A RUIN MODEL WITH DEPENDENCE BETWEEN CLAIM SIZES AND CLAIM INTERVALS

Size: px
Start display at page:

Download "A RUIN MODEL WITH DEPENDENCE BETWEEN CLAIM SIZES AND CLAIM INTERVALS"

Transcription

1 A RUIN MODEL WITH DEPENDENCE BETWEEN CLAIM SIZES AND CLAIM INTERVALS Hansjörg Albreher a, Onno J. Boxma b a Graz University of Tehnology, Steyrergasse 3, A-8 Graz, Austria b Eindhoven University of Tehnology and EURANDOM, P.O. Box 53, 56 MB Eindhoven, The Netherlands Abstrat We onsider a generalization of the lassial ruin model to a dependent setting, where the distribution of the time between two laim ourrenes depends on the previous laim size. Exat analytial expressions for the Laplae transform of the ruin funtion are derived. The results are illustrated by several examples. Introdution The lassial Cramer-Lundberg model to desribe the surplus proess of an insurane portfolio relies on the assumption of independene among laim sizes and between laim sizes and laim inter-ourrene times. However, in pratie this assumption is often too restritive and there is a need for more general models where the independene assumptions an be relaxed. Reently, various results have been obtained onerning the asymptoti behaviour of the probability of ruin for dependent laims. In the ase of light-tailed laim sizes, Nyrhinen 2, 3 derived Lundberg-type limiting results using large deviations tehniques and Müller and Pflug introdued dependene orderings to relate the limiting ruin probabilities. The behaviour of the Lundberg exponent as a funtion of a dependene measure has been investigated in Albreher and Kantor 2. For heavy-tailed laim size distributions, the asymptoti behaviour of the ruin probability with dependent laims was studied e.g. in Asmussen et al. 5 and Mikosh and Samorodnitsky 9,. However, all these results are of asymptoti nature and it is a hallenging problem to obtain results on the probability of ruin in a dependent setting, also for smaller values of the initial apital. Motivated by a related model in queueing theory (f. Boxma and Perry 6), in this paper a generalization of the lassial ruin model is onsidered, where the distribution of the time between two laim ourrenes depends on the previous laim size. presented at the 7th International Congress on Insurane: Mathematis & Eonomis in Lyon, June 25-27, 23 Supported by the Researh Counil of the K.U. Leuven and the Austrian Siene Foundation Projet S-838-MAT

2 For this speifi dependent model, we derive exat solutions for the probability of survival by means of Laplae-Stieltjes transforms. This seems to be the first exat formula for the ruin probability in a ontinuous-time risk model allowing for dependeny and thus should be viewed as a starting point for deriving analytial solutions in more general dependent senarios. For example, we would like to onsider (i) more general laim inter-ourrene distributions, and (ii) situations in whih the laim sizes and laim inter-ourrene times depend on a ommon Markov hain (f., 8). The paper is organized in the following way: In Setion 2 we introdue the risk model and derive the exat expressions for the probability of survival. In Setion 3, several related models that allow for a similar treatment are disussed. Setion 4 ontains some numerial illustrations and investigates the effet of ignoring the dependene struture. 2 The Model Let us onsider the following risk model for the surplus proess R(t) of an insurane portfolio: N(t) R(t) = x + t B j, where x is the initial apital, is the premium density whih is assumed to be onstant, B j is the size of the jth laim and N(t) is the number of laims up to time t. Let B i be a sequene of i.i.d. random variables with distribution funtion B( ), mean β and Laplae-Stieltjes transform (LST) b( ). We assume the laim ourrene proess to be of the following Markovian type: If a laim B i is larger than a threshold T i, then the time until the next laim is exponentially distributed with rate λ, otherwise it is exponentially distributed with rate λ 2. The quantities T i are assumed to be i.i.d. random variables with distribution funtion T ( ). In the sequel, B (T ) shall denote a generi laim size (threshold) with distribution B( ) (T ( )). 2. Exat Solutions We are interested in the probability of survival φ(x), i.e. P(R(t) t > R() = x). Let us assume that j= β < P(B > T ) λ + P(B T ) λ 2, () whih is the net profit ondition, and P(B > ) = P(T > ) =. Let φ i (x) (i =, 2) denote the probability of survival with initial apital x given that the first laim ours aording to the exponential distribution with rate λ i. Then we get 2

3 φ (x) = ( λ dt)φ (x + dt)+ x+ dt + λ dt P(T y)φ (x + dt y) + P(T > y)φ 2 (x + dt y) db(y). Taylor expansion and rearranging yields dφ x dx (x) λ φ (x) + λ Similarly we obtain dφ x 2 dx (x) λ 2φ 2 (x) + λ 2 Define, for Re s : P(T y)φ (x y)db(y)+ + λ x P(T y)φ (x y)db(y)+ χ (s) := Ee sb (B>T ) = χ 2 (s) := Ee sb (B T ) = + λ 2 x x= and denote the Laplae transform of φ i (x) by Note that χ (s) + χ 2 (s) = b(s). φ i (s) := x= P(T > y)φ 2 (x y)db(y) =. (2) P(T > y)φ 2 (x y)db(y) =. (3) e sx T (x)db(x), e sx ( T (x))db(x), e sx φ i (x) dx. From (2) and (3) it follows that for Re s we have φ (s) s λ + λ χ (s) + λ φ2 (s)χ 2 (s) = φ (+), φ 2 (s) s λ 2 + λ 2 χ 2 (s) + λ 2 φ (s)χ (s) = φ 2 (+), whih an further be simplified to 3

4 φ (+) s λ 2 + λ 2 χ 2 (s) λ χ 2 (s)φ 2 (+) φ (s) = s λ + λ χ (s) s λ 2 + λ 2 χ 2 (s) λ λ 2 χ (s)χ 2 (s) (4) and φ 2 (s) = φ 2 (+) s λ + λ χ (s) λ 2 χ (s)φ (+). (5) s λ + λ χ (s) s λ 2 + λ 2 χ 2 (s) λ λ 2 χ (s)χ 2 (s) Note that the denominators on the right-hand side of (4) and (5) oinide. Remark: If we set λ = λ 2 := λ in (4) we obtain φ (s) = φ (+) s λ + λχ 2 (s) λχ 2 (s)φ (+) ( s λ + λχ (s))( s λ + λχ 2 (s)) λ 2 χ (s)χ 2 (s) = φ (+) s λ + λ b(s), and thus we retain the lassial Pollazek-Khinthine formula for the independent setting. For omplete solution we now need to determine the quantities φ i (+). Sine lim φ i(x) = we have x lim s φ i (s) = (i =, 2). (6) s Using (6) w.l.o.g. in (4) (equation (5) would lead to the same result), we obtain = lim s ( s ) φ (+) s λ 2 + λ 2 χ 2 (s) λ χ 2 (s)φ 2 (+) s λ + λ χ (s) s λ 2 + λ 2 χ 2 (s) λ λ 2 χ (s)χ 2 (s) = λ 2φ (+)( + χ 2 ()) λ χ 2 ()φ 2 (+) = lim s ( s λ +λ χ (s)) ( s λ 2 +λ 2 χ 2 (s)) λ λ 2 χ (s)χ 2 (s) s λ 2 φ (+)( + χ 2 ()) λ χ 2 ()φ 2 (+). (7) λ (χ () ) + λ 2 (χ 2 () ) λ λ 2 (χ () + χ 2()) Now we an use the relations χ 2 () = P(B T ), χ () = P(B > T ) and thus χ () + χ 2 () = and also E(B (B T ) ) = χ 2(), E(B (B>T ) ) = χ () and β = χ () χ 2(). In this way (7) an be substantially simplified yielding ( φ (+)) P(B > T ) λ + ( φ 2 (+)) P(B T ) λ 2 = β. (8) 4

5 Remark: For the speial ase λ = λ 2 := λ we obtain from (8) φ (+) = φ 2 (+) = λβ, (9) whih is the well-known formula for the survival probability with zero initial apital in the lassial independent ase. We now need a seond equation for φ (+) and φ 2 (+). Using Rouhé s theorem, one an show the following: Lemma. The denominator of (4) has exatly one zero σ with Re σ >. Proof. Rewrite the denominator of (4) and (5) as s(h (s) + h 2 (s)), in whih h (s) := s λ λ 2, h 2 (s) := λ χ (s) + λ 2 χ 2 (s) + λ λ 2 β b(s). βs We wish to show that this denominator has exatly one zero for Re s > ; note that the behaviour of φ i (s) at s = has already been analysed and exploited in (7). Let us now apply Rouhé s theorem to the losed ontour C, onsisting of the imaginary axis from ir to +ir and a semi-irle in the right halfplane with radius r and origin O; we shall let r. h (s) and h 2 (s) are analyti inside C; notie that b(s) βs is the LST of x B(y) dy whih is the residual (forward reurrene) laim β size distribution. Hene it is analyti and (as will be used below) bounded by one in absolute value in the right halfplane. Furthermore, h (s) has exatly one zero inside C for r large enough. For the appliation of Rouhé s theorem it remains to show that h (s) > h 2 (s) on C. This is learly true on the semi-irle. On the imaginary axis, h (s) λ + λ 2, whereas, under the ondition (), h 2 (s) λ χ () + λ 2 χ 2 () + λ λ 2 β < λ + λ 2. () In fat, it is easy to see that σ is real, with < σ < λ +λ 2, sine h () + h 2 () < and h ( λ +λ 2 ) + h 2 ( λ +λ 2 ) >. Sine φ i (s) is an analyti funtion for Re s, σ must also be a zero of the numerators of (4) and (5). In both ases this yields the same relation between φ (+) and φ 2 (+), namely φ 2 (+) = σ λ 2 + λ 2 χ 2 (σ) φ (+) = λ χ 2 (σ) λ 2 χ (σ) σ λ + λ χ (σ) φ (+). () Combined with (4), (5) and (8), this ompletes the determination of φ i (s), i =, 2. 5

6 Remark. Note that whenever χ i (s) (i =, 2) are rational funtions (whih is e.g. fulfilled if the orresponding onditional distributions are phase-type), then the Laplae-Stieltjes transforms (4) and (5) an be inverted expliitly to yield exat formulae for φ i (x) (i =, 2) (see e.g. Spiegel 4). Sine the lass of phase-type distributions is dense (in the sense of weak onvergene) in the lass of all distributions on the positive half-line, one an approximate any given distribution arbitrarily losely by a phase-type distribution and use the exat solutions above (algorithms for phase-type fitting are e.g. disussed in Asmussen 3). Example. For the speial ase T Exp(µ) we obtain χ 2 (s) = x= χ (s) = b(s) b(s + µ). e sx e µx db(x) = b(s + µ), If in addition B Exp(ν), with ν = /β, then we have ν χ 2 (s) = ν + s + µ, χ (s) = ν ν + s ν ν + s + µ, and thus σ in () is the unique solution s with Re s > of ( λ µν )( s + (ν + s)(ν + µ + s) λ λ 2 ν ) s + ν + µ + s λ λ λ 2 µν 2 2 (ν + µ + s) 2 (ν + s) =. Sine the Laplae-Stieltjes transforms are rational funtions in this ase, they an be inverted expliitly for any given parameter values (see Setion 4 for a speifi numerial example). Example 2. For a deterministi threshold (i.e. T i = T a.s. for all i and some onstant T > ) and exponential laim sizes (B i Exp(ν)) we obtain χ (s) = ν ν + s e (ν+s)t and χ 2 (s) = ν ν + s ( e (ν+s)t ). (2) 2.2 Comparison to Model with Independene The availability of analytial solutions for the survival probability allows one to investigate the error produed by negleting a dependeny struture of the above kind. Indeed, assuming independene when in fat the dependeny struture of Model is present, an estimation of distribution of the inter-ourrene time W i would lead to the mixing density f Wi (x) = P(B i > T i )λ e λ x + P(B i T i )λ 2 e λ 2x, i.e. one would assume to have a renewal model (also alled Sparre Andersen risk model) with a hyper-exponential inter-arrival distribution. For suh a model, the Lundberg oeffiient R, given it exists, an easily be determined as the unique positive solution of b( R) w(r) =, where w( ) denotes the Laplae transform of f Wi (x) (see e.g. Asmussen 4). An illustrative example for the differene of the orresponding survival probabilities is given in Setion 4. 6

7 3 Related Models In the following, we list a number of related dependeny models for whih exat solutions for the survival probability an be derived in an analogous way: 3. Model 2 Let for every t > the risk proess be in one of the two states i =, 2, orresponding to the rate λ i of the exponential distribution for the time until the next laim ours. At the time of a laim ourrene the state of the system may hange depending on the orresponding laim size. If a laim B j is smaller than a threshold T j, then the state of the risk proess hanges, otherwise it does not. The quantities T j are again assumed to be i.i.d. random variables with distribution funtion T ( ). The net profit ondition in this model is 2β < ( λ + λ 2 ). (3) Then the analysis of φ i (x) (whih is the survival probability with initial apital x, given that the system starts out in state i) is analogous to the previous setion and we obtain and dφ x dx (x) λ φ (x) + λ dφ x 2 dx (x) λ 2φ 2 (x) + λ 2 P(T y)φ (x y)db(y)+ + λ x P(T y)φ 2 (x y)db(y)+ + λ 2 x P(T > y)φ 2 (x y)db(y) = (4) P(T > y)φ (x y)db(y) =, (5) from whih it follows that for Re s φ (+) s λ 2 + λ 2 χ (s) λ χ 2 (s)φ 2 (+) φ (s) = s λ + λ χ (s) s λ 2 + λ 2 χ (s) λ λ 2 χ 2 2(s) and (6) φ 2 (+) s λ + λ χ (s) λ 2 χ 2 (s)φ (+) φ 2 (s) =, (7) s λ + λ χ (s) s λ 2 + λ 2 χ (s) λ λ 2 χ 2 2(s) 7

8 where φ i (s) is again the Laplae transform of φ i (x). Note that the denominators on the right-hand side of (6) and (7) again oinide. Let us now determine φ (+) and φ 2 (+). As for Model, one equation for these two unknowns follows from lim s s φ i (s) =, yielding λ 2 ( φ (+)) + λ ( φ 2 (+)) = 2 λ λ 2 β. (8) A seond equation is obtained by notiing that there is a real number τ (, λ +λ 2 ) that makes the denominator of (6), and similarly (7), zero. Indeed, write the denominator of (6) and (7) as s(k (s) + k 2 (s)), in whih k (s) := s λ λ 2, k 2 (s) := (λ + λ 2 )χ (s) + λ λ 2 s ( χ (s)) 2 χ 2 (s) 2. Now observe that k () + k 2 () < if the net profit ondition (3) holds, whereas k ( λ +λ 2 ) + k 2 ( λ +λ 2 ) >. Sine φ i (s) is an analyti funtion for Re s, τ must also be a zero of the numerators of (6) and (7). In both ases this yields the same relation between φ (+) and φ 2 (+), namely φ 2 (+) = τ λ 2 + λ 2 χ (τ) φ (+) = λ χ 2 (τ) λ 2 χ 2 (τ) τ λ + λ χ (τ) φ (+). (9) We have not proved that τ is the only zero of the denominator of (6) for Re s > (appliation of Rouhé s theorem seems muh more involved here than in the ase of Model ). However, that is not needed: If (3) holds, then there should be unique solutions φ (x) and φ 2 (x) of the integro-differential equations (4) and (5). φ (s) and φ 2 (s) as given in (6) and (7) with φ (+) and φ 2 (+) given by (8) and (9) are the Laplae transforms of funtions φ (x) and φ 2 (x) that satisfy those integrodifferential equations, so we need not look further. See Cohen and Down 7 for more general ideas about handling queueing systems without taking reourse to Rouhé s theorem. Remark: For the speial ase λ = λ 2 := λ we again obtain from (8) the survival probability (9) with zero initial apital in the independent ase. If, alternatively, the state of the risk proess hanges at the time of a laim ourrene, given that B j is larger than a threshold T j and remains in its state otherwise, we get instead of (6) and (7): and φ (s) = φ (+) s λ + λ χ 2 (s) s λ 2 + λ 2 χ 2 (s) s λ 2 + λ 2 χ 2 (s) λ χ (s)φ 2 (+), (2) λ λ 2 χ 2 (s) φ 2 (+) s λ + λ χ 2 (s) λ 2 χ (s)φ (+) φ 2 (s) =, (2) s λ + λ χ 2 (s) s λ 2 + λ 2 χ 2 (s) λ λ 2 χ 2 (s) 8

9 and φ (+) and φ 2 (+) follow from (8) and φ 2 (+) = ζ λ 2 + λ 2 χ 2 (ζ) φ (+) = λ χ (ζ) λ 2 χ (ζ) ζ λ + λ χ 2 (ζ) φ (+), (22) where, similar to τ above, ζ is the real zero of the denominator of (2) in (, λ +λ 2 ). 3.2 Another Variant of Model Let us now look at the following variant of Model with appliations in reinsurane: As in Model, we take the laim intervals W i+ Exp(λ ) if B i > T i, and W i+ Exp(λ 2 ) if B i T i for all i, where T i are again i.i.d. threshold variables. However, now the atual laim payment is min(b i, T i ). Thus the threshold T i an be interpreted as the retention level of an XL-type reinsurane on the laim size (note that a deterministi threshold is a speial ase of this model). For the analysis of this model, we have to introdue the Laplae-Stieltjes transform ψ(s) := Ee st (T <B) = x= e sx ( B(x))dT (x). Note that χ 2 (s) + ψ(s) = Ee s min(b,t ) and thus Emin(B, T ) = χ 2() ψ (). A similar derivation along the lines of Setion 2. leads to φ (+) s λ 2 + λ 2 χ 2 (s) λ χ 2 (s)φ 2 (+) φ (s) = (23) s λ + λ ψ(s) s λ 2 + λ 2 χ 2 (s) λ λ 2 ψ(s)χ 2 (s) and φ 2 (s) = φ 2 (+) s λ + λ ψ(s) λ 2 ψ(s)φ (+), (24) s λ + λ ψ(s) s λ 2 + λ 2 χ 2 (s) λ λ 2 ψ(s)χ 2 (s) where φ i (+) (i=,2) are the solutions of the two equations λ 2 P(B > T )( φ (+)) + λ P(B T )( φ 2 (+)) = λ λ 2 Emin(B, T ) (25) and φ 2 (+) = γ λ 2 + λ 2 χ 2 (γ) λ 2 ψ(γ) φ (+) = λ χ 2 (γ) γ λ + λ ψ(γ) φ (+), where here γ is the unique positive zero of the denominator of (23). Note that the existene and uniqueness of γ an, as in Model, be easily shown by Rouhé type arguments. Remark. In Boxma and Perry 6 a queueing model with the above dependene struture between servie and subsequent interarrival times has been investigated. However, sample path duality between the orresponding workload proess and our risk proess does not hold for this partiular dependene struture, as an also be seen from the differene between (23) and (24) and the formulae (3.8) and (3.9) of 6. 9

10 4 Numerial Illustrations Example. Let T Exp(2), B Exp(), = 2, λ = 3, λ 2 =. The net profit ondition () is obviously fulfilled. Then the inversion of the Laplae transforms (4) and (5) yields φ (x) =.7 e 3.6 x.938 e.65 x, φ 2 (x) =.3 e 3.6 x.867 e.65 x, (26) where here and in the sequel all numerial values are rounded to their last digit (f. Figure a). Let us now ompare (26) to φ(x) in a model with the assumption of independene as desribed in Setion 2.2. The inter-arrival density in the independent model is then given by f Wi (x) = 2 e 3x + 3 e x. The Lundberg exponent in this renewal risk model is the positive solution of R ( 3 + 3R + 2 ) 3 + R =, i.e. R =.77. In this speifi example, there is even an analytial solution for the survival probability in the orresponding renewal model available, sine the laim size distribution is exponential. This solution an be derived utilizing a sample path duality to a related queuing proess (see e.g. Asmussen 4) and we obtain φ ind (x) =.923e.77x. This should be ompared with the stationary version of the dependent setting φ dep (x) = 2 3 φ (x) + 3 φ 2(x) =.6e 3.6x.95e.65x. Note that onerning the asymptoti behavior, the Lundberg exponent of φ dep (x) is smaller than the one of φ ind (x), i.e. ignoring the dependene struture underestimates the inherent risk, espeially for larger values of initial apital x (f. Figure b). Example 2. Let T Exp(), B Exp(), = 2, λ =, λ 2 = 2. Then the inversion of the Laplae transforms (4) and (5) yields φ (x) =.632 e.355 x +.7 e.889 x, φ 2 (x) =.798 e.355 x +.28 e.889 x. (27) If we again ompare (27) to φ(x) in a model with the assumption of independene, then the inter-arrival density is now given by f Wi (x) = e 2x + 2 e x. The Lundberg exponent in this renewal risk model is the positive solution of R ( 2( + R) + ) 2 + R =,

11 x x Figure : Survival probabilities in Example. Left: φ (x) (solid line) and φ 2 (x) (dashed line). Right: φ dep (x) (solid line) and φ ind (x) (dotted line) x x Figure 2: Survival probabilities in Example 2. Left: φ (x) (solid line) and φ 2 (x) (dashed line). Right: φ dep (x) (solid line) and φ ind (x) (dotted line) i.e. R =.39. Again, we even have an analytial solution for φ ind (x) in the orresponding renewal model available: φ ind (x) =.69e.39x. The stationary version of the dependent setting yields φ dep (x) = 2 φ (x) + 2 φ 2(x) =.75e.355x +.23e.889x. Note that in this ase, the Lundberg exponent of φ ind (x) is smaller than the one of φ dep (x), i.e. the independent setting is more dangerous. This is, heuristially, due to the fat that for this hoie of parameters a larger laim is likely to be followed by a longer inter-ourrene time (see also Figure 2b). Example 3. Let us again onsider the setting of Example 2, but now with a deterministi threshold T i = a.s. for all i (so the value of T i equals the expeted value of the threshold variable of Example 2). Aording to (2) we have χ (s) = +s e s and χ 2 (s) = ( +s e s ) and we obtain φ (+) =.337 and φ 2 (+) =.9. The resulting Laplae transforms (4) and (5) an easily be inverted numerially by a Bromwih ontour integration. Table illustrates the fat that the distribution of the threshold has a signifiant effet on the survival probabilities.

12 T = T Exp() x φ (x) φ 2 (x) φ (x) φ 2 (x) Referenes Table : Comparison of φ i (x) for Examples 2 and 3 I. Adan and V. Kulkarni. Single-server queue with Markov dependent interarrival and servie times. Queueing Systems, to appear, H. Albreher and J. Kantor. Simulation of ruin probabilities for risk proesses of Markovian type. Monte Carlo Methods & Appl., 8(2): 27, S. Asmussen. Matrix-analyti models and their analysis. Sand. J. Statist., 27(2):93 226, 2. 4 S. Asmussen. Ruin probabilities. World Sientifi, Singapore, 2. 5 S. Asmussen, H. Shmidli, and V. Shmidt. Tail probabilities for non-standard risk and queueing proesses with subexponential jumps. Adv. in Appl. Probab., 3(2): , O. Boxma and D. Perry. A queueing model with dependene between servie and interarrival times. European J. Oper. Res., 28(3):6 624, 2. 7 J. Cohen and D. Down. On the role of Rouhé s theorem in queueing analysis. Queueing Systems, 23:28 29, M. Combé and O. Boxma. BMAP modelling of a orrelated queue. In J. Walrand, K. Baghi, and G. Zobrist, editors, Network Performane Modeling and Simulation, pages Gordon and Breah Siene Publ., Newark, T. Mikosh and G. Samorodnitsky. Ruin probability with laims modeled by a stationary ergodi stable proess. Ann. Probab., 28(4):84 85, 2. T. Mikosh and G. Samorodnitsky. The supremum of a negative drift random walk with dependent heavy-tailed steps. Ann. Appl. Probab., (3):25 64, 2. 2

13 A. Müller and G. Pflug. Asymptoti ruin probabilities for risk proesses with dependent inrements. Insurane: Mathematis and Eonomis, 28(3):38 392, 2. 2 H. Nyrhinen. Rough desriptions of ruin for a general lass of surplus proesses. Adv. Appl. Prob., 3:8 26, H. Nyrhinen. Large deviations for the time of ruin. J. Appl. Probab., 36(3): , M. Spiegel. Theory and problems of Laplae transforms. Shaum, New York,

The Hanging Chain. John McCuan. January 19, 2006

The Hanging Chain. John McCuan. January 19, 2006 The Hanging Chain John MCuan January 19, 2006 1 Introdution We onsider a hain of length L attahed to two points (a, u a and (b, u b in the plane. It is assumed that the hain hangs in the plane under a

More information

Computer Science 786S - Statistical Methods in Natural Language Processing and Data Analysis Page 1

Computer Science 786S - Statistical Methods in Natural Language Processing and Data Analysis Page 1 Computer Siene 786S - Statistial Methods in Natural Language Proessing and Data Analysis Page 1 Hypothesis Testing A statistial hypothesis is a statement about the nature of the distribution of a random

More information

The Decompositions of the Discounted Penalty Functions and Dividends-Penalty Identity in a Markov-modulated Risk Model

The Decompositions of the Discounted Penalty Functions and Dividends-Penalty Identity in a Markov-modulated Risk Model The Deompositions of the Disounted Penalty Funtions and Dividends-Penalty Identity in a Markov-modulated Risk Model Shuanming Li a and Yi Lu b a Centre for Atuarial Studies, Department of Eonomis The University

More information

The Effectiveness of the Linear Hull Effect

The Effectiveness of the Linear Hull Effect The Effetiveness of the Linear Hull Effet S. Murphy Tehnial Report RHUL MA 009 9 6 Otober 009 Department of Mathematis Royal Holloway, University of London Egham, Surrey TW0 0EX, England http://www.rhul.a.uk/mathematis/tehreports

More information

A Queueing Model for Call Blending in Call Centers

A Queueing Model for Call Blending in Call Centers A Queueing Model for Call Blending in Call Centers Sandjai Bhulai and Ger Koole Vrije Universiteit Amsterdam Faulty of Sienes De Boelelaan 1081a 1081 HV Amsterdam The Netherlands E-mail: {sbhulai, koole}@s.vu.nl

More information

The law of the iterated logarithm for c k f(n k x)

The law of the iterated logarithm for c k f(n k x) The law of the iterated logarithm for k fn k x) Christoph Aistleitner Abstrat By a lassial heuristis, systems of the form osπn k x) k 1 and fn k x)) k 1, where n k ) k 1 is a rapidly growing sequene of

More information

Control Theory association of mathematics and engineering

Control Theory association of mathematics and engineering Control Theory assoiation of mathematis and engineering Wojieh Mitkowski Krzysztof Oprzedkiewiz Department of Automatis AGH Univ. of Siene & Tehnology, Craow, Poland, Abstrat In this paper a methodology

More information

arxiv: v2 [math.pr] 9 Dec 2016

arxiv: v2 [math.pr] 9 Dec 2016 Omnithermal Perfet Simulation for Multi-server Queues Stephen B. Connor 3th Deember 206 arxiv:60.0602v2 [math.pr] 9 De 206 Abstrat A number of perfet simulation algorithms for multi-server First Come First

More information

Some advances on the Erlang(n) dual risk model

Some advances on the Erlang(n) dual risk model Some advanes on the Erlang(n dual risk model Eugenio V. Rodríguez-Martínez, Rui M.R. Cardoso & Alfredo D. Egídio dos Reis CEMAPRE and ISEG, Tehnial University of Lisbon, Portugal & CMA and FCT, New University

More information

ON A PROCESS DERIVED FROM A FILTERED POISSON PROCESS

ON A PROCESS DERIVED FROM A FILTERED POISSON PROCESS ON A PROCESS DERIVED FROM A FILTERED POISSON PROCESS MARIO LEFEBVRE and JEAN-LUC GUILBAULT A ontinuous-time and ontinuous-state stohasti proess, denoted by {Xt), t }, is defined from a proess known as

More information

Hankel Optimal Model Order Reduction 1

Hankel Optimal Model Order Reduction 1 Massahusetts Institute of Tehnology Department of Eletrial Engineering and Computer Siene 6.245: MULTIVARIABLE CONTROL SYSTEMS by A. Megretski Hankel Optimal Model Order Redution 1 This leture overs both

More information

Quasi-Monte Carlo Algorithms for unbounded, weighted integration problems

Quasi-Monte Carlo Algorithms for unbounded, weighted integration problems Quasi-Monte Carlo Algorithms for unbounded, weighted integration problems Jürgen Hartinger Reinhold F. Kainhofer Robert F. Tihy Department of Mathematis, Graz University of Tehnology, Steyrergasse 30,

More information

Complexity of Regularization RBF Networks

Complexity of Regularization RBF Networks Complexity of Regularization RBF Networks Mark A Kon Department of Mathematis and Statistis Boston University Boston, MA 02215 mkon@buedu Leszek Plaskota Institute of Applied Mathematis University of Warsaw

More information

On maximal inequalities via comparison principle

On maximal inequalities via comparison principle Makasu Journal of Inequalities and Appliations (2015 2015:348 DOI 10.1186/s13660-015-0873-3 R E S E A R C H Open Aess On maximal inequalities via omparison priniple Cloud Makasu * * Correspondene: makasu@uw.a.za

More information

SQUARE ROOTS AND AND DIRECTIONS

SQUARE ROOTS AND AND DIRECTIONS SQUARE ROOS AND AND DIRECIONS We onstrut a lattie-like point set in the Eulidean plane that eluidates the relationship between the loal statistis of the frational parts of n and diretions in a shifted

More information

Ruin by Dynamic Contagion Claims

Ruin by Dynamic Contagion Claims Ruin by Dynami Contagion Claims Angelos Dassios, Hongbiao Zhao Department of Statistis, London Shool of Eonomis, Houghton Street, London WC2A 2AE, United Kingdom Abstrat In this paper, we onsider a risk

More information

A Functional Representation of Fuzzy Preferences

A Functional Representation of Fuzzy Preferences Theoretial Eonomis Letters, 017, 7, 13- http://wwwsirporg/journal/tel ISSN Online: 16-086 ISSN Print: 16-078 A Funtional Representation of Fuzzy Preferenes Susheng Wang Department of Eonomis, Hong Kong

More information

Modal Horn Logics Have Interpolation

Modal Horn Logics Have Interpolation Modal Horn Logis Have Interpolation Marus Kraht Department of Linguistis, UCLA PO Box 951543 405 Hilgard Avenue Los Angeles, CA 90095-1543 USA kraht@humnet.ula.de Abstrat We shall show that the polymodal

More information

Wavetech, LLC. Ultrafast Pulses and GVD. John O Hara Created: Dec. 6, 2013

Wavetech, LLC. Ultrafast Pulses and GVD. John O Hara Created: Dec. 6, 2013 Ultrafast Pulses and GVD John O Hara Created: De. 6, 3 Introdution This doument overs the basi onepts of group veloity dispersion (GVD) and ultrafast pulse propagation in an optial fiber. Neessarily, it

More information

Millennium Relativity Acceleration Composition. The Relativistic Relationship between Acceleration and Uniform Motion

Millennium Relativity Acceleration Composition. The Relativistic Relationship between Acceleration and Uniform Motion Millennium Relativity Aeleration Composition he Relativisti Relationship between Aeleration and niform Motion Copyright 003 Joseph A. Rybzyk Abstrat he relativisti priniples developed throughout the six

More information

Discrete Random Walks on One-Sided Periodic Graphs

Discrete Random Walks on One-Sided Periodic Graphs Disrete Mathematis and Theoretial Computer Siene (sum), y the authors, rev Disrete Random Walks on One-Sided Periodi Graphs Mihael Drmota Department of Geometry, TU Wien, Wiedner Hauptstrasse 8-0, A-040

More information

ON THE MOVING BOUNDARY HITTING PROBABILITY FOR THE BROWNIAN MOTION. Dobromir P. Kralchev

ON THE MOVING BOUNDARY HITTING PROBABILITY FOR THE BROWNIAN MOTION. Dobromir P. Kralchev Pliska Stud. Math. Bulgar. 8 2007, 83 94 STUDIA MATHEMATICA BULGARICA ON THE MOVING BOUNDARY HITTING PROBABILITY FOR THE BROWNIAN MOTION Dobromir P. Kralhev Consider the probability that the Brownian motion

More information

Predicting the confirmation time of Bitcoin transactions

Predicting the confirmation time of Bitcoin transactions Prediting the onfirmation time of Bitoin transations D.T. Koops Korteweg-de Vries Institute, University of Amsterdam arxiv:189.1596v1 [s.dc] 21 Sep 218 September 28, 218 Abstrat We study the probabilisti

More information

IMPEDANCE EFFECTS OF LEFT TURNERS FROM THE MAJOR STREET AT A TWSC INTERSECTION

IMPEDANCE EFFECTS OF LEFT TURNERS FROM THE MAJOR STREET AT A TWSC INTERSECTION 09-1289 Citation: Brilon, W. (2009): Impedane Effets of Left Turners from the Major Street at A TWSC Intersetion. Transportation Researh Reord Nr. 2130, pp. 2-8 IMPEDANCE EFFECTS OF LEFT TURNERS FROM THE

More information

EXACT TRAVELLING WAVE SOLUTIONS FOR THE GENERALIZED KURAMOTO-SIVASHINSKY EQUATION

EXACT TRAVELLING WAVE SOLUTIONS FOR THE GENERALIZED KURAMOTO-SIVASHINSKY EQUATION Journal of Mathematial Sienes: Advanes and Appliations Volume 3, 05, Pages -3 EXACT TRAVELLING WAVE SOLUTIONS FOR THE GENERALIZED KURAMOTO-SIVASHINSKY EQUATION JIAN YANG, XIAOJUAN LU and SHENGQIANG TANG

More information

Optimization of Statistical Decisions for Age Replacement Problems via a New Pivotal Quantity Averaging Approach

Optimization of Statistical Decisions for Age Replacement Problems via a New Pivotal Quantity Averaging Approach Amerian Journal of heoretial and Applied tatistis 6; 5(-): -8 Published online January 7, 6 (http://www.sienepublishinggroup.om/j/ajtas) doi:.648/j.ajtas.s.65.4 IN: 36-8999 (Print); IN: 36-96 (Online)

More information

A NONLILEAR CONTROLLER FOR SHIP AUTOPILOTS

A NONLILEAR CONTROLLER FOR SHIP AUTOPILOTS Vietnam Journal of Mehanis, VAST, Vol. 4, No. (), pp. A NONLILEAR CONTROLLER FOR SHIP AUTOPILOTS Le Thanh Tung Hanoi University of Siene and Tehnology, Vietnam Abstrat. Conventional ship autopilots are

More information

Average Rate Speed Scaling

Average Rate Speed Scaling Average Rate Speed Saling Nikhil Bansal David P. Bunde Ho-Leung Chan Kirk Pruhs May 2, 2008 Abstrat Speed saling is a power management tehnique that involves dynamially hanging the speed of a proessor.

More information

Methods of evaluating tests

Methods of evaluating tests Methods of evaluating tests Let X,, 1 Xn be i.i.d. Bernoulli( p ). Then 5 j= 1 j ( 5, ) T = X Binomial p. We test 1 H : p vs. 1 1 H : p>. We saw that a LRT is 1 if t k* φ ( x ) =. otherwise (t is the observed

More information

A two storage inventory model with variable demand and time dependent deterioration rate and with partial backlogging

A two storage inventory model with variable demand and time dependent deterioration rate and with partial backlogging Malaya Journal of Matematik, Vol. S, No., 35-40, 08 https://doi.org/0.37/mjm0s0/07 A two storage inventory model with variable demand and time dependent deterioration rate and with partial baklogging Rihi

More information

HILLE-KNESER TYPE CRITERIA FOR SECOND-ORDER DYNAMIC EQUATIONS ON TIME SCALES

HILLE-KNESER TYPE CRITERIA FOR SECOND-ORDER DYNAMIC EQUATIONS ON TIME SCALES HILLE-KNESER TYPE CRITERIA FOR SECOND-ORDER DYNAMIC EQUATIONS ON TIME SCALES L ERBE, A PETERSON AND S H SAKER Abstrat In this paper, we onsider the pair of seond-order dynami equations rt)x ) ) + pt)x

More information

Discrete Bessel functions and partial difference equations

Discrete Bessel functions and partial difference equations Disrete Bessel funtions and partial differene equations Antonín Slavík Charles University, Faulty of Mathematis and Physis, Sokolovská 83, 186 75 Praha 8, Czeh Republi E-mail: slavik@karlin.mff.uni.z Abstrat

More information

Asymptotic non-degeneracy of the solution to the Liouville Gel fand problem in two dimensions

Asymptotic non-degeneracy of the solution to the Liouville Gel fand problem in two dimensions Comment. Math. Helv. 2 2007), 353 369 Commentarii Mathematii Helvetii Swiss Mathematial Soiety Asymptoti non-degeneray of the solution to the Liouville Gel fand problem in two dimensions Tomohio Sato and

More information

A Characterization of Wavelet Convergence in Sobolev Spaces

A Characterization of Wavelet Convergence in Sobolev Spaces A Charaterization of Wavelet Convergene in Sobolev Spaes Mark A. Kon 1 oston University Louise Arakelian Raphael Howard University Dediated to Prof. Robert Carroll on the oasion of his 70th birthday. Abstrat

More information

LOGISTIC REGRESSION IN DEPRESSION CLASSIFICATION

LOGISTIC REGRESSION IN DEPRESSION CLASSIFICATION LOGISIC REGRESSIO I DEPRESSIO CLASSIFICAIO J. Kual,. V. ran, M. Bareš KSE, FJFI, CVU v Praze PCP, CS, 3LF UK v Praze Abstrat Well nown logisti regression and the other binary response models an be used

More information

arxiv:math/ v4 [math.ca] 29 Jul 2006

arxiv:math/ v4 [math.ca] 29 Jul 2006 arxiv:math/0109v4 [math.ca] 9 Jul 006 Contiguous relations of hypergeometri series Raimundas Vidūnas University of Amsterdam Abstrat The 15 Gauss ontiguous relations for F 1 hypergeometri series imply

More information

Differential Equations 8/24/2010

Differential Equations 8/24/2010 Differential Equations A Differential i Equation (DE) is an equation ontaining one or more derivatives of an unknown dependant d variable with respet to (wrt) one or more independent variables. Solution

More information

Research Article Ruin Probabilities in the Mixed Claim Frequency Risk Models

Research Article Ruin Probabilities in the Mixed Claim Frequency Risk Models Mathematial Problems in Engineering, Artile ID 31437, 7 pages http://dx.doi.org/1.1155/214/31437 Researh Artile Ruin Probabilities in the Mixed Claim Frequeny Risk Models Zhao Xiaoqin 1 and Chuangxia Huang

More information

The Distributors of Change Points in Long 11ennoryProcesses

The Distributors of Change Points in Long 11ennoryProcesses Summer Researh Projet 25-26 The Distributors of Change Points in Long 11ennoryProesses Guan Yu Zheng Department of Mathematis and Statistis University of Canterbury The distributions of hange points in

More information

Subject: Introduction to Component Matching and Off-Design Operation % % ( (1) R T % (

Subject: Introduction to Component Matching and Off-Design Operation % % ( (1) R T % ( 16.50 Leture 0 Subjet: Introdution to Component Mathing and Off-Design Operation At this point it is well to reflet on whih of the many parameters we have introdued (like M, τ, τ t, ϑ t, f, et.) are free

More information

max min z i i=1 x j k s.t. j=1 x j j:i T j

max min z i i=1 x j k s.t. j=1 x j j:i T j AM 221: Advaned Optimization Spring 2016 Prof. Yaron Singer Leture 22 April 18th 1 Overview In this leture, we will study the pipage rounding tehnique whih is a deterministi rounding proedure that an be

More information

REFINED UPPER BOUNDS FOR THE LINEAR DIOPHANTINE PROBLEM OF FROBENIUS. 1. Introduction

REFINED UPPER BOUNDS FOR THE LINEAR DIOPHANTINE PROBLEM OF FROBENIUS. 1. Introduction Version of 5/2/2003 To appear in Advanes in Applied Mathematis REFINED UPPER BOUNDS FOR THE LINEAR DIOPHANTINE PROBLEM OF FROBENIUS MATTHIAS BECK AND SHELEMYAHU ZACKS Abstrat We study the Frobenius problem:

More information

Cavity flow with surface tension past a flat plate

Cavity flow with surface tension past a flat plate Proeedings of the 7 th International Symposium on Cavitation CAV9 Paper No. ## August 7-, 9, Ann Arbor, Mihigan, USA Cavity flow with surfae tension past a flat plate Yuriy Savhenko Institute of Hydromehanis

More information

arxiv:gr-qc/ v2 6 Feb 2004

arxiv:gr-qc/ v2 6 Feb 2004 Hubble Red Shift and the Anomalous Aeleration of Pioneer 0 and arxiv:gr-q/0402024v2 6 Feb 2004 Kostadin Trenčevski Faulty of Natural Sienes and Mathematis, P.O.Box 62, 000 Skopje, Maedonia Abstrat It this

More information

Non-Markovian study of the relativistic magnetic-dipole spontaneous emission process of hydrogen-like atoms

Non-Markovian study of the relativistic magnetic-dipole spontaneous emission process of hydrogen-like atoms NSTTUTE OF PHYSCS PUBLSHNG JOURNAL OF PHYSCS B: ATOMC, MOLECULAR AND OPTCAL PHYSCS J. Phys. B: At. Mol. Opt. Phys. 39 ) 7 85 doi:.88/953-75/39/8/ Non-Markovian study of the relativisti magneti-dipole spontaneous

More information

Singular Event Detection

Singular Event Detection Singular Event Detetion Rafael S. Garía Eletrial Engineering University of Puerto Rio at Mayagüez Rafael.Garia@ee.uprm.edu Faulty Mentor: S. Shankar Sastry Researh Supervisor: Jonathan Sprinkle Graduate

More information

FINITE WORD LENGTH EFFECTS IN DSP

FINITE WORD LENGTH EFFECTS IN DSP FINITE WORD LENGTH EFFECTS IN DSP PREPARED BY GUIDED BY Snehal Gor Dr. Srianth T. ABSTRACT We now that omputers store numbers not with infinite preision but rather in some approximation that an be paed

More information

Integration of the Finite Toda Lattice with Complex-Valued Initial Data

Integration of the Finite Toda Lattice with Complex-Valued Initial Data Integration of the Finite Toda Lattie with Complex-Valued Initial Data Aydin Huseynov* and Gusein Sh Guseinov** *Institute of Mathematis and Mehanis, Azerbaijan National Aademy of Sienes, AZ4 Baku, Azerbaijan

More information

22.54 Neutron Interactions and Applications (Spring 2004) Chapter 6 (2/24/04) Energy Transfer Kernel F(E E')

22.54 Neutron Interactions and Applications (Spring 2004) Chapter 6 (2/24/04) Energy Transfer Kernel F(E E') 22.54 Neutron Interations and Appliations (Spring 2004) Chapter 6 (2/24/04) Energy Transfer Kernel F(E E') Referenes -- J. R. Lamarsh, Introdution to Nulear Reator Theory (Addison-Wesley, Reading, 1966),

More information

When p = 1, the solution is indeterminate, but we get the correct answer in the limit.

When p = 1, the solution is indeterminate, but we get the correct answer in the limit. The Mathematia Journal Gambler s Ruin and First Passage Time Jan Vrbik We investigate the lassial problem of a gambler repeatedly betting $1 on the flip of a potentially biased oin until he either loses

More information

3 Tidal systems modelling: ASMITA model

3 Tidal systems modelling: ASMITA model 3 Tidal systems modelling: ASMITA model 3.1 Introdution For many pratial appliations, simulation and predition of oastal behaviour (morphologial development of shorefae, beahes and dunes) at a ertain level

More information

Error Bounds for Context Reduction and Feature Omission

Error Bounds for Context Reduction and Feature Omission Error Bounds for Context Redution and Feature Omission Eugen Bek, Ralf Shlüter, Hermann Ney,2 Human Language Tehnology and Pattern Reognition, Computer Siene Department RWTH Aahen University, Ahornstr.

More information

Ordered fields and the ultrafilter theorem

Ordered fields and the ultrafilter theorem F U N D A M E N T A MATHEMATICAE 59 (999) Ordered fields and the ultrafilter theorem by R. B e r r (Dortmund), F. D e l o n (Paris) and J. S h m i d (Dortmund) Abstrat. We prove that on the basis of ZF

More information

Institut de Science Financière et d Assurances

Institut de Science Financière et d Assurances Institut de Siene Finanière et d Assuranes Les Cahiers de Reherhe de l ISFA ROBUSTNESS ANALYSIS AND CONVERGENCE OF EMPIRICAL FINITE-TIME RUIN PROBABILITIES AND ESTIMATION RISK SOLVENCY MARGIN Stéphane

More information

Aharonov-Bohm effect. Dan Solomon.

Aharonov-Bohm effect. Dan Solomon. Aharonov-Bohm effet. Dan Solomon. In the figure the magneti field is onfined to a solenoid of radius r 0 and is direted in the z- diretion, out of the paper. The solenoid is surrounded by a barrier that

More information

Estimating the probability law of the codelength as a function of the approximation error in image compression

Estimating the probability law of the codelength as a function of the approximation error in image compression Estimating the probability law of the odelength as a funtion of the approximation error in image ompression François Malgouyres Marh 7, 2007 Abstrat After some reolletions on ompression of images using

More information

Time Domain Method of Moments

Time Domain Method of Moments Time Domain Method of Moments Massahusetts Institute of Tehnology 6.635 leture notes 1 Introdution The Method of Moments (MoM) introdued in the previous leture is widely used for solving integral equations

More information

arxiv:gr-qc/ v7 14 Dec 2003

arxiv:gr-qc/ v7 14 Dec 2003 Propagation of light in non-inertial referene frames Vesselin Petkov Siene College, Conordia University 1455 De Maisonneuve Boulevard West Montreal, Quebe, Canada H3G 1M8 vpetkov@alor.onordia.a arxiv:gr-q/9909081v7

More information

Remark 4.1 Unlike Lyapunov theorems, LaSalle s theorem does not require the function V ( x ) to be positive definite.

Remark 4.1 Unlike Lyapunov theorems, LaSalle s theorem does not require the function V ( x ) to be positive definite. Leture Remark 4.1 Unlike Lyapunov theorems, LaSalle s theorem does not require the funtion V ( x ) to be positive definite. ost often, our interest will be to show that x( t) as t. For that we will need

More information

the following action R of T on T n+1 : for each θ T, R θ : T n+1 T n+1 is defined by stated, we assume that all the curves in this paper are defined

the following action R of T on T n+1 : for each θ T, R θ : T n+1 T n+1 is defined by stated, we assume that all the curves in this paper are defined How should a snake turn on ie: A ase study of the asymptoti isoholonomi problem Jianghai Hu, Slobodan N. Simić, and Shankar Sastry Department of Eletrial Engineering and Computer Sienes University of California

More information

Some recent developments in probability distributions

Some recent developments in probability distributions Proeedings 59th ISI World Statistis Congress, 25-30 August 2013, Hong Kong (Session STS084) p.2873 Some reent developments in probability distributions Felix Famoye *1, Carl Lee 1, and Ayman Alzaatreh

More information

Determining both sound speed and internal source in thermo- and photo-acoustic tomography

Determining both sound speed and internal source in thermo- and photo-acoustic tomography Inverse Problems Inverse Problems (05) 05005 (0pp) doi:0.088/06656//0/05005 Determining both sound speed and internal soure in thermo and photoaousti tomography Hongyu Liu,,5 and Gunther Uhlmann,4 Department

More information

ON THE LEAST PRIMITIVE ROOT EXPRESSIBLE AS A SUM OF TWO SQUARES

ON THE LEAST PRIMITIVE ROOT EXPRESSIBLE AS A SUM OF TWO SQUARES #A55 INTEGERS 3 (203) ON THE LEAST PRIMITIVE ROOT EPRESSIBLE AS A SUM OF TWO SQUARES Christopher Ambrose Mathematishes Institut, Georg-August Universität Göttingen, Göttingen, Deutshland ambrose@uni-math.gwdg.de

More information

Simplification of Network Dynamics in Large Systems

Simplification of Network Dynamics in Large Systems Simplifiation of Network Dynamis in Large Systems Xiaojun Lin and Ness B. Shroff Shool of Eletrial and Computer Engineering Purdue University, West Lafayette, IN 47906, U.S.A. Email: {linx, shroff}@en.purdue.edu

More information

KAMILLA OLIVER AND HELMUT PRODINGER

KAMILLA OLIVER AND HELMUT PRODINGER THE CONTINUED RACTION EXPANSION O GAUSS HYPERGEOMETRIC UNCTION AND A NEW APPLICATION TO THE TANGENT UNCTION KAMILLA OLIVER AND HELMUT PRODINGER Abstrat Starting from a formula for tan(nx in the elebrated

More information

SOA/CAS MAY 2003 COURSE 1 EXAM SOLUTIONS

SOA/CAS MAY 2003 COURSE 1 EXAM SOLUTIONS SOA/CAS MAY 2003 COURSE 1 EXAM SOLUTIONS Prepared by S. Broverman e-mail 2brove@rogers.om website http://members.rogers.om/2brove 1. We identify the following events:. - wathed gymnastis, ) - wathed baseball,

More information

Bäcklund Transformations: Some Old and New Perspectives

Bäcklund Transformations: Some Old and New Perspectives Bäklund Transformations: Some Old and New Perspetives C. J. Papahristou *, A. N. Magoulas ** * Department of Physial Sienes, Helleni Naval Aademy, Piraeus 18539, Greee E-mail: papahristou@snd.edu.gr **

More information

Closed-form Ruin Probabilities in Classical Risk Models with Gamma Claims

Closed-form Ruin Probabilities in Classical Risk Models with Gamma Claims Closed-form Ruin Probabilities in Classial Risk Models with Gamma Claims Corina Constantinesu, Gennady Samorodnitsky, Wei Zhu University of Liverpool, Liverpool, L69 7ZL, UK Cornell University, Ithaa,

More information

Tail-robust Scheduling via Limited Processor Sharing

Tail-robust Scheduling via Limited Processor Sharing Performane Evaluation Performane Evaluation 00 200) 22 Tail-robust Sheduling via Limited Proessor Sharing Jayakrishnan Nair a, Adam Wierman b, Bert Zwart a Department of Eletrial Engineering, California

More information

Maximum Entropy and Exponential Families

Maximum Entropy and Exponential Families Maximum Entropy and Exponential Families April 9, 209 Abstrat The goal of this note is to derive the exponential form of probability distribution from more basi onsiderations, in partiular Entropy. It

More information

LECTURE NOTES FOR , FALL 2004

LECTURE NOTES FOR , FALL 2004 LECTURE NOTES FOR 18.155, FALL 2004 83 12. Cone support and wavefront set In disussing the singular support of a tempered distibution above, notie that singsupp(u) = only implies that u C (R n ), not as

More information

Design and evaluation of a connection management mechanism for an ATM-based connectionless service

Design and evaluation of a connection management mechanism for an ATM-based connectionless service Distributed Systems Engineering Design and evaluation of a onnetion management mehanism for an ATM-based onnetionless servie To ite this artile: Geert Heijenk and Boudewijn R Haverkort 1996 Distrib Syst

More information

QCLAS Sensor for Purity Monitoring in Medical Gas Supply Lines

QCLAS Sensor for Purity Monitoring in Medical Gas Supply Lines DOI.56/sensoren6/P3. QLAS Sensor for Purity Monitoring in Medial Gas Supply Lines Henrik Zimmermann, Mathias Wiese, Alessandro Ragnoni neoplas ontrol GmbH, Walther-Rathenau-Str. 49a, 7489 Greifswald, Germany

More information

Aircraft CAS Design with Input Saturation Using Dynamic Model Inversion

Aircraft CAS Design with Input Saturation Using Dynamic Model Inversion International Journal of Control, Automation, and Systems Vol., No. 3, September 003 35 Airraft CAS Design with Input Saturation sing Dynami Model Inversion Sangsoo Lim and Byoung Soo Kim Abstrat: This

More information

SECOND HANKEL DETERMINANT PROBLEM FOR SOME ANALYTIC FUNCTION CLASSES WITH CONNECTED K-FIBONACCI NUMBERS

SECOND HANKEL DETERMINANT PROBLEM FOR SOME ANALYTIC FUNCTION CLASSES WITH CONNECTED K-FIBONACCI NUMBERS Ata Universitatis Apulensis ISSN: 15-539 http://www.uab.ro/auajournal/ No. 5/01 pp. 161-17 doi: 10.1711/j.aua.01.5.11 SECOND HANKEL DETERMINANT PROBLEM FOR SOME ANALYTIC FUNCTION CLASSES WITH CONNECTED

More information

The Second Postulate of Euclid and the Hyperbolic Geometry

The Second Postulate of Euclid and the Hyperbolic Geometry 1 The Seond Postulate of Eulid and the Hyperboli Geometry Yuriy N. Zayko Department of Applied Informatis, Faulty of Publi Administration, Russian Presidential Aademy of National Eonomy and Publi Administration,

More information

23.1 Tuning controllers, in the large view Quoting from Section 16.7:

23.1 Tuning controllers, in the large view Quoting from Section 16.7: Lesson 23. Tuning a real ontroller - modeling, proess identifiation, fine tuning 23.0 Context We have learned to view proesses as dynami systems, taking are to identify their input, intermediate, and output

More information

Advances in Radio Science

Advances in Radio Science Advanes in adio Siene 2003) 1: 99 104 Copernius GmbH 2003 Advanes in adio Siene A hybrid method ombining the FDTD and a time domain boundary-integral equation marhing-on-in-time algorithm A Beker and V

More information

RIEMANN S FIRST PROOF OF THE ANALYTIC CONTINUATION OF ζ(s) AND L(s, χ)

RIEMANN S FIRST PROOF OF THE ANALYTIC CONTINUATION OF ζ(s) AND L(s, χ) RIEMANN S FIRST PROOF OF THE ANALYTIC CONTINUATION OF ζ(s AND L(s, χ FELIX RUBIN SEMINAR ON MODULAR FORMS, WINTER TERM 6 Abstrat. In this hapter, we will see a proof of the analyti ontinuation of the Riemann

More information

The Capacity Loss of Dense Constellations

The Capacity Loss of Dense Constellations The Capaity Loss of Dense Constellations Tobias Koh University of Cambridge tobi.koh@eng.am.a.uk Alfonso Martinez Universitat Pompeu Fabra alfonso.martinez@ieee.org Albert Guillén i Fàbregas ICREA & Universitat

More information

arxiv: v1 [physics.gen-ph] 5 Jan 2018

arxiv: v1 [physics.gen-ph] 5 Jan 2018 The Real Quaternion Relativity Viktor Ariel arxiv:1801.03393v1 [physis.gen-ph] 5 Jan 2018 In this work, we use real quaternions and the basi onept of the final speed of light in an attempt to enhane the

More information

Coefficients of the Inverse of Strongly Starlike Functions

Coefficients of the Inverse of Strongly Starlike Functions BULLETIN of the MALAYSIAN MATHEMATICAL SCIENCES SOCIETY Bull. Malaysian Math. S. So. (Seond Series) 6 (00) 6 7 Coeffiients of the Inverse of Strongly Starlie Funtions ROSIHAN M. ALI Shool of Mathematial

More information

Supporting Information

Supporting Information Supporting Information Olsman and Goentoro 10.1073/pnas.1601791113 SI Materials Analysis of the Sensitivity and Error Funtions. We now define the sensitivity funtion Sð, «0 Þ, whih summarizes the steepness

More information

Most results in this section are stated without proof.

Most results in this section are stated without proof. Leture 8 Level 4 v2 he Expliit formula. Most results in this setion are stated without proof. Reall that we have shown that ζ (s has only one pole, a simple one at s =. It has trivial zeros at the negative

More information

Nonreversibility of Multiple Unicast Networks

Nonreversibility of Multiple Unicast Networks Nonreversibility of Multiple Uniast Networks Randall Dougherty and Kenneth Zeger September 27, 2005 Abstrat We prove that for any finite direted ayli network, there exists a orresponding multiple uniast

More information

A Ruin Model with Compound Poisson Income and Dependence Between Claim Sizes and Claim Intervals

A Ruin Model with Compound Poisson Income and Dependence Between Claim Sizes and Claim Intervals Acta Mathematicae Applicatae Sinica, English Series Vol. 3, No. 2 (25) 445 452 DOI:.7/s255-5-478- http://www.applmath.com.cn & www.springerlink.com Acta Mathema cae Applicatae Sinica, English Series The

More information

Lyapunov Exponents of Second Order Linear Systems

Lyapunov Exponents of Second Order Linear Systems Reent Researhes in Computational Intelligene and Information Seurity Lyapunov Exponents of Seond Order Linear Systems ADAM CZORNIK and ALEKSANDER NAWRAT Department of Automati Control Silesian Tehnial

More information

The homopolar generator: an analytical example

The homopolar generator: an analytical example The homopolar generator: an analytial example Hendrik van Hees August 7, 214 1 Introdution It is surprising that the homopolar generator, invented in one of Faraday s ingenious experiments in 1831, still

More information

A NETWORK SIMPLEX ALGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM

A NETWORK SIMPLEX ALGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM NETWORK SIMPLEX LGORITHM FOR THE MINIMUM COST-BENEFIT NETWORK FLOW PROBLEM Cen Çalışan, Utah Valley University, 800 W. University Parway, Orem, UT 84058, 801-863-6487, en.alisan@uvu.edu BSTRCT The minimum

More information

Risk Analysis in Water Quality Problems. Souza, Raimundo 1 Chagas, Patrícia 2 1,2 Departamento de Engenharia Hidráulica e Ambiental

Risk Analysis in Water Quality Problems. Souza, Raimundo 1 Chagas, Patrícia 2 1,2 Departamento de Engenharia Hidráulica e Ambiental Risk Analysis in Water Quality Problems. Downloaded from aselibrary.org by Uf - Universidade Federal Do Ceara on 1/29/14. Coyright ASCE. For ersonal use only; all rights reserved. Souza, Raimundo 1 Chagas,

More information

SINCE Zadeh s compositional rule of fuzzy inference

SINCE Zadeh s compositional rule of fuzzy inference IEEE TRANSACTIONS ON FUZZY SYSTEMS, VOL. 14, NO. 6, DECEMBER 2006 709 Error Estimation of Perturbations Under CRI Guosheng Cheng Yuxi Fu Abstrat The analysis of stability robustness of fuzzy reasoning

More information

MOLECULAR ORBITAL THEORY- PART I

MOLECULAR ORBITAL THEORY- PART I 5.6 Physial Chemistry Leture #24-25 MOLECULAR ORBITAL THEORY- PART I At this point, we have nearly ompleted our rash-ourse introdution to quantum mehanis and we re finally ready to deal with moleules.

More information

Measuring & Inducing Neural Activity Using Extracellular Fields I: Inverse systems approach

Measuring & Inducing Neural Activity Using Extracellular Fields I: Inverse systems approach Measuring & Induing Neural Ativity Using Extraellular Fields I: Inverse systems approah Keith Dillon Department of Eletrial and Computer Engineering University of California San Diego 9500 Gilman Dr. La

More information

Likelihood-confidence intervals for quantiles in Extreme Value Distributions

Likelihood-confidence intervals for quantiles in Extreme Value Distributions Likelihood-onfidene intervals for quantiles in Extreme Value Distributions A. Bolívar, E. Díaz-Franés, J. Ortega, and E. Vilhis. Centro de Investigaión en Matemátias; A.P. 42, Guanajuato, Gto. 36; Méxio

More information

Robust Recovery of Signals From a Structured Union of Subspaces

Robust Recovery of Signals From a Structured Union of Subspaces Robust Reovery of Signals From a Strutured Union of Subspaes 1 Yonina C. Eldar, Senior Member, IEEE and Moshe Mishali, Student Member, IEEE arxiv:87.4581v2 [nlin.cg] 3 Mar 29 Abstrat Traditional sampling

More information

Faster Data-access in Large-scale Systems: Network-scale Latency Analysis under General Service-time Distributions

Faster Data-access in Large-scale Systems: Network-scale Latency Analysis under General Service-time Distributions arxiv:807.02253v [s.dc 6 Jul 208 Faster Data-aess in Large-sale Systems: Networ-sale Lateny Analysis under General Servie-time Distributions Avishe Ghosh Department of EECS University of California, Bereley,

More information

University of Groningen

University of Groningen University of Groningen Port Hamiltonian Formulation of Infinite Dimensional Systems II. Boundary Control by Interonnetion Mahelli, Alessandro; van der Shaft, Abraham; Melhiorri, Claudio Published in:

More information

Critical Reflections on the Hafele and Keating Experiment

Critical Reflections on the Hafele and Keating Experiment Critial Refletions on the Hafele and Keating Experiment W.Nawrot In 1971 Hafele and Keating performed their famous experiment whih onfirmed the time dilation predited by SRT by use of marosopi loks. As

More information

Thermodynamic Properties of Supercritical Fluids: Example of n-hexane

Thermodynamic Properties of Supercritical Fluids: Example of n-hexane Thermodynami Properties of Superritial Fluids: Example of n-hexane A. Azzouz 2, A. Rizi, A. Aidi, A. Abbai *, Faulté des Sienes, Département de Chimie, Université Badji Mokhtar, B. P. 2, El-Hadjar, Annaba

More information

A. Shirani*and M. H. Alamatsaz

A. Shirani*and M. H. Alamatsaz IJST (013) A1: 9-34 Iranian Journal of Siene & Tehnology http://www.shirazu.a.ir/en Calulion of exposure buildup fators for point isotropi gamma ray soures in strified spherial shields of wer surrounded

More information