Electronic Journal of Differential Equations, Vol. 2020 (2020), No. 65, pp. 1–27. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu CONVERGENCE OF DELAY EQUATIONS DRIVEN BY A HÖLDER CONTINUOUS FUNCTION OF ORDER 1/3 < β < 1/2 MIREIA BESALÚ, GIULIA BINOTTO, CARLES ROVIRA Abstract. In this article we show that, when the delay approaches zero, the solution of multidimensional delay differential equations driven by a Hölder continuous function of order 1/3 < β < 1/2 converges with the supremum norm to the solution for the equation without delay. Finally we discuss the applications to stochastic differential equations 1. Introduction Hu and Nualart [9] used fractional calculus to establish the existence and unique- ness of a solution for the dynamical system dxt = f(xt) dyt, where y is a Hölder continuous function of order 1/3 < β < 1/2. They give an explicit expression for the integral ∫ t 0 f(xs)dys that depends on the functions x, y and a quadratic multiplicative functional x ⊗ y. As an example of a path-wise approach to classical stochastic calculus, they apply these results to solve stochastic differential equations driven by a multidimensional Brownian motion. Using the same approach, Besalú and Nualart [2] obtained estimates for the supremum norm of the solution and Besalú et al. [1] studied delay equations with non-negativity constraints. The work by Hu and Nualart [9] is an extension of the previous paper of Nualart and Răşcanu [16], where they study the dynamical systems dxt = f(xt)dyt and the control function y is Hölder continuous of order β > 1/2. In this case the Riemann-Stieltjes integral ∫ t 0 f(xs)dys can be expressed as a Lebesgue integral using fractional derivatives following the ideas by Zähle [19]. All these papers have to be seen in the framework of the theory of rough path analysis and the path-wise approach to classical stochastic calculus. This theory has been developed from the initial paper by Lyons [12] and has generated many publications (see, for instance, Lyons and Qian [13], Friz and Victoir [5], Lejay [11] or Gubinelli [8]). We refer to Coutin and Lejay [3], Friz and Victoir [6], Friz [7] and Ledoux et al. [14] for some applications of rough path analysis to stochastic calculus. 2010 Mathematics Subject Classification. 60H05, 60H07. Key words and phrases. Delay equation; stochastic differential equation; convergence; fractional integral. c©2020 Texas State University. Submitted October 30, 2018. Published June 26, 2020. 1 2 M. BESALÚ, G. BINOTTO, C. ROVIRA EJDE-2020/65 Delay differential equations rise from the need to study models that behave more like real processes. They find their applications in dynamical systems with afteref- fects or when the dynamics are subjected to propagation delay. Some examples are epidemiological models with incubation periods that postpone the transmission of disease, or neuronal models where the spatial distribution of neurons can cause a delay in the transmission of the impulse. Sometimes the delay avoids some usual problems, but in general, it adds difficulties and cumbersome notations. The purpose of our paper is to consider the differential equation with delay xrt = η0 + ∫ t 0 b(u, xr) du+ ∫ t 0 σ(xru−r) dyu, t ∈ (0, T ], xrt = ηt, t ∈ [−r, 0], where r denotes a strictly positive time delay, η : [−r, 0]→ Rd is a smooth function, y is a Hölder continuous function of order β ∈ ( 1 3 , 1 2 ) and the hereditary term b(u, x) depends on the path {xs, 0 ≤ s ≤ u}. From Hu and Nualart [9] and Besalú et al. [1] it is easy to check that there exists a unique solution to this equation. Our aim is to prove that it converges almost surely in the supremum norm to the solution of the differential equation without delay xt = η0 + ∫ t 0 b(u, xu) du+ ∫ t 0 σ(xu) dyu, t ∈ [0, T ], when the delay tends to zero. Our approach is based on the techniques of the classical fractional calculus and it is inspired by [9]. Finally, we apply these results to stochastic differential equations driven by Brownian motion. The case when β > 1/2 has been studied by Ferrante and Rovira in [4]. They proved that the solution to the delay equation converges, almost surely and in Lp, to the solution to the equation without delay and then apply the result pathwise to fractional Brownian motion with Hurst parameter H > 1/2. With a different approach based on a slight variation of the Young integration theory, called algebraic integration, León and Tindel [10] prove the existence of a unique solution for a general class of delay differential equations driven by a Hölder continuous function with parameter greater than 1/2. They obtain some estimates of the solution which allow to show that the solution to a delay differential equation driven by a fractional Brownian motion with Hurst parameter H > 1/2 has a C∞- density. When β < 1/2 more difficulties appear. In the literature we find results only up to the value β > 1/3, eventually extended to β > 1/4. In [15], Neuenkirch, Nourdin and Tindel consider delay differential equation driven by a β-Hölder continuous function with β > 1/3. The authors show the existence of a unique solution for these equations under suitable hypothesis. Then, they apply these results to a delay differential equation driven by a fractional Brownian motion with Hurst parameter H > 1/3. These results are extended by Tindel and Torrecilla in [18] to the deterministic case with β > 1/4 and the corresponding stochastic case with Hurst parameter H > 1/4. This article is organized as follows. The following section is devoted to introduce some notation. In section 3 we define the equations and the solutions we work with and we describe our main result. Section 4 contains technical estimates for the study of the integrals. In section 5 we give some estimates for the solutions of our equations. In section 6 we give the proof of the main theorem. In the last EJDE-2020/65 CONVERGENCE OF DELAY EQUATIONS 3 section we give an example of applications of the main theorem, studying stochastic differential equations driven by Brownian motion. 2. Preliminaries First, we recall some definitions and results presented in Hu and Nualart [9]. Fix a time interval [0, T ] and 0 < β ≤ 1. For any function x : [0, T ]→ Rd, the β-Hölder norm of x on the interval [s, t] ⊂ [0, T ] will be denoted by ‖x‖β(s,t) = sup s≤u 1 β − 2. (H2) b : [0, T ] × Rd → Rd is a measurable function such that there exists b0 ∈ Lρ(0, T ;Rd) with ρ ≥ 2 and ∀N ≥ 0 there exists LN > 0 such that: (1) |b(t, xt)− b(t, yt)| ≤ LN |xt − yt|, ∀x, y such that |xt| ≤ N , |yt| ≤ N ∀t ∈ [0, T ], (2) |b(t, xt)| ≤ L0|xt|+ b0(t), ∀t ∈ [0, T ]. (H3) σ and b are bounded functions. Conditions (H1) and (H2) are a particular case of the hypotheses for the proof of existence and uniqueness of solution to the delay equation (3.1), while condition (H3) is necessary to prove that the solution is bounded. We denote by (x, y, x⊗y) ∈Mβ d,m(0, T ) the solution to the stochastic differential equation on Rd without delay xt = η0 + ∫ t 0 b(u, xu) du+ ∫ t 0 σ(xu) dyu, t ∈ [0, T ]. (3.2) Assuming that σ : Rd → Rd × Rm is a continuously differentiable function such that σ′ is λ-Hölder continuous with λ > 1 β − 2, σ and σ′ are bounded and (y, y, y⊗ y) ∈Mβ m,m(0, T ), Hu and Nualart [9] prove the existence of a bounded solution in Mβ d,m(0, T ) for the differential equation (3.2) with b ≡ 0. Moreover, if σ is twice continuously differentiable with bounded derivatives and σ′′ is λ-Hölder continuous, with λ > 1 β − 2, the solution is unique. Here the authors deal with the equation without the hereditary term, but the results can be easily extended to the case where the hereditary term does not vanish. If (y, y, y ⊗ y) ∈ Mβ m,m(0, T ), then we can consider (x⊗ y)s,t = ∫ t s (yt − yu)b(u, xu) du+ ∫ t s σ(xu) du(y ⊗ y)·,t . (3.3) And (x, y, x ⊗ y) ∈ Mβ d,m(0, T ) will be a solution to (3.2) for x and (x ⊗ y) such that (3.2) and (3.3) hold, respectively. EJDE-2020/65 CONVERGENCE OF DELAY EQUATIONS 5 On the other hand, following the ideas contained in [1], it is easy to show that there exists a unique solution to the delay equation (3.1) in Mβ d,m(−r, T ). It can be easily proved assuming that σ and b satisfy the hypotheses (H1) and (H2), respectively, with ρ ≥ 1 1−β and that (η·−r, y, η·−r ⊗ y) ∈ Mβ d,m(0, r) and (y·−r, y, y·−r ⊗ y) ∈ Mβ m,m(r, T ). If we also assume that hypothesis (H3) is satis- fied, we can obtain that the solution is bounded. So, (xr, y, xr ⊗ y) ∈Mβ d,m(−r, T ) is the unique solution to (3.1) for xr such that (3.1) holds and (xr⊗ y)s,t is defined as follows: • for s < t ∈ [−r, 0), (xr ⊗ y)s,t = (η ⊗ y)s,t = ∫ t s (yt − yu) dηu, • for s ∈ [−r, 0) and t ∈ [0, T ], (xr ⊗ y)s,t = (η ⊗ y)s,0 + ∫ t 0 (yt − yu)b(u, xru) du + ∫ t 0 σ(xru−r) du(y ⊗ y)·,t + (η0 − ηs)⊗ (yt − y0), • for 0 ≤ s < t ≤ T , (xr ⊗ y)s,t = ∫ t s (yt − yu)b(u, xru) du+ ∫ t s σ(xru−r) du(y ⊗ y)·,t. Let β ∈ ( 1 3 , 1 2 ) and set β′ = β − ε, where ε > 0 is such that β − 2ε > 0 and λ > 1 β−ε − 2. Set r0 ∈ (0, T ). The main result of this article is the following theorem. Theorem 3.1. Suppose that (y, y, y⊗y) belongs to Mβ m,m(0, T ) and (y·−r, y, y·−r⊗ y) belongs to Mβ m,m(r, T ) for all 0 < r ≤ r0. Assume that σ and b satisfy (H1) and (H2), respectively, and both satisfy (H3). Assume also that (η·−r0 , y, η·−r0 ⊗ y) ∈ Mβ d,m(0, r0), ‖η‖β(−r0,0) < ∞ and supr≤r0 Φβ(0,r)(η·−r, y) < ∞. Suppose that ‖(y−y·−r)⊗y‖2β′(r,T ) → 0 and ‖y·−r⊗(y−y·−r)‖2β′(r,T ) → 0 when r tends to zero. Then, (x, y, x⊗ y) ∈Mβ d,m(0, T ) the solution to the stochastic differential equation without delay (3.2) and (xr, y, xr⊗y) ∈Mβ d,m(−r, T ) the solutions to the stochastic differential equations with delay (3.1) satisfy that lim r→0 ‖x− xr‖∞ = 0 and lim r→0 ‖(x⊗ y)− (xr ⊗ y)‖∞ = 0. 4. Estimates of integrals In this section we will give some estimates for the integrals appearing in our equations. We begin recalling versions of [9, Propositions 3.4 and 3.9 ]. Proposition 4.1. Let (x, y, x⊗y) be in Mβ d,m(0, T ). Assume that f : Rd → Rm is a continuous differentiable function such that f ′ is bounded and λ-Hölder continuous, where λ > 1 β − 2. Then, for any 0 ≤ a < b ≤ T , we have∣∣ ∫ b a f(xu) dyu ∣∣ ≤ K|f(xa)| ‖y‖β(a,b)(b− a)β +K Φβ(a,b)(x, y) × ( ‖f ′‖∞ + ‖f ′‖λ‖x‖λβ(a,b)(b− a)λβ ) (b− a)2β , 6 M. BESALÚ, G. BINOTTO, C. ROVIRA EJDE-2020/65 where Φβ(a,b)(x, y) is defined by (2.1). Proposition 4.2. Suppose that (x, y, x⊗ y) and (y, z, y⊗ z) belong to Mβ d,m(0, T ). Let f : Rd → Rm be a continuously differentiable function such that f ′ is λ-Hölder continuous and bounded, where λ > 1 β − 2. Then, the following estimate holds∣∣ ∫ b a f(xu) du(y ⊗ z)·,b ∣∣ ≤ K|f(xa)|Φβ(a,b)(y, z)(b− a)2β +K ( ‖f ′‖∞ + ‖f ′‖λ‖x‖λβ(a,b)(b− a)λβ ) Φβ(a,b)(x, y, z)(b− a)3β , where Φβ(a,b)(x, y, z) is defined in (2.2). The following propositions give some useful estimates for proving Theorem 3.1. First, we give an estimate for a function b that fulfills conditions (H2). Proposition 4.3. Assume that b satisfies (H2). Let x, x̃ ∈ C(0, T ;Rd) such that ‖x‖∞ ≤ N and ‖x̃‖∞ ≤ N . Then, for 0 ≤ a < b ≤ T ,∣∣ ∫ b a [ b(u, xu)− b(u, x̃u) ] du ∣∣ ≤ LN (b− a)‖x− x̃‖∞(a,b). The proof of the above proposition follows easily using the Lipschitz property of hypothesis (H2). To give some results for a function f under conditions (H1) we need to introduce some notation. Let G1 β(a,b)(f, x, x̃, y) = K [ ‖y‖β ‖f ′‖∞ + ( ‖f ′′‖∞ + ‖f ′′‖λ(‖x‖λβ(a,b) + ‖x̃‖λβ(a,b))(b− a)λβ )( Φβ(a,b)(x, y) + ‖y‖β ‖x̃‖β(a,b) )] , G2 β(a,b)(f, x, x̃, y) = K [ ‖y‖β ‖f ′‖∞ + ‖f ′′‖∞ ( Φβ(a,b)(x, y) + ‖y‖β ‖x̃‖β(a,b) ) (b− a)β ] , G3 β(a,b)(f, x̃) = K [ ‖f ′‖∞ + ‖f ′′‖∞‖x̃‖β(a,b)(b− a)β ] . The first result corresponds to Hu and Nualart [9, Proposition 6.4]. Proposition 4.4. Suppose that (x, y, x⊗ y) and (x̃, y, x̃⊗ y) belong to Mβ d,m(0, T ). Assume that f satisfies (H1). Then, for 0 ≤ a < b ≤ T ,∣∣ ∫ b a [f(xu)− f(x̃u)] dyu ∣∣ ≤ G1 β(a,b)(f, x, x̃, y)(b− a)2β‖x− x̃‖∞(a,b) +G2 β(a,b)(f, x, x̃, y)(b− a)2β‖x− x̃‖β(a,b) +G3 β(a,b)(f, x̃)(b− a)2β‖(x− x̃)⊗ y‖2β(a,b). From this we can deduce the following estimate. Proposition 4.5. Assume (x, y, x⊗y) and (x·−r, y, x·−r⊗y) belong to Mβ d,m(0, T ), and f satisfies (H1). Then, for 0 ≤ a < b ≤ T ,∣∣ ∫ b a [f(xu)− f(xu−r)] dyu ∣∣ ≤ G1 β(a,b)(f, x, x·−r, y)(b− a)2β‖x− x·−r‖∞(a,b) EJDE-2020/65 CONVERGENCE OF DELAY EQUATIONS 7 +G2 β(a,b)(f, x, x·−r, y)(b− a)2β‖x− x·−r‖β(a,b) +G3 β(a,b)(f, x·−r)(b− a)2β‖(x− x·−r)⊗ y‖2β(a,b). The above proposition is a particular case of Proposition 4.4 with x̃ ≡ x·−r. Let us introduce more useful notation: G4 β(a,b)(f, x, x̃, y, z) = K [ ‖f ′‖∞Φβ(a,b)(y, z) + ( ‖f ′′‖∞ + ‖f ′′‖λ(‖x‖λβ(a,b) + ‖x̃‖λβ(a,b))(b− a)λβ ) × ( Φβ(a,b)(x, y, z) + ‖x̃‖β(a,b)Φβ(a,b)(y, z) )] , G5 β(a,b)(f, x, x̃, y, z) = K [( ‖f ′‖∞ + ‖f ′′‖∞‖x̃‖β(a,b)(b− a)β ) Φβ(a,b)(y, z) + ‖f ′′‖∞Φβ(a,b)(x, y, z)(b− a)β ] , G6 β(a,b)(f, x̃, z) = KG3 β(a,b)(f, x̃)‖z‖β(a,b). From the previous results it is possible to prove the following two propositions. Proposition 4.6. Suppose that (x, y, x ⊗ y), (x̃, y, x̃ ⊗ y) and (y, z, y ⊗ z) belong to Mβ d,m(0, T ). Assume that f satisfies (H1). Then, for 0 ≤ a < b ≤ T , ∣∣ ∫ b a [f(xu)− f(x̃u)] du(y ⊗ z)·,b ∣∣ ≤ G4 β(a,b)(f, x, x̃, y, z)(b− a)3β‖x− x̃‖∞(a,b) +G5 β(a,b)(f, x, x̃, y, z)(b− a)3β‖x− x̃‖β(a,b) +G6 β(a,b)(f, x̃, z)(b− a)3β‖(x− x̃)⊗ y‖2β(a,b). Proof. To simplify the proof we will assume d = m = 1. Observe that from in- equalities (2.3) and (2.4) we obtain Φβ(a,b)(x, y ⊗ z) ≤ KΦβ(a,b)(x, y, z)(b− a)β , (4.1)∥∥(x− x̃)⊗ (y ⊗ z)·,b ∥∥ 2β(a,b) ≤ KΦβ(a,b)(y, z)(b− a)β‖x− x̃‖β(a,b) +K‖z‖β(a,b)(b− a)β‖(x− x̃)⊗ y‖2β(a,b). (4.2) The proof of the proposition is obtained by applying Proposition 4.4 and using inequalities (2.3), (2.4), (4.1) and (4.2). � Proposition 4.7. Suppose that (x, y, x ⊗ y), (x·−r, y, x·−r ⊗ y) and (y, z, y ⊗ z) belong to Mβ d,m(0, T ). Assume that f satisfies (H1). Then, for 0 ≤ a < b ≤ T , ∣∣ ∫ b a [f(xu)− f(xu−r)] du(y ⊗ z)·,b ∣∣ ≤ G4 β(a,b)(f, x, x·−r, y, z)(b− a)3β‖x− x·−r‖∞(a,b) +G5 β(a,b)(f, x, x·−r, y, z)(b− a)3β‖x− x·−r‖β(a,b) +G6 β(a,b)(f, x·−r, z)(b− a)3β‖(x− x·−r)⊗ y‖2β(a,b). (4.3) The above proposition is a particular case of Proposition 4.6 with x̃ ≡ x·−r. We conclude this section with a general result on β-Hölder functions. 8 M. BESALÚ, G. BINOTTO, C. ROVIRA EJDE-2020/65 Lemma 4.8. Let y : [0, T ] → Rm be a β-Hölder continuous function and β′ = β − ε > 0 with ε > 0, then ‖y − y·−r‖∞(r,T ) ≤ ‖y‖βrβ , (4.4) ‖y − y·−r‖β′(r,T ) ≤ 2‖y‖βrε. (4.5) Proof. On the one hand, ‖y − y·−r‖∞(r,T ) = sup t∈[r,T ] |yt − yt−r| rβ · rβ ≤ ‖y‖βrβ . On the other hand, sup s 0 with β − 2ε > 0, λ > 1 β−ε − 2 and β′ = β − ε. First of all, let us introduce x̂rt = xrt−r where xr is the solution to (3.1). Then (x̂r ⊗ y)s,t can be expressed as follows: • for s < t ∈ [0, r), (x̂r ⊗ y)s,t = (η·−r ⊗ y)s,t = ∫ t s (yt − yu) dηu−r, (5.1) • for s ∈ [0, r) and t ∈ [r, T ], (x̂r ⊗ y)s,t = (η·−r ⊗ y)s,r + ∫ t r (yt − yu)b(u− r, x̂ru) du + ∫ t r σ(x̂ru−r) du(y·−r ⊗ y)·,t + (η0 − ηs−r)⊗ (yt − yr), (5.2) • for s < t ∈ [r, T ], (x̂r ⊗ y)s,t = ∫ t s (yt − yu)b(u− r, x̂ru) du+ ∫ t s σ(x̂ru−r) du(y·−r ⊗ y)·,t. EJDE-2020/65 CONVERGENCE OF DELAY EQUATIONS 9 We will prove that the norms ‖x̂r‖β′ and ‖x̂r⊗y‖2β′ are bounded and their upper bound does not depend on r. To this aim, the following lemma will be useful. Lemma 5.1. Let (η·−r, y, η·−r⊗y) ∈Mβ d,m(0, r) and (y·−r, y, y·−r⊗y) ∈Mβ d,d(r, T ). Let (xr, y, xr ⊗ y) ∈Mβ d,m(0, T ) be the solution to (3.1). Then ‖x̂r‖β′ ≤ ‖x̂r‖β′(0,r) + ‖x̂r‖β′(r,T ), (5.3) ‖x̂r ⊗ y‖2β′ ≤ ‖x̂r ⊗ y‖2β′(0,r) + ‖x̂r ⊗ y‖2β′(r,T ) + ‖η‖β′(−r,0)‖y‖β′ . (5.4) Proof. On the one hand, observe that ‖x̂r‖β′ ≤ max ( sup 0≤s 0 is such that β − 2ε > 0 and λ > 1 β−ε − 2. Suppose that (x, y, x ⊗ y), (xr, y, xr ⊗ y), (x̂r, y, x̂r ⊗ y) belong to Mβ d,m(0, T ) and (y, y, y ⊗ y) belongs to Mβ m,m(0, T ). Assume that σ and b satisfy (H1) and (H2) respectively, and both satisfy (H3). Assume also that ‖η‖β(−r0,0) < EJDE-2020/65 CONVERGENCE OF DELAY EQUATIONS 15 ∞ and supr≤r0 Φβ(0,r)(η·−r, y) < ∞ and suppose that ‖(y − y·−r) ⊗ y‖2β′(r,T ) → 0 and ‖y·−r ⊗ (y − y·−r)‖2β′(r,T ) → 0 when r tends to zero. Then ‖xr − x̂r‖∞ ≤ KρΛrβ ′ ‖xr − x̂r‖β′ ≤ KρΛrε∥∥(xr − x̂r)⊗ y ∥∥ 2β′ ≤ KMρ3Λ3rε +KMρ3Λ2Λr where K ≥ 1, M ≥ 1 are constants depending on β, β′, r0, T, σ, y and ρ = ( 1 + 3‖b‖∞T 1−β′ + 3‖σ‖∞(1 + T β ′ ) + 2‖σ′‖∞(1 + T β ′ ) + 3‖σ′‖∞T β ′−ε + ‖σ′‖λ ( 2 sup r≤r0 ‖xr‖λβ′ + ‖η‖λβ′(−r0,0) ) T (λ+1)β′−ε + ‖σ′′‖∞T β ′ (1 + T β ′ ) + 2‖σ′′‖λ sup r≤r0 ‖x̂r‖λβ′T (λ+1)β′ ) (1 + T ε), Λ = max ( 1, ‖η‖β(−r0,0), sup r≤r0 Φβ′(0,r)(η·−r, y),Φβ(0,T )(y, y), sup r≤r0 Φβ′(r,T )(y·−r, y), sup r≤r0 Φβ′(0,r)(η·−r, y, y), sup r≤r0 Φβ′(0,T )(x r, y), sup r≤r0 Φβ′(0,T )(x̂ r, y) )( 1 + sup r≤r0 ‖xr‖β′(r) )( 1 + ‖y‖β ) , Λr = max ( 1, sup r≤r0 ‖xr‖β′ )( ‖(y − y·−r)⊗ y‖2β′(r,T ) + ‖y·−r ⊗ (y − y·−r)‖2β′(r,T ) ) . Remark 5.5. Since ρ and Λ are finite (from Proposition 5.2) and Λr converges to zero when r tends to zero (by hypothesis), Proposition 5.4 implies: ‖xr − x̂r‖∞ r↓0−−→ 0, ‖xr − x̂r‖β′ r↓0−−→ 0,∥∥(xr − x̂r)⊗ y ∥∥ 2β′ r↓0−−→ 0. Proof of Proposition 5.4. We start studying the supremum norm. On the one hand, using Proposition 4.1, for r ≤ r0, we obtain ‖xr − x̂r‖∞(0,r) ≤ ‖η‖β′(−r,0)r β′ + ‖b‖∞r +K‖σ‖∞‖y‖β′rβ ′ +KΦβ′(0,r)(η·−r, y) ( ‖σ′‖∞ + ‖σ′‖λ‖η·−r‖λβ′(0,r)r λβ′ ) r2β′ ≤ [ ‖η‖β(−r0,0)T ε + ‖b‖∞T 1−β′ +K‖σ‖∞‖y‖βT ε +KΦβ′(0,r)(η·−r, y) ( ‖σ′‖∞ + ‖σ′‖λ‖η‖λβ′(−r0,0)T λβ′ ) T β ′ ] rβ ′ where we have used that ‖η‖β′(−r,0) ≤ ‖η‖β(−r0,0)T ε and ‖y‖β′ ≤ ‖y‖βT ε. On the other hand, using Proposition 4.1 we obtain ‖xr − x̂r‖∞(r,T ) ≤ ‖b‖∞r +K‖σ‖∞‖y‖β′rβ ′ +KΦβ′(0,T )(x̂ r, y) ( ‖σ′‖∞ + ‖σ′‖λ‖x̂r‖λβ′(r,T )r λβ′ ) r2β′ ≤ [ ‖b‖∞T 1−β′ +K‖σ‖∞‖y‖βT ε 16 M. BESALÚ, G. BINOTTO, C. ROVIRA EJDE-2020/65 +KΦβ′(0,T )(x̂ r, y) ( ‖σ′‖∞ + ‖σ′‖λ‖xr‖λβ′Tλβ ′) T β ′ ] rβ ′ . Hence, we have ‖xr − x̂r‖∞ ≤ KρΛrβ ′ . (5.32) Now we study the Hölder norms. Following the proof of Lemma 5.1 we easily obtain ‖xr − x̂r‖β′ ≤ ‖xr − x̂r‖β′(0,r) + ‖xr − x̂r‖β′(r,T ), (5.33) ‖(xr − x̂r)⊗ y‖2β′ ≤ ‖(xr − x̂r)⊗ y‖2β′(0,r) + ‖(xr − x̂r)⊗ y‖2β′(r,T ) + ‖xr − x̂r‖β′(0,r)‖y‖β′ . (5.34) So we can study the Hölder norms independently in the intervals [0, r) and [r, T ]. We deal with the Hölder norm of (xr − x̂r). By (5.27) and Proposition 4.1 we have ‖xr − x̂r‖β′(0,r) ≤ ‖η‖β′(−r,0) + ‖b‖∞r1−β′ +K‖σ‖∞‖y‖β′(0,r) +KΦβ′(0,r)(η·−r, y) ( ‖σ′‖∞ + ‖σ′‖λ‖η·−r‖λβ′(0,r)r λβ′ ) rβ ′ ≤ [ ‖η‖β(−r0,0) + ‖b‖∞T 1−β +K‖σ‖∞‖y‖β +KΦβ′(0,r)(η·−r, y) × ( ‖σ′‖∞ + ‖σ′‖λ‖η‖λβ′(−r0,0)T λβ′ ) T β ′−ε ] rε. (5.35) In the interval [r, T ], observe that ‖xr − x̂r‖β′(r,T ) ≤ max ( sup s r. Applying integration by parts, we have ‖B ⊗ (B −B·−r)‖2β′(r,T ) = sup s,t∈[r,T ] t−s>r 1 (t− s)2β′ ∣∣∣(Bit −Bis)(Bjt−r −Bjs−r)− ∫ t s (Bju−r −B j s−r) d ◦Biu + ∫ t s (Bju −Bjs) d◦Biu − (Bit −Bis)(B j t −Bjs) ∣∣∣ ≤ sup s,t∈[r,T ] t−s>r 1 (t− s)2β′ ∣∣(Bit −Bis)(Bjt−r −Bjt )∣∣ + sup s,t∈[r,T ] t−s>r 1 (t− s)2β′ ∣∣∣ ∫ t s (Bju −B j u−r) d ◦Biu ∣∣∣ = A1 +A2. (7.4) On the one hand, by (4.4), A1 ≤ sup s,t∈[r,T ] t−s>r ‖B‖β′ |Bjt −B j t−r| (t− s)β′ ≤ sup s,t∈[r,T ] t−s>r 1 (t− s)β′ ‖B‖β′‖B −B·−r‖∞ ≤ sup s,t∈[r,T ] t−s>r rβ (t− s)β′ ‖B‖2βT ε ≤ ‖B‖2βT εrε that approaches zero when r tends to zero. On the other hand, we have that∫ t s (Bju−B j u−r) d ◦Biu is a continuous martingale, so it can be represented as a time- changed Brownian motion: W∫ t s (Bju−Bju−r)2 du, where W is a Brownian motion. Now we choose a ∈ (0, 1 2 ) such that 2β−2ε 2β+1 < a < 2β − 2ε. Applying Hölder property of the Brownian motion, we have A2 = sup s,t∈[r,T ] t−s>r 1 (t− s)2β′ ∣∣W∫ t s (Bju−Bju−r)2 du ∣∣ ≤ sup s,t∈[r,T ] t−s>r Ca,T (t− s)2β′ ∣∣∣ ∫ t s (Bju −B j u−r) 2 du ∣∣∣a ≤ sup s,t∈[r,T ] t−s>r Ca,T ‖B‖2aβ r2aβ(t− s)a−2β′ ≤ Ca,T ‖B‖2aβ r2aβ+a−2β′ , that clearly appraoches zero as r tends to zero. EJDE-2020/65 CONVERGENCE OF DELAY EQUATIONS 25 Now assume that t− s ≤ r. By integration by part formula, we have ‖B ⊗ (B −B·−r)‖2β′(r,T ) ≤ sup s,t∈[r,T ] t−s≤r 1 (t− s)2β′ ∣∣(Bit −Bis)(Bjt−r −Bjs−r)∣∣ + sup s,t∈[r,T ] t−s≤r 1 (t− s)2β′ ∣∣∣ ∫ t s (Bju−r −B j s−r) d ◦Biu ∣∣∣ + sup s,t∈[r,T ] t−s≤r 1 (t− s)2β′ ∣∣∣ ∫ t s (Biu −Bis) d◦Bju ∣∣∣ = V1 + V2 + V3. (7.5) The first term is easy to bound. Indeed, V1 = sup s,t∈[r,T ] t−s≤r |Bit −Bis| (t− s)β · |Bjt−r −B j s−r| (t− s)β · (t− s)2β (t− s)2β′ ≤ ‖B‖2βr2ε. For the other two terms we use inequality (5.8) of Hu and Nualart [9]. It states that there exists a random variable Z such that, almost surely, for all s, t ∈ [0, T ] we have ∣∣∣ ∫ t s (Biu −Bis) d◦Bju ∣∣∣ ≤ Z|t− s| log 1 |t− s| . Set M ′t = ∫ t s (Bju−r −B j s−r) d ◦Biu. Since the process {M ′t , t ∈ [s, T ]} is a continuous martingale, we can follow the ideas in [9] to get that there exists a random variable Z ′ such that, almost surely, for all s, t ∈ [0, T ] we have∣∣ ∫ t s (Bju−r −B j s−r) d ◦Biu ∣∣ ≤ Z ′|t− s| log 1 |t− s| . Hence V2 ≤ Z ′(t− s)1−2β′ log 1 (t− s) ≤ Z ′r1−2β′ log 1 r and V2 goes to zero when r tends to zero. V3 can be studied using the same arguments. It only remains to prove the case where i = j. To simplify the notation we will not write the supra-index i. For t − s ≤ r, we apply again the integration by parts formula and we obtain that ‖B ⊗ (B −B·−r)‖2β′(r,T ) ≤ V ′1 + V ′2 + V ′3 + V ′4 , where V ′1 , V ′2 and V ′3 are the terms defined in (7.5) with i = j and V ′4 := sup s,t∈[r,T ] t−s≤r 1 2 |t− s|1−β ′ ≤ 1 2 r1−β′ . So it only remains to study the terms V ′1 , V ′2 and V ′3 . Easily, for V ′1 we can repeat the same arguments used for V1 and we also obtain that V ′1 ≤ ‖B‖2βr2ε. If we focus 26 M. BESALÚ, G. BINOTTO, C. ROVIRA EJDE-2020/65 in the second term, it can be written as V ′2 = sup s,t∈[r,T ] t−s≤r 1 (t− s)2β′ ∣∣∣ ∫ t s (Bu−r −Bs−r)dBu + 1 2 ∫ t s Du(Bu−r −Bs−r)du ∣∣∣, where Du denotes the de Malliavin derivative. It is easy to check that this Malliavin derivative is zero. So, V ′2 is now a martingale and proceeding as in the case i 6= j we obtain that V ′2 ≤ Cr1−2β′ log 1 r . Finally, for the last term we have V ′3 ≤ sup s,t∈[r,T ] t−s≤r 1 2(t− s)2β′ (Bt −Bs)2 ≤ 1 2 ‖B‖2βr2ε. Therefore, when t− s ≤ r, the three terms tend to zero when r tends to zero. For the case t− s > r, by integration by parts formula we have ‖B ⊗ (B −B·−r)‖2β′(r,T ) ≤ sup s,t∈[r,T ] t−s>r 1 (t− s)2β′ ∣∣(Bt −Bs)(Bt−r −Bt)∣∣ + sup s,t∈[r,T ] t−s>r 1 (t− s)2β′ ∣∣∣ ∫ t s (Bu −Bu−r) d◦Bu − 1 2 (t− s) ∣∣∣. The first term is analogous to the term A1 defined in (7.4), so it is bounded by ‖B‖2βT εrε. For the second term, we can use the relation between Stratonovich and Itô integrals, ∫ t s (Bu −Bu−r) d◦Bu = ∫ t s (Bu −Bu−r) dBu + 1 2 (t− s). Set M ′′t = ∫ t s (Bu−Bu−r) dBu. Fixed s, the process {M ′′t , t ∈ [s, T ]} is a continuous martingale. So following the ideas used for A2, we obtain sup s,t∈[r,T ] t−s>r 1 (t− s)2β′ ∣∣∣ ∫ t s (Bu −Bu−r) d◦Bu − 1 2 (t− s) ∣∣∣ ≤ sup s,t∈[r,T ] t−s>r 1 (t− s)2β′ ∣∣∣ ∫ t s (Bu −Bu−r) dBu ∣∣∣ ≤ Ca,T ‖B‖2aβ r2aβ+a−2β′ , where a ∈ (0, 1 2 ) such that 2β−2ε 2β+1 < a < 2β − 2ε. Thus we obtain that ‖B ⊗ (B − B·−r)‖2β′(r,T ) → 0 as we wish. Inequality (7.2) can be proved with similar computations and the proof of (7.3) follows immediately from the fact that ‖(B −B·−r)⊗B‖2β′(r,T ) ≤ V2 + V3. � EJDE-2020/65 CONVERGENCE OF DELAY EQUATIONS 27 Acknowledgements. This work was supported by the grant MTM2015-65092-P from MINECO, Spain. References [1] M. Besalú, D. Márquez-Carreras, C. Rovira; Delay equations with non-negativity constraints driven by a Hölder continuous function of order β ∈ ( 1 3 , 1 2 ), Potential Anal. 41 (2014), 117–141. [2] M. Besalú, D. 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Mireia Besalú Departament de Genètica, Microbiologia i Estad́ıstica, Universitat de Barcelona, Barcelona, Spain Email address: mbesalu@ub.edu Giulia Binotto Departament de Matemàtiques, Universitat Autònoma de Barcelona, Barcelona, Spain Email address: gbinotto@mat.uab.cat Carles Rovira Departament de Matemàtiques i Informàtica, Universitat de Barcelona, Barcelona, Spain Email address: carles.rovira@ub.edu 1. Introduction 2. Preliminaries 3. Main result 4. Estimates of integrals 5. Estimates of the solutions 6. Proof of main results 7. Stochastic case Acknowledgements References