
Using the GARCH-MIDAS model, we investigated the impact of Chinese and global macro-level determinants on the return volatility of Shanghai crude oil futures, covering Chinese and global economic policy uncertainty, Chinese and global crude oil demand as well as production, Chinese crude oil import, and global crude oil speculation. The in-sample empirical results showed that Chinese crude oil demand, Chinese crude oil production, Chinese economic policy uncertainty, and global crude oil speculation have significant impact on the long-term volatility component of Shanghai crude oil futures. The out-of-sample prediction results show that Chinese current crude oil production and previous crude oil import have the relatively best predictive power for the return volatility of Shanghai crude oil futures. As a whole, Chinese domestic macro-factors have a stronger impact and higher predictive power on the return volatility of Shanghai crude oil futures compared with corresponding global macro-factors. Besides, the global crude oil speculation is the global macro-level determinant, which deserves most attention.
Citation: Xiaoling Yu, Kaitian Xiao, Javier Cifuentes-Faura. Closer is more important: The impact of Chinese and global macro-level determinants on Shanghai crude oil futures volatility[J]. Quantitative Finance and Economics, 2024, 8(3): 573-609. doi: 10.3934/QFE.2024022
[1] | Haiquan Wang, Hans-Dietrich Haasis, Menghao Su, Jianhua Wei, Xiaobin Xu, Shengjun Wen, Juntao Li, Wenxuan Yue . Improved artificial bee colony algorithm for air freight station scheduling. Mathematical Biosciences and Engineering, 2022, 19(12): 13007-13027. doi: 10.3934/mbe.2022607 |
[2] | Yutao Lai, Hongyan Chen, Fangqing Gu . A multitask optimization algorithm based on elite individual transfer. Mathematical Biosciences and Engineering, 2023, 20(5): 8261-8278. doi: 10.3934/mbe.2023360 |
[3] | Rami AL-HAJJ, Mohamad M. Fouad, Mustafa Zeki . Evolutionary optimization framework to train multilayer perceptrons for engineering applications. Mathematical Biosciences and Engineering, 2024, 21(2): 2970-2990. doi: 10.3934/mbe.2024132 |
[4] | Shijing Ma, Yunhe Wang, Shouwei Zhang . Modified chemical reaction optimization and its application in engineering problems. Mathematical Biosciences and Engineering, 2021, 18(6): 7143-7160. doi: 10.3934/mbe.2021354 |
[5] | Qing Wu, Chunjiang Zhang, Mengya Zhang, Fajun Yang, Liang Gao . A modified comprehensive learning particle swarm optimizer and its application in cylindricity error evaluation problem. Mathematical Biosciences and Engineering, 2019, 16(3): 1190-1209. doi: 10.3934/mbe.2019057 |
[6] | Zhenao Yu, Peng Duan, Leilei Meng, Yuyan Han, Fan Ye . Multi-objective path planning for mobile robot with an improved artificial bee colony algorithm. Mathematical Biosciences and Engineering, 2023, 20(2): 2501-2529. doi: 10.3934/mbe.2023117 |
[7] | Junhua Liu, Wei Zhang, Mengnan Tian, Hong Ji, Baobao Liu . A double association-based evolutionary algorithm for many-objective optimization. Mathematical Biosciences and Engineering, 2023, 20(9): 17324-17355. doi: 10.3934/mbe.2023771 |
[8] | Wenqiang Zhang, Chen Li, Mitsuo Gen, Weidong Yang, Zhongwei Zhang, Guohui Zhang . Multiobjective particle swarm optimization with direction search and differential evolution for distributed flow-shop scheduling problem. Mathematical Biosciences and Engineering, 2022, 19(9): 8833-8865. doi: 10.3934/mbe.2022410 |
[9] | Yijie Zhang, Yuhang Cai . Adaptive dynamic self-learning grey wolf optimization algorithm for solving global optimization problems and engineering problems. Mathematical Biosciences and Engineering, 2024, 21(3): 3910-3943. doi: 10.3934/mbe.2024174 |
[10] | Jian Si, Xiaoguang Bao . A novel parallel ant colony optimization algorithm for mobile robot path planning. Mathematical Biosciences and Engineering, 2024, 21(2): 2568-2586. doi: 10.3934/mbe.2024113 |
Using the GARCH-MIDAS model, we investigated the impact of Chinese and global macro-level determinants on the return volatility of Shanghai crude oil futures, covering Chinese and global economic policy uncertainty, Chinese and global crude oil demand as well as production, Chinese crude oil import, and global crude oil speculation. The in-sample empirical results showed that Chinese crude oil demand, Chinese crude oil production, Chinese economic policy uncertainty, and global crude oil speculation have significant impact on the long-term volatility component of Shanghai crude oil futures. The out-of-sample prediction results show that Chinese current crude oil production and previous crude oil import have the relatively best predictive power for the return volatility of Shanghai crude oil futures. As a whole, Chinese domestic macro-factors have a stronger impact and higher predictive power on the return volatility of Shanghai crude oil futures compared with corresponding global macro-factors. Besides, the global crude oil speculation is the global macro-level determinant, which deserves most attention.
Special polynomials play a significantly important role in the development of several branches of mathematics, engineering, and physics by providing us with useful identities and properties. The study of special polynomials provides many useful identities, their relations, and representations associated with special numbers and polynomials. One of the powerful tools in this study is to investigate their generating functions [1,2] and connections[3,4,5,6] using the umbral calculus [7]. Furthermore, to better understand generating functions in special polynomials, the degenerate type of special polynomials has been extensively studied in many areas such as probability theory, fuzzy theory, connection problems, and other combinatorial theories in recent years by many mathematicians [8,9,10,11]. Since the introduction of degenerate versions of special polynomials and numbers by Carlitz [12], many researchers have been interested in the relationships between them. In addition, the degenerate version of umbral calculus, called λ-umbral calculus, plays a very powerful role in studying the relationships between degenerate versions of special polynomials and numbers. Recently, the Daehee polynomials and numbers were originally introduced as a new type of special polynomials by Kim and Kim [13] and thereafter their related properties and relationships with other polynomials have been extensively studied.
In this study, we derive the formulas expressing degenerate higher-order Daehee polynomials in terms of the degenerate versions of other special polynomials by making use of λ-umbral calculus. These formulas provide the degenerate Daehee polynomials by taking r=1 and the Daehee polynomials by letting λ→0. We first review the λ-analogue of umbral calculus: a class of λ-linear functionals on the polynomials, λ-differential operators based on the family of λ-linear functionals, and also λ-Sheffer sequences. See [14] and the references therein for more details on these contents.
The rest of this section briefly recalls some necessary notations and definitions that are needed throughout this paper. Throughout this paper, we assume that λ∈R∖{0} for simplicity.
The degenerate exponential function exλ(t) is defined by
exλ(t):=(1+λt)xλ=∞∑n=0(x)n,λtnn!,eλ(t):=e1λ(t)=∞∑n=0(1)n,λtnn!, (see [10, 13, 15, 16]), | (1.1) |
where (x)n,λ is a λ-analogue of the falling factorial sequence which is given by
(x)n,λ=x(x−λ)⋯(x−(n−1)λ) for n≥1 and (x)0,λ=1, (see [14, 17]). | (1.2) |
Also, the degenerate logarithm function is given by logλ(t):=1λ(tλ−1), which is the compositional inverse of eλ(t), i.e.,
logλ(eλ(t))=eλ(logλ(t))=t. |
In this study, we consider the degenerate higher-order Daehee polynomials D(r)n,λ(x) which are given by the generating function to be
(logλ(1+t)t)r(1+t)x=∞∑n=0D(r)n,λ(x)tnn!,r∈N, (see [10, 15, 16]). | (1.3) |
Especially, we call Dn,λ(x):=D(1)n,λ(x) the degenerate Daehee polynomials when r=1 and Dn,λ:=Dn,λ(0) the degenerate Daehee numbers when x=0.
The degenerate Stirling numbers of the first kind S1,λ(n,m) and the second kind S2,λ(n,m) are respectively given by
1m!(logλ(1+t))m=∞∑n=mS1,λ(n,m)tnn!,(m≥0), (see [9, 18]) | (1.4) |
and
1m!(eλ(t)−1)m=∞∑n=mS2,λ(n,m)tnn!,(m≥0), (see [9, 18]). | (1.5) |
Note that the falling factorial sequence (t)n is given by
(t)n={t(t−1)(t−2)⋯(t−(n−1)) for n≥1,(t)0=1 when n=0, (see [19]), |
which provides the relation with the λ-analogue of the falling factorial sequence such as
(t)n,λ=n∑m=0S2,λ(n,m)(t)m,(n≥0). |
The main contribution of this paper is to provide various representations of the degenerate higher-order Daehee polynomials and numbers using λ-umbral calculus in terms of other well-known special polynomials and numbers. In more detail, we derive formulas for the n-th order of degenerate Daehee polynomials with the degenerate falling factorial polynomials, the degenerate type 2 Bernoulli polynomials, the degenerate Bernoulli polynomials, the degenerate Euler polynomials, the degenerate Mittag-Leffer polynomials, the degenerate Bell polynomials, and the degenerate Frobenius-Euler polynomials (see Theorems 2.1–2.7) as well as their inversion formulas. Therefore, we see that this technique enables us to represent various well-known polynomials in terms of degenerate higher-order Daehee polynomials and vice versa as a classical connection problem. In addition, to confirm the formulas, we present computational results between the degenerate higher-order Daehee polynomials and the degenerate Bernoulli polynomials for fixed variables. Moreover, we investigate the pattern of the root distribution of the polynomials.
Now, we provide brief review of λ-umbral calculus: Let P be the algebra of polynomials in t over C, i.e.,
P=C[t]={∞∑n=0antn|an∈C with an=0 for all but finite number of n}. |
and let F be the algebra of formal power series in t over the field C of complex numbers
F={f(t)=∞∑n=0antnn!|an∈C}. |
Then, the λ-linear functional ⟨f(t)|⋅⟩λ on P for f(t)=∑∞n=0antnn!∈F is given by
⟨f(t)|(x)n,λ⟩λ=an,(n≥0), (see [14]), | (2.1) |
and it satisfies
⟨tk|(x)n,λ⟩λ=n!δn,k, (see [14]), | (2.2) |
where δn,k is the Kronecker delta.
Note that the order of the formal power series for a nontrivial f(t), o(f(t)), is represented by the smallest integer k for which ak does not vanish. Especially, we call f(t) a delta series when o(f(t))=1, and also we say f(t) an invertible series when o(f(t))=0, (see [1,7,14] for details).
For a non-negative integer order k, the λ-differential operator (tk)λ on P is defined by
(tk)λ(x)n,λ={(n)k(x)n−k,λ if 0≤k≤n,0, if k>n, (see [14, 20]). | (2.3) |
In general, for f(t)=∑∞k=0aktkk!∈F, the λ-differential operator (f(t))λ is satisfied with
(f(t))λ(x)n,λ=n∑k=0(nk)ak(x)n−k,λ. | (2.4) |
Or equivalently, one can express (f(t))λ as
(f(t))λ=∞∑k=0akk!(tk)λ. |
For a delta series f(t) and an invertible series g(t), i.e., o(f(t))=1 and o(g(t))=0, there exists a unique sequence pn,λ(x) of polynomials deg(pn,λ(x))=n satisfying the orthogonality condition
⟨g(t)(f(t))k|pn,λ(x)⟩λ=n!δn,k,(n,k≥0). | (2.5) |
Here, pn,λ(x) is called the λ-Sheffer sequence for (g(t),f(t)) denoted by pn,λ(x)∼(g(t),f(t))λ.
We recall that pn,λ(x)∼(g(t),f(t))λ if and only if
1g(ˉf(t))exλ(ˉf(t))=∞∑n=0pn,λ(x)tnn!,(see [7, 20]). | (2.6) |
Here ˉf(t) represents the compositional inverse of f(t), i.e., f(ˉf(t))=ˉf(f(t))=t.
For given a pair of λ-Sheffer sequences pn,λ(x)∼(g(t),f(t))λ and qn,λ(x)∼(h(t),ℓ(t))λ, we have the relation:
pn,λ(x)=n∑k=0μn,kqk,λ(x), | (2.7) |
where μn,k is obtained by
μn,k=1k!⟨h(ˉf(t))g(ˉf(t))(ℓ(ˉf(t)))k|(x)n,λ⟩λ. |
Likewise, if qn,λ(x) is expressed in terms of pn,λ(x) as
qn,λ(x)=n∑k=0νn,kpk,λ(x), | (2.8) |
then νn,k can be obtained by
νn,k=1k!⟨g(ˉℓ(t))h(ˉℓ(t))(f(ˉℓ(t)))k|(x)n,λ⟩λ. |
It is easily shown that for f(t),g(t)∈F and p(x)∈P,
⟨f(t)g(t)|p(x)⟩λ=⟨g(t)|(f(t))λp(x)⟩λ=⟨f(t)|(g(t))λp(x)⟩λ,(see [14]). |
We also note that from (x)n,λ∼(1,t)λ, any λ-Sheffer sequence pn,λ(x)∼(g(t),f(t))λ is represented by
pn,λ(x)=n∑k=01k!⟨1g(ˉf(t))(ˉf(t))k|(x)n,λ⟩λ(x)k,λ. | (2.9) |
Now, we want to present representations of the degenerate higher-order Daehee polynomials D(r)n,λ(x) by using the algebraic properties of λ-Sheffer sequences.
From (1.3), we have that ∑∞n=0D(r)n,λ(x)tnn!=(logλ(1+t)t)rexλ(logλ(1+t)), so that we consider f(t)=eλ(t)−1,ˉf(t)=logλ(1+t), and g(t)=eλ(t)−1t in the view of (2.6) to obtain
D(r)n,λ(x)∼((eλ(t)−1t)r,eλ(t)−1)λ. | (2.10) |
If we let pn,λ(x)=∑nℓ=0μℓD(r)ℓ,λ(x), then, by using (2.5) we have
⟨(eλ(t)−1t)r(eλ(t)−1)k|pn,λ(x)⟩λ=n∑ℓ=0μℓ⟨(eλ(t)−1t)r(eλ(t)−1)k|D(r)ℓ,λ(x)⟩λ=n∑ℓ=0μℓℓ!δk,ℓ=k!μk, |
which implies
μk=1k!⟨(eλ(t)−1t)r(eλ(t)−1)k|pn,λ(x)⟩λ. |
Thus, for pn,λ(x)∈P we have
pn,λ(x)=n∑k=01k!⟨(eλ(t)−1t)r(eλ(t)−1)k|pn,λ(x)⟩λD(r)k,λ(x). |
Then, the formula between D(r)n,λ(x) and (x)n,λ is obtained.
Theorem 2.1. For n∈N∪{0} and r∈N, we have
D(r)n,λ(x)=n∑k=0(n∑ℓ=k(nℓ)S1,λ(ℓ,k)D(r)n−ℓ,λ)(x)k,λ. |
Reversely, we have the inversion formula given by
(x)n,λ=n∑k=0(n∑ℓ=kr∑j=0(nℓ)(rj)(−1)r−jS2,λ(ℓ,k)(j)n+r−ℓ,λ(n−ℓ+r)r)D(r)k,λ(x). |
Proof. Let D(r)n,λ(x)=∑nk=0μn,k(x)k,λ. Then, by (1.4), (2.3), and (2.9), we can obtain
μn,k=1k!⟨(logλ(1+t)t)r(logλ(1+t))k|(x)n,λ⟩λ=⟨(logλ(1+t)t)r|(1k!(logλ(1+t))k)λ(x)n,λ⟩λ=1ℓ!∞∑ℓ=kS1,λ(ℓ,k)⟨(logλ(1+t)t)r|(tℓ)λ(x)n,λ⟩λ=n∑ℓ=k(nℓ)S1,λ(ℓ,k)⟨(logλ(1+t)t)r|(x)n−ℓ,λ⟩λ=n∑ℓ=k(nℓ)S1,λ(ℓ,k)D(r)n−ℓ,λ, |
which shows the first formula.
For the inversion formula, we first note that
(eλ(t)−1t)r=r∑j=0(rj)(−1)r−j∞∑m=0(j)m,λtm−rm!, |
which implies
⟨(eλ(t)−1t)r|(x)n−ℓ,λ⟩λ=r∑j=0(rj)(−1)r−j(j)n+r−ℓ,λ(n−ℓ)!(n−ℓ+r)!=r∑j=0(rj)(−1)r−j(j)n+r−ℓ,λ1(n−ℓ+r)r. | (2.11) |
Now, let (x)n,λ=∑∞k=0νn,kD(r)k,λ(x). Then, from (1.5), (2.7), and (2.11), νk satisfies
νn,k=1k!⟨(eλ(t)−1t)r(eλ(t)−1)k|(x)n,λ⟩λ=⟨(eλ(t)−1t)r|(1k!(eλ(t)−1)k)λ(x)n,λ⟩λ=n∑ℓ=k(nℓ)S2,λ(ℓ,k)⟨(eλ(t)−1t)r|(x)n−ℓ,λ⟩λ=n∑ℓ=k(nℓ)r∑j=0(rj)(−1)r−jS2,λ(ℓ,k)(j)n+r−ℓ,λ(n−ℓ+r)r, |
which shows the second result.
Next, we consider the degenerate Bernoulli polynomials βn,λ(x), which is defined by the generating function to be
teλ(t)−1exλ(t)=∞∑n=0βn,λ(x)tnn!, (see [21]). |
Then, the connection formulas between D(r)n,λ(x) and βn,λ(x) are as follows.
Theorem 2.2. For n∈N∪{0}, we have
D(r)n,λ(x)=n∑k=0(k+r−1)r−1(n+r−1)r−1S1,λ(n+r−1,k+r−1)βk,λforr∈N. |
As the inversion formula, we have
βn,λ(x)=n∑k=0(n∑ℓ=kr−1∑j=0(nℓ)(r−1j)(−1)r−1−j(j)n−ℓ+r−1,λ(n−ℓ+r−1)r−1S2,λ(ℓ,k))D(r)k,λ(x)forr>1, |
and
βn,λ(x)=n∑k=0S2,λ(n,k)Dk,λ(x)forr=1. |
Proof. First, note that βn,λ(x) is the λ-Sheffer sequence for
βn,λ(x)∼(eλ(t)−1t,t)λ. | (2.12) |
Let us consider D(r)ℓ,λ(x)=n∑k=0μn,kβk,λ(x). By (1.4), (2.9), (2.10) and (2.12), we obtain
μn,k=1k!⟨tlogλ(1+t)(tlogλ(1+t))r(logλ(1+t))k|(x)n,λ⟩λ=1k!⟨t1−r(logλ(1+t))k+r−1|(x)n,λ⟩λ=⟨k+1⟩r−1(k+r−1)!⟨t1−r(logλ(1+t))k+r−1|(x)n,λ⟩λ=(k+r−1)r−1(n+r−1)r−1S1,λ(n+r−1,k+r−1), |
which implies the first formula.
To find the inversion formula, we first note that from (1.1) for r>1
(eλ(t)−1t)r−1=t1−rr−1∑j=0(r−1j)(−1)r−1−jejλ(t)=r−1∑j=0(r−1j)(−1)r−1−j∞∑m=0(j)m,λtm+1−rm!. | (2.13) |
Thus, by (2.2) and (2.13)
⟨(eλ(t)−1t)r−1|(x)n−ℓ,λ⟩λ=r−1∑j=0(r−1j)(−1)r−1−j(j)n−ℓ+r−1,λ(n−ℓ)!(n−ℓ+r−1)!={r−1∑j=0(r−1j)(−1)r−1−j(j)n−ℓ+r−1,λ(n−ℓ+r−1)r−1 if r>1,δn,ℓ if r=1. | (2.14) |
Now, if we consider βn,λ(x)=∞∑k=0νn,kD(r)k,λ(x), then by (1.5), (2.7), and (2.14), νn,k satisfies
νn,k=1k!⟨(eλ(t)−1t)reλ(t)−1t(eλ(t)−1)k|(x)n,λ⟩λ=n∑ℓ=k(nℓ)S2,λ(ℓ,k)⟨(eλ(t)−1t)r−1|(x)n−ℓ,λ⟩λ={n∑ℓ=k(nℓ)S2,λ(ℓ,k)r−1∑j=0(r−1j)(−1)r−1−j(j)n−ℓ+r−1,λ(n−ℓ+r−1)r−1 if r>1,S2,λ(n,k) if r=1, |
which provides the formula.
Next, we consider the degenerate type 2 Bernoulli polynomials bn,λ(x), which are defined by the generating functions to be
teλ(t)−e−1λ(t)exλ(t)=∞∑n=0bn,λ(x)tnn!, (see [22]). |
Note that bn,λ(x) satisfies
bn,λ(x)∼(eλ(t)−e−1λ(t)t,t)λ. | (2.15) |
Then, we can have the following relation between D(r)n,λ(x) and bn,λ(x).
Theorem 2.3. For n∈N∪{0} and r∈N, we have
D(r)n,λ(x)={n∑k=0n∑m=k(nm)S1,λ(m,k)(D(r−1)n−m,λ+n−m∑ℓ=0(−1)ℓ(n−m)ℓD(r−1)n−m−ℓ,λ)bk,λforr>1.S1,λ(n,k)+n∑m=k(nm)S1,λ(m,k)(−1)n−m(n−m)n−mforr=1. |
For the inversion formula, we have
bn,λ(x)=12n∑k=0(n∑ℓ=kr−1∑j=0n+r−1∑m=0(nℓ)(r−1j)(n+r−1m)S2,λ(ℓ,k)(−1)r−1−j(j)m,λ(n+r−1)r−1×En+r−1−m,λ(12))D(r)k,λ(x)forr>1 |
and
bn,λ(x)=12n∑k=0(n∑m=k(nm)S2,λ(m,k)En−m,λ(12))Dk,λ(x)forr=1. |
Proof. Let us consider D(r)n,λ(x)=∑nk=0μn,kbk,λ(x). By (1.4), (2.9), (2.10), and (2.15), we get
μn,k=1k!⟨1+t−11+tlogλ(1+t)(tlogλ(1+t))r(logλ(1+t))k|(x)n,λ⟩λ=⟨(t(t+2)t+1)(logλ(1+t)t)r1k!(logλ(1+t))k−1|(x)n,λ⟩λ=⟨(t+2t+1)(logλ(1+t)t)r−11k!(logλ(1+t))k|(x)n,λ⟩λ=n∑m=k(nm)S1,λ(m,k)⟨(logλ(1+t)t)r−1|(1+∞∑ℓ=0(−t)ℓ)λ(x)n−m,λ⟩λ. | (2.16) |
From (2.3), it is noted that
(1+∞∑ℓ=0(−t)ℓ)λ(x)n−m,λ=(x)n−m,λ+n−m∑ℓ=0(−1)ℓ(n−m)ℓ(x)n−m−ℓ,λ. | (2.17) |
By applying the note (2.17) in (2.16), we have
μn,k={n∑m=k(nm)S1,λ(m,k)(D(r−1)n−m,λ+n−m∑ℓ=0(−1)ℓ(n−m)ℓD(r−1)n−m−ℓ,λ) for r>1,S1,λ(n,k)+n∑m=k(nm)S1,λ(m,k)(−1)n−m(n−m)n−m for r=1. |
To find the inversion formula, let us consider bn,λ(x)=∑∞k=0νn,kD(r)k,λ(x). From (1.5), (2.7), and (2.15), νn,k satisfies
νn,k=1k!⟨(eλ(t)−1t)reλ(t)−e−1λ(t)t(logλ(t+1))k|(x)n,λ⟩λ=n∑ℓ=k(nℓ)S2,λ(ℓ,k)⟨eλ(t)eλ(t)+1(eλ(t)−1t)r−1|(x)n−ℓ,λ⟩λ=12n∑ℓ=k(nℓ)S2,λ(ℓ,k)⟨2e12λ(t)e12λ(t)+e−12λ(t)(eλ(t)−1t)r−1|(x)n−ℓ,λ⟩λ. | (2.18) |
Since exλ(t)−1t=∑∞n=0(x)n+1,λn+1tnn!, we have that for r>1
(eλ(t)−1t)r−1=t1−rr−1∑j=0(r−1j)ejλ(t)(−1)r−1−j=t1−rr−1∑j=0(r−1j)(−1)r−1−j∞∑m=0(j)m,λtmm!. | (2.19) |
Then, (2.19) implies that for r>1
2e12λ(t)e12λ(t)+e−12λ(t)(eλ(t)−1t)r−1=t1−rr−1∑j=0(r−1j)(−1)r−1−j(∞∑m=0(j)m,λtmm!)(∞∑k=0Ek,λ(12)tkk!)=t1−rr−1∑j=0(r−1j)(−1)r−1−j∞∑m=0m∑k=0(mk)(j)k,λEm−k,λ(12)tmm!=r−1∑j=0(r−1j)(−1)r−1−j∞∑m=0m∑k=0(mk)(j)k,λEm−k,λ(12)tm+1−rm!, | (2.20) |
where En,λ(x) are the type 2 degenerate Euler polynomials defined by the following generating function
2e12λ(t)+e−12λ(t)exλ(t)=∞∑n=0En,λ(x)tnn!,(see [23]). | (2.21) |
Here we call En,λ:=En,λ(0) the type 2 degenerate Euler numbers if x=0. Thus, for m=n−ℓ+r−1 in (2.20) for r>1
⟨2e12λ(t)e12λ(t)+e−12λ(t)(eλ(t)−1t)r−1|(x)n−ℓ,λ⟩λ=r−1∑j=0(r−1j)(−1)r−1−jn−ℓ+r−1∑k=0(n−ℓ+r−1k)(j)k,λ×En−ℓ+r−1−k,λ(12)n!(n+r−1)!=r−1∑j=0(r−1j)(−1)r−1−jn−ℓ+r−1∑k=0(n−ℓ+r−1k)(j)k,λ×En−ℓ+r−1−k,λ(12)1(n−ℓ+r−1)r−1, |
and
⟨2e12λ(t)e12λ(t)+e−12λ(t)|(x)n−ℓ,λ⟩λ=En−ℓ,λ(12) for r=1, |
which provides the inversion formula with (2.18).
We consider the degenerate Euler polynomials Ek,λ that is defined by the generating function to be
(2eλ(t)+1)exλ(t)=∞∑n=0En,λ(x)tnn!,(see [12, 21]), |
which satisfies that
En,λ(x)∼(eλ(t)+12,t)λ. | (2.22) |
Then, the representation formula between D(r)n,λ(x) and En,λ(x) holds true.
Theorem 2.4. For n∈N∪{0} and r∈N, we have
D(r)n,λ(x)=12n∑k=0(n∑ℓ=kS1,λ(ℓ,k)(nℓ)((n−ℓ)D(r)n−ℓ−1,λ+2D(r)n−ℓ,λ))Ek,λ(x). |
As the inversion formula, we have
En,λ(x)=n∑k=0(n∑ℓ=kr∑j=0n+r∑l=0(nℓ)(rj)(n+rl)S2,λ(ℓ,k)(−1)r−j(j)l,λ(n+r)rEn+r−l,λ)Dk,λ(x). |
Proof. Let D(r)n,λ(x)=∑nk=0μn,kEk,λ. Then, By (1.4), (2.9), (2.10), and (2.22), we can obtain
μn,k=1k!⟨(1+t)+12(tlogλ(1+t))r(logλ(1+t))k|(x)n,λ⟩λ=⟨t+22(logλ(1+t)t)r1k!(logλ(1+t))k|(x)n,λ⟩λ=12∞∑ℓ=k(nℓ)S1,λ(ℓ,k)⟨(t+2)(logλ(1+t)t)r|(x)n−ℓ,λ⟩λ, | (2.23) |
where
⟨t(logλ(1+t)t)r|(x)n−ℓ,λ⟩λ=⟨n∑k=0D(r)k,λtk+1k!|(x)n−ℓ,λ⟩λ=D(r)n−ℓ−1,λ(n−ℓ) | (2.24) |
and
⟨n∑k=0D(r)k,λtkk!|(x)n−ℓ,λ⟩λ=D(r)n−ℓ,λ. | (2.25) |
Therefore, combining (2.24) and (2.25) to (2.23), we have
μn,k=12n∑ℓ=k(nℓ)S1,λ(ℓ,k)((n−ℓ)D(r)n−ℓ−1,λ+2D(r)n−ℓ,λ). |
To find the inversion formula, let En,λ(x)=∑∞k=0νn,kD(r)k,λ(x), where νn,k satisfies
νn,k=1k!⟨(eλ(t)−1t)reλ(t)+12(eλ(t)−1)k|(x)n,λ⟩λ=n∑ℓ=k(nℓ)S2,λ(ℓ,k)⟨(eλ(t)−1t)r2eλ(t)+1|(x)n,λ⟩λ. | (2.26) |
We note that
(eλ(t)−1t)r=t−rr∑j=0(rj)ejλ(t)(−1)r−j=t−rr∑j=0(rj)(−1)r−j∞∑m=0(j)m,λtmm!=r∑j=0(rj)(−1)r−j∞∑m=0(j)m,λtm−rm! |
and
(eλ(t)−1t)r2eλ(t)+1=r∑j=0(rj)(−1)r−j∞∑m=0(m∑l=0(ml)(j)l,λEm−l,λ)tm−rm!. |
Thus,
⟨(eλ(t)−1t)r2eλ(t)+1|(x)n,λ⟩λ=r∑j=0(rj)(−1)r−jn+r∑l=0(n+rl)(j)l,λ(n+r)rEn+r−l,λ. | (2.27) |
Combining (2.27) to (2.26) gives
νn,k=n∑ℓ=kr∑j=0n+r∑l=0(nℓ)(rj)(n+rl)S2,λ(ℓ,k)(−1)r−j(j)l,λ(n+r)rEn+r−l,λ. |
The degenerate Mittag-Leffer polynomials Mn,λ(x) are given by the generating function to be
exλ(logλ(1+t1−t))=∞∑n=0Mn,λ(x)tnn!,(see [24]). |
It is noted that
Mn,λ(x)∼(1,eλ(t)−1eλ(t)+1)λ. | (2.28) |
Then, we have the representation formulas between D(r)n,λ(x) and Mn,λ(x).
Theorem 2.5. For n∈N∪{0} and r∈N, we have
D(r)n,λ(x)=n∑k=0(1k!n∑m=0D(r)m,λ(nm)(n−m−1n−m−k)(−1)n−m−k2n−m(n−m)!)Mk,λ. |
As the inversion formula, we have
Mn,λ(x)=∞∑k=0(n∑m=0n!k!m!Km(λ)2m+k+r−1)D(r)k,λ(x), |
where Kn(x|λ) are the Korobov polynomials of the first kind given by the generating function
λt(1+t)λ−1(1+t)x=∞∑n=0Kn(x|λ)tnn!,(see[25]). |
In particular, when x=0 Kn(λ):=Kn(0|λ) are called Korobov numbers of the first kind, that is,
tlogλ(1+t)=∞∑n=0Kn(λ)tnn!. |
Proof. Let D(r)ℓ,λ(x)=∑nk=0μn,kMk,λ. Then, by (1.4), (2.9), (2.10), and (2.28), we can obtain
μn,k=1k!⟨1((1+t)−1logλ(1+t))r(1+t−11+t+1)k|(x)n,λ⟩λ=1k!⟨(logλ(1+t)t)r(tt+2)k|(x)n,λ⟩λ=1k!n∑m=0D(r)m,λ(nm)⟨(tt+2)k|(x)n−m,λ⟩λ, |
where
⟨(tt+2)k|(x)n−m,λ⟩λ=⟨∞∑ℓ=0(−1)ℓ2k+ℓ(k+ℓ−1ℓ)tk+ℓ|(x)n−m,λ⟩λ=(−1)n−m−k2n−m(n−m−1n−m−k)(n−m)!. | (2.29) |
Thus,
μn,k=1k!n∑m=0D(r)m,λ(nm)(n−m−1n−m−k)(−1)n−m−k2n−m(n−m)!. |
To find the inversion formula, let Mn,λ(x)=∑∞k=0νn,kD(r)k,λ(x), where
νn,k=1k!⟨(1+t1−t−1)rlogλ(1+t1−t)(1+t1−t−1)k|(x)n,λ⟩λ=1k!⟨(1+t−(1−t)1−t)rlogλ(1+t1−t)(1+t−1+t1−t)k|(x)n,λ⟩λ=1k!⟨(2t1−t)rlogλ(1+t1−t)(2t1−t)k|(x)n,λ⟩λ=1k!n∑m=01m!Km(λ)⟨(2t1−t)m+k+r−1|(x)n,λ⟩λ, |
where
⟨(2t1−t)m+k+r−1|(x)n,λ⟩λ=2m+k+r−1⟨∞∑ℓ=0tℓ+m+k+r−1|(x)n,λ⟩λ=2m+k+r−1n!. |
Thus,
νn,k=1k!n∑m=0n!m!Km(λ)2m+k+r−1. |
Next, let us consider the degenerate Bell polynomials Beln,λ(x), which are defined by the generating function to be
ex(eλ(t)−1)λ=∞∑n=0Beln,λ(x)tnn!,(see [26, 27]). |
Note that Beln,λ(x) are the λ-Sheffer sequences of
Beln,λ(x)∼(1,logλ(1+t))λ, | (2.30) |
which satisfies that
Beln,λ(x)=n∑k=0S2,λ(n,k)(x)k,λ, (see [26]). |
Then, we have the representation formulas between D(r)n,λ(x) and Beln,λ(x).
Theorem 2.6. For n∈N∪{0} and r∈N, it holds:
D(r)n,λ(x)=n∑k=0(n∑m=kn∑ℓ=m(nℓ)S1,λ(m,k)S1,λ(ℓ,m)D(r)n−ℓ,λ)Belk,λ(x). |
Also the inversion formula are established
Beln,λ(x)=n∑k=0(n∑m=kn∑ℓ=0r∑j=0(rj)S2,λ(m,k)S2,λ(n,ℓ)(−1)r−jm!(j)ℓ+r−m,λ)D(r)k,λ(x). |
Proof. Let D(r)ℓ,λ(x)=∑nk=0μn,kBelk,λ(x). Then, by (1.4), (2.9), (2.10), and (2.30), we can obtain
μn,k=1k!⟨1((1+t)−1logλ(1+t))r(logλ(1+logλ(1+t)))k|(x)n,λ⟩λ=1k!⟨(logλ(1+t)t)r(logλ(1+logλ(1+t)))k|(x)n,λ⟩λ=⟨(logλ(1+t)t)r|((1k!logλ(1+logλ(1+t)))k)λ(x)n,λ⟩λ=n∑m=kS1,λ(m,k)n∑ℓ=m(nℓ)S1,λ(ℓ,m)⟨(logλ(1+t)t)r|(x)n−ℓ,λ⟩λ=n∑m=kn∑ℓ=m(nℓ)S1,λ(m,k)S1,λ(ℓ,m)D(r)n−ℓ,λ. |
To find the inversion formula, let Beln,λ(x)=∑nk=0νn,kD(r)k,λ(x), then νn,k satisfies
νn,k=1k!⟨(eλ(t)−1t)r(eλ(t)−1)k|Beln,λ(x)⟩λ=∞∑m=kS2,λ(m,k)⟨(eλ(t)−1t)rtmm!|n∑ℓ=0S2,λ(n,ℓ)(x)ℓ,λ⟩λ=n∑m=kS2,λ(m,k)n∑ℓ=0S2,λ(n,ℓ)⟨(eλ(t)−1t)rtmm!|(x)ℓ,λ⟩λ, |
where
⟨(eλ(t)−1t)rtmm!|(x)ℓ,λ⟩λ=⟨r∑j=0(rj)(−1)r−j∞∑l=0(j)l,λtl+m−rl!m!|(x)ℓ,λ⟩λ=r∑j=0(rj)(−1)r−j(j)ℓ+r−m,λ1m!. |
Therefore, we have
νn,k=n∑m=kn∑ℓ=0r∑j=0(rj)S2,λ(m,k)S2,λ(n,ℓ)(−1)r−jm!(j)ℓ+r−m,λ. |
The degenerate Frobenius-Euler polynomials h(α)n,λ(x|u) of order α are defined by the generating function as
(1−ueλ(t)−u)αexλ(t)=∞∑n=0h(α)n,λ(x|u)tnn!,u(≠1)∈C. |
When x=0, h(α)n,λ(u):=h(α)n,λ(0|u) are called the degenerate Frobenius-Euler numbers.
We note that h(α)n,λ(x|u) satisfy
h(α)n,λ(x|u)∼((eλ(t)−u1−u)α,t)λ. | (2.31) |
Then, we have the representation formulas between D(r)n,λ(x) and h(α)n,λ(x|u).
Theorem 2.7. For n∈N∪{0} and r∈N, the representation holds:
D(r)n,λ(x)=n∑k=0(n∑m=kα∑ℓ=0(nm)(αℓ)(n−m)ℓ(1−u)ℓS1,λ(m,k)D(r)n−m−ℓ,λ)h(α)k,λ(x|u). |
As the inversion formula, we have
h(α)n,λ(x|u)=n∑k=0(n∑ℓ=0(nk+ℓ)(r+k)!k!(ℓ+r+k)!S2,λ(r+k+ℓ,r+k)h(α)n−k−ℓ,λ(u))D(r)k,λ(x). |
Proof. Let D(r)n,λ(x)=∑nk=0μn,kh(α)k,λ(x|u). By (1.4), (2.9), (2.10), and (2.31), we have
μn,k=1k!⟨(1+t−u1−u)α(tlogλ(1+t))r(logλ(1+t))k|(x)n,λ⟩λ=⟨(logλ(1+t)t)r(1+t1−u)α|(1k!(logλ(1+t))k)λ(x)n,λ⟩λ=n∑m=k(nm)S1,λ(m,k)⟨(logλ(1+t)t)r(1+t1−u)α|(x)n−m,λ⟩λ=n∑m=k(nm)S1,λ(m,k)⟨(logλ(1+t)t)r|(α∑ℓ=0(αℓ)(t1−u)ℓ)λ(x)n−m,λ⟩λ=n∑m=k(nm)S1,λ(m,k)α∑ℓ=0(αℓ)(n−m)ℓ(1−u)ℓ⟨(logλ(1+t)t)r|(x)n−m−ℓ,λ⟩λ=n∑m=k(nm)S1,λ(m,k)α∑ℓ=0(αℓ)(n−m)ℓ(1−u)ℓD(r)n−m−ℓ,λ, |
which implies the first formula.
Conversely, we assume that h(α)n,λ(x|u)=∑nk=0nun,kD(r)k,λ(x). Then, νn,k satisfies
νn,k=1k!⟨(eλ(t)−1t)r(eλ(t)−u1−u)α(eλ(t)−1)k|(x)n,λ⟩λ=1k!⟨(1−ueλ(t)−u)α(eλ(t)−1)r+ktr|(x)n,λ⟩λ=n∑ℓ=0(nk+ℓ)(r+k)!k!(ℓ+r+k)!S2,λ(r+k+ℓ,r+k)⟨(1−ueλ(t)−u)α|(x)n−k−ℓ,λ⟩λ=n∑ℓ=0(nk+ℓ)(r+k)!k!(ℓ+r+k)!S2,λ(r+k+ℓ,r+k)h(α)n−k−ℓ,λ(u), |
which shows the second assertion.
In this subsection, we present the pattern of the zeros of the polynomials. The understanding of patterns of zeros of degenerate polynomials can provide useful information about the original polynomials which can be obtained as limit of λ approaches zero. For example, the first three consecutive degenerate higher-order Daehee polynomials of degree r are given by
D(r)1,λ(x)=x+r(λ−1)2,D(r)2,λ(x)=x2+(r(λ−1)−1)x+112r(λ−1)(3r(λ−1)+λ−5),D(r)3,λ(x)=x3+12(3r(λ−1)−9)x2+14(8+r(λ−1)(3r(λ−1)+λ−11))x+18r(λ−1)(r(λ−1)−2)(r(λ−1)+λ−3), |
which approach to the higher-order Daehee polynomials of degree r as λ→0. We observe the patterns of roots by the changing parameters λ and r on the polynomials. In order to do this, we fix the degree of the polynomials as n=40, and compute the roots of D(r)40,λ(x) with fixed r=3 and six different parameters λ=±1, ±10, ±100 with the help of the Mathematica tool. The results are displayed in Figure 1. Next, we increase the degree of the polynomials and investigate the distribution of the roots of the polynomials.
For further investigation, we computed the roots of the polynomials by increasing the degree n of polynomials from 1 to 40 in Figure 2.
Finally, we investigated the distribution of the roots of D(r)40,λ(x) with a fixed λ=10 and three different parameters r=3, 4, 5 and the results were displayed in Figure 3.
In this subsection, we provide the explicit formulas presented in Theorem 2.2 that show the representations of the degenerate higher-order Daehee polynomials in terms of the degenerate Bernoulli polynomials and vice versa. To better understand, we present the graphs of D(r)n,λ(x) with λ=0.1 and r=3 for n=0, 1, ⋯, 5 and of D(r)n,λ(x) with λ=0.1 for various orders r=1, 2, ⋯, 5 in Figure 4.
Next, we compute the combinatorial results of μn,k and νn,k presented in the proof of Theorem 2.2 to confirm the connection formulas presented. To do this, we compute D(r)n,λ(x) and βn,λ(x) for r=3, λ=0.1, and n=0, 1, ⋯, 5 and expand them using the coefficients μn,k and νn,k which are computed with two decimal place accuracy. The expressions presented confirm the results of Theorem 2.2.
The degenerate higher-order Daehee polynomials D(r)n,λ(x) with λ=0.1, r=3 for n=1, 2, ⋯, 5 are expressed in terms of βn,λ(x) as follows:
D(3)5,λ(x)=x5−674x4+4194x3−30083100x2+386814310000x−68088951400000=β5,λ(x)−272β4,λ(x)+69β3,λ(x)−8195β2,λ(x)+174984310000β1,λ(x)−6312807100000β0,λ(x),D(3)4,λ(x)=x4−575x3+1794x2−34941500x+174984350000=β4,λ(x)−9β3,λ(x)+141350β2,λ(x)−8883250β1,λ(x)+70742750000β0,λ(x),D(3)3,λ(x)=x3−14120x2+59340x−88831000=β3,λ(x)−275β2,λ(x)+35140β1,λ(x)−80372000β0,λ(x),D(3)2,λ(x)=x2−3710x+11740=β2,λ(x)−2710β1,λ(x)+309200β0,λ(x),D(3)1,λ(x)=x−2720=β1,λ(x)−910β0,λ(x). |
Conversely, the degenerate Bernoulli polynomials βn,λ(x) with λ=0.1, r=3 for n=1, 2, ⋯, 5 are represented in terms of D(r)n,λ(x):
β5,λ(x)=x5−134x4+6720x3−2625x2−350x+9009400000=D(3)5,λ(x)+272D(3)4,λ(x)+1052D(3)3,λ(x)+6579100D(3)2,λ(x)+13527625D(3)1,λ(x)+28983125D(3)0,λ(x),β4,λ(x)=x4−125x3+4125x2−625x−2673100000,=D(3)4,λ(x)+9D(3)3,λ(x)+101750D(3)2,λ(x)+45940D(3)1,λ(x)+57516250D(3)0,λ(x),β3,λ(x)=x3−3320x2+1320x−994000,=D(3)3,λ(x)+275D(3)2,λ(x)+1161200D(3)1,λ(x)+910D(3)0,λ(x),β2,λ(x)=x2−x+33200=D(3)2,λ(x)+2710D(3)1,λ(x)+177200D(3)0,λ(x),β1,λ(x)=x−920=D(3)1,λ(x)+910D(3)0,λ(x). |
The study of special polynomials provides useful tools in differential equations, fuzzy theory, probability, orthogonal polynomials, and special functions and numbers. These researches are conducted using various tools, including generating functions, p-adic analysis, combinatorial methods, and umbral calculus. Recently, degenerate versions of special polynomials and numbers have been investigated using λ-analogues of these methods, and their arithmetical and combinatorial properties and relations have been studied by several mathematicians. These degenerate versions of special polynomials and numbers have been applied in differential equations and probability theories, providing new applications. In this paper, we explore the connection problems between the degenerate higher-order Daehee polynomials and other degenerate types of special polynomials. We present explicit formulas for representations with the help of umbral calculus and vice versa. In addition, we illustrate the results with some explicit examples. In order to better understanding the polynomials, the distribution of roots are presented.
The authors declare there is no conflict of interest.
[1] |
Bei S, Yang A, Pei H, et al. (2023) Price Risk Analysis using GARCH Family Models: Evidence from Shanghai Crude Oil Futures Market. Econ Model 125: 106367. http://doi.org/10.1016/j.econmod.2023.106367 doi: 10.1016/j.econmod.2023.106367
![]() |
[2] |
Bu H (2014) Effect of inventory announcements on crude oil price volatility. Energy Econ 46: 485–494. http://doi.org/10.1016/j.eneco.2014.05.015 doi: 10.1016/j.eneco.2014.05.015
![]() |
[3] |
Corbet S, Hou YG, Hu Y, et al. (2022) The growth of oil futures in China: Evidence of market maturity through global crises. Energy Econ 114: 106243. http://doi.org/10.1016/j.eneco.2022.106243 doi: 10.1016/j.eneco.2022.106243
![]() |
[4] |
Dai P, Xiong X, Zhang J, et al. (2022) The role of global economic policy uncertainty in predicting crude oil futures volatility: Evidence from a two-factor GARCH-MIDAS model. Resour Policy 78: 102849. http://doi.org/10.1016/j.resourpol.2022.102849 doi: 10.1016/j.resourpol.2022.102849
![]() |
[5] |
Dai Z, Zhu J, Zhang X (2022) Time-frequency connectedness and cross-quantile dependence between crude oil, Chinese commodity market, stock market and investor sentiment. Energy Econ 114: 106226. http://doi.org/10.1016/j.eneco.2022.106226 doi: 10.1016/j.eneco.2022.106226
![]() |
[6] |
Diaz-Rainey I, Roberts H, Lont DH (2017) Crude inventory accounting and speculation in the physical oil market. Energy Econ 66: 508–522. http://doi.org/10.1016/j.eneco.2017.03.029 doi: 10.1016/j.eneco.2017.03.029
![]() |
[7] |
Diebold FX, Mariano RS (1995) Comparing Predictive Accuracy. J Bus Econ Stat 13: 253–263. https://doi.org/10.1080/07350015.1995.10524599 doi: 10.1080/07350015.1995.10524599
![]() |
[8] |
Engle RF, Ghysels E, Sohn B (2013) Stock market volatility and macroeconomic fundamentals. Rev Econ Stat 3: 776–797. https://doi.org/10.1162/REST_a_00300 doi: 10.1162/REST_a_00300
![]() |
[9] |
Fu J, Qiao H (2022) The Time-Varying Connectedness Between China's Crude Oil Futures and International Oil Markets: A Return and Volatility Spillover Analysis. Lett Spat Resour Sci 15: 341–376. http://doi.org/10.1007/s12076-021-00288-z doi: 10.1007/s12076-021-00288-z
![]() |
[10] |
Giacomini R, Rossi B (2010) Forecast comparisons in unstable environments. J Appl Econom 25: 595–620. https://doi.org/10.1002/jae.1177 doi: 10.1002/jae.1177
![]() |
[11] |
Gong W, Li Y, Wang C, et al. (2022) The Catastrophe Analysis of Shanghai Crude Oil Futures Price from the Perspective of Volatility Factors. Complexity 2022: 1–12. http://doi.org/10.1155/2022/5367693 doi: 10.1155/2022/5367693
![]() |
[12] |
Guo Y, Li P, Wu H (2023) Jumps in the Chinese crude oil futures volatility forecasting: New evidence. Energy Econ 126: 106955. http://doi.org/10.1016/j.eneco.2023.106955 doi: 10.1016/j.eneco.2023.106955
![]() |
[13] |
He C, Li G, Fan H, et al. (2021) Correlation between Shanghai crude oil futures, stock, foreign exchange, and gold markets: a GARCH-vine-copula method. Appl Econ 53: 1249–1263. http://doi.org/10.1080/00036846.2020.1828566 doi: 10.1080/00036846.2020.1828566
![]() |
[14] |
Hu G, Jiang H (2023) Time-varying jumps in China crude oil futures market impacted by COVID-19 pandemic. Resour Policy 82: 103510. http://doi.org/10.1016/j.resourpol.2023.103510 doi: 10.1016/j.resourpol.2023.103510
![]() |
[15] |
Huang Y, Xu W, Huang D, et al. (2023) Chinese crude oil futures volatility and sustainability: An uncertainty indices perspective. Resour Policy 80: 103227. http://doi.org/10.1016/j.resourpol.2022.103227 doi: 10.1016/j.resourpol.2022.103227
![]() |
[16] |
Jiang W, Tang W, Liu X (2023) Forecasting realized volatility of Chinese crude oil futures with a new secondary decomposition ensemble learning approach. Financ Res Lett 57: 104254. http://doi.org/10.1016/j.frl.2023.104254 doi: 10.1016/j.frl.2023.104254
![]() |
[17] |
Jin D, He M, Xing L, et al. (2022) Forecasting China's crude oil futures volatility: How to dig out the information of other energy futures volatilities? Resour Policy 78: 102852. http://doi.org/10.1016/j.resourpol.2022.102852 doi: 10.1016/j.resourpol.2022.102852
![]() |
[18] |
Joo K, Jeong M, Seo Y, et al. (2021) Shanghai crude oil futures: Flagship or burst? Energy Rep 7: 4197–4204. http://doi.org/10.1016/j.egyr.2021.06.098 doi: 10.1016/j.egyr.2021.06.098
![]() |
[19] |
Kang B, Nikitopoulos CS, Prokopczuk M (2020) Economic determinants of oil futures volatility: A term structure perspective. Energy Econ 88: 104743. http://doi.org/10.1016/j.eneco.2020.104743 doi: 10.1016/j.eneco.2020.104743
![]() |
[20] |
Kilian L, Murphy DP (2014) The role of inventories and speculative trading in the global market for crude oil. J Appl Econ 29: 454–478. https://doi.org/10.1002/jae.2322 doi: 10.1002/jae.2322
![]() |
[21] |
Li J, Umar M, Huo J (2023) The spillover effect between Chinese crude oil futures market and Chinese green energy stock market. Energy Econ 119: 106568. http://doi.org/10.1016/j.eneco.2023.106568 doi: 10.1016/j.eneco.2023.106568
![]() |
[22] |
Lin B, Su T (2021) Do China's macro-financial factors determine the Shanghai crude oil futures market? Int Rev Financ Anal 78: 101953. http://doi.org/10.1016/j.irfa.2021.101953 doi: 10.1016/j.irfa.2021.101953
![]() |
[23] |
Liu M, Lee C (2021) Capturing the dynamics of the China crude oil futures: Markov switching, co-movement, and volatility forecasting. Energy Econ 103: 105622. http://doi.org/10.1016/j.eneco.2021.105622 doi: 10.1016/j.eneco.2021.105622
![]() |
[24] |
Lu X, Ma F, Wang J, et al. (2022) Forecasting oil futures realized range‐based volatility with jumps, leverage effect, and regime switching: New evidence from MIDAS models. J Forecast 41: 853–868. http://doi.org/10.1002/for.2837 doi: 10.1002/for.2837
![]() |
[25] |
Luo J, Ji Q (2018) High-frequency volatility connectedness between the US crude oil market and China's agricultural commodity markets. Energy Econ 76: 424–438. http://doi.org/10.1016/j.eneco.2018.10.031 doi: 10.1016/j.eneco.2018.10.031
![]() |
[26] |
Lv F, Yang C, Fang L (2020) Do the crude oil futures of the Shanghai International Energy Exchange improve asset allocation of Chinese petrochemical-related stocks? Int Rev Financ Anal 71: 101537. http://doi.org/10.1016/j.irfa.2020.101537 doi: 10.1016/j.irfa.2020.101537
![]() |
[27] |
Ma R, Zhou C, Cai H, et al. (2019) The forecasting power of EPU for crude oil return volatility. Energy Rep 5: 866–873. http://doi.org/10.1016/j.egyr.2019.07.002 doi: 10.1016/j.egyr.2019.07.002
![]() |
[28] |
Niu J, Ma C, Chang C (2023) The arbitrage strategy in the crude oil futures market of shanghai international energy exchange. Econ Chang Restruct 56: 1201–1223. http://doi.org/10.1007/s10644-022-09468-3 doi: 10.1007/s10644-022-09468-3
![]() |
[29] |
Shao M, Hua Y (2022) Price discovery efficiency of China's crude oil futures: Evidence from the Shanghai crude oil futures market. Energy Econ 112: 106172. http://doi.org/10.1016/j.eneco.2022.106172 doi: 10.1016/j.eneco.2022.106172
![]() |
[30] |
Sun C, Min J, Sun J, et al. (2023) The role of China's crude oil futures in world oil futures market and China's financial market. Energy Econ 120: 106619. http://doi.org/10.1016/j.eneco.2023.106619 doi: 10.1016/j.eneco.2023.106619
![]() |
[31] |
Sun C, Peng Y, Zhan Y (2023) How does China's crude oil futures affect the crude oil prices at home and abroad? Evidence from the cross-market exchange rate spillovers. Int Rev Econ Financ 88: 204–222. http://doi.org/10.1016/j.iref.2023.06.013 doi: 10.1016/j.iref.2023.06.013
![]() |
[32] |
Sun C, Zhan Y, Peng Y, et al. (2022) Crude oil price and exchange rate: Evidence from the period before and after the launch of China's crude oil futures. Energy Econ 105: 105707. http://doi.org/10.1016/j.eneco.2021.105707 doi: 10.1016/j.eneco.2021.105707
![]() |
[33] |
Stock JH, Watson MW (2002) Forecasting Using Principal Components From a Large Number of Predictors. J Am Stat Assoc 97: 1167–1179. https://doi.org/10.1198/016214502388618960 doi: 10.1198/016214502388618960
![]() |
[34] |
Wang H, Qiu S, Yick HY, et al. (2022) A Study on the Oil Price Cointegration Dynamic Process: Evidence From the Shanghai Crude Oil Futures. Front Environ Sci 10: 901236. http://doi.org/10.3389/fenvs.2022.901236 doi: 10.3389/fenvs.2022.901236
![]() |
[35] |
Wang J, Qiu S, Yick HY (2022) The influence of the Shanghai crude oil futures on the global and domestic oil markets. Energy 245: 123271. http://doi.org/10.1016/j.energy.2022.123271 doi: 10.1016/j.energy.2022.123271
![]() |
[36] |
Wang X, Wang Y (2019) Volatility spillovers between crude oil and Chinese sectoral equity markets: Evidence from a frequency dynamics perspective. Energy Econ 80: 995–1009. http://doi.org/10.1016/j.eneco.2019.02.019 doi: 10.1016/j.eneco.2019.02.019
![]() |
[37] |
Wang Z, Liu B, Fan Y (2023) Network connectedness between China's crude oil futures and sector stock indices. Energy Econ 125: 106848. http://doi.org/10.1016/j.eneco.2023.106848 doi: 10.1016/j.eneco.2023.106848
![]() |
[38] |
Wei Y, Liu J, Lai X, et al. (2017) Which determinant is the most informative in forecasting crude oil market volatility: Fundamental, speculation, or uncertainty? Energy Econ 68: 141–150. http://doi.org/10.1016/j.eneco.2017.09.016 doi: 10.1016/j.eneco.2017.09.016
![]() |
[39] |
Wei Y, Zhang Y, Wang Y (2022) Information connectedness of international crude oil futures: Evidence from SC, WTI, and Brent. Int Rev Financ Anal 81: 102100. http://doi.org/10.1016/j.irfa.2022.102100 doi: 10.1016/j.irfa.2022.102100
![]() |
[40] |
Wu X, Cui H, Wang L (2023) Forecasting oil futures price volatility with economic policy uncertainty: a CARR-MIDAS model. Appl Econ Lett 30: 120–125. http://doi.org/10.1080/13504851.2021.1977232 doi: 10.1080/13504851.2021.1977232
![]() |
[41] |
Yang C, Lv F, Fang L, et al. (2020) The pricing efficiency of crude oil futures in the Shanghai International Exchange. Financ Res Lett 36: 101329. http://doi.org/10.1016/j.frl.2019.101329 doi: 10.1016/j.frl.2019.101329
![]() |
[42] |
Yang K, Wei Y, Li S, et al. (2021) Global financial uncertainties and China's crude oil futures market: Evidence from interday and intraday price dynamics. Energy Econ 96: 105149. http://doi.org/10.1016/j.eneco.2021.105149 doi: 10.1016/j.eneco.2021.105149
![]() |
[43] |
Yang Y, Ma Y, Hu M, et al. (2021) Extreme risk spillover between chinese and global crude oil futures. Financ Res Lett 40: 101743. http://doi.org/10.1016/j.frl.2020.101743 doi: 10.1016/j.frl.2020.101743
![]() |
[44] |
Yu X, Xiao K (2022) Dependencies and Volatility Spillovers among Chinese Stock and Crude Oil Future Markets: Evidence from Time-Varying Copula and BEKK-GARCH Models. J Risk Financ Manag 15: 491. http://doi.org/10.3390/jrfm15110491 doi: 10.3390/jrfm15110491
![]() |
[45] |
Yu X, Huang Y, Xiao K (2021) Global economic policy uncertainty and stock volatility: evidence from emerging economies. J Appl Econ 24: 416–440. http://doi.org/10.1080/15140326.2021.1953913 doi: 10.1080/15140326.2021.1953913
![]() |
[46] |
Yu Z, Yang J, Webb RI (2023) Price discovery in China's crude oil futures markets: An emerging Asian benchmark? J Futures Mark 43: 297–324. http://doi.org/10.1002/fut.22384 doi: 10.1002/fut.22384
![]() |
[47] |
Zagaglia P (2010) Macroeconomic factors and oil futures prices: A data-rich model. Energy Econ 32: 409–417. http://doi.org/10.1016/j.eneco.2009.11.003 doi: 10.1016/j.eneco.2009.11.003
![]() |
[48] |
Zhang D, Farnoosh A, Ma Z (2022) Does the Launch of Shanghai Crude Oil Futures Stabilize the Spot Market? A Financial Cycle Perspective. Int Econ J 36: 39–58. http://doi.org/10.1080/10168737.2021.2001027 doi: 10.1080/10168737.2021.2001027
![]() |
[49] |
Zhang Q, Di P, Farnoosh A (2021) Study on the impacts of Shanghai crude oil futures on global oil market and oil industry based on VECM and DAG models. Energy 223: 120050. http://doi.org/10.1016/j.energy.2021.120050 doi: 10.1016/j.energy.2021.120050
![]() |
[50] |
Zhu P, Lu T, Chen S (2022) How do crude oil futures hedge crude oil spot risk after the COVID-19 outbreak? A wavelet denoising-GARCHSK-SJC Copula hedge ratio estimation method. Physica A 607: 128217. http://doi.org/10.1016/j.physa.2022.128217 doi: 10.1016/j.physa.2022.128217
![]() |
![]() |
![]() |
1. | Eduardo G. Pardo, Sergio Gil-Borrás, Antonio Alonso-Ayuso, Abraham Duarte, Order Batching Problems: taxonomy and literature review, 2023, 03772217, 10.1016/j.ejor.2023.02.019 | |
2. | Daniel Alejandro Rossit, Fernando Tohmé, Máximo Méndez-Babey, Mariano Frutos, Diego Broz, Diego Gabriel Rossit, Special Issue: Mathematical Problems in Production Research, 2022, 19, 1551-0018, 9291, 10.3934/mbe.2022431 | |
3. | Giorgia Casella, Andrea Volpi, Roberto Montanari, Letizia Tebaldi, Eleonora Bottani, Trends in order picking: a 2007–2022 review of the literature, 2023, 11, 2169-3277, 10.1080/21693277.2023.2191115 | |
4. | Fabio Maximiliano Miguel, Mariano Frutos, Máximo Méndez, Fernando Tohmé, Begoña González, Comparison of MOEAs in an Optimization-Decision Methodology for a Joint Order Batching and Picking System, 2024, 12, 2227-7390, 1246, 10.3390/math12081246 |