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R E S E A R C H

Open Access

Parameter estimation for

Ornstein–Uhlenbeck processes driven by

fractional Lévy process

Guangjun Shen

1,2*

, Yunmeng Li

2

and Zhenlong Gao

3

*Correspondence:[email protected] 1School of Mathematics and

Finance, Chuzhou University, Chuzhou, China

2Department of Statistics, Anhui

Normal University, Wuhu, China Full list of author information is available at the end of the article

Abstract

We study the minimum Skorohod distance estimation

θ

ε∗and minimumL1-norm

estimation

θ

εof the drift parameter

θ

of a stochastic differential equation

dXt=

θ

Xtdt+

ε

dLdt,X0=x0, where{Ldt, 0≤tT}is a fractional Lévy process,

ε

∈(0, 1].

We obtain their consistency and limit distribution for fixed T, when

ε

→0. Moreover, we also study the asymptotic laws of their limit distributions forT→ ∞.

MSC: 60G18; 65C30; 93E24

Keywords: Fractional Lévy process; Minimum Skorohod distance estimation; MinimumL1-norm estimation; Consistency; Limit distribution; Asymptotic law

1 Introduction

Statistical inference for stochastic equations is a main research direction in probability theory and its applications. The asymptotic theory of parametric estimation for diffusion processes with small noise is well developed. Genon-Catalot [8] and Laredo [17] consid-ered the efficient estimation for drift parameters of small diffusions from discrete observa-tions as→0 andn→ ∞. Using martingale estimating function, Sørensen [27] obtained consistency and asymptotic normality of the estimators of drift and diffusion coefficient parameters as→0 andnis fixed. Using a contrast function under suitable conditions on

andn, Sørensen and Uchida [28] and Gloter and Sørensen [9] considered the efficient estimation for unknown parameters in both drift and diffusion coefficient functions. Long [20], Ma [21] studied parameter estimation for Ornstein–Uhlenbeck processes driven by small Lévy noises for discrete observations when→0 andn→ ∞simultaneously. Shen and Yu [26] obtained consistency and the asymptotic distribution of the estimator for Ornstein–Uhlenbeck processes with small fractional Lévy noises.

Recently, Diop and Yode [4] obtained the minimum Skorohod distance estimate for the parameterθ of a stochastic differential equation with a centered Lévy processes{Zt, 0≤

tT},∈(0, 1],

dXt=θXtdt+dZt, X0=x0.

When{Zt, 0≤tT}is a Brownian motion, Millar [24] obtained the asymptotic behavior

of the estimator of the parameterθ. The minimum uniform metric estimate of parameters

(2)

of diffusion-type processes was considered in Kutoyants and Pilibossian [14,15]. Hénaff [10] considered the asymptotics of a minimum distance estimator of the parameter of the Ornstein–Uhlenbeck process. Prakasa Rao [25] studied the minimumL1-norm estimates of the drift parameter of Ornstein–Uhlenbeck process driven by fractional Brownian mo-tion and investigated the asymptotic properties following Kutoyants and Pilibossian [14,

15]. Some surveys on the parameter estimates of fractional Ornstein–Uhlenbeck process can be found in Hu and Nualart [11], El Onsy, Es-Sebaiy and Ndiaye [5], Xiao, Zhang and Xu [29], Jiang and Dong [12], Liu and Song [19].

Motivated by the above results, in this paper we consider the minimum Skorohod dis-tance estimationθε∗ and minimumL1-norm estimation θε of the drift parameterθ for

Ornstein–Uhlenbeck processes driven by the fractional Lévy process {Ld

t, 0≤tT}

which satisfies the following stochastic differential equation:

dXt=θXtdt+dLdt, X0=x0, (1)

where the shift parameterθΘ= (θ1,θ2)⊆Ris unknown,ε∈(0, 1]. Denote byθ0the true

value of the unknown parameterθ. Note that

Xt(θ) =xt(θ) +εeθt

t

0

eθsdLds,

wherext(θ) =x0eθtis a solution of (1) withε= 0.

Recall that fractional Lévy processes is a natural generalization of the integral represen-tation of fractional Brownian motion. Analogously to Mandelbrot and Van Ness [22] for fractional Brownian motion we introduce the following definition.

Definition 1.1(Marquardt [23]) LetL= (L(t),tR) be a zero-mean two-sided Lévy

pro-cess withE[L(1)2] <and without a Brownian component. Ford(0,1

2), a stochastic

process

Ldt := 1

Γ(d+ 1)

–∞

(ts)d+– (–s)+dL(ds), tR, (2)

is called a fractional Lévy process (fLp), where

L(t) =L1(t), t≥0, L(t) = –L2(–t–), t< 0. (3)

{L1(t),t≥0}and{L2(t),t≥0}are two independent copies of a one-side Lévy process.

Lemma 1.1(Marquardt [23]) Let gH,H is the completion of L1(R)∩L2(R)with respect to the normg2

H=E[L(1)2]

R(I d

g)2(u)du,then

R

g(s)dLds=

R

Idg(u)dL(u), (4)

where the equality holds in the L2sense and Id

g denotes the Riemann–Liouville fractional integral defined by

Idg(x) = 1

Γ(d)

x

(3)

Lemma 1.2(Marquardt [23]) Let|f|,|g| ∈H.Then

E

R

f(s)dLds

R

g(s)dLds

=Γ(1 – 2d)E[L(1)

2]

Γ(d)Γ(1 –d)

R

R

f(t)g(s)|ts|2d–1ds dt. (5)

Lemma 1.3(Bender et al. [2]) Let Ld

t be a fLp.Then for every p≥2andδ> 0such that

d+δ<12there exists a constant Cp,δ,dindependent of the driving Lévy process L such that

for every T≥1

E

sup

0≤tT

Ldtp

Cp,δ,dEL(1)p

Tp(d+1/2+δ).

For the study of fLp see Bender et al. [3], Fink and Klüppelberg [7], Lin and Cheng [18], Benassi et al. [1], Lacaux [16], Engelke [6] and the references therein.

The rest of this paper is organized as follows. In Sect.2, we consider the minimum Skoro-hod distance estimationθε∗of the drift parameterθ, its consistency and limit distribution

are studied for fixed T, whenε→0. Moreover, the asymptotic law of its limit distribution are also studied forT → ∞. The similar problems for minimumL1-norm estimationθε

of the drift parameterθwere studied in Sect.3.

2 Minimum Skorohod distance estimation

In this section, we consider the minimum Skorohod distance estimation which defined by

θε∗=arg min

θΘρ

X,x(θ), (6)

where

ρ(x,y) = inf

μΛ([0,T])

H(μ) +sup(t)–y(t) (7)

on the Skorohod spaceD([0,T],R) consists of càdlàg functions on [0,T],Λ([0,T]) is the set of functionsμdefined on [0,T] with values in [0,T], continuous, strictly increasing such thatμ(0) = 0 andμ(T) =T, and

H(μ) = sup s,t∈[0,T],s=t

log

μ(s) –μ(t)

st

<∞.

Let

ηT=arg min u

Y(θ0),ux˙(θ0)

, (8)

wherex˙(θ0) =x0teθ0t is the derivative ofxt(θ0) with respect toθ0and

Yt(θ0) =0t

t

0

0sdLd

s. (9)

Let

f(κ) = inf

|θθ0|>κ

Xtx(θ0)= inf |θθ0|>κ0≤suptT

Xtx(θ0), κ> 0 (10)

(4)

Theorem 2.1(Consistency) For every p≥2andκ> 0such that,for every T≥1,we have

P(θε0)θ

εθ0>κ

Cp,κ,dEL(1)p

Tp(d+1/2+κ)

2εe|θ0|T

f(κ) p

=Of(κ)–pεp, (11)

where constant Cp,κ,dis only dependent on p,κ,d.

Proof Fixedκ> 0 and let

I0=

ω: inf

|θθ0|<κρ

X,x(θ)> inf

|θθ0|>κ

ρX,x(θ).

Then we can obtainI0={|θε∗–θ0|>κ}. In fact, forωI0, we have

inf

|θθ0|<κ

ρX(ω),x(θ)≥inf

θΘρ

X(ω),x(θ)=ρX(ω),ε∗,

thus,|θε∗(ω) –θ0|>κ. On the other hand, assume that|θε∗(ω) –θ0|>κ,

ρX(ω),ε∗= inf

|θθ0|>κρ

X(ω),x(θ)< inf

|θθ0|<κρ

X(ω),x(θ).

For anyκ> 0, we have

P(θε0)(I0) =P (ε)

θ0

inf

|θθ0|<κρ

X,x(θ)> inf

|θθ0|>κρ

X,x(θ)

Pθ(ε0)

inf

|θθ0|<κρ

X,x(θ)> inf

|θθ0|>κ

ρX,x(θ)–ρx(θ0),x(θ)

Pθ(ε0) inf

|θθ0|<κρ

X,x(θ)> inf

|θθ0|>κρ

x(θ0),x(θ)

ρX,x(θ0)

(ε0)

inf

|θθ0|<κρ

x(θ),x(θ0)

+ 2ρX,x(θ0)

> inf

|θθ0|>κρ

x(θ0),x(θ)

(ε0)

Xx(θ0)> f(κ)

2

.

Besides, since the processXtsatisfies the stochastic differential Eqs. (1), it follows that

Xtxt(θ0) =x0+θ0

t

0

Xsds+εLdtxt(θ0) =θ0

t

0

Xsxs(θ0)

ds+εLdt. (12)

Then

Xtxt(θ0)=

θ0

t

0

Xsxs(θ0)

ds+εLdt≤ |θ0|

t

0

Xsxs(θ0)ds+εLdt. (13)

Hence, we have

Xx(θ0)= sup 0≤tT

Xtxt(θ0)≤εe|θ0T| sup 0≤tT

Ldt (14)

because of the Gronwall–Bellman lemma. Thus,

P(θε0)

Xx(θ0)> f(κ)

2

P

sup

0≤tT

Ldtf(κ)

2εe|θ0T|

(5)

According to Lemma1.3and Chebyshev’s inequality, for allp≥2, we get

P(θε0)θ

εθ0>κ

E

sup

0≤tT

Ld t

p2εe|θ0T|

f(κ) p

Cp,κ,dEL(1) p

Tp(d+1/2+κ)2pe|θ0T|pf(κ)pεp

=Of(κ)–pεp. (16)

This completes the proof.

Remark2.1 As a consequence of the above theorem, we obtain the result thatθε∗converges in probability toθ0underP(

ε)

θ0-measure asε→0. Furthermore, the rate of convergence is

of orderO(εp) for everyp≥2.

Theorem 2.2(Limit distribution) For any hD([0,T],R)satisfying h(0) = 0,φα

h =ρ(h,u·

a), a(t) =teαt, αR,uR admits a unique minimum at u. Then we have, asε0,

ε–1(θε∗–θ0) d

ζT,where the notation “ d

” denotes “convergence in distribution”.

Remark2.2 φα

h is a convex function andφhα→+∞when|u| →+∞, soφhαadmits a

min-imum.

The following lemma due to Diop and Yode [4] which is vital for our proof of Theo-rem2.2.

Lemma 2.1 Let{}ε>0be a sequence of continuous functions on R and K0 be a convex

function which admits a unique minimum ηon R.Let{}ε>0be a sequence of positive numbers such that Lε→+∞asε→0.We suppose that

lim

ε→0|usup|≤L

ε

(u) –K0(u)= 0.

Then

lim

ε→0arg min|u|≤

(u) =η,

where if there are several minima of Kε,we choose one of them arbitrarily.

Proof of Theorem2.2 We introduce the following notations:

(u) =ρ

Y,1

ε

x(θ0+εu) –x(θ0)

,

K0(u) =ρY,ux˙(θ0)

.

Since

(u) –K0(u)=

inf

μΛ([0,T])

H(μ) +

1

ε

x(θ0+εu) –x(θ0)

– inf

μΛ([0,T])

(6)

= inf

μΛ([0,T])

H(μ) +ux˙(θ0) –

1 2εu

2x¨(θ)

)

– inf

μΛ([0,T])

H(μ) +ux˙(θ0)

withθ=θε,u,t∈(θ0,θ0+εu), where the second equality is because of the Taylor expansion.

If we take=εδ–1withδ∈(1/2, 1), we get

sup

|u|≤

(u) –K0(u)=

inf

μΛ([0,T])

H(μ) +ux˙(θ0) –

1 2εu

2x¨(θ)

– inf

μΛ([0,T])

H(μ) +ux˙(θ0)

≤ sup

|u|≤ 1 2εu

2 sup 0≤tT¨

x(θ)

εL2ε

2 |x0|T

2e(|θ0|+εLε)T

= ε

2δ–1

2 |x0|T

2e(|θ0|+εLε)T0 (ε0).

Therefore, we get the desired results by Lemma2.1.

In the following, we will consider the limiting behavior ofηTforT→+∞. Let us

intro-duce the following notations:

At=

+∞

t

eθ0sdLd

s,

Bt=

t

0

eθ0sdLd s.

From Theorem 3.6.6 of Jurek and Mason [13] and Lemma 4 of Diop and Yode [4], we can get the logarithmic moment condition is necessary and sufficient for the existence of the improper integralA0.

Lemma 2.2 Suppose that E(log(1 +|L1|)) < +∞.Then

At=deθ0sA0 (17)

where “=d” denotes “identical distribution”.

Proof It is not hard to see,

At=

+∞

t

eθ0sdLd

s=

+∞

t

Ideθ0u(s)dL(s)

=

+∞

t

1

Γ(d)

s

eθ0u(us)d–1du

dL(s)

=

+∞

t

1

Γ(d)

0

eθ0(s+x)xd–1dx

dL(s)

=

+∞

t

1

Γ(d)e

θ0sθd 0

s

eθ0x(θ0x)d–1d(θ0x)

dL(s)

=θ0d

+∞

t

(7)

In a similar way,

A0=θ0d

+∞

0

eθ0sdL(s).

From Lemma 4 of Diop and Yode [4], we have immediately

At d

=eθ0sA0.

The next theorem gives the asymptotic behavior of the limit distributionηTfor largeT.

Theorem 2.3 Suppose thatθ0> 0and E(log(1 +|L1|)) < +∞.ThenξT=x0TηTconverges

in distribution to A0as T→+∞.

Proof Recall that

ηT=arg min u

Y(θ0),ux˙(θ0)

.

By changing variable, we have

ξT=arg min ω

Y(θ0),Mt(ω)

:=arg min

ωRN(ω), (18)

whereMt(ω) =ωte

θ0t

T andN(·) =ρ(Y(θ0),M(·)).

We want to show that, for every> 0,

lim T→+∞0

|ξTA0|>

= 0. (19)

Therefore, let us consider the set

V=

ω:|ωA0|>,

where0is the probability measure induced by the processXtwhenθ0is the true

param-eter andε→0. We can get

N(A0) =ρY(θ0),M(A0)

Y(θ0) –M(A0)

=0t

t

0

eθ0sdLd

s

A0t

TA0+A0

=0t

t

0

eθ0sdLd

sA0+

1 – t

T

A0

=0t

t

0

eθ0sdLd sA0

+|A0t|

1 – t

T

0t

.

On the other hand, forωV, we have

N(ω) =ρY(θ0),M(ω)

ρM(A0),M(ω)–ρY(θ0),M(A0)

(8)

=M(ω) –M(A0)N(A0)

=|ωA0|

teθ0t

T

N(A0)

te

θ0t

T

N(A0).

Hence, we have

N(ω)

N(A0)≥

teTθ0tN(A0) – 1,

infωVN(ω)

N(A0) ≥

Teθ0t(t 0e

θ0sdLd

sA0)∞

teθ0t +

|A0|(Tt)0t

teθ0t

–1

– 1

= Te

θ0t(B

tA0)∞

teθ0t +

|R0|(Tt)0t

teθ0t

–1

– 1

= eθ0Teθ0tA t+ |

A0| 0e

–1

– 1,

where we get the maximum value of the function (Tt)0tby taking the derivative.

We obtain

|A0|

0e→0 a.s. asT→+∞. (20)

Using Lemma2.2we have

0

eθ0Teθ0tA

t>

=0

|A0|>0Teθ0TEθ0(|A0|)

→0, T→+∞. (21)

By (20) and (21), we obtain

infωVN(ω)

N(A0)

P

−→+∞, T→+∞. (22)

In addition, using (18),ξTV, we have

N(ξT) = inf ωV

N(ω)≤N(A0). (23)

We can get the desired result (19) by Eqs. (22) and (23).

3 MinimumL1-norm estimation

In this section, we will study the minimumL1-norm estimationθεof the drift parameterθ.

Let

DT(θ) =

T

0

Xtxt(θ)dt. (24)

It is well known thatθε is the minimumL1-norm estimator if there exists a measurable

selectionθεsuch that

DT(θε) = inf

(9)

Suppose that there exists a measurable selectionθεsatisfying the above equation. We can

also define the estimatorθεby the relation

θε=arg inf θΘ

T

0

Xtxt(θ)dt. (26)

For anyκ> 0, we define

f(κ) = inf

|θθ0|>κ

T

0

Xt(θ) –xt(θ0)dt> 0, for anyκ> 0. (27)

Theorem 3.1(Consistency) For any p≥2,there exists a constant Cp,κ,d(only depending

the p,κ,d),such that,for everyκ> 0,we have

P(θε0)

|θεθ0|>κ

Cp,κ,dEL(1) p

Tp(d+1/2+κ)

2εe|θ0|T

f(κ) p

=Of(κ)–pεp. (28)

Proof Set · denotes theL1-norm, then we have

P(θε0)

|θεθ0|>κ

=(ε0)

inf

|θθ0|≤κ

Xx(θ)> inf

|θθ0|>κ

Xx(θ)

Pθ(ε0)

inf

|θθ0|≤κ

Xx(θ0)+x(θ) –x(θ0)

> inf

|θθ0|>κ

x(θ) –x(θ0)–Xx(θ0)

=(ε0)

2Xx(θ)> inf

|θθ0|>κ

x(θ) –x(θ0)

=(ε0)

Xx(θ)>1 2f(κ)

.

Since the processXtsatisfies the stochastic differential equation (1), it follows that

Xtxt(θ0) =x0+θ0

t

0

Xsds+εLdtxt(θ0) =θ0

t

0

Xsxs(θ0)

ds+εLdt, (29)

wherext(θ) =x0eθt.

Similar to the proof of Theorem2.1, we have

sup

0≤tT

Xtxt(θ0)≤εe|θ0T| sup 0≤tT

Ldt. (30)

Thus,

P(θε0)

Xx(θ)>1 2f(κ)

P

sup

0≤tT

Ldtf(κ)

2εe|θ0T|

. (31)

Applying Lemma1.3to the estimate obtained above, we have

P(θε0)

|θεθ0|>κ

E

sup

0≤tT

Ldtp

2εe|θ0T|

(10)

Cp,κ,dEL(1) p

Tp(d+1/2+κ)2pe|θ0T|pf(κ)pεp

=Of(κ)–pεp.

This completes the proof.

Remark3.1 It follows from Theorem3.1that we haveθε converges in probability toθ0

underP(θε0)-measure asε→0. Furthermore, the rate of convergence is of orderO(ε

p) for

everyp≥2.

Theorem 3.2(Limit distribution) Asε→0,ε–1(θ

εθ0)

d

ξ,ξ has the same probability distribution asηunder P(θε0)

η=arg inf

–∞<u<+∞

T

0

Yt(θ) –utx0eθ0tdt. (32)

Proof Let

(u) =Yε–1

x(θ0+εu) –x(θ0) (33)

and

Z0(u) =Yux˙(θ0). (34)

Furthermore, let

=

ω:|θεθ0|<δε

, δε=εττ,τ

1 2, 1

, =ετ–1. (35)

It is easy to see that the random variable=ε–1(θεθ0) satisfies the equation

() = inf

|u|<

(u), ω. (36)

Define

ηε=arg inf

|u|<

Z0(u). (37)

Observe that, with probability one,

sup

|u|<

Zε(u) –Z0(u)=Yux˙(θ0) – 1/2εu2x¨(θ)–Yux˙(θ0)

ε 2L

2

ε sup

|θθ0|<δε

T

0

x¨(θ)dt2τ–1→0, ε→0, (38)

whereθ=θ0+α(θθ0) for someα∈(0, 1]. Note that the last term in the above inequality

tends to zero asε→0. This follows from the arguments given in Theorem 2 of Kutoyants and Pilibossian [14,15]. In addition, we can choose the interval [–L,L] such that

P(θε0)

uε∈(–L,L)

(11)

and

Pu∗∈(–L,L)≥1 –βf(L)–p, β> 0. (40)

Note thatf(L) increases asLincreases. The process{(u),u∈[–L,L]}and{Z0(u),u

[–L,L]}satisfy the Lipschitz conditions and(u) converges uniformly toZ0(u) overu

[–L,L]. Hence the minimizer of(·) converges to the minimizer ofZ0(u). This completes

the proof.

Although the distribution ofη is not clear, we can consider its limiting behaviors as

T→+∞.

Theorem 3.3(Asymptotic law) Suppose thatθ0> 0and E(log(1 +|L1|)) < +∞.Then

ξT=x0TηT d

A0, T→+∞,

where L1,A0and other notations in the following are the same as Theorem2.3.

Proof Recall that

ηT=arg inf uR

T

0

Yt(θ0) –utx0eθ0tdt.

Let · denote theL1-norm. By changing variable, we have the following:

ξT=arg inf ωR

YM(ω):=arg inf

ωRN(ω), (41)

whereMt(ω) =ωte

θ0t

T andN(·) =YM(·).

We want to show that, for every> 0,

lim T→+∞0

|ξTA0|>

= 0. (42)

Therefore, we consider the set

V=

ω:|ωA0|>,

where0is the probability measure induced by the processXtwhenθ0is the true

param-eter andε→0. Besides, we have

N(A0) =YN(A0)

=0t

t

0

eθ0sdLd

s

A0t

TA0+A0

=0t

t

0

eθ0sdLd

sA0+

1 – t

T

A0

=0t

t

0

eθ0sdLd

sA0

+|A0t|

1 – t

T

(12)

On the other hand, forωV, we can get

N(ω) =YM(ω)

M(A0) –M(ω)–YM(A0)

=M(ω) –M(A0)–N(A0)

=|ωR0|te

θ0t

T

N(A0)

te

θ0t

T

N(A0).

Obviously, we have

N(ω)

N(A0)≥

teTθ0t

N(A0) – 1,

infωVN(ω)

N(A0)

Te

θ0t(t 0e

θ0sdMd

sA0)

teθ0t +

|A0|(Tt)0t

teθ0t

–1

– 1

= Te

θ0t(B

tA0)

teθ0t +

|A0|(Tt)0t

teθ0t

–1

– 1

=(I1+I2)–1– 1,

with

I1=Te

θ0t(B

tA0)

teθ0t =

Teθ0tA

t

T

0 teθ0tdt

= Te

θ0tA

t

θ0–1Teθ0Tθ–2

0 0T+θ0–2

,

I2=

|A0|(Tt)0t

teθ0t =

|A0|0Teθ0tdt

T

0 teθ0tdt

=|A0|(θ

–2

0 0Tθ0T–θ0–2) θ–1

0 Teθ0Tθ0–20T+θ0–2

.

We obtain with probability one

lim

T→+∞I2=Tlim→+∞

|A0|(θ0–20Tθ0Tθ0–2) θ0–1Teθ0Tθ–2

0 0T+θ0–2

= lim T→+∞

|A0|θ–2 0 0T

θ0–1Teθ0T =T→+∞lim

|A0|

θ0T = 0. (43)

Moreover, using Lemma2.2we obtain

lim

T→+∞0(I1>) = lim

T→+∞0

Teθ0tR

t

θ0–1Teθ0Tθ–2

0 0T+θ0–2

>

= lim T→+∞0

Teθ0tR

t

θ–1 0 Teθ0T

>

= lim T→+∞0

|R0|>θ0eθ0Tlim

T→+∞θ

–1 0 e

θ0TEθ0(|R0|)

(13)

By (43) and (44), we obtain asT→+∞

infωVN(ω)

N(A0)

P

→+∞. (45)

Using (41),ξTVimplies

N(ξT) = inf ωV

N(ω)≤N(A0). (46)

Therefore, from Eqs. (45) and (46), we have the result (42).

Remark3.2 IfLd

t is a Brownian motion, thenξTis asymptotically Gaussian, this is treated

by Kutoyants and Pilibossian [14,15].

Acknowledgements

The authors are grateful to the referee for carefully reading the manuscript and for providing some comments and suggestions which led to improvements in this paper.

Funding

This research is supported by the Distinguished Young Scholars Foundation of Anhui Province (1608085J06), the National Natural Science Foundation of China (11271020, 11601260), the Top Talent Project of University Discipline (Speciality) (gxbjZD03), the Natural Science Foundation of Chuzhou University (2016QD13), and Natural Science Foundation of Shandong Province (ZR2016AB01).

Competing interests

The authors declare that they have no competing interests.

Authors’ contributions

All authors contributed equally to this work. All authors read and approved the final manuscript.

Author details

1School of Mathematics and Finance, Chuzhou University, Chuzhou, China.2Department of Statistics, Anhui Normal

University, Wuhu, China. 3School of Statistics, Qufu Normal University, Qufu, China.

Publisher’s Note

Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Received: 11 September 2018 Accepted: 18 December 2018

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