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P OPULATION CTMC A population model is thus given by a tuple X ( N ) - - PowerPoint PPT Presentation

F LUID M ODEL C HECKING F LUID A PPROXIMATION FOR C HECKING L OGIC P ROPERTIES IN M ARKOV P OPULATION M ODELS Luca Bortolussi 1 , 2 1 Dipartimento di Matematica e Geoscienze Universit degli studi di Trieste 2 CNR/ISTI, Pisa luca@dmi.units.it


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FLUID MODEL CHECKING

FLUID APPROXIMATION FOR CHECKING LOGIC PROPERTIES IN MARKOV POPULATION MODELS Luca Bortolussi1,2

1Dipartimento di Matematica e Geoscienze

Università degli studi di Trieste

2CNR/ISTI, Pisa

luca@dmi.units.it

Joint work with Jane Hillston and Roberta Lanciani

Bertinoro Summer School in Formal Methods June 17-21, 2013

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INTRODUCTION FLUID APPROXIMATION BEHAVIOUR SPECIFICATION MC ICTMC LOCAL2GLOBAL 2 / 123

COLLECTIVE DYNAMICS

The behaviour of many systems can be interpreted as the result of the collective behaviour of a large number of interacting entities. For such systems we are often as interested in the population level behaviour as we are in the behaviour of the individual entities.

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COLLECTIVE BEHAVIOUR

In the natural world there are many instances of collective behaviour and its consequences:

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COLLECTIVE BEHAVIOUR

In the natural world there are many instances of collective behaviour and its consequences:

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COLLECTIVE BEHAVIOUR

This is also true in the man-made and engineered world: Spread of H1N1 virus in 2009

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COLLECTIVE BEHAVIOUR

This is also true in the man-made and engineered world: Love Parade, Germany 2006

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COLLECTIVE BEHAVIOUR

This is also true in the man-made and engineered world: Self assessment tax returns 31st January each year

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SOLVING DISCRETE STATE MODELS

With compositional modelling approaches we have a CTMC with global states determined by the local states of all the participating components.

c b a c b a c b a

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SOLVING DISCRETE STATE MODELS

When the size of the state space is not too large they are amenable to NUMERICAL

SOLUTION (linear algebra) to

determine a STEADY STATE or

TRANSIENT PROBABILITY DISTRIBUTION.

Q =      q1,1 q1,2 · · · q1,N q2,1 q2,2 · · · q2,N . . . . . . . . . qN,1 qN,2 · · · qN,N      π(t) = (π1(t), π2(t), . . . , πN(t))

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SOLVING DISCRETE STATE MODELS

Alternatively they may be studied using STOCHASTIC

  • SIMULATION. Each run

generates a single trajectory through the state space. Many runs are needed in

  • rder to obtain average

behaviours.

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STATE SPACE EXPLOSION

As the size of the state space becomes large it becomes infeasible to carry out numerical solution and extremely time-consuming to conduct stochastic simulation. In these cases we would like to take advantage of the MEAN FIELD or

FLUID APPROXIMATION techniques.

Use CONTINUOUS STATE VARIABLES to approximate the discrete state space. ❞ ❞ ❞ ❞ ❞ ❞ ✲ ✛ ✛ ✲ ❞ ❞ ❞ ❞ ✲ ✛ ✲ ✛ ✲ ✛ ✲ ✛ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ✲ ✛ ✲ ✛ ✲ ✛ ✲ ✛ ✲ ✛ ✲ ✛ ✲ ✛ ✲ ✛ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ✲ ✛ ✲ ✛ ✲ ✛ ✲ ✛ ✲ ✛ ✲ ✛ ✲ ✛ ✲ ✛ ✲ ✛ ✲ ✛ ✲ ✛ ✲ ✛ ✲ ✛ ✲ ✛ ✲ ✛ ✲ ✛ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ ❞ Use ORDINARY DIFFERENTIAL EQUATIONS to represent the evolution of those variables over time. Appropriate for models in which there are large numbers of components of the same type, i.e. models of populations and situations of collective dynamics.

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POPULATION MODELS - TIME SERIES ANALYSIS

Population model CTMC Fluid ODE Solution/Simulation

(small populations) (large populations)

Simulation Fluid methods: approximate description of the collective (average) behaviour, estimate of certain passage times

  • M. Tribastone, S. Gilmore, J. Hillston: Scalable Differential Analysis of Process Algebra Models. IEEE Trans.

Softw Eng. 2012. R.A. Hayden, A. Stefanek, J.T. Bradley. Fluid computation of passage-time distributions in large Markov

  • models. Theor. Comput. Sci. 2012.
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POPULATION MODELS - MODEL CHECKING

Population model Property specification Stochastic MC Fluid approximation

(small populations) ??

Understand how and to what extent fluid methods can be used to efficiently approximate stochastic model checking.

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GOALS

We will consider population models, composed of many interacting agents of one or more classes. We will focus on questions related to the behaviour of individual agents for medium and large population size. We will investigate: individual properties, concerned with the behaviour of a single or a few agents collective properties, concerned with the behaviour at the population level.

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LECTURE PLAN

Introduction to population CTMC and fluid approximation for collective and individual behaviour; Individual properties: model checking time-inhomogeneous CTMC, decidability, and correctness Collective properties: linear noise approximation (if there will be time — not in the book chapter).

  • L. Bortolussi, J. Hillston, D. Latella, M. Massink.Continuous Approximation of Collective Systems Behaviour:

a Tutorial. Performance Evaluation, 2013.

  • L. Bortolussi, J. Hillston: Fluid Model Checking. CONCUR 2012.
  • L. Bortolussi, J. Hillston: Model Checking Single Agent Behaviours by Fluid Approximation, submitted to

Information and Computation.

  • L. Bortolussi, R. Lanciani. Model Checking Markov Population Models by Central Limit Approximation.

QEST 2013.

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OUTLINE

1 INTRODUCTION 2 FLUID APPROXIMATION

Markov population models Fluid approximation theorems

3 BEHAVIOUR SPECIFICATION

Individual Properties CSL model checking for time-homogeneous CTMC

4 MODEL CHECKING CSL FOR ICTMC

Model checking non-nested properties Time-dependent probabilities Nested CSL-formulae Theoretical results

5 FROM INDIVIDUAL TO COLLECTIVE BEHAVIOUR

From local properties to global properties Central Limit Approximation Examples Conclusions

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EXAMPLE: P2P NETWORK EPIDEMICS

Network node Y

suscept. infected inactive patched infected active ext_inf infect infect activate deactivate patch_high patch_low patch_low loss

A network is composed of N interconnected nodes Indistinguishable individual nodes ⇒ we only count of how many nodes are in each state Dynamics specified at the collective level

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POPULATION CTMC: INDIVIDUALS AND COLLECTIVES

INDIVIDUALS

We have N individuals with state Y (N)

i

∈ S, S = {1, 2, . . . , n} in the system (we can have multiple classes; the population is assumed constant for simplicity).

COLLECTIVE VARIABLES

X (N)

j

= N

i=1 1{Y (N) i

= j}, and X(N) = (X (N)

1

, . . . , X (N)

n

)

EXAMPLE: NETWORK EPIDEMICS

Individual state space: S = {susceptible (s),infected and inactive (d), infected and active (i), patched (p) } Collective variables: X (N)

s

= n

j=1 1{Y (N) j

= s}, X (N)

d

, X (N)

i

, X (N)

p

.

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POPULATION CTMC: COLLECTIVE DYNAMICS

COLLECTIVE TRANSITIONS T (N)

τ ∈ T (N) describes a possible action/ event. τ = (Rτ, r (N)

τ

), where r (N)

τ

= r (N)

τ

(X(N)) is the rate function, giving the speed at which the event happens. Rτ is the multi-set of update rules, Rτ = {i1 → j1, . . . , ik → jk}. mτ,i→j is the multiplicity of i → j in Rτ

UPDATE VECTOR

With each transition τ, we associate an update vector vτ, giving the net change in collective variables due to τ: vτ,i =

  • (i→j)∈Rτ

mτ,i→jej −

  • (i→j)∈Rτ

mτ,i→jei,

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EXAMPLE: P2P NETWORK EPIDEMICS

suscept. infected inactive patched infected active ext_inf infect infect activate deactivate patch_high patch_low patch_low loss

ext_inf: Rext_inf = {s → d}, r (N)

ext_inf = kextXs;

infect: Rinfect = {s → d, i → i}, r (N)

infect = kinf N XsXi;

activate: Ractivate = {d → i}, r (N)

activate = kactXd;

deactivate: Rdeactivate = {i → d}, r (N)

deactivate = kdeactXi;

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EXAMPLE: P2P NETWORK EPIDEMICS

suscept. infected inactive patched infected active ext_inf infect infect activate deactivate patch_high patch_low patch_low loss

patch_s: Rpatch_s = {s → p}, r (N)

patch_s = klowXs;

patch_d: Rpatch_d = {d → p}, r (N)

patch_d = klowXd;

patch_i: Rpatch_i = {i → p}, r (N)

patch_i = khighXi;

loss: Rloss = {p → s}, r (N)

loss = klXp;

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POPULATION CTMC

A population model is thus given by a tuple X (N) = (X(N), T (N), x(N) ), where X(N) are the collective variables; T (N) are the collective transitions; x(N) is the initial state.

STATE SPACE

S(N) = {x ∈ Nn | xi = N}

CTMC INFINITESIMAL GENERATOR Q = (qx,x′)

qx,x′ =

  • {rτ(x) | τ ∈ T , x′ = x + vτ}.
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EXAMPLE: CLIENT SERVER INTERACTION

request think wait recover request reply think recover timeout ready process reply log request logging process reply

CLIENT SERVER

timeout timeout

Crq Cw Crc Ct Srq Srp Sp Sl

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EXAMPLE: CLIENT SERVER INTERACTION

VARIABLES

4 variables for the client states: Crq, Cw, Crc, Ct. 4 variables for the server states: Srq, Sp, Srp, Sl.

TRANSITIONS

There are 7 transition in totals. request: Crq → Cw, Srq → Sp; kr · min(Crq, Srq) reply: Cw → Ct, Srp → Sl; min(kwCw, krpSrp) timeout: Cw → Crc; ktoCw . . .

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OUTLINE

1 INTRODUCTION 2 FLUID APPROXIMATION

Markov population models Fluid approximation theorems

3 BEHAVIOUR SPECIFICATION

Individual Properties CSL model checking for time-homogeneous CTMC

4 MODEL CHECKING CSL FOR ICTMC

Model checking non-nested properties Time-dependent probabilities Nested CSL-formulae Theoretical results

5 FROM INDIVIDUAL TO COLLECTIVE BEHAVIOUR

From local properties to global properties Central Limit Approximation Examples Conclusions

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FLUID APPROXIMATION

It applies to population CTMC models with large population size N (studies the limit as N → ∞) It applies to population densities (normalisation step), under suitable scaling of rate functions. It is a functional version of the law of large numbers: in any finite time horizon, the trajectories of the PCTMC converge to a deterministic trajectory, solution of the fluid ODE.

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AN INTUITION

As population increases, we observe more events each having a smaller impact on the population density vector.

time X

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AN INTUITION

As population increases, we observe more events each having a smaller impact on the population density vector.

time X

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NORMALIZATION

The normalized model ˆ X (N) = (ˆ X, ˆ T (N), ˆ x(N) ) associated with X (N) = (X, T (N), x(N) ) is defined by: Variables: ˆ X = X

N

Initial conditions: ˆ x(N) =

x(N) N

Normalized transition ˆ τ = (Rτ,ˆ r (N)

τ

(ˆ X)) from τ ∈ T (N):

rate ˆ r (N)

τ

X

N

  • = r (N)

τ

(X). update vector 1

N vτ.

We assume to have a sequence of (normalised) models ˆ X (N), N > 0, that differ only in the total population size.

EXAMPLE

We will consider the normalised P2P network epidemics model, for an increasing number of netwkr nodes.

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SCALING ASSUMPTIONS

E ⊂ Rn is a open (or compact) set containing the state space of each ˆ X(N)(t) for each N. As here the population remains constant, it can be taken as the unit simplex in Rn: {x ∈ [0, 1]n |

i xi = 1}. 1 Nˆ

r (N)

τ

is required to converge uniformly to a locally Lipschitz continuous and locally bounded function fτ: sup

x∈E

  • 1

N ˆ r (N)

τ

(x) − fτ(x)

  • → 0.

If 1

r (N)

τ

= fτ does not depend on N, the rate satisfies the density dependence condition. The following theorem works also under less restrictive assumptions (e.g. random increments with bounded variance and average).

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DRIFT AND LIMIT VECTOR FIELD

DRIFT

The drift or mean increment at level N is F (N)(x) =

  • τ∈T

vτ N ˆ r (N)

τ

(x) By the scaling assumptions, F (N) converges uniformly to F, the limit vector field (locally bounded and Lipschitz continuous): F(x) =

  • τ∈T

vτfτ(x).

THE FLUID ODE IS

dx(t) dt = F(x(t))

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CONVERGENCE TO THE FLUID ODE

THEOREM (KURTZ 1970)

If ˆ x(N) → ˆ x0 ∈ E in probability, then for any finite time horizon T < ∞, it holds that: P

  • sup

0≤t≤T

||ˆ X(N)(t) − x(t)|| > ε

  • → 0.

THE MOMENT CLOSURE POINT OF VIEW

Alternatively, the fluid ODE can be seen as a (first order) approximation of the ODE for the average of the PCTMC.

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A LOOK AT K. THEOREM PROOF FOR DENSITY DEPENDENT RATES

ODE SOLUTION, INTEGRAL FORM

x(t) = x(0) + t F(x(s))ds

PERTURBED ODE REPRESENTATION OF A CTMC

ˆ X(N)(t) = ˆ X(N)(0) + t F(ˆ X(N)(s))ds + M(N)(t) M(N)(t) is a stochastic process, in particular a martingale, and by applying some martingale inequality (e.g. Doob’s), one has that εN = sup

s≤t

M(N)(s) → 0 as N → ∞ The theorem then follows as for proving uniqueness of solutions for Lipschitz vector fields (Grönwall inequality).

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EXAMPLE: P2P NETWORK EPIDEMICS NORMALISED MODEL

suscept. infected inactive patched infected active ext_inf infect infect activate deactivate patch_high patch_low patch_low loss

ext_inf: vext_inf = 1

N (−1, 1, 0, 0),

ˆ r (N)

ext_inf = Nkext Xs N = Nkext ˆ

Xs; infect: vinfect = 1

N (−1, 1, 0, 0),

ˆ r (N)

infect = Nkinf Xs N Xi N = Nkinf ˆ

Xs ˆ Xi; activate: vact = 1

N (0, −1, 1, 0),

ˆ r (N)

act = Nkact ˆ

Xd;

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P2P NETWORK EPIDEMICS: FLUID EQUATIONS

                       dxs(t) dt = −kextxs − kinfxsxi − klowxs + klossxp dxd(t) dt = kextxs + kinfxsxi − kactxd − klowxd + kdeactxi dxi(t) dt = kactxd − kdeactxi − khighxi dxp(t) dt = klowxs + klowxd + khighxi − klossxp

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P2P NETWORK EPIDEMICS: FLUID AT WORK

20 40 60 80 100 120 0.0 0.2 0.4 0.6 0.8 1.0 time probability

  • CTMC N=100

ODE

  • s

d i p

N = 100

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P2P NETWORK EPIDEMICS: FLUID AT WORK

20 40 60 80 100 120 0.0 0.2 0.4 0.6 0.8 1.0 time probability

  • CTMC N=1000

ODE

  • s

d i p

N = 1000

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STEADY STATE BEHAVIOUR

Kurtz theorem in general cannot be extended to convergence of the steady state. The problem is for instance with multi-stable fluid ODEs (more than one attracting equilibrium): in this case, in the long run the CTMC will always keep jumping between these different equilibria, although it will spend a long time in each attractor. Kurtz theorem holds also for steady state distributions only if the fluid ODE has a unique globally attracting steady state.

  • L. Bortolussi, J. Hillston, D. Latella, M. Massink. Continuous Approximation of Collective Systems

Behaviour: a Tutorial. Performance Evaluation, 2013.

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SINGLE AGENT ASYMPTOTIC BEHAVIOUR

Focus on single individuals Y (N)

h

. Fix h and let Z (N) = Y (N)

h

be the single-agent stochastic process with state space S (not necessarily Markov). Let Q(N)(x) be defined by P{Y (N)

h

(t + dt) = j | Y (N)

h

(t) = i, ˆ X(N)(t) = x} = q(N)

i,j (x)dt,

with Q(N)(x) → Q(x). Let z(t) be the time inhomogeneous-CTMC on S with infinitesimal generator Q(t) = Q(x(t)), x(t) fluid limit.

THEOREM (FAST SIMULATION THEOREM)

For any T < ∞, P{Z (N)(t) = z(t), t ≤ T} → 0.

  • R. Darling, J. Norris. Differential equation approximations for Markov chains. Probability Surveys, 2008.
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P2P NETWORK EPIDEMICS

SINGLE NODE

Y (N) ∈ {s, d, i, p}

RATES OF Z (N)

ext_inf:

1 X (N)

s

r (N)

ext_inf(X(N)) = 1 X (N)

s

kextX (N)

s

= kext infect:

1 X (N)

s

r (N)

infect(X(N)) = 1 N kinfX (N) i

= kinf ˆ Xi

(N)

RATES OF z

ext_inf: kext infect: kinfxi

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P2P NETWORK EPIDEMICS

The single agent infinitesimal generator is then Q(N)(x) = Q(x), giving the following time dependent Q-matrix Q(x(t)), where x(t) is the solution of the fluid equations.

    −kext − kinfxi(t) − klow kext + kinfxi(t) klow −kact − klow kact klow kdeact −kdeact − khigh khigh kloss − kloss    

Transient probabilities for the fluid approximation of the single agent can be computed by solving the forward Kolmogorov equations dΠ(0, t) dt = Π(0, t)Q(t).

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P2P NETWORK EPIDEMICS: TRANSIENT PROBABILITIES

20 40 60 80 100 120 0.0 0.2 0.4 0.6 0.8 1.0 time probability

  • CTMC N=100

ODE

  • s

d i p

N = 100

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P2P NETWORK EPIDEMICS: TRANSIENT PROBABILITIES

20 40 60 80 100 120 0.0 0.2 0.4 0.6 0.8 1.0 time probability

  • CTMC N=1000

ODE

  • s

d i p

N = 1000

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CLIENT SERVER EXAMPLE

SINGLE CLIENT

Y (N) ∈ {rq, w, t, rc}

RATES OF Z (N)

request:

1 C(N)

rq kr min(C(N)

rq , S(N) rq )

reply:

1 C(N)

w

min(kwC(N)

w , krpS(N) rp )

timeout: kto; recover: krc

RATES OF z

request: kr min(1, srq(t)

crq(t))

reply: min(kw, krp

srp(t) cw(t))

timeout: kto; recover: krc

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CLIENT-SERVER: TRANSIENT PROBABILITIES

100 200 300 400 500 0.0 0.2 0.4 0.6 0.8 1.0

Transient probability RQ

time probability CTMC N = 15 (10000 runs) CTMC N = 150 (10000 runs) fluid CTMC

request

100 200 300 400 500 0.0 0.1 0.2 0.3 0.4 0.5 0.6

Transient probability W

time probability CTMC N = 15 (10000 runs) CTMC N = 150 (10000 runs) fluid CTMC

wait

100 200 300 400 500 0.00 0.10 0.20 0.30

Transient probability T

time probability CTMC N = 15 (10000 runs) CTMC N = 150 (10000 runs) fluid CTMC

think

100 200 300 400 500 0.000 0.002 0.004 0.006

Transient probability RC

time probability CTMC N = 15 (10000 runs) CTMC N = 150 (10000 runs) fluid CTMC

recover

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OUTLINE

1 INTRODUCTION 2 FLUID APPROXIMATION

Markov population models Fluid approximation theorems

3 BEHAVIOUR SPECIFICATION

Individual Properties CSL model checking for time-homogeneous CTMC

4 MODEL CHECKING CSL FOR ICTMC

Model checking non-nested properties Time-dependent probabilities Nested CSL-formulae Theoretical results

5 FROM INDIVIDUAL TO COLLECTIVE BEHAVIOUR

From local properties to global properties Central Limit Approximation Examples Conclusions

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INDIVIDUAL PROPERTIES

We are interested in the behaviour of a (random) individual. We will specify such a behaviour in Continuous Stochastic Logic (CSL). Other possibilities include DFA, DTA, LTL, MiTL.

P2P NETWORK EPIDEMICS EXAMPLE

What is the probability of a node being infected within T units of time? Is the probability of a single node remaining infected for T units of time smaller than p1? Is the probability of a node being patched before getting infected larger than p2? What is the probability of being patched within time T1, and then remaining uninfected with probability at least p3 for T2 units of time?

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COLLECTIVE PROPERTIES

We will concentrate on collective properties of the form: ”What is the probability that a given fraction of individuals satisfies the local property φ (by time T)”?

P2P NETWORK EPIDEMICS EXAMPLE

What is the probability of at most one tenth of nodes being infected within T units of time? Is the probability of at least one third of nodes remaining infected for T units of time smaller than p1? Is the probability of at least half of nodes being patched before getting infected larger than p2?

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(TIME-BOUNDED) CONTINUOUS STOCHASTIC LOGIC

SYNTAX

φ = a | φ1 ∧ φ2 | ¬φ | P⊲

⊳p(X[T1,T2]φ) | P⊲ ⊳p(φ1U[T1,T2]φ2)

a is an atomic proposition; φ1 ∧ φ2 and ¬φ are the usual boolean connectives; P⊲

⊳p(X[T1,T2]φ) is the next state temporal modality.

P⊲

⊳p(φ1U[T1,T2]φ2) is the until temporal modality.

DERIVED MODALITIES

EVENTUALLY: F [0,T]φ ≡ true U[0,T]φ ALWAYS: G[0,T]φ ≡ ¬F [0,T]¬φ

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CSL - RESTRICTIONS

SYNTAX

φ = a | φ1 ∧ φ2 | ¬φ | P⊲

⊳p(X[T1,T2]φ) | P⊲ ⊳p(φ1U[T1,T2]φ2)

We do not consider timed-unbounded operators: 0 ≤ T1, T2 < ∞; We do not consider steady state probabilities; We do not consider rewards. Rewards can be easily added. Time unbounded and steady state properties are more problematic: Kurtz theorem works only for time-bounded horizons.

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CSL - NOTATION

We will interpret CSL formulae on a generic stochastic process Z(t) on S, such that all relevant sets of paths (i.e. those satisfying until or next formulae) are measurable.

PATHS

A path σ of Z(t) is a sequence σ = s0

t0

→ s1

t1

→ . . . , with non null probability of jumping from si to si+1, for each i;

NOTATION

σ@t is the state of σ at time t; σ[i] is the i-th state of σ; tσ[i] is the time of the i-th jump in σ;

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CSL- SEMANTICS

STATE FORMULAE

s, t0 | = a if and only if a ∈ L(s); s, t0 | = ¬φ if and only if s, t0 | = φ; s, t0 | = φ1 ∧ φ2 if and only if s, t0 | = φ1 and s, t0 | = φ2; s, t0 | = P⊲

⊳p(ψ) if and only if P{σ | σ, t0 |

= ψ} ⊲ ⊳ p.

PATH FORMULAE

σ, t0 | = X[T1,T2]φ if and only if tσ[1] ∈ [T1, T2] and σ[1], t0 + tσ[1] | = φ. σ, t0 | = φ1U[T1,T2]φ2 if and only if ∃¯ t ∈ [t0 + T1, t0 + T2] s.t. σ@¯ t,¯ t | = φ2 and ∀t0 ≤ t < ¯ t, σ@t, t | = φ1.

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EXAMPLE: P2P NETWORK INFECTION

ψ1 = F [0,T]ainfected (a node is infected within T units of time); φ1 = P<p1(G[0,T]ainfected) (the probability of a single node remaining infected for T units of time is smaller than p1); φ2 = P>p2(¬ainfectedU[0,T]apatched) (the probability of a node being patched before getting infected is larger than p2); ψ2 = F [0,T1](apatched ∧ P≥p3(G[0,T2]¬ainfected)) (a node is patched within time T1, and then remains not infected with probability at least p3 for T2 units of time).

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THE IDEA

Approximate the behaviour of an agent Z in the system using the time-inhomogeneous Markov chain z. Model check temporal logic formulae on z.

OUTLINE OF FOLLOWING TOPICS

A model checking algorithm for CSL on time-inhomogeneous CTMC (ICTMC). Investigation of its decidability. Convergence results (asymptotic correctness for large N).

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OUTLINE

1 INTRODUCTION 2 FLUID APPROXIMATION

Markov population models Fluid approximation theorems

3 BEHAVIOUR SPECIFICATION

Individual Properties CSL model checking for time-homogeneous CTMC

4 MODEL CHECKING CSL FOR ICTMC

Model checking non-nested properties Time-dependent probabilities Nested CSL-formulae Theoretical results

5 FROM INDIVIDUAL TO COLLECTIVE BEHAVIOUR

From local properties to global properties Central Limit Approximation Examples Conclusions

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CSL MODEL CHECKING: BASIC IDEAS

The model checking algorithm works by processing bottom up the parse tree of a formula. The intuition is that each state formula determines the set

  • f states satisfying it. Once this set has been computed,
  • ne can treat the state formula as an atomic proposition.

Dealing with atomic propositions and boolean connectives is easy: we just need to explain how to compute the satisfaction probability of path formulae.

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CSL MODEL CHECKING: NEXT STATE OPERATOR

PATH PROBABILITY X[T1,T2]φ

We just need to evaluate the probability that, being in a state s, we jump within time [T1, T2] to a state that satisfies φ. We know the set {s′ | s′ | = φ} by (inductive) hypothesis. We consider time-homogeneous CTMCs. The exit rate in state s is q(s) =

s′∈S, s′=s q(s, s′).

The rate at which we jump to a φ-state is qφ(s) =

s′| =φ, s′=s q(s, s′).

PROBABILITY DENSITY OF Xφ

qφ(s) q(s) q(s) exp(−q(s)t) = qφ(s) exp(−q(s)t)

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CSL MODEL CHECKING: NEXT STATE OPERATOR

PROBABILITY DENSITY OF Xφ

qφ(s) q(s) q(s) exp(−q(s)t) = qφ(s) exp(−q(s)t)

PROBABILITY OF X[T1,T2]φ

P(s, X[T1,T2]φ) = T2

T1

qφ(s) exp(−q(s)t)dt = qφ(s) q(s) (exp(−q(s)T1) − exp(−q(s)T2)) We then need to solve the inequality P(s, X[T1,T2]φ) ⊲ ⊳ p to decide if s satisfies P⊲

⊳p(X[T1,T2]φ).

This method requires the CTMC to be time-homogeneous

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CSL MODEL CHECKING: UNTIL OPERATOR

We start by considering the until path formula φ1U[0,T]φ2. We need to compute the probability of all paths that remain in a φ1-state before entering a φ2 state before time T. The idea is that if we enter a ¬φ1-state, we should discard the path, while if we enter a φ2-state, we are done. We can monitor these two events by “stopping” when they happen, making ¬φ1 and φ2-states absorbing (i.e. removing outgoing transitions).

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EXAMPLE

Consider the property notinfectedU[0,T]patched. We need to make infected and patched states absorbing.

suscept. infected inactive patched infected active ext_inf infect infect activate deactivate patch_high patch_low patch_low loss

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EXAMPLE

Consider the property notinfectedU[0,T]patched.

suscept. infected inactive patched infected active ext_inf infect patch_low

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CSL MODEL CHECKING: UNTIL OPERATOR

Let Π be the probability matrix: Π(0, T)[s, s′] gives the probability of being in s′ at time T, starting in s at time 0.

MODEL CHECKING ALGORITHM FOR φ1U[0,T]φ2

1

Make ¬φ1 and φ2 states absorbing

2

Compute the transient probability of the so modified CTMC at time T (using uniformisation or solving Kolmogorov equations): Π¬φ1∨φ2(0, T),

3

The desired probability is P(σ | = φ1U[0,T]φ2 | σ[0] = s) =

  • s′|

=φ2

Π¬φ1∨φ2[s, s′](0, T)

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CSL MODEL CHECKING: φ1U[T1,T2]φ2

We split the problem in two parts:

1

Compute the probability of not entering a ¬φ1 in the first T1 units of time, by making ¬φ1 states absorbing.

2

Compute the probability of the until formula φ1U[0,T2−T1]φ2

MODEL CHECKING ALGORITHM FOR φ1U[T1,T2]φ2

1

Compute Π¬φ1(0, T1) by transient analysis;

2

Compute Π¬φ1∨φ2(0, T2 − T1) by transient analysis;

3

The desired probability P(σ | = φ1U[T1,T2]φ2 | σ[0] = s) is

  • s1|

=φ1

  • s2|

=φ2

Π¬φ1(0, T1)[s, s1]Π¬φ1∨φ2[s1, s2](0, T2 − T1) The method works only for time-homogeneous CTMCs.

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OUTLINE

1 INTRODUCTION 2 FLUID APPROXIMATION

Markov population models Fluid approximation theorems

3 BEHAVIOUR SPECIFICATION

Individual Properties CSL model checking for time-homogeneous CTMC

4 MODEL CHECKING CSL FOR ICTMC

Model checking non-nested properties Time-dependent probabilities Nested CSL-formulae Theoretical results

5 FROM INDIVIDUAL TO COLLECTIVE BEHAVIOUR

From local properties to global properties Central Limit Approximation Examples Conclusions

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CSL MODEL CHECKING FOR ICTMC

The fluid limit z of a single agent in a population model is a time-inhomogeneous CTMC.

IMPLICATIONS

We cannot use the same algorithms sketched before, because we cannot always start transient computations from time 0. Non-nested properties can still be dealt with similarly, the difficulties arises with nested properties.

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CSL MODEL CHECKING FOR ICTMC

Consider a ICTMC with state space S and rates Q = Q(t). Focus on a non-nested until formula of the type P⊲

⊳p(φ1U[0,T]φ2)

which can be model checked as customary by solving the following reachability problem: What is the probability of reaching a φ2-state within time T without entering a ¬φ1-state?

SOLUTION

Make ¬φ1 ∨ φ2-states absorbing, and compute the probability of reaching a goal state at time T (e.g., by solving the Kolmogorov equations or by uniformisation for ICTMC).

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P2P NETWORK EPIDEMICS: THE MODEL

suscept. infected inactive patched infected active ext_inf infect infect activate deactivate patch_high patch_low patch_low loss

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P2P NETWORK EPIDEMICS: F [0,T]ainfected FROM STATE s

5 10 15 20 0.0 0.2 0.4 0.6 0.8 1.0 time probability

  • stat mc N=100 (10000 runs)

stat mc N=1000 (10000 runs) fluid mc

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P2P NETWORK EPIDEMICS: ¬ainfectedU[0,T]apatched FROM

STATE s

5 10 15 20 0.00 0.01 0.02 0.03 0.04 0.05 time probability

  • stat mc N=100 (10000 runs)

stat mc N=1000 (10000 runs) fluid mc

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NEXT-STATE PROBABILITY

PROBABILITY OF X[T1,T2]φ STARTING AT TIME t0

Pnext(t0)[s] = t0+T2

t0+T1

qφ(s, t) · e−Λ(t0,t)[s]dt where Λ(t0, t)[s] = t

t0 −qs,s(τ)dτ is the cumulative rate.

We can reduce the computation of the previous integral to the following initial value problem from t0 + T1 to t0 + T2.        d dt P(t) = qs,S0(t) · e−L(t) d dt L(t) = −qs,s(t) with P(t0 + T1) = 0 and L(t0 + T1) = Λ(t0, t0 + T1).

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P2P NETWORK EPIDEMICS: X[0,T]ainfected FROM STATE s

5 10 15 20 0.0 0.2 0.4 0.6 0.8 1.0 time probability

  • stat mc N=100 (10000 runs)

stat mc N=1000 (10000 runs) fluid mc

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CLIENT-SERVER: THE MODEL

request think wait recover request reply think recover timeout ready process reply log request logging process reply

CLIENT SERVER

timeout timeout

Crq Cw Crc Ct Srq Srp Sp Sl

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CLIENT-SERVER: P=?(F ≤Tatimeout)

500 1000 1500 2000 2500 3000 0.0 0.2 0.4 0.6 0.8 1.0

Pr=?[F<=T timeout] −− 10 clients, 5 servers

time probability stat mc (10000 runs) fluid mc

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CLIENT-SERVER: P=?(arequest ∨ awaitU≤Tatimeout)

20 40 60 80 100 0.00 0.02 0.04 0.06 0.08 0.10

Pr=?[(request or wait) U<=T timeout] −− 10 clients, 5 servers

time probability stat mc (10000 runs) fluid mc

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CLIENT-SERVER: COMPUTATIONAL COST

500 1000 1500 2000 2500 3000 0.0 0.2 0.4 0.6 0.8 1.0 Pr=?[F<=T timeout] −− 10 clients, 5 servers time probability stat mc (10000 runs) fluid mc 20 40 60 80 100 0.00 0.02 0.04 0.06 0.08 0.10 Pr=?[(request or wait) U<=T timeout] −− 10 clients, 5 servers time probability stat mc (10000 runs) fluid mc

COMPUTATIONAL COST

The cost of analysing the limit fluid system is independent

  • f N.

For the client server example (10 clients - 5 servers) it is ∼100 times faster than the simulation-based approach (which increases linearly with N).

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P2P NETWORK EPIDEMICS: COMPUTATIONAL COST

5 10 15 20 0.0 0.2 0.4 0.6 0.8 1.0 time probability

  • stat mc N=100 (10000 runs)

stat mc N=1000 (10000 runs) fluid mc 5 10 15 20 0.00 0.01 0.02 0.03 0.04 0.05 time probability

  • stat mc N=100 (10000 runs)

stat mc N=1000 (10000 runs) fluid mc

COMPUTATIONAL COST

Checked property Fluid MC SMC (N = 100) SMC (N = 1000) Kolmogorov Equations ∼ 0.1 s ∼ 64 s ∼ 101 s X[0,T]ainfected ∼ 0.06 s ∼ 6 s ∼ 24 s ¬ainfectedU[0,T]apatched ∼ 0.05 s ∼ 5 s ∼ 20 s

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OUTLINE

1 INTRODUCTION 2 FLUID APPROXIMATION

Markov population models Fluid approximation theorems

3 BEHAVIOUR SPECIFICATION

Individual Properties CSL model checking for time-homogeneous CTMC

4 MODEL CHECKING CSL FOR ICTMC

Model checking non-nested properties Time-dependent probabilities Nested CSL-formulae Theoretical results

5 FROM INDIVIDUAL TO COLLECTIVE BEHAVIOUR

From local properties to global properties Central Limit Approximation Examples Conclusions

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CSL MODEL CHECKING FOR ICTMC

Consider a ICTMC with state space S and rates Q = Q(t). φ1U[0,T]φ2 and X[T1,T2]φ Time-homogeneity ⇒ we can run each transient analysis/ integral computation from time t0 = 0! This is no more true in time-inhomogeneous CTMCs, as the probability of a path formula depends on the time at which we evaluate it. Problems arise when we consider nested until formulae. The truth value of φ in a state s depends on the time t at which we evaluate it.

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TIME-DEPENDENT PROBABILITY OF X[T1,T2]φ

PROBABILITY OF X[T1,T2]φ STARTING AT TIME t0

Pnext(t0)[s] = t0+T2

t0+T1

qφ(s, t) · e−Λ(t0,t)[s]dt where Λ(t0, t)[s] = t

t0 −qs,s(τ)dτ is the cumulative rate.

INTUITION

Compute

d dt0 Pnext(t0)[s]

Construct an ODE for Pnext(t0) and solve the i.v. problem.

CHECKING P⊲

⊳p(X[T1,T2]φ)

Compute the path probability Pnext(t0)[s] of X[T1,T2]φ as a function of t0 Solve the inequality Pnext(t0)[s] ⊲ ⊳ p

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P2P NETWORK EPIDEMICS: X[0,10]ainfected

2 4 6 8 10 0.5 0.6 0.7 0.8 0.9 1.0 1.1 time probability

false true T~ 2.26 Prob(p,t0 |=X[0,10] infected)

t0 varying (Red line: P≥0.8(X[0,10]ainfected))

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TIME-DEPENDENT REACHABILITY PROBABILITY

Focus on P⊲

⊳p(φ1U[0,T]φ2). Assume that the truth of φ1 and φ2

does not depend on time. Let Π(t1, t2) = (πsi,sj(t1, t2))i,j be the probability matrix giving the probability of being in state sj at time t2, given that we are in state si at time t1. We consider Π = Π¬φ1∨φ2, the probability matrix of the CTMC in which ¬φ1 ∨ φ2 states are made absorbing.

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FORWARD AND BACKWARD KOLMOGOROV EQUATIONS

The device to compute the time dependent probability of an until formula φ1U[0,T]φ2 are the Kolmogorov equations for ICTMCs.

FORWARD KOLMOGOROV EQUATION

d dt Π(s, t) = Π(s, t)Q(t)

BACKWARD KOLMOGOROV EQUATION

d dsΠ(s, t) = −Q(s)Π(s, t)

COMPUTING Π(t, t + T), FOR FIXED T

We just need to combine the two backward and forward equations by chain rule.

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TIME-DEPENDENT REACHABILITY PROBABILITY

  • 1. COMPUTE Π(t, t + T), FOR t ∈ [0, Tf]

Π(t, t + T), as a function of t, with initial conditions Π(0, T), satisfies: dΠ(t, t + T) dt = Π(t, t + T)Q(t + T) − Q(t)Π(t, t + T)

  • 2. ADD PROBABILITY FOR GOAL STATES

Pφ1U[0,T]φ2(s, t) is equal to

s′| =φ2 Π¬φ1∨φ2(t, t + T)[s, s′].

  • 3. COMPARE WITH THRESHOLD p

The truth value T(φ, s, t) of formula φ in state s at time t is

  • btained by solving the inequality Pφ1U[0,T]φ2(s, t) ⊲

⊳ p. We need to find the zeros of the function Pφ1U[0,T]φ2(s, t) − p.

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P2P NETWORK EPIDEMICS: G[0,10]¬ainfected

50 100 150 0.95 0.96 0.97 0.98 time probability

false true T~81.8 Prob(p,t0 |= G[0,10] not_infected p,t0 |= P>0.97(G[0,10] not_infected)

from state p (patched)

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CLIENT SERVER: P=?F ≤50atimeout AS A FUNCTION OF t0

  • 5

10 15 20 25 0.00 0.05 0.10 0.15 0.20

Pr=?[F<=50 timeout] −− t0 varying −− 10 clients, 5 servers

initial time probability

  • stat mc (10000 runs)

fluid mc

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CLIENT-SERVER: P<0.167(F ≤50timeout)

20 40 60 80 100 0.00 0.05 0.10 0.15 0.20

Pr=?[F<=50 timeout] −− t0 varying

initial time probability false true 0.167 t ~ 2.1 rq truth−value

P<0.167(F ≤50timeout) from state rq of client.

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COMPUTING THE TIME-DEPENDENT TRUTH IN PRACTICE

The equation dΠ(t,t+T)

dt

= Π(t, t + T)Q(t + T) − Q(t)Π(t, t + T) is utterly stiff. Its integration error blows up even for the most accurate Matlab/Octave solvers.

5 10 15 20 25 30 35 40 time 5.000 10.000 15.000 20.000 25.000 30.000 35.000 40.000 45.000 50.000 55.000 60.000 65.000 70.000 75.000 80.000 85.000 90.000 95.000 100.000 values

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COMPUTING THE TIME-DEPENDENT TRUTH IN PRACTICE

The equation dΠ(t,t+T)

dt

= Π(t, t + T)Q(t + T) − Q(t)Π(t, t + T) is utterly stiff. Its integration error blows up even for the most accurate Matlab/Octave solvers. time T0 = 0 T1 = 1 · T T2 = 2 · T Tk = k · T · · · Practically, we can exploit the semigroup property Π(t, t + T) = Π(t, Tj)Π(Tj, t + T) and solve backward and forward equations separately, looping

  • ver j.
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OUTLINE

1 INTRODUCTION 2 FLUID APPROXIMATION

Markov population models Fluid approximation theorems

3 BEHAVIOUR SPECIFICATION

Individual Properties CSL model checking for time-homogeneous CTMC

4 MODEL CHECKING CSL FOR ICTMC

Model checking non-nested properties Time-dependent probabilities Nested CSL-formulae Theoretical results

5 FROM INDIVIDUAL TO COLLECTIVE BEHAVIOUR

From local properties to global properties Central Limit Approximation Examples Conclusions

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TIME-DEPENDENT TRUTH

When computing the truth value of an until formula, we

  • btain a time dependent value T(φ, s, t) in each state.

When we consider nested temporal operators, we need to take this into account. The problem is that in this case the TOPOLOGY OF GOAL

AND UNSAFE STATES in the CTMC can CHANGE IN TIME.

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TIME DEPENDENT TRUTH: F ≤Tφ

t false true Td T(φ, s, t) At discontinuity times, changes in topology introduce discontinuities in the probability values.

BUT...

Discontinuities happen at specific and FIXED time instants. We can solve Kolmogorov equations piecewise!

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k DISCONTINUITIES T1, . . . , Tk IN [t, t + T]

time t t + T T1 T2 Tk Tk+1 · · ·

THE GENERIC CK EQUATION

Π(t, t + T) = Π1(t, T1)ζ(T1)Π2(T1, T2)ζ(T2) · · · ζ(Tk)Πk+1(Tk, t + T).

ζ(Tj) apply the proper bookkeeping operations to deal with changes in the topology of absorbing states. We can compute Π(t, t + T) by an ODE obtained by derivation and application of chain rule. In advancing time, when we hit a discontinuity point (from below or above), the structure of the previous equation changes: integration has to be stopped and restarted.

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THE ALGORITHM (SKETCHED)

Proceed bottom-up on the parse tree of a formula. Case T(P⊲

⊳p(φ1U[0,T]φ2), t):

Compute T(φ1, t) and T(φ2, t) Let T1, . . . , Tm be all the discontinuity points of T(φ1, t) and T(φ2, t) up to a final time Tf. Compute Π(Ti, Ti + 1) for each i Compute Π(0, T) using generalized CK equations Integrate d

dt Π(t, t + T) up to Tf.

Return T(P⊲

⊳p(φ1U[0,T]φ2), t) = Π(t, t + T) ⊲

⊳ p. The use of Kolmogorov equations is feasible if the state space is small (few dozens of states). This is usually the case for single agent mean field models.

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P2P NETWORK EPIDEMICS: F [0,T](apatched ∧ P≥0.97(G[0,10]¬ainfected))

50 100 150 0.0 0.2 0.4 0.6 0.8 1.0 time probability

T~81.8 Prob(p,t0 |= F[0,T] (patched AND P>0.97(G[0,10] not_infected))

from state p (patched)

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CLIENT-SERVER: F ≤T(P<0.167(F ≤50timeout))

10 20 30 40 0.0 0.2 0.4 0.6 0.8 1.0

F<=t(Pr<0.167[F<=50 timeout])

time probability R(0)=1 W(0)=1 T(0)=1 A(0)=1

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OUTLINE

1 INTRODUCTION 2 FLUID APPROXIMATION

Markov population models Fluid approximation theorems

3 BEHAVIOUR SPECIFICATION

Individual Properties CSL model checking for time-homogeneous CTMC

4 MODEL CHECKING CSL FOR ICTMC

Model checking non-nested properties Time-dependent probabilities Nested CSL-formulae Theoretical results

5 FROM INDIVIDUAL TO COLLECTIVE BEHAVIOUR

From local properties to global properties Central Limit Approximation Examples Conclusions

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DECIDABILITY

DECIDABILITY

We use algorithms to solve ODEs with error guarantee (interval analysis). We need to find zeros of function P(s, t) − p (root finding), and guarantee their number to be finite (restrict to piecewise-real analytic functions). To answer the CSL query for main until formulae, we need to know if P(s, 0) ⊲ ⊳ p (zero test). It is not known if root finding and zero test are decidable. p

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DECIDABILITY

DECIDABILITY

We use algorithms to solve ODEs with error guarantee (interval analysis). We need to find zeros of function P(s, t) − p (root finding), and guarantee their number to be finite (restrict to piecewise-real analytic functions). To answer the CSL query for main until formulae, we need to know if P(s, 0) ⊲ ⊳ p (zero test). It is not known if root finding and zero test are decidable.

THEOREM (QUASI-DECIDABILITY)

Let φ = φ(p) be a CSL formula, with constants p = (p1, . . . , pk) ∈ [0, 1]k appearing in until formulae. The CSL model checking for ICTMC problem is decidable for p ∈ E, where E is an open subset of [0, 1]k, of measure 1.

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CONVERGENCE OF CSL TRUTH

We considered also convergence of CSL properties: are properties that are true in z(t) ultimately true in Z (N)(t)? Convergence suffers from similar issues as decidability (e.g., non-simple zeros , P(s, 0) = p).

THEOREM (ASYMPTOTIC CORRECTNESS)

Let φ = φ(p) be a CSL formula, with constants p = (p1, . . . , pk) ∈ [0, 1]k appearing in until formulae. Then, for p ∈ E, an open subset of [0, 1]k of measure 1, there exists N0 such that ∀N ≥ N0 s, 0 | =Z (N) φ ⇔ s, 0 | =z φ.

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OUTLINE

1 INTRODUCTION 2 FLUID APPROXIMATION

Markov population models Fluid approximation theorems

3 BEHAVIOUR SPECIFICATION

Individual Properties CSL model checking for time-homogeneous CTMC

4 MODEL CHECKING CSL FOR ICTMC

Model checking non-nested properties Time-dependent probabilities Nested CSL-formulae Theoretical results

5 FROM INDIVIDUAL TO COLLECTIVE BEHAVIOUR

From local properties to global properties Central Limit Approximation Examples Conclusions

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FROM LOCAL TO GLOBAL

We restrict the set of properties we consider to non-nested CSL path formulae ψ.

LOCAL PROPERTY

What is the probability that a given agent Z satisfies ψ? P{Z (N) | = ψ} =?

GLOBAL PROPERTY

What is the probability that a fraction α of agents satisfy ψ? P

j

1{Z (N)

j

| = ψ} ⊲ ⊳ Nα

  • =?
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FROM LOCAL TO GLOBAL

Consider the client-server model, and the local property: ψ = (arequest ∨ await)U≤Tatimeout

20 40 60 80 100 0.00 0.02 0.04 0.06 0.08 0.10 Pr=?[(request or wait) U<=T timeout] −− 10 clients, 5 servers time probability stat mc (10000 runs) fluid mc

P{Z (N) | = ψ} can be approximated by P{z | = ψ}, using the fluid method presented above. But how can we compute P

j 1{Z (N) j

| = ψ} ≥ Nα

  • ?
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FROM LOCAL TO GLOBAL: DECOUPLING OF AGENTS

One consequence of the fluid approximation theorem is that, in the limit, individual agents become independent. Hence P{Z (N)

1

| = ψ, Z (N)

2

| = ψ} ≈ P{Z (N)

1

| = ψ}P{Z (N)

2

| = ψ}

BINOMIAL APPROXIMATION

  • j

1{Z (N)

j

| = ψ} ∼ Bin(N, P{z | = ψ})

20 40 60 80 100 0.0 0.2 0.4 0.6 0.8 1.0 100 clients, 50 servers

time horizon probability

stat mc (10000 runs) binomial fluid mc

We ignore correlations between agents for finite N!

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OUTLINE

1 INTRODUCTION 2 FLUID APPROXIMATION

Markov population models Fluid approximation theorems

3 BEHAVIOUR SPECIFICATION

Individual Properties CSL model checking for time-homogeneous CTMC

4 MODEL CHECKING CSL FOR ICTMC

Model checking non-nested properties Time-dependent probabilities Nested CSL-formulae Theoretical results

5 FROM INDIVIDUAL TO COLLECTIVE BEHAVIOUR

From local properties to global properties Central Limit Approximation Examples Conclusions

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CENTRAL LIMIT APPROXIMATION

Master equation:

∂P(¯ X(N), t) ∂t =

  • τ∈T
  • f (N)

τ

(¯ X(N) − ¯ vτ)P(¯ X(N) − ¯ vτ, t) − f (N)

τ

(¯ X(N))P(¯ X(N), t)

  • If we approximate populations continuously and assume

¯ X(N)(t) = x(t) + N− 1

2 ζ(t)

then the master equation can be approximated at zeroth order in N by a Fokker-Planck equation: ∂Π(ζ(t), t) ∂t = −

  • s,h

∂ ∂Φs Fh(x(t)) ∂ ∂ζh ζsΠ (ζ(t), t)

  • +

+

  • ℓ,r

1 2Gℓr(x(t)) ∂2 ∂ζℓζr Π (ζ(t), t)

  • ;

G(x) =

  • τ∈T

vτvT

τ fτ(x).

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CENTRAL LIMIT APPROXIMATION

The solution Π(ζ, t) of the Fokker-Planck equation is a Gaussian distribution mean E[ζ(t)] such that

  • ∂tE[ζ(t)] = JF(x(t))E[ζ(t)]

E[ζ(0)] = 0 covariance matrix Cov[ζ(t)] such that

  • ∂tCov[ζ(t)] = JF(x(t))Cov[ζ(t)] + Cov[ζ(t)]JT

F(x(t)) + G(x(t))

Cov[ζ(0)] = 0 Hence X(N)(t) ∼ Norm

  • N · x(t),
  • N · Cov[ζ(t)]
  • .
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OUTLINE

1 INTRODUCTION 2 FLUID APPROXIMATION

Markov population models Fluid approximation theorems

3 BEHAVIOUR SPECIFICATION

Individual Properties CSL model checking for time-homogeneous CTMC

4 MODEL CHECKING CSL FOR ICTMC

Model checking non-nested properties Time-dependent probabilities Nested CSL-formulae Theoretical results

5 FROM INDIVIDUAL TO COLLECTIVE BEHAVIOUR

From local properties to global properties Central Limit Approximation Examples Conclusions

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COMPUTING GLOBAL PROPERTIES

  • 1. Modify the local agent model by creating unsafe and goal copies of

its states. Client-server model, local property φ = (arequest ∨ await)U≤Tatimeout:

CG

rc

CU

rc

Crc CG

rq

CU

rq

Crq CG

w

CU

w

Cw CG

t

CU

t

Ct goal unsafe safe timeout think rec req reply timeout think rec req reply timeout req reply

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COMPUTING GLOBAL PROPERTIES

CG

rc

CU

rc

Crc CG

rq

CU

rq

Crq CG

w

CU

w

Cw CG

t

CU

t

Ct goal unsafe safe timeout think rec req reply timeout think rec req reply timeout req reply

  • 2. From the modified local model, construct a population model. Add

a new variable Gφ, counting how many agents are in a goal state.

  • 3. Apply central limit approximation to this new model.
  • 4. Compute P{G(N)

φ

≥ αN} by G(N)

φ

∼ Norm

  • Ngφ(t),
  • NVar[ζgφ(t)]
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CLIENT-SERVER - P{G(N)

arequest∨awaitU≤Tatimeout ≥ Nθ}

10 20 30 40 50 0.0 0.2 0.4 0.6 0.8 1.0

100 clients, 50 servers

time horizon probability

stat mc (10000 runs) linear noise mc

N = 150, θ = 0.05

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CLIENT-SERVER - P{G(N)

arequest∨awaitU≤Tatimeout ≥ Nθ}

5 10 15 20 25 30 0.0 0.2 0.4 0.6 0.8 1.0

500 clients, 250 servers

time horizon probability

stat mc (10000 runs) linear noise mc

N = 750, θ = 0.05

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CLIENT-SERVER - P{G(N)

arequest∨awaitU≤Tatimeout ≥ Nθ}

5 10 15 20 25 30 0.0 0.2 0.4 0.6 0.8 1.0

1000 clients, 500 servers

time horizon probability

stat mc (10000 runs) linear noise mc

N = 1500, θ = 0.05

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CLIENT-SERVER - P{G(N)

arequest∨awaitU≤Tatimeout ≥ Nθ}

20 40 60 0.000 0.010 0.020 0.030

500 clients, 250 servers

time number

ctmc (10000 runs) linear noise corrected ln

N = 1500, θ = 0.2

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CLIENT-SERVER - P{G(N)

arequest∨awaitU≤Tatimeout ≥ Nθ}

20 40 60 20 40 60 80

500 clients, 250 servers

time number

ctmc (10000 runs) linear noise

N = 1500, average value of Ngφ and G(N)

φ .

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CLIENT-SERVER - P{G(N)

arequest∨awaitU≤Tatimeout ≥ Nθ}

20 40 60 0.000 0.010 0.020 0.030

500 clients, 250 servers

time number

ctmc (10000 runs) linear noise corrected ln

N = 1500, θ = 0.2, corrected central limit

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OUTLINE

1 INTRODUCTION 2 FLUID APPROXIMATION

Markov population models Fluid approximation theorems

3 BEHAVIOUR SPECIFICATION

Individual Properties CSL model checking for time-homogeneous CTMC

4 MODEL CHECKING CSL FOR ICTMC

Model checking non-nested properties Time-dependent probabilities Nested CSL-formulae Theoretical results

5 FROM INDIVIDUAL TO COLLECTIVE BEHAVIOUR

From local properties to global properties Central Limit Approximation Examples Conclusions

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CONCLUSIONS

We discussed an application of mean field theory to model check properties of medium and large population models. We considered first single agent properties, focussing on CSL and providing a method to model check CSL formulae versus time-inhomogeneous CTMC. We provided convergence results that guarantee quasi-consistence of the method. We then extended (non-nested) single agent properties to population level, using the central limit approximation. For collective properties, we have also considered a richer class of path properties specified by (restricted) DTA .

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FUTURE WORK

Use error bounds for mean field convergence to provide a (very rough) estimate of the error. Include rewards, and time-unbounded/ steady state, when possible. Working implementation. Consider other logics on single agents (e.g. MTL, LTL). Consider different properties for collective probabilities, specified by timed automata or LTL (in a local to global perspective and in a global perspective). Understand accuracy of central limit theorem.

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BIBLIOGRAPHY

COURSE TOPICS

  • L. Bortolussi, J. Hillston, D. Latella, M. Massink.Continuous

Approximation of Collective Systems Behaviour: a Tutorial. Performance Evaluation, 2013.

  • L. Bortolussi, J. Hillston: Fluid Model Checking. CONCUR 2012.
  • L. Bortolussi, J. Hillston: Model Checking Single Agent

Behaviours by Fluid Approximation, submitted to Information and Computation.

  • L. Bortolussi, R. Lanciani. Model Checking Markov Population

Models by Central Limit Approximation. QEST 2013.

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BIBLIOGRAPHY

RELATED WORK

  • M. Tribastone, S. Gilmore, J. Hillston: Scalable Differential

Analysis of Process Algebra Models. IEEE Trans. Softw Eng. 2012. R.A. Hayden, A. Stefanek, J.T. Bradley. Fluid computation of passage-time distributions in large Markov models. Theor.

  • Comput. Sci. 2012.
  • R. A. Hayden and J. T. Bradley and A. Clark: Performance

Specification and Evaluation with Unified Stochastic Probes and Fluid Analysis, IEEE Trans. Software Eng., 2013.

  • R. Darling, J. Norris. Differential equation approximations for

Markov chains. Probability Surveys, 2008.

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BIBLIOGRAPHY

MODEL CHECKING ICTMC

J.P . Katoen, A. Mereacre. Model Checking HML on Piecewise-Constant Inhomogeneous Markov Chains. FORMATS 2008.

  • T. Chen, T. Han, J.P

. Katoen, A. Mereacre: LTL Model Checking

  • f Time-Inhomogeneous Markov Chains. ATVA 2009.
  • T. Chen, T. Han, J.P

. Katoen, A. Mereacre: Model Checking of Continuous-Time Markov Chains Against Timed Automata

  • Specifications. Logical Methods in Computer Science 7, 2011.
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THE END!

Thanks for the attention Questions?