : (a, b] → Q is called f -Ob-escapable, where Ob is a
connected neighborhood of b, if there exists c ∈ (a, b) ∩ Ob, d ∈ [0, max{a −
f (c − a), 0}], and a trajectory s0 : [d, c] ∩ Ob → Q such that s(c) = s0(c).
– A right- or left- dead-end path is called f -escapable, if it is f -T -escapable.
This definition is illustrated in Fig. 4. Note that a sufix of a right dead-end path
s : [a, b) → Q (i.e. a restriction of the form s|[a0,b), where a0 ∈ [a, b)) is a right
dead-end path. Analogously, a prefix of a left dead-end path s : (a, b] → Q (i.e.
a restriction of the form s|(a,b0], where b0 ∈ (a, b]) is a left dead-end path.</p>
      <p>Let Σ = (M, T, Q, T r) be a NCMS. For each t ∈ T let Ot ⊆ T be some
connected neighborhood of t and Dt be the set of all dead-end paths s (in Σ)
such that t is the end of s and dom(s) ⊆ Ot.</p>
    </sec>
    <sec id="sec-3">
      <title>Theorem 3. The following conditions are equivalent:</title>
      <p>(1) for each partial trajectory s : A → Q such that A is a compact segment there
exists a trajectory s0 : T → Q such that s = s0|A
(2) each dead-end path (in Σ) is f -escapable
(3) for each t ∈ T and s ∈ Dt, s is f -Ot-escapable.</p>
      <p>Note that this theorem holds for an arbitrary fixed f and arbitrary fixed choice
of neighborhoods Ot, t ∈ T .</p>
      <p>This theorem gives an answer to the question Q2. The condition 3 of this
theorem shows in which sense Theorem 3 reduces the question of global-in-time
existence of trajectories to the analysis of local existence of trajectories in the
neighborhood of each time moment.
We have studied the question of existence of global-in-time trajectories for each
initial condition of a (non-time-invariant) non-deterministic complete Markovian
system. We have shown that this question can be answered using analysis of
existence of locally defined trajectories in a neighborhood of each time. The
results can be useful for studying the problems of well-posedness and reachability
for continuous and discrete-continuous (hybrid) dynamical systems.</p>
    </sec>
  </body>
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