Startseite Mathematik p-variation and Chung's LIL of sub-bifractional Brownian motion and applications
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p-variation and Chung's LIL of sub-bifractional Brownian motion and applications

  • Nenghui Kuang EMAIL logo und Huantian Xie
Veröffentlicht/Copyright: 13. Oktober 2025

Abstract

Let S H , K = { S H , K ( t ) , t 0 } be the sub-bifractional Brownian motion, with H ( 0 , 1 ) and K ( 0 , 1 ] . We investigate its p -variation and Chung’s law of the iterated logarithm. In addition, we give some applications of these properties.

MSC 2020: 60G15; 60G18; 60F25

1 Introduction

El-Nouty and Journé [1] introduced the process S H , K = { S H , K ( t ) , t 0 } with H ( 0 , 1 ) and K ( 0 , 1 ] , named the sub-bifractional Brownian motion (sbfBm) and defined by

S H , K ( t ) = 1 2 ( 2 K ) 2 ( B H , K ( t ) + B H , K ( t ) ) ,

where { B H , K ( t ) , t R } is a bifractional Brownian motion (bfBm) with H ( 0 , 1 ) and K ( 0 , 1 ] . Clearly, the sbfBm is a centered Gaussian process such that S H , K ( 0 ) = 0 , with probability 1, and Var ( S H , K ( t ) ) = ( 2 K 2 2 H K 1 ) t 2 H K . Note that ( 2 H 1 ) K 1 < K 1 0 , we have 2 H K 1 < K . We can prove that S H , K is self-similar with index HK. When K = 1 , S H , 1 is the subfractional Brownian motion (sfBm). We can easily obtain that for all s , t 0 ,

(1.1) E ( S H , K ( t ) S H , K ( s ) ) = ( t 2 H + s 2 H ) K 1 2 ( t + s ) 2 H K 1 2 t s 2 H K

and

(1.2) C 1 t s 2 H K E [ ( S H , K ( t ) S H , K ( s ) ) 2 ] C 2 t s 2 H K ,

where

C 1 = min { 2 K 1 , 2 K 2 2 H K 1 } , C 2 = max { 1 , 2 2 2 H K 1 } .

(See [1]).

El-Nouty and Journé [1] proved that the sbfBm is a quasi-helix in the sense of Kahane, and the upper classes of some of its increments are characterized by an integral test. Kuang [2] investigated the collision local time of two independent sbfBms. Kuang and Li [3] obtained Berry-Esséen bounds and proved the almost sure central limit theorem for the quadratic variation in the sbfBm. Finally, Kuang and Xie [4] studied least squares-type estimators for the drift parameters in the sub-bifractional Vasicek processes.

In this article, we investigate p -variation and Chung’s law of the iterated logarithm (Chung’s LIL) of sbfBm. In addition, we give some applications of these properties.

Throughout this article, some specific constants in Section i are numbered as c i , 1 , c i , 2 , .

This study is organized as follows: In Section 2, we study p -variation. Section 3 is devoted to Chung’s LIL. Section 4 contains some applications of its properties.

2 p -variation

The variation in Gaussian processes was studied extensively since the works of [5], which proved almost sure convergence to 1 of the quadratic variation j = 1 2 n B ( j 2 n ) B ( ( j 1 ) 2 n ) 2 of the Brownian motion B on [0, 1]. Many new results about the variation in Gaussian processes with stationary increments were obtained (refer [69] and references therein). Wang [10] studied the p -variation in bfBm. Shen et al. [11] obtained the power variation in the sfBm.

We will consider p -variation in sbfBm by using the ideas of Wang [10] and Shen et al. [11]. However, the increments of sbfBm are not independent and not stationary, this causes some difficulties to investigate the variation in the process. In order to overcome the difficulties, we develop a stochastic integral representation of sbfBm.

Now, we state our main results in this section as follows.

Theorem 2.1

Let T > 0 , a > 0 , and v n = n a . Then, for any p 1 , we have, as n ,

(2.1) 1 v n 1 p H K j = 1 [ T v n ] S H , K j v n S H , K j 1 v n p T 2 p 2 Γ ( p + 1 2 ) Γ ( 1 2 ) , a.s. ,

where [ x ] denotes the integer part of x > 0 , and Γ ( x ) 0 t x 1 e t d t for x > 0 , which is a Gamma function.

Corollary 2.2

Let T > 0 , a > 0 , and v n = n a . Then, for any p 1 , we have, as n ,

(2.2) 1 v n 1 p H K j = 1 [ T v n ] S H , K j v n 2 S H , K j 1 v n 2 p T 2 ( 3 p ) 2 Γ ( p + 1 2 ) Γ 1 2 0 T S H , K ( x ) p d x , a.s.

Theorem 2.3

Let T > 0 , a > 0 , and v n = n a . Then, we have, as n ,

(2.3) 1 v n 1 H K j = 1 [ T v n ] sup j 1 v n < t , u < j v n S H , K ( t ) S H , K ( u ) 2 E ( sup 0 t T 1 ( H K ) S H , K ( t ) ) , a.s.

In order to prove Theorems 2.1 and 2.3, we give some technical lemmas. Lemma 2.1 is a Fernique-type inequality for S H , K .

Lemma 2.1

For any ε > 0 , there exists a positive constant c 2,1 = c 2,1 ( ε ) > 0 such that

(2.4) P { sup 0 t T sup 0 s a S H , K ( t + s ) S H , K ( t ) x a H K } c 2,1 T a + 1 e x 2 2 ( 1 + ε ) ,

for any T 0 , a > 0 , and x x 0 > 0 with some x 0 > 0 .

Proof

By (1.2) and the inequality for the normal distribution function Φ ( x ) : 1 Φ ( x ) 1 x e x 2 2 for all x > 0 , we obtain that

P { S H , K ( t + h ) S H , K ( t ) x h H K } c 2,2 e x 2 2

for any t 0 , h > 0 , and x x * > 0 with some x * > 0 . Therefore, by Lemmas 2.1 and 2.2 in [8] (when applied to σ 1 ( h ) = h H K and σ 2 ( ) 0 ), we obtain (2.4) immediately.□

Lemma 2.2 is from [12].

Lemma 2.2

Let X = { X ( t ) , t R } be a centered Gaussian process in R and let F R be a closed set equipped with the canonical metric defined by

(2.5) d ( s , t ) = [ E ( X ( s ) X ( t ) ) 2 ] 1 2 .

Then, there exists a positive constant c 2,3 such that for all u > 0 ,

(2.6) P sup s , t F X ( s ) X ( t ) c 2,3 u + 0 D log N d ( F , ε ) d ε exp u 2 D 2 ,

where N d ( F , ε ) denotes the smallest number of open d-balls of radius ε needed to cover F and where D = sup { d ( s , t ) : s , t F } is the diameter of F.

Lemma 2.3

If X ( t ) and Y ( t ) are a.s. bounded, centered Gaussian processes on Λ such that E ( X 2 ( t ) ) = E ( Y 2 ( t ) ) for all t Λ , and

E [ ( X ( t ) X ( s ) ) 2 ] E [ ( Y ( t ) Y ( s ) ) 2 ] , s , t Λ ,

then for all real λ ,

P ( sup t Λ X ( t ) > λ ) P ( sup t Λ Y ( t ) > λ )

and

E ( sup t Λ X ( t ) ) E ( sup t Λ Y ( t ) ) .

Proof

It is Slepian’s inequality (see, p. 49 in [13]).□

In order to solve the dependence structure of S H , K and to create independence, we will develop the stochastic integral representation of S H , K . By Lamperti’s transformation [14], we define Gaussian process Y = { Y ( t ) , t R } as follows:

(2.7) Y ( t ) = e H K t S H , K ( e t ) , t R .

The covariance function r ( t ) E ( Y ( 0 ) Y ( t ) ) is given by

(2.8) r ( t ) = e H K t ( 1 + e 2 H t ) K 1 2 ( 1 + e t ) 2 H K 1 2 1 e t 2 H K = e H K t ( 1 + e 2 H t ) K 1 2 ( 1 + e t ) 2 H K 1 2 1 e t 2 H K = r ( t ) .

Hence, r ( t ) is an even function and, by (2.8) and the Taylor expansion, we verify that r ( t ) = O ( e β t ) as t , where β = H ( 2 K ) . It follows that r ( ) L 1 ( R ) . By (2.8) and the Taylor expansion we obtain

(2.9) r ( t ) 2 K 2 2 H K 1 1 2 t 2 H K , t 0 .

By Bochner’s theorem [15], Y has the stochastic integral representation:

(2.10) Y ( t ) = R e i λ t W ( d λ ) , t R ,

where W is a complex Gaussian measure with control measure Δ , whose Fourier transform is r ( ) . The measure Δ is called the spectral measure of Y .

Since r ( ) L 1 ( R ) , the spectral measure Δ of Y has a continuous density function f ( λ ) , which can be represented as the inverse Fourier transform of r ( )

(2.11) f ( λ ) = 1 π 0 r ( t ) cos ( t λ ) d t .

Similar to the proof of (2.10) in [16], we can obtain

(2.12) f ( λ ) c 2,4 λ ( 1 + 2 H K ) , as λ ,

where c 2,4 > 0 is an explicit constant depending only on H K .

By (2.7) and (2.10), we obtain

(2.13) S H , K ( t ) = t H K R e i λ log t W ( d λ ) , t > 0 .

We list two properties of the spectral density f ( λ ) of Y . They follow from (2.12), or from (2.9) and the truncation inequalities in [17], page 209, refer also [18].

Lemma 2.4

There exist positive constants c 2,5 and c 2,6 such that for u > 1 ,

(2.14) λ < u λ 2 f ( λ ) d λ c 2,5 u 2 ( 1 H K )

and

(2.15) λ u f ( λ ) d λ c 2,6 u 2 H K .

Proof of Theorem 2.1

Without loss of generality, we suppose T v n is an integer. For integers n and j 1 , we take a n , j = ( j n ) β , where β > 0 is a constant. Define two Gaussian processes

X n , j ( 1 ) ( t ) = t H K λ ( a n , j , a n , j + 1 ] e i λ log t W ( d λ )

and

X n , j ( 2 ) ( t ) = t H K λ ( a n , j , a n , j + 1 ] e i λ log t W ( d λ ) .

Clearly, by (2.13), we have

(2.16) S H , K ( t ) = X n , j ( 1 ) ( t ) + X n , j ( 2 ) ( t ) , for all t 0 .

It is important to note that for a fixed n , the Gaussian processes X n , j ( 1 ) ( t ) , j = 1 , 2 , , are independent; moreover, for every j 1 , X n , j ( 1 ) ( t ) and X n , j ( 2 ) ( t ) are also independent. Since

1 v n 1 p H K j = 1 T v n S H , K j v n S H , K j 1 v n p T 2 p 2 Γ ( p + 1 2 ) Γ ( 1 2 ) 1 v n j = 1 T v n v n p H K S H , K j v n S H , K j 1 v n p X n , j ( 1 ) j v n X n , j ( 1 ) j 1 v n p + 1 v n j = 1 T v n v n p H K E S H , K j v n S H , K j 1 v n p E X n , j ( 1 ) j v n X n , j ( 1 ) j 1 v n p + 1 v n j = 1 T v n v n p H K X n , j ( 1 ) j v n X n , j ( 1 ) j 1 v n p E X n , j ( 1 ) j v n X n , j ( 1 ) j 1 v n p + 1 v n j = 1 T v n v n p H K E S H , K j v n S H , K j 1 v n p T 2 p 2 Γ ( p + 1 2 ) Γ ( 1 2 ) I 1 + I 2 + I 3 + I 4 .

In the following, we will show that the terms I 1 and I 3 almost surely converge to zero, I 2 and I 4 converge to zero, as n , respectively.

First, we prove for a > 0 , T > 0 , and p 1 , as n ,

(2.17) I 1 = 1 v n j = 1 T v n v n p H K S H , K j v n S H , K j 1 v n p X n , j ( 1 ) j v n X n , j ( 1 ) j 1 v n p 0 , a.s.

In fact,

(2.18) v n p H K S H , K j v n S H , K j 1 v n p X n , j ( 1 ) j v n X n , j ( 1 ) j 1 v n p c 2,7 ( sup 0 t T S H , K ( t ) p 1 + sup 0 t T X n , j ( 1 ) ( t ) p 1 ) v n ( p 1 ) H K Y n , j ,

where

(2.19) Y n , j = v n H K sup j 1 v n < t , u < j v n X n , j ( 2 ) ( t ) X n , j ( 2 ) ( u ) ,

and where we use the fact

x p y p p 2 p 1 x p 1 + y p 1 x y .

We have

(2.20) v n p H K E S H , K j v n S H , K j 1 v n p E X n , j ( 1 ) j v n X n , j ( 1 ) j 1 v n p c 2,8 ( E sup 0 t T S H , K ( t ) 2 ( p 1 ) + E sup 0 t T X n , j ( 1 ) ( t ) 2 ( p 1 ) ) 1 2 v n ( p 1 ) H K ( E Y n , j 2 ) 1 2 .

For Y n , j , by Lemmas 2.2 and 2.4, elementary calculus can show that there exists n 0 such that for any n n 0 , for every 1 j T v n and for any t > 0 ,

(2.21) P ( Y n , j > t ) c 2,9 n a + β exp ( c 2,10 n 2 β H K 2 a t 2 ) .

Thus, for any ε > 0 , we obtain

P 1 v n j = 1 T v n v n ( p 1 ) H K Y n , j > ε P max 1 j T v n Y n , j > ε T v n ( p 1 ) H K j = 1 T v n P Y n , j > ε T v n ( p 1 ) H K c 2,11 n 2 a + β exp ( c 2,12 n 2 β H K 2 a 2 a ( p 1 ) H K ) .

Taking β > 0 large enough such that 2 β H K 2 a 2 a ( p 1 ) H K > 0 , by the Borel-Cantelli lemma, we have

(2.22) lim n 1 v n j = 1 T v n v n ( p 1 ) H K Y n , j = 0 , a.s.

Combining (2.18) and (2.22), we prove that (2.17) holds.

Second, we prove for a > 0 , T > 0 , and p 1 , as n ,

(2.23) I 2 = 1 v n j = 1 T v n v n p H K E S H , K j v n S H , K j 1 v n p E X n , j ( 1 ) j v n X n , j ( 1 ) j 1 v n p 0 .

In fact, for any 1 j T v n and r > 2 , by (2.21) and Hölder’s inequality, we obtain

(2.24) ( E ( Y n , j ) 2 ) 1 2 ( E ( Y n , j ) r ) 1 r = 0 P ( ( Y n , j ) r > s ) d s 1 r c 2,9 n a + β 0 exp c 2,10 n 2 β H K 2 a s 2 r d s 1 r = c 2,13 n β H K + a + a + β r ,

where we use by letting s 2 r = t , then

0 exp c 2,10 n 2 β H K 2 a s 2 r d s = r 2 0 t r 2 1 exp ( c 2,10 n 2 β H K 2 a t ) d t = r 2 0 y c 2,10 n 2 β H K 2 a r 2 1 e y d y c 2,10 n 2 β H K 2 a = r 2 Γ ( r 2 ) n ( β H K + a ) r ( c 2,10 ) r 2 .

Hence,

1 v n j = 1 T v n v n ( p 1 ) H K ( E ( Y n , j ) 2 ) 1 2 c 2,14 n a ( p 1 ) H K β H K + a + a + β r .

Taking first β > 0 large enough and then taking r > 2 large enough such that a ( p 1 ) H K β H K + a + a + β r < 0 . Therefore, we obtain

(2.25) lim n 1 v n j = 1 T v n v n ( p 1 ) H K ( E ( Y n , j ) 2 ) 1 2 = 0 .

Similar to (2.24), by using (2.4), for any p > 1 , we have that

(2.26) E ( sup 0 t T S H , K ( t ) 2 ( p 1 ) ) c 2,15 .

Since, for any j 1 , t 0 , h > 0 , we have

E ( X n , j ( 1 ) ( t + h ) X n , j ( 1 ) ( t ) ) 2 E ( S H , K ( t + h ) S H , K ( t ) ) 2 .

Then, (2.4) remains true for X n , j ( 1 ) . Thus, similar to (2.26), we obtain for any 1 j T v n ,

E ( sup 0 t T X n , j ( 1 ) ( t ) 2 ( p 1 ) ) c 2,16 .

Hence, combining (2.20) and (2.25), we have that (2.23) holds.

Third, we prove that for a > 0 , T > 0 , and p 1 , as n ,

(2.27) I 3 = 1 v n j = 1 T v n v n p H K X n , j ( 1 ) j v n X n , j ( 1 ) j 1 v n p E X n , j ( 1 ) j v n X n , j ( 1 ) j 1 v n p 0 , a.s.

In fact, since for a fixed n , the processes { X n , j ( 1 ) ( t ) , t 0 } , j = 1 , 2 , , T v n are independent and so are X n , j ( 1 ) j v n X n , j ( 1 ) j 1 v n p , j = 1 , 2 , , T v n . For any ε > 0 and r > 1 , by Markov inequality and the moment inequality of partial sums of independent random variables, we have

(2.28) P j = 1 T v n v n p H K X n , j ( 1 ) j v n X n , j ( 1 ) j 1 v n p E X n , j ( 1 ) j v n X n , j ( 1 ) j 1 v n p > ε v n c 2,17 v n r E j = 1 T v n v n p H K X n , j ( 1 ) j v n X n , j ( 1 ) j 1 v n p E X n , j ( 1 ) j v n X n , j ( 1 ) j 1 v n p r c 2,18 v n r v n r 2 1 j = 1 T v n E v n p r H K X n , j ( 1 ) j v n X n , j ( 1 ) j 1 v n p E X n , j ( 1 ) j v n X n , j ( 1 ) j 1 v n p r c 2,19 v n r 2 + 1 j = 1 T v n E v n p H K X n , j ( 1 ) j v n X n , j ( 1 ) j 1 v n p r .

Since

σ n , j 2 E X n , j ( 1 ) j + t v n X n , j ( 1 ) j + u v n 2 E S H , K j + t v n S H , K j + u v n 2

and

(2.29) E S H , K j + t v n S H , K j + u v n 2 1 v n 2 H K = ( 2 K 2 2 H K 1 ) ( j + t ) 2 H K + ( 2 K 2 2 H K 1 ) ( j + u ) 2 H K 2 ( ( j + t ) 2 H + ( j + u ) 2 H ) K + ( 2 j + t + u ) 2 H K + t u 2 H K t u 2 H K , as j ,

for any t , u [ 0 , 1 ] and n 1 .

Hence, for t = 1 , u = 0 , there exists j 0 1 such that for any j j 0 ,

E v n p H K X n , j ( 1 ) j v n X n , j ( 1 ) j 1 v n p r c 2,20 v n p r H K σ n , j p r c 2,21 ,

where we have used the fact: let X be a random variable following an N ( 0 , σ 2 ) , then for any γ > 0 ,

(2.30) E ( X γ ) = 2 γ 2 Γ γ + 1 2 Γ 1 2 σ γ .

Therefore,

P j = 1 T v n v n p H K X n , j ( 1 ) j v n X n , j ( 1 ) j 1 v n p E X n , j ( 1 ) j v n X n , j ( 1 ) j 1 v n p > ε v n c 2,22 n a r 2 .

Taking r > 1 large enough such that a r 2 > 1 and by Borel-Cantelli lemma, we obtain (2.27) holds.

Finally, we prove that for a > 0 , T > 0 , and p 1 , as n ,

(2.31) I 4 = 1 v n j = 1 T v n v n p H K E S H , K j v n S H , K j 1 v n p T 2 p 2 Γ ( p + 1 2 ) Γ ( 1 2 ) 0 .

In fact, by (2.29) and (2.30), we have for large j ,

v n p H K E S H , K j v n S H , K j 1 v n p 2 p 2 Γ ( p + 1 2 ) Γ ( 1 2 ) .

Hence, (2.31) holds. Thus, the proof of Theorem 2.1 is complete.□

Proof of Corollary 2.2

By Theorem 2.1, following the same lines as the proof of Theorem 1.2 in [19], we can easily prove the corollary, and omit the details.□

Proof of Theorem 2.3

For simplicity, we assume that T v n is an integer. For a > 0 , we denote

ξ n , j = ξ n , j ( S H , K , a ) = sup j 1 v n < t , u < j v n S H , K ( t ) S H , K ( u ) , η n , j = η n , j ( S H , K , a ) = v n H K ξ n , j .

We first prove that for every a > 0 ,

(2.32) lim n 1 v n 1 H K j = 1 T v n ξ n , j E ξ n , j = 0 , a.s.

Denote ζ n , j = ξ n , j ( X n , j ( 1 ) , a ) , Y n , j = v n H K ξ n , j ( X n , j ( 2 ) , a ) ( Y n , j is actually defined by (2.19)). In order to show (2.32), it is enough to prove that

(2.33) lim n 1 v n 1 H K j = 1 T v n ζ n , j E ζ n , j = 0 , a.s. ,

(2.34) lim n 1 v n j = 1 T v n Y n , j = 0 , a.s. ,

and

(2.35) lim n 1 v n 1 H K j = 1 T v n E ζ n , j E ξ n , j = 0 ,

By equalities (2.22) and (2.23), we can obtain equalities (2.34) and (2.35), respectively. We are preparing to prove (2.33).

In fact, since for a fixed n , X n , j ( 1 ) , j = 1 , 2 , , T v n , are independent; so are v n H K ζ n , j , j = 1 , 2 , , T v n , similar to (2.28), for any ε > 0 and r > 1 , we have

(2.36) P j = 1 T v n v n H K ζ n , j E ( v n H K ζ n , j ) > ε v n c 2,23 v n r 2 + 1 j = 1 T v n E [ ( v n H K ζ n , j ) r ] .

By Lemma 2.1, we obtain for every t > t 0 with some t 0 > 0 and 1 j T v n ,

P ( η n , j > t ) = P sup j 1 v n < t , u < j v n S H , K ( t ) S H , K ( u ) t v n H K c 2,24 v n e c 2,25 t 2 .

Hence, by (2.16) and (2.21), we obtain

P ( v n H K ζ n , j > t ) P η n , j > t 2 + P Y n , j > t 2 c 2,26 n a + β e c 2,27 t 2 .

Therefore, for every 1 j T v n ,

E ( v n H K ζ n , j ) r = 0 P v n H K ζ n , j > t 1 r d t t 0 + t 0 P v n H K ζ n , j > t 1 r d t t 0 + c 2,28 n a + β 0 exp ( c 2,29 t 2 r ) d t c 2,30 n a + β .

Hence, by (2.36), we obtain

P j = 1 T v n v n H K ζ n , j E ( v n H K ζ n , j ) > ε v n c 2,31 n a + β v n r 2 = c 2,32 n a r 2 + a + β .

Taking r > 1 large enough such that a r 2 + a + β < 1 , by the Borel-Cantelli lemma, we have

1 v n 1 H K j = 1 T v n ζ n , j E ζ n , j 0 , a.s. ,

as n . Thus, (2.33) holds.

In order to finish the proof of Theorem 2.3, by the self-similarity of S H , K , we only need to show

(2.37) lim n 1 v n j = 1 T v n E ( η n , j ) = 2 T E ( sup 0 t 1 S H , K ( t ) ) .

By (2.29), there exists j 0 > 0 such that for every t , u [ 0 , 1 ] and all j j 0 ,

lim n E S H , K j + t v n S H , K j + u v n 2 t u 2 H K v n 2 H K = 1 .

Hence, by Lemma 2.3, for every j j 0 ,

lim n E sup 0 < t < 1 S H , K j 1 + t v n S H , K j 1 v n = lim n E sup 0 < t < 1 S H , K t v n .

Therefore,

lim n E ( ξ n , j ) = lim n E sup 0 < t , u < 1 S H , K j 1 + t v n S H , K j 1 v n S H , K j 1 + u v n S H , K j 1 v n = lim n E sup 0 < t , u < 1 S H , K j 1 + t v n S H , K j 1 v n S H , K j 1 + u v n S H , K j 1 v n = lim n 2 E sup 0 < t < 1 S H , K j 1 + t v n S H , K j 1 v n = lim n 2 E sup 0 < t < 1 S H , K t v n .

Hence, by the self-similarity of S H , K , for any j j 0 ,

lim n E ( η n , j ) = lim n E ( v n H K ξ n , j ) = 2 lim n v n H K E sup 0 < t < 1 S H , K t v n = 2 E [ sup 0 < t < 1 ( S H , K ( t ) ) ] .

By (2.26), we have

max 1 j j 0 E ( η n , j ) E v n H K sup 0 < t , u < j 0 v n S H , K ( t ) S H , K ( u ) = 2 E v n H K sup 0 < t < j 0 v n S H , K ( t ) = 2 j 0 H K E ( sup 0 < t < 1 S H , K ( t ) ) c 2,33 .

Therefore,

lim n 1 v n j = 1 T v n E ( η n , j ) = lim n 1 v n j = 1 j 0 E ( η n , j ) + lim n 1 v n j = j 0 + 1 T v n E ( η n , j ) = 2 T E [ sup 0 < t < 1 ( S H , K ( t ) ) ] .

The proof of Theorem 2.3 is completed.□

3 Chung’s LIL

In [16,18,20,21] the authors established Chung’s LIL for fBm and other strongly locally nondeterministic Gaussian processes with stationary increments. Luan [22] obtained Chung’s LIL for sbfBm. In this section, we prove the Chung’s LIL for sbfBm S H , K in R .

Theorem 3.1

Let S H , K = { S H , K ( t ) , t 0 } be the sbfBms in R , with H ( 0 , 1 ) and K ( 0 , 1 ] . Then, there exists a positive and finite constant c 3,1 such that

(3.1) liminf r 0 max t [ 0 , r ] S H , K ( t ) r H K ( log log ( 1 r ) ) H K = c 3,1 , a.s.

In order to prove Theorem 3.1, we need several lemmas. Lemma 3.1 shows that the sbfBms S H , K has strong local nondeterminism. Lemma 3.2 gives estimates on the small ball probability of S H , K .

Lemma 3.1

For all constants 0 < a < b , S H , K is strongly locally φ -nondeterministic on I = [ a , b ] with φ ( r ) = r 2 H K . That is, there exist positive constants c 3,2 and r 0 such that for all t I and all 0 < r min { t , r 0 } ,

(3.2) Var { S H , K ( t ) S H , K ( s ) : s I , r s t r 0 } c 3,2 φ ( r ) .

Proof

See the proof of Proposition 2.1 in [2], the proof follows the same line as Proposition 2.1 in [16].□

Lemma 3.2

There exist positive constants c 3,3 and c 3,4 such that for all t 0 [ 0 , 1 ] and x ( 0 , 1 ) ,

(3.3) exp c 3,3 x 1 ( H K ) P { max t [ 0 , 1 ] S H , K ( t ) S H , K ( t 0 ) x } exp c 3,4 x 1 ( H K ) .

Proof

By Lemma 3.1 and (1.2), we know that S H , K satisfies conditions ( C 1 ) and ( C 2 ) of [23]. Hence, this lemma holds by Theorem 3.1 of [23].□

The following Lemma 3.3 is from [16], which provides a zero-one law for ergodic self-similar processes.

Lemma 3.3

Let X = { X t , t R } be a separable, self-similar process with index k. We assume that X 0 = 0 and that X is ergodic. Then, for any increasing function ψ : R + R + , we have P ( E k , ψ ) = 0 or 1, where

E k , ψ = { ω : t h e r e e x i s t s δ > 0 s u c h t h a t sup 0 s t X s t k ψ ( t ) f o r a l l 0 < t δ } .

By a result of [24] on ergodicity and mixing properties of stationary Gaussian processes, we see that S H , K is mixing. Hence, we can obtain the following lemma.

Lemma 3.4

There exists a constant c 3,5 [ 0 , ] such that

(3.4) liminf t 0 + ( log log ( 1 t ) ) H K t H K max 0 s t S H , K ( s ) = c 3,5 , a.s.

Proof

We take ψ c ( t ) = c ( log log ( 1 t ) ) H K and define c 3,5 = sup { c 0 : P ( E k , ψ c ) = 1 } . Then, (3.4) holds from Lemma 3.3.□

Theorem 3.1 will be established if we prove c 3,5 ( 0 , ) from Lemma 3.4. This is where Lemmas 3.2 and 2.2 are needed.

Now, we proceed to prove Theorem 3.1.

Proof of Theorem 3.1

We prove the lower bound first. For any integer n 1 , let r n = e n . Let 0 < γ < c 3,4 be a constant and consider the event

(3.5) A n = { max 0 s r n S H , K ( s ) γ H K r n H K ( log log ( 1 r n ) ) H K } .

Then, by the self-similarity of S H , K and Lemma 3.2,

(3.6) P { A n } = P { max 0 s r n S H , K ( s ) γ H K r n H K ( log log ( 1 r n ) ) H K } = P { max 0 s 1 S H , K ( r n s ) γ H K r n H K ( log log ( 1 r n ) ) H K } = P { r n H K max 0 s 1 S H , K ( s ) γ H K r n H K ( log log ( 1 r n ) ) H K } = P { max 0 s 1 S H , K ( s ) γ H K ( log log ( 1 r n ) ) H K } exp c 3,4 γ log n = n c 3,4 γ .

Since n = 1 P { A n } < , by the Borel-Cantelli lemma, we obtain

(3.7) liminf n max 0 s r n S H , K ( s ) r n H K ( log log ( 1 r n ) ) H K c 3,4 a.s.

By (3.7) and a standard monotonicity argument, we have

(3.8) liminf r 0 max 0 s r S H , K ( s ) r H K ( log log ( 1 r ) ) H K c 3,6 a.s.

We will prove the upper bound by the following stochastic integral representation of S H , K . For every t > 0 , by (2.13), we have

S H , K ( t ) = t H K R e i λ log t W ( d λ ) .

For every integer n 1 , we take

(3.9) t n = n n and d n = n β ,

where β > 0 is a constant whose value will be determined later. It is sufficient to prove that there exists a finite constant c 3,7 such that

(3.10) liminf n max 0 s t n S H , K ( s ) t n H K ( log log ( 1 t n ) ) H K c 3,7 a.s.

Define two Gaussian processes, X n 1 and X n 2 , by

(3.11) X n 1 ( t ) t H K λ ( d n 1 , d n ] e i λ log t W ( d λ )

and

(3.12) X n 2 ( t ) t H K λ ( d n 1 , d n ] e i λ log t W ( d λ ) ,

respectively. Clearly, S H , K ( t ) = X n 1 ( t ) + X n 2 ( t ) for all t 0 . It is important to note that the Gaussian processes X n 1 ( n = 1 , 2 , ) are independent; moreover, for every n 1 , the processes X n 1 and X n 2 are also independent.

Let h ( r ) = r H K ( log log ( 1 r ) ) H K . We make the following two claims:

(i) There is a constant γ > 0 such that

(3.13) n = 1 P { max s [ 0 , t n ] X n 1 ( s ) γ H K h ( t n ) } = .

(ii) For every ε > 0 ,

(3.14) n = 1 P { max s [ 0 , t n ] X n 2 ( s ) > ε h ( t n ) } < .

Since the events in (3.13) are independent, we see that (3.10) follows from (3.13), (3.14), and a standard Borel-Cantelli argument.

It remains to verify the claims (i) and (ii) above. By Lemma 3.2 and Anderson’s inequality [25], we obtain

(3.15) P { max s [ 0 , t n ] X n 1 ( s ) γ H K h ( t n ) } P { max s [ 0 , t n ] S H , K ( s ) γ H K h ( t n ) } = P { max s [ 0 , 1 ] S H , K ( t n s ) γ H K h ( t n ) } = P { t n H K max s [ 0 , 1 ] S H , K ( s ) γ H K h ( t n ) } = P { max s [ 0 , 1 ] S H , K ( s ) γ H K ( log log ( 1 t n ) ) H K } exp c 3,3 γ log ( n log n ) = ( n log n ) c 3,3 γ .

Thus, (i) holds for γ c 3,3 .

In order to prove (ii), we divide [ 0 , t n ] into p n + 1 non-overlapping subintervals J n , j = [ a n , j 1 , a n , j ] , j = 0 , 1 , , p n , and then apply Lemma 2.2 to X n 2 on each of J n , j . Let β > 0 be the constant in (3.9) and take J n , 0 = [ 0 , t n n β ] . After J n , 0 has been defined, we take a n , j + 1 = a n , j ( 1 + n β ) . It can be verified that the number of such subintervals of [ 0 , t n ] satisfies the following bound:

(3.16) p n + 1 c n β log n .

Moreover, for every j 1 , if s , t J n , j and s < t , then we have t s 1 n β and this yields

(3.17) t s s n β and log t s n β .

(1.2) implies that the canonical metric d for the process X n 2 satisfies

(3.18) d ( s , t ) c s t H K for all s , t > 0

and d ( 0 , s ) c t n H K n β H K for every s J n , 0 . It follows that D 0 sup { d ( s , t ) ; s , t J n , 0 } c t n H K n β H K , and

(3.19) N d ( J n , 0 , ε ) t n n β ( ε c ) 1 ( H K ) .

Some simple calculations yield

(3.20) 0 D 0 log N d ( J n , 0 , ε ) d ε 0 c t n H K n β H K log t n n β ( ε c ) 1 ( H K ) d ε = 0 1 c t n H K n β H K log 1 u 1 ( H K ) d u = c 1 ( H K ) t n H K n β H K 0 1 log 1 u d u = c 3,8 t n H K n β H K .

It follows from Lemma 2.2 and (3.20) that

(3.21) P { max s J n , 0 X n 2 ( s ) > ε h ( t n ) } = P { max s J n , 0 X n 2 ( s ) X n 2 ( 0 ) > ε h ( t n ) } P { max s , t J n , 0 X n 2 ( s ) X n 2 ( t ) > c 3,9 2 u } P max s , t J n , 0 X n 2 ( s ) X n 2 ( t ) > c 3,9 u + 0 D 0 log N d ( J n , 0 , ε ) d ε exp u 2 ( D 0 ) 2 exp c t n 2 H K ( log ( n log n ) ) 2 H K t n 2 H K n 2 β H K = exp c n 2 β H K ( log ( n log n ) ) 2 H K ,

where u = ε 2 c 3,9 h ( t n ) , which is larger than 0 D 0 log N d ( J n , 0 , ε ) d ε .

For every 1 j p n , we estimate the d -diameter of J n , j . It follows from (3.12) that for any s , t J n , j with s < t ,

(3.22) E ( X n 2 ( s ) X n 2 ( t ) ) 2 = λ d n 1 t H K e i λ log t s H K e i λ log s 2 f ( λ ) d λ + λ > d n t H K e i λ log t s H K e i λ log s 2 f ( λ ) d λ T 1 + T 2 .

For T 2 , we have, for all s , t J n , j ,

(3.23) T 2 4 t n 2 H K λ > d n f ( λ ) d λ c 3,10 t n 2 H K n 2 β H K ,

where the last inequality follows from (2.15).

For T 1 , we use the elementary inequalities 1 cos x x 2 for every x R and x α 1 ( x 1 ) α for x > 1 and 0 < α < 1 to derive that, for all s , t J n , j with s < t ,

(3.24) T 1 = λ d n 1 t H K e i λ log t s H K e i λ log s 2 f ( λ ) d λ = λ d n 1 ( t H K s H K ) 2 + 2 t H K s H K 1 cos λ log t s f ( λ ) d λ s 2 H K t s H K 1 2 R f ( λ ) d λ + 2 t 2 H K λ d n 1 1 cos λ log t s f ( λ ) d λ s 2 H K t s 1 2 H K + 2 t 2 H K log t s 2 λ d n 1 λ 2 f ( λ ) d λ t n 2 H K n 2 β H K + 2 t n 2 H K n 2 β c 1 ( n 1 ) 2 β ( 1 H K ) c 3,11 t n 2 H K n 2 β H K ,

where in deriving the last but one inequality, we have used (3.17) and (2.14), respectively.

It follows from (3.22), (3.23), and (3.24) that the d -diameter of J n , j satisfies

(3.25) D j c 3,12 t n H K n β H K .

Hence, similar to (3.21), we use Lemma 2.2 and (3.25) to deduce

(3.26) P { max s J n , j X n 2 ( s ) > ε h ( t n ) } exp c n 2 β H K ( log ( n log n ) ) 2 H K .

By (3.16), (3.21), and (3.26), we deduce that for every ε > 0 ,

(3.27) n = 1 P { max s [ 0 , t n ] X n 2 ( s ) > ε h ( t n ) } n = 1 j = 0 p n P { max s J n , j X n 2 ( s ) > ε h ( t n ) } c n = 1 ( n β log n ) exp c n 2 β H K ( log ( n log n ) ) 2 H K < .

This proves (3.14) and hence the theorem.□

By the decomposition of sbfBm and Chung’s LIL for the sfBm, we give simple proof of Theorem 3.1.

Lemma 3.5

Let S H , K be an sbfBm, and assume that { W t , t 0 } is a standard Brownian motion independent of S H , K . Let X K be the process defined by

(3.28) X t K = 0 ( 1 e θ t ) θ 1 + K 2 d W θ .

Then, the processes K Γ ( 1 K ) X t 2 H K + S H , K ( t ) , t 0 and { S t H K , t 0 } have the same distribution, where { S t H K , t 0 } is an sfBm with Hurst parameter H K .

Proof

See the proof of Lemma 2.1 in [26]. For the convenience of readers, we give the proof. By (3.28), we know that X K is a centered Gaussian process with covariance

(3.29) E ( X t K X s K ) = 0 ( 1 e θ t ) ( 1 e θ s ) θ 1 K d θ = 0 ( 1 e θ t ) θ 1 K d θ 0 ( 1 e θ t ) e θ s θ 1 K d θ = 0 0 t θ e θ u d u θ 1 K d θ 0 0 t θ e θ u d u e θ s θ 1 K d θ = 0 t ( 0 θ K e θ u d θ ) d u 0 t ( 0 θ K e θ ( u + s ) d θ ) d u = Γ ( 1 K ) K [ t K + s K ( t + s ) K ] .

Let Y t = K Γ ( 1 K ) X t 2 H K + S H , K ( t ) . Then, from (1.1) and (3.29), we have, for s , t 0 ,

E ( Y s Y t ) = K Γ ( 1 K ) E ( X s 2 H K X t 2 H K ) + E ( S H , K ( s ) S H , K ( t ) ) = t 2 H K + s 2 H K ( t 2 H + s 2 H ) K + ( t 2 H + s 2 H ) K 1 2 ( t + s ) 2 H K 1 2 t s 2 H K = t 2 H K + s 2 H K 1 2 ( t + s ) 2 H K 1 2 t s 2 H K ,

which completes the proof.□

Lemma 3.5 implies that

(3.30) { S H , K ( t ) , t 0 } = d S t H K K Γ ( 1 K ) X t 2 H K , t 0 ,

where = d means equality of all finite dimensional distributions.

Simple proof of Theorem 3.1

[22] established Chung’s LIL for sfBm S H . Namely, there exists a positive and finite constant c 3,13 such that

liminf r 0 max t [ 0 , r ] S t H r H ( log log ( 1 r ) ) H = c 3,13 , a.s.

The decomposition (3.30) allows us deduce Chung’s LIL for the sbfBm, from the same result for the sfBm with Hurst parameter H K , with the same constant.

4 Applications

In this section, we give some applications of the results in this article. For estimating the self-similar index H K of a sbfBm. We introduce an estimator for the index H K of S H , K given by

H K ˆ n ( p ) = 1 p log n log S n ( p ) S n 2 ( p ) ,

where

S v n ( p ) = 1 v n j = 1 [ v n ] S H , K j v n S H , K j 1 v n p .

Theorem 4.1

For any p 1 , we have H K ˆ n ( p ) H K almost surely as n .

Proof

By Theorem 2.1, we have, as n ,

H K ˆ n ( p ) = 1 p log n log S n ( p ) S n 2 ( p ) = 1 p log n log n p H K S n ( p ) n 2 p H K S n 2 ( p ) n p H K = 1 p log n log n p H K S n ( p ) n 2 p H K S n 2 ( p ) + H K H K , a.s.

Thus, we finish the proof.□

Remark 4.1

We cannot obtain the estimators of H and K , respectively, similar to the estimators of H and K for bfBm in [10]. Because the limit in (2.1) has no relation to K .

In the following, we give some applications of the decomposition of sbfBm.

Recall that a continuous process { X t , t [ 0 , T ] } admits α -variation (resp. α -strong variation) if the limit in probability

lim n i = 0 n 1 X ( i + 1 ) t n X i t n α

(resp.

lim ε 0 1 ε 0 t X s + ε X s α d s ) ,

exists for every t [ 0 , T ] .

Then, we have:

Theorem 4.2

The α -variation (resp. α -strong variation) of sbfBm is C H K t , where C H K = E ( ξ H K ) and ξ is a standard normal random variable.

Proof

The results follow easily from (3.29) and the variation in X k is 0, since X k is absolutely continuous. (Refer also the proofs of Proposition 4 in [27] and Proposition 3.6(a) in [28]).□

Acknowledgments

NK was supported by the Natural Science Foundation of Hunan Province under Grant 2021JJ30233 and by the Scientific Research Project of the Education Department of Hunan Province under Grant 24A0345. HX was partly supported by NSF of China (No. 12271233), Improving innovation ability of enterprises in Shandong province (No. 2023TSGC0466), and NSF of Shandong Province (No. ZR2019YQ05, 2019KJI003). The authors wish to thank anonymous referees for careful reading of the previous version of this study and also their comments which improved the study.

  1. Funding information: The authors state no funding involved.

  2. Author contributions: Both authors have accepted responsibility for the entire content of this manuscript and consented to its submission to the journal, reviewed all the results and approved the final version of the manuscript. HX has given some ideas about the proofs of p -variation and Chung’s LIL of Sub-bifractional Brownian motion. NK wrote this article.

  3. Conflict of interest: The authors state no conflicts of interest.

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Received: 2024-12-11
Revised: 2025-06-30
Accepted: 2025-09-18
Published Online: 2025-10-13

© 2025 the author(s), published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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  73. Dynamical properties of two-diffusion SIR epidemic model with Markovian switching
  74. A note on weighted measure-theoretic pressure
  75. Pullback attractors for a class of second-order delay evolution equations with dispersive and dissipative terms on unbounded domain
  76. Pullback attractor of the 2D non-autonomous magneto-micropolar fluid equations
  77. Functional Analysis
  78. Spectrum boundary domination of semiregularities in Banach algebras
  79. Approximate multi-Cauchy mappings on certain groupoids
  80. Investigating the modified UO-iteration process in Banach spaces by a digraph
  81. Tilings, sub-tilings, and spectral sets on p-adic space
  82. Continuity and essential norm of operators defined by infinite tridiagonal matrices in weighted Orlicz and l spaces
  83. A family of commuting contraction semigroups on l 1 ( N ) and l ( N )
  84. q-Stirling sequence spaces associated with q-Bell numbers
  85. Chlodowsky variant of Bernstein-type operators on the domain
  86. Hyponormality on a weighted Bergman space of an annulus with a general harmonic symbol
  87. Characterization of derivations on strongly double triangle subspace lattice algebras by local actions
  88. Fixed point approaches to the stability of Jensen’s functional equation
  89. Geometry
  90. The regularity of solutions to the Lp Gauss image problem
  91. Solving the quartic by conics
  92. Group Theory
  93. On a question of permutation groups acting on the power set
  94. A characterization of the translational hull of a weakly type B semigroup with E-properties
  95. Harmonic Analysis
  96. Eigenfunctions on an infinite Schrödinger network
  97. Maximal function and generalized fractional integral operators on the weighted Orlicz-Lorentz-Morrey spaces
  98. Subharmonic functions and associated measures in ℝn
  99. Mathematical Logic, Model Theory and Foundation
  100. A topology related to implication and upsets on a bounded BCK-algebra
  101. Boundedness of fractional sublinear operators on weighted grand Herz-Morrey spaces with variable exponents
  102. Number Theory
  103. Fibonacci vector and matrix p-norms
  104. Recurrence for probabilistic extension of Dowling polynomials
  105. Carmichael numbers composed of Piatetski-Shapiro primes in Beatty sequences
  106. The number of rational points of some classes of algebraic varieties over finite fields
  107. Classification and irreducibility of a class of integer polynomials
  108. Decompositions of the extended Selberg class functions
  109. Joint approximation of analytic functions by the shifts of Hurwitz zeta-functions in short intervals
  110. Fibonacci Cartan and Lucas Cartan numbers
  111. Recurrence relations satisfied by some arithmetic groups
  112. The hybrid power mean involving the Kloosterman sums and Dedekind sums
  113. Numerical Methods
  114. A modified predictor–corrector scheme with graded mesh for numerical solutions of nonlinear Ψ-caputo fractional-order systems
  115. A kind of univariate improved Shepard-Euler operators
  116. Probability and Statistics
  117. Statistical inference and data analysis of the record-based transmuted Burr X model
  118. Multiple G-Stratonovich integral in G-expectation space
  119. p-variation and Chung's LIL of sub-bifractional Brownian motion and applications
  120. Real Analysis
  121. Chebyshev polynomials of the first kind and the univariate Lommel function: Integral representations
  122. Multiple solutions for a class of fourth-order elliptic equations with critical growth
  123. Majorization-type inequalities for (m, M, ψ)-convex functions with applications
  124. The evaluation of a definite integral by the method of brackets illustrating its flexibility
  125. Some new Fejér type inequalities for (h, g; α - m)-convex functions
  126. Some new Hermite-Hadamard type inequalities for product of strongly h-convex functions on ellipsoids and balls
  127. Topology
  128. Unraveling chaos: A topological analysis of simplicial homology groups and their foldings
  129. A generalized fixed-point theorem for set-valued mappings in b-metric spaces
  130. On SI2-convergence in T0-spaces
  131. Generalized quandle polynomials and their applications to stuquandles, stuck links, and RNA folding
Heruntergeladen am 21.1.2026 von https://www.degruyterbrill.com/document/doi/10.1515/math-2025-0203/html
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