Statistical inference for rough volatility Central limit theorems

2025-04-15
0
0
552.77KB
49 页
10玖币
侵权投诉
arXiv:2210.01216v3 [math.ST] 14 Jun 2024
STATISTICAL INFERENCE FOR ROUGH VOLATILITY:
CENTRAL LIMIT THEOREMS
BYCARSTEN H. CHONG1,a, MARC HOFFMANN2,b, YANGHUI LIU3,c,
MATHIEU ROSENBAUM4,dAND GRÉGOIRE SZYMANSKI4,e
1Department of Information Systems, Business Statistics and Operations Management, The Hong Kong University of Science
and Technology, acarstenchong@ust.hk
2CEREMADE, Université Paris Dauphine-PSL, bhoffmann@ceremade.dauphine.fr
3Department of Mathematics, Baruch College CUNY, cyanghui.liu@baruch.cuny.edu
4CMAP, École Polytechnique, dmathieu.rosenbaum@polytechnique.edu;egregoire.szymanski@polytechnique.edu
In recent years, there has been a substantive interest in rough volatility
models. In this class of models, the local behavior of stochastic volatility is
much more irregular than semimartingales and resembles that of a fractional
Brownian motion with Hurst parameter H < 0.5. In this paper, we derive a
consistent and asymptotically mixed normal estimator of Hbased on high-
frequency price observations. In contrast to previous works, we work in a
semiparametric setting and do not assume any a priori relationship between
volatility estimators and true volatility. Furthermore, our estimator attains a
rate of convergence that is known to be optimal in a minimax sense in para-
metric rough volatility models.
1. Introduction. For many years, continuous-time stochastic volatility models were pre-
dominantly based on stochastic differential equations driven by Brownian motion or Lévy
processes. But more recently, [29] found empirical evidence that stochastic volatility is ac-
tually much rougher than semimartingales, in the sense that it locally resembles a fractional
Brownian motion with Hurst index H < 0.5, a statement that was further supported by other
empirical work based on both return data [13,28,30] and options data [11,27,41].
The data-driven approach of [29] to uncover rough volatility starts by considering high-
frequency log-price data {xiδn:i= 0,...,[T/δn]}, where for example δn= 5 min and T=
1year. In a next step, daily spot variance estimates are calculated from the formula
(1.1) ˆcj=1
knδn
kn
X
i=1
(δn
(j−1)kn+ix)2, j = 1,...,[T/(knδn)],
where δn
ix=xiδn−x(i−1)δnand kn= 78 is the number of 5 min increments during one
trading day. Afterwards, realized power variations of log ˆcj, that is,
m(q, ∆) = 1
[T/∆]
[T/∆]
X
j=1 |log ˆcj∆−log ˆc(j−1)∆|q
are computed for different values of q > 0and ∆∈ {1day,2days,...}. If log ˆcjwere discrete
observations of a continuous Itô semimartingale, then one would expect that m(q, ∆) scales
as ∆q/2, implying that the slope ζqin a regression of log m(q, ∆) on log ∆ satisfies
ζq/q ≈1
2.
MSC2020 subject classifications:Primary 62G15, 62G20, 62M09; secondary 60F05, 62P20.
Keywords and phrases: Central limit theorem, fractional Brownian motion, Hurst parameter, nonparametric
estimation, rough volatility, spot volatility, volatility of volatility.
1
2
However, for large set of high-frequency data, [29] consistently found values of ζq/q < 1
2,
indicating that stochastic volatility locally behaves as a fractional Brownian motion with
Hurst parameter H < 1
2. (To be precise, [29] actually computed the realized q-variations of
daily realized variance, that is, of log RVj=knδnˆcj. But since log RVj∆−log RV(j−1)∆ =
log ˆcj∆−log ˆc(j−1)∆, this amounts to the same as computing m(q, ∆).)
As was pointed out by [13,28], the above approach rests on the assumption that realized
variances have the same scaling behavior as the true unobserved volatility. At the same time,
it is well known (see e.g., [4, Chapter 8]) that in the absence of jumps and if volatility is a
semimartingale, spot variance estimators of the type (1.1) converge to true spot variance plus
a small modulated white noise. In a first attempt to take estimation errors for spot variance
into account, [13,28] assume that
(1.2) log ˆcj= log true spot variancej+εj,
where εjis a zero-mean iid sequence that is independent of everything else. Under assump-
tion (1.2), [13,28] derive consistent estimators of the roughness parameter Hin parametric
rough volatility models and uphold the conclusion of [29] that volatility is rough in a large
set of financial time series. We also refer to [14], where the authors assume (1.2) with slightly
different assumptions on (log ˆcj, εj), and to [46], where a central limit theorem (CLT) for H
is established under (1.2) (see also [50]).
This paper aims to substantially generalize the aforementioned results in two directions:
first, we establish consistent and asymptotically mixed normal estimators of Hin a semipara-
metric setting, where except for Hall other model ingredients are fully nonparametric; and
second, we shall do so without assuming any relationship (such as (1.2)) between volatility
proxies and true volatility. The rate of convergence of our best estimator is
(1.3) δ−1/(4H+2)
n,
which as our companion paper [18] shows is optimal in a minimax sense in parametric rough
volatility models.
The remaining paper is structured as follows: in Section 2, after introducing the model
assumptions, we state the main technical result of this paper, Theorem 2.2, a CLT for volatility
of volatility (VoV) estimators in a rough volatility framework. Section 3discusses how we turn
Theorem 2.2 into rate-optimal and feasible estimators of H. In addition to a usual application
of the delta method, the rough volatility setting requires us overcome two distinct challenges:
• eliminating a nonnegligible asymptotic bias term for which we do not have a sufficiently
fast estimator;
• constructing an optimal sequence knfor spot variance estimation that depends on the un-
known parameter Hwithout losing a marginal bit of convergence rate.
Our final estimator Hnfor His given in Equation (3.34). As Theorems 3.3 and 3.5 show,
Hnis a feasible and rate-optimal estimator of Hif H∈(0,1
2)and is equal to 1
2with high
probability if volatility is a continuous Itô semimartingale. In Section 4, we report the results
of a short simulation study. Section 5contains the main steps of the proof of Theorem 2.2,
with certain technical details postponed to Appendices A–C.
In what follows, we write A.Bif there is a constant C∈(0,∞)that does not depend on
any important parameter such that A≤CB. Furthermore, if An(t)and Bn(t)are stochas-
tic processes, we write An≈Bnif E[supt∈[0,T ]|An(t)−Bn(t)|]→0as n→ ∞. For two
sequences anand bnwe write an∼bnif an/bn→1as n→ ∞. If x∈Rn, we denote its
Euclidean norm by |x|. For any α∈R, we write xα
+=xαif x > 0and xα
+= 0 otherwise. We
also use the notation N={1,2,...}and N0={0,1,2,...}.
STATISTICAL INFERENCE FOR ROUGH VOLATILITY 3
2. Model and CLT for VoV estimators. On a filtered probability space (Ω,F,F=
(Ft)t≥0,P)satisfying the usual conditions, we assume that the log-price xof an asset is
given by a continuous Itô semimartingale of the form
(2.1) xt=x0+Zt
0
bsds +Zt
0
σsdWs, t ≥0.
We assume that the squared volatility process c=σ2satisfies
(2.2) ct=c0+Zt
0
asds +Zt
0
˜g(t−s)˜ηsds +Zt
0
g(t−s)(ηsdWs+ ˆηsdˆ
Ws),
where
η2
t=η2
0+Zt
0
aη
sds +Zt
0
˜gη(t−s)˜
θsds +Zt
0
gη(t−s)θsd¯
Ws,
ˆη2
t= ˆη0+Zt
0
aˆη
sds +Zt
0
˜gˆη(t−s)˜
ϑsds +Zt
0
gˆη(t−s)ϑsd¯
Ws.
(2.3)
The ingredients of (2.1)–(2.3) are assumed to satisfy the following conditions.
ASSUMPTION CLT. Suppose that the log-price process xis given by (2.1)with the fol-
lowing specifications:
1. There is H∈(0,1
2]such that the squared volatility process ct=σ2
tsatisfies (2.2)with η
and ˆηgiven by (2.3). The variables x0,c0,η2
0and ˆη2
0are F0-measurable.
2. The processes a,b,aηand aˆη(resp., θand ϑ) are adapted and locally bounded real-
valued (resp., R1×4-dimensional) processes. Moreover, for all T > 0, we assume that
(2.4) lim
h→0sup
s,t∈[0,T ],|s−t|≤hE[1 ∧|bt−bs|] + E[1 ∧|at−as|]= 0.
3. The processes ˜η,˜
θand ˜
ϑare adapted, locally bounded and for all T > 0, there is KT∈
(0,∞)such that
(2.5) sup
s,t∈[0,T ]E[1 ∧|˜ηt−˜ηs|] + E[1 ∧|˜
θt−˜
θs|] + E[1 ∧|˜
ϑt−˜
ϑs|]≤KT|t−s|H.
4. The processes Wand ˆ
Ware independent standard F-Brownian motions and ¯
Wis a four-
dimensional F-Brownian motion that is jointly Gaussian with (W, ˆ
W). The components
of ¯
Wmay depend on each other and on (W, ˆ
W).
5. We have
(2.6) g(t) = gH(t) + g0(t), gη(t) = gHη(t) + gη
0(t), gˆη(t) = gHˆη(t) + gˆη
0(t),
˜g(t) = g˜
H(t) + ˜g0(t),˜gη(t) = g˜
Hη(t) + ˜gη
0(t),˜gˆη(t) = g˜
Hˆη(t) + ˜gˆη
0(t),
where
(2.7) gH(t) = K−1
HtH−1/2
+, KH=Γ(H+1
2)
psin(πH)Γ(2H+ 1) ,
and Hη, Hˆη∈(0,1
2],˜
H, ˜
Hη,˜
Hˆη∈[H, 1
2]and g0, gη
0, gˆη
0,˜g0,˜gη
0,˜gˆη
0∈C1([0,∞)) are func-
tions vanishing at t= 0.
4
Let us comment on the conditions imposed in Assumption CLT. Except for the parameter
H, the assumptions on x,c,ηand ˆηare fully nonparametric and designed in such a way that it
contains the rough Heston model [25,26] as an example, which is a particular important one
as it is founded in the microstructure of financial markets [24,36]. Note that we allow c,ηand
ˆηto have both a usual (differentiable) and a rough (non-differentiable) drift. Moreover, by
considering W,ˆ
Wand ¯
W, we allow for the most general dependence between the Brownian
motions driving x,c,η,ˆη. Also note that Hηand Hˆηare not coupled with H, so the VoV
processes ηand ˆηcan be much rougher than the volatility process citself.
The structural assumptions in (2.3) for η2and ˆη2are important and cannot be replaced by
just merely assuming that η2and ˆη2are H-Hölder regular (see the paragraph after (5.27) for
the reason). At the same time, (2.3) is a mild assumption: it is not only satisfied by the rough
Heston model but by any model in which VoV is assumed to be continuous and stationary,
thanks to the Wold–Karhunen representation theorem. (Due to the coefficients θsand ϑs,
the processes η2and ˆη2do not have to be stationary.) Also, in the estimation of VoV in a
semimartingale context, (2.3) with Hη=Hˆη=1
2is typically assumed; see [39,48].
REMARK 2.1 (Rough volatility vs. long memory vs. jumps).
1. There is long-standing debate in the literature whether volatility has long memory or not
(see, e.g., [6,20,22,23]). Because we include various g0-functions in (2.6), the kernels in
(2.2) and (2.3) are only specified around t= 0. In particular, H,Hηand Hˆηare parameters
of roughness and are not related to long-range dependence / long-memory / persistence. In
particular, in our model, volatility can be rough and have long memory at the same time,
which is important as [13,44,45] point out.
2. In some parts of the previous literature, the notion of “roughness” is used as a synonym
for jumps or discontinuities (see, e.g., [5,15]). Since our model neither includes price nor
volatility jumps, one may ask whether rough volatility can be explained through jumps,
which are a well-documented feature of high-frequency price series [3]. In this respect,
we first note that [19] shows that rough volatility (in the sense that H < 1
2in (2.2)) can
be statistically distinguished from both price and volatility jumps. In order to make the
estimators developed in this paper robust to jumps, a natural idea is to include truncation in
(2.8) and (2.9) below. We leave it to future work to study the details of such an extension.
3. While this paper focuses on the rough case H≤1/2, we conjecture that the results of this
paper can be extended to H < 3
4without major obstacles. Since noncentral limit theorems
are known to appear for variation statistics of directly observable processes if H≥3
4(see,
e.g., [42]), we do not know whether our results extend to H≥3
4.
If cwas directly observable, a classical way to feasibly estimate Hwould be to prove a
joint CLT for realized autocovariances δ1−2H
nP[T/δn]−ℓ
i=1 δn
ic δn
i+ℓcwith different values of
ℓ∈N0and then to obtain an estimator of Hfrom the ratio of two such functionals; see [9,
16,17,21,32,34,40]. Since we do not observe c, we first consider spot variance estimators
ˆcn
t,s =1
knδn
ˆ
Cn
t,s,ˆ
Cn
t,s =
[(t+s)/δn]−1
X
i=[t/δn]
(δn
ix)2, δn
ix=xiδn−x(i−1)δn,(2.8)
where kn∈Nand kn∼θδ−κ
nfor some κ, θ > 0. Then we form realized autocovariances of
these spot variance estimators by defining
˜
Vn,ℓ,kn
t= (knδn)1−2H1
kn
[t/δn]−(ℓ+2)kn+1
X
i=1 ˆcn
(i+kn)δn,knδn−ˆcn
iδn,knδn
׈cn
(i+(ℓ+1)kn)δn,knδn−ˆcn
(i+ℓkn)δn,knδn
(2.9)
STATISTICAL INFERENCE FOR ROUGH VOLATILITY 5
for ℓ≥0. Note that we write [x]and {x}for the integer and fractional part of x, respec-
tively. The normalization in the last line is chosen in such a way that ˜
Vn,ℓ,kn
tconverges in
probability. In the semimartingale context (with H=1
2and ℓ= 0), the functional ˜
Vn,0,kn
t
was used in [48] (see also [31,39]) to estimate the integrated VoV process Rt
0(η2
s+ ˆη2
s)ds (to
be very precise, this is actually the integrated variance of variance). Still in the semimartin-
gale framework, functionals similar to (2.9) have also been investigated in the literature to
estimate the leverage effect; see [2,7,8,37,47,49].
To state a CLT for ˜
Vn,ℓ,knfor H < 1
2, we have to introduce some additional notation:
for n∈N,h > 0and a function f:R→R, we define the forward and central difference
operators by
∆n
hf(t) =
n
X
i=0
(−1)n−in
if(t+ih), δn
hf(t) =
n
X
i=0
(−1)in
if(x+ (n
2−i)h),
respectively. For n= 1, we simply write ∆hf(t) = ∆1
hf(t) = f(t+h)−f(t)and δhf(t) =
δ1
hf(t) = f(t+h
2)−f(t−h
2). Moreover, given α∈R, we use the shorthand notation ∆n
htα
+
or ∆n
h|t|αfor ∆n
hf(t)where f(t) = tα
+or f(t) = |t|α(δn
htα
+and δn
h|t|αare used similarly).
Finally, for any d∈N, we use st
=⇒to denote functional stable convergence in law in the space
of càdlàg functions [0,∞)→Rdequipped with the local uniform topology. The following
CLT is the main technical result of this paper.
THEOREM 2.2. Let d∈Nand ℓ1,...,ℓd≥2be integers. Furthermore, consider deter-
ministic integer sequences (k(1)
n)n∈N,...,(k(d)
n)n∈Nsuch that for some κ∈[2H
2H+1 ,1
2]and
θ1,...,θd∈(0,∞)we have k(j)
n∼θjδ−κ
nfor all j= 1,...,d. For each j= 1,...,d, let
(2.10) Zn,j
t=δ−(1−κ)/2
n(˜
Vn,ℓj,k(j)
n
t−Vℓj
t−An,ℓj,k(j)
n
t),
where for ℓ≥2, we define
(2.11) Vℓ
t= ΦH
ℓZt
0
(η2
s+ ˆη2
s)ds
with
ΦH
ℓ=δ4
1|ℓ|2H+2
2(2H+ 1)(2H+ 2)
=(ℓ+ 2)2H+2 −4(ℓ+ 1)2H+2 + 6ℓ2H+2 −4(ℓ−1)2H+2 + (ℓ−2)2H+2
2(2H+ 1)(2H+ 2)
(2.12)
and for a general integer sequence kn,
An,ℓ,kn
t=−2K−1
H
H+1
2
(knδn)−1/2−HZt
0
1
kn
kn−1
X
i=0
∆3
1(ℓ−1−i+{u/δn}
kn)H+1/2
+
×Zu
[u/δn]δn
σvdWv(σuηu−σ[u/δn]δnη[u/δn]δn)du.
(2.13)
Under Assumption CLT, the process Zn
t= (Zn,1
t,...,Zn,d
t)Tsatisfies the joint CLT
(2.14) Znst
=⇒Z,
where Z= ((Z1
t,...,Zd
t)T)t≥0is a continuous Rd-valued process that is defined on a very
good filtered extension (¯
Ω,¯
F,¯
F= ( ¯
Ft)t≥0,¯
P)of the original probability space (see e.g. [35,
摘要:
展开>>
收起<<
arXiv:2210.01216v3[math.ST]14Jun2024STATISTICALINFERENCEFORROUGHVOLATILITY:CENTRALLIMITTHEOREMSBYCARSTENH.CHONG1,a,MARCHOFFMANN2,b,YANGHUILIU3,c,MATHIEUROSENBAUM4,dANDGRÉGOIRESZYMANSKI4,e1DepartmentofInformationSystems,BusinessStatisticsandOperationsManagement,TheHongKongUniversityofScienceandTechno...
声明:本站为文档C2C交易模式,即用户上传的文档直接被用户下载,本站只是中间服务平台,本站所有文档下载所得的收益归上传人(含作者)所有。玖贝云文库仅提供信息存储空间,仅对用户上传内容的表现方式做保护处理,对上载内容本身不做任何修改或编辑。若文档所含内容侵犯了您的版权或隐私,请立即通知玖贝云文库,我们立即给予删除!
相关推荐
-
VIP免费2024-11-14 22
-
VIP免费2024-11-23 3
-
VIP免费2024-11-23 4
-
VIP免费2024-11-23 3
-
VIP免费2024-11-23 4
-
VIP免费2024-11-23 28
-
VIP免费2024-11-23 11
-
VIP免费2024-11-23 21
-
VIP免费2024-11-23 12
-
VIP免费2024-11-23 5
分类:学术论文
价格:10玖币
属性:49 页
大小:552.77KB
格式:PDF
时间:2025-04-15
作者详情
-
Voltage-Controlled High-Bandwidth Terahertz Oscillators Based On Antiferromagnets Mike A. Lund1Davi R. Rodrigues2Karin Everschor-Sitte3and Kjetil M. D. Hals1 1Department of Engineering Sciences University of Agder 4879 Grimstad Norway10 玖币0人下载
-
Voltage-controlled topological interface states for bending waves in soft dielectric phononic crystal plates10 玖币0人下载