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Bootstrapping high-frequency jump tests

Prosper Dovonon

Department of Economics, Concordia University S´ılvia Gon¸calves

Department of Economics, University of Western Ontario Ulrich Hounyo

CREATES, Department of Economics and Business Economics, Aarhus University Nour Meddahi

Toulouse School of Economics, Toulouse University December 19, 2016

Abstract

The main contribution of this paper is to propose a bootstrap test for jumps based on functions of realized volatility and bipower variation. Bootstrap intraday returns are randomly generated from a mean zero Gaussian distribution with a variance given by a local measure of integrated volatility (which we call {vˆni}). We first discuss a set of high level conditions on{ˆvni} such that any bootstrap test of this form has the correct asymptotic size and is alternative-consistent. Our results show that the choice of {vˆni} is crucial for the power of the test. In particular, we should choose {ˆvin} in a way that is robust to jumps. We then focus on a thresholding-based estimator for{vˆin}and provide a set of primitive conditions under which our bootstrap test is asymptotically valid. We also discuss the ability of the bootstrap to provide second-order asymptotic refinements under the null of no jumps. The cumulants expansions that we develop show that our proposed bootstrap test is unable to mimic the first-order cumulant of the test statistic. The main reason is that it does not replicate the bias of the bipower variation as a measure of integrated volatility. We propose a modification of the original bootstrap test which contains an appropriate bias correction term and for which second-order asymptotic refinements obtain.

1 Introduction

A well accepted fact in financial economics is the fact that asset prices do not always evolve continuously over a given time interval, being instead subject to the possible occurrence of jumps (or discontinuous movements in prices). The detection of such jumps is crucial for asset pricing and risk management because the presence of jumps has important consequences for the performance of asset pricing models and hedging strategies, often introducing parameters that are hard to estimate (see e.g. Bakshi et al. (1997), Bates (1996), and Johannes (2004)). For this reason, many tests for jumps have been

We are grateful for comments from participants at the SoFie Annual Conference in Toronto, June 2014, and at the IAAE 2014 Annual Conference, Queen Mary, University of London, June 2014. We are also grateful to two anonymous referees and an associate editor for many valuable suggestions. Dovonon, Gon¸calves and Meddahi acknowledge financial support from a ANR-FQRSC grant. In addition, Ulrich Hounyo acknowledges support from CREATES - Center for Research in Econometric Analysis of Time Series (DNRF78), funded by the Danish National Research Foundation, as well as support from the Oxford-Man Institute of Quantitative Finance. Finally, Nour Meddahi has also benefited from the financial support of the chair “March´e des risques et cr´eation de valeur” Fondation du risque/SCOR.

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proposed in the literature over the years, most of the recent ones exploiting the rich information contained in high frequency data. These include tests based on bipower variation measures (such as in Barndorff-Nielsen and Shephard (2004, 2006), henceforth BN-S (2004, 2006), Huang and Tauchen (2005), Andersen et al. (2007), Jiang and Oomen (2008), and more recently Mykland, Shephard and Sheppard (2012)); tests based on power variation measures sampled at different frequencies (such as in A¨ıt-Sahalia and Jacod (2009), A¨ıt-Sahalia, Jacod and Li (2012)), and tests based on the maximum of a standardized version of intraday returns (such as in Lee and Mykland (2008, 2012)). In addition, tests based on thresholding or truncation-based estimators of volatility have also been proposed with the objective of disentangling big from small jumps, as in A¨ıt-Sahalia and Jacod (2009) and Cont and Mancini (2011), based on Mancini (2001). See A¨ıt-Sahalia and Jacod (2012, 2014) for a review of the literature on the econometrics of high frequency-based jump tests.

In this paper, we focus on the class of tests based on bipower variation originally proposed by Barndorff-Nielsen and Shephard (2004, 2006). Our main contribution is to propose a bootstrap im- plementation of these tests with better finite sample properties than the original tests based on the asymptotic normal distribution. In particular, our aim is to improve finite sample size while retaining good power. In order to do so, we generate the bootstrap observations under the null of no jumps, by drawing them randomly from a mean zero Gaussian distribution with a variance given by a local measure of integrated volatility (which we call {vˆni}).

Our first contribution is to give a set of high level conditions on {vˆin} such that any bootstrap method of this form has the correct asymptotic size and is alternative-consistent. We then verify these conditions for a specific example of {ˆvni} based on a threshold-based volatility estimator constructed from blocks of intraday returns which are appropriately truncated to remove the effect of the jumps. In particular, we provide primitive assumptions on the continuous price process such that the bootstrap jump test based on the thresholding local volatility estimator is able to replicate the null distribution of the BN-S test (2004, 2006) under both the null and the alternative of jumps. Our assumptions are very general, allowing for leverage effects and general activity jumps both in prices and volatility. We show that although truncation is not needed for the bootstrap jump test to control the asymptotic size under the null of no jumps, it is important to ensure that the bootstrap jump test is consistent under the alternative of jumps. Other choices of{vˆin}could be considered provided they are robust to jumps.

For instance, we could rely on multipower variation volatility measures rather than truncation-based methods to compute {ˆvni} and use our high level conditions to show the first order validity of this bootstrap method. For brevity, we focus on the thresholding-based volatility estimator, which is one of the most popular methods of obtaining jump robust test statistics.

The second contribution of this paper is to prove that an appropriate version of the bootstrap jump test based on thresholding provides a second-order asymptotic refinement under the null of no jumps. To do so, we impose more restrictive assumptions on the data generating process that assume away the presence of drift and leverage effects. For this simplified model, we develop second-order asymptotic expansions of the first three cumulants of the BN-S test statistic and of its bootstrap version. Our results show that the first-order cumulant of the BN-S test depends on the bias of bipower variation under the null of no jumps. Even though this bias does not impact the validity of the test to first order because bipower variation is a consistent estimator of integrated volatility under the null, it has an impact on the first order cumulant of the statistic at the second order (i.e. at the orderO(

n1/2)

). Our bootstrap test statistic is unable to capture this higher order bias and therefore does not provide a second-order refinement. We propose a modification of the bootstrap statistic that is able to do so. Specifically, the modified bootstrap test statistic contains a correction term that is based on an estimate of the contribution to the first order cumulant of the test statistic due to the bias of bipower variation. Our simulations show that although both bootstrap versions of the test outperform the asymptotic test, the modified bootstrap test statistic has lower size distortions than the original bootstrap statistic. In the empirical application, where we apply the bootstrap jump tests

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to 5-minutes returns on the SPY index over the period June 15, 2004 through June 13, 2014, this version of the bootstrap test detects about half of the number of jump days detected by the asymptotic theory-based tests.

The rest of the paper is organized as follows. In Section 2, we provide the framework and state our assumptions. In Section 3, we investigate the first-order asymptotic validity of the Gaussian wild bootstrap based on a given {vˆin}. Specifically, Section 3.1 contains a set of high level conditions on {vˆin} such that any bootstrap method is asymptotically valid when testing for jumps. Section 3.2 provides a set of primitive assumptions under which the bootstrap based on a thresholding estimator {vˆin} verifies these high level conditions and is therefore asymptotically valid to first order. Section 4 investigates the ability of the bootstrap to provide asymptotic refinements. In particular, Section 4.1 contains the second-order expansions of the cumulants of the original statistic whereas Section 4.2 contains their bootstrap versions. Section 5 gives the Monte Carlo simulations while Section 6 provides an empirical application. Section 7 concludes. Appendix A contains a law of large numbers for smooth functions of consecutive local truncated volatility estimates. This result is crucial for establishing the properties of the bootstrap jump test based on the thresholding approach. It is of independent interest as it extends some existing results in the literature, namely results by Jacod and Protter (2012), Jacod and Rosenbaum (2013) and Li, Todorov and Tauchen (2016)), who focused on smooth functions of a single local volatility estimate. In addition, an online supplementary appendix contains the proofs of all the results in the main text. Specifically, Appendix S1 contains the proofs of the bootstrap consistency results presented in Section 3 whereas Appendix S2 contains the proofs of the results in Section 4 (on the asymptotic refinements of the bootstrap). Finally, Appendix S3 contains formulas for the log version of our tests.

To end this section, a word on notation. As usual in the bootstrap literature, we letPdescribe the probability of bootstrap random variables, conditional on the observed data. Similarly, we writeEand V arto denote the expected value and the variance with respect toP, respectively. For any bootstrap statistic Zn Zn(·, ω) and any (measurable) set A, we write P(Zn ∈A) = P(Zn(·, ω)∈A) = Pr (Zn(·, ω)∈A|Xn), where Xn denotes the observed sample. We say that Zn P 0 in prob-P (or Zn=oP(1) in prob-P) if for anyε, δ >0,P(P(|Zn|> ε)> δ)→0 asn→ ∞. Similarly, we say that Zn=OP(1) in prob-P if for anyδ >0, there exists 0< M <∞such thatP(P(|Zn| ≥M)> δ)→0 as n → ∞. For a sequence of random variables (or vectors) Zn, we also need the definition of convergence in distribution in prob-P. In particular, we write Zn d Z, in prob-P (a.s.-P), if E(f(Zn))→E(f(Z)) in prob-P for every bounded and continuous function f (a.s.−P).

2 Assumptions and statistics of interest

We assume that the log-price process Xt is an Itˆo semimartingale defined on a probability space (Ω,F, P) equipped with a filtration (Ft)t0 such that

Xt=Yt+Jt, t≥0, (1)

where Yt is a continuous Brownian semimartingale process and Jt is a jump process. Specifically, Yt is defined by the equation

Yt=Y0+

t

0

asds+

t

0

σsdWs,t≥0, (2)

where a and σ are two real-valued random processes and W is a standard Brownian semimartingale process. The jump process is defined as

Jt=

t

0

R

(δ(s, x)I{|δ(s,x)|≤1})

−ν) (ds, dx) +

t

0

R

(δ(s, x)I{|δ(s,x)|>1})

µ(ds, dx), (3)

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whereµis a Poisson random measure onR+×Rwith intensity measure ν(ds, dx) =ds⊗λ(dx), with λthe Lebesgue measure onR, andδ a real function on Ω×R+×R. The first term in the definition of Jt represents the “small” jumps of the process whereas the second term represents the “big” jumps.

We make the following assumptions on a, σ andJt, wherer∈[0,2].

Assumption H-r The process a is locally bounded, σ is c`adl`ag, and there exists a sequence of stopping times (τn) and a deterministic nonnegative functionγnonRsuch that∫

γn(x)rλ(dx)<

and (ω, s, x)| ∧1≤γn(x) for all (ω, s, x) satisfying s≤τn(ω).

Assumption H-r is rather standard in this literature, implying that the rth absolute power value of the jumps size is summable over any finite time interval, i.e. ∑

st|∆Xs|r<∞ for all t >0. Since H-r for some r implies that H-r holds for all r > r, the weakest form of this assumption occurs for r = 2 (and essentially corresponds to the class of Itˆo semimartingales). Asrdecreases towards 0, fewer jumps of bigger size are allowed. In the limit, when r= 0, we get the case of finite activity jumps.

The quadratic variation process of X is given by [X]t = IVt+J Vt, where IVt t

0 σ2sds is the quadratic variation of Yt, also known as the integrated volatility, and J Vt

st(∆Js)2 is the jump quadratic variation, with ∆Js =Js−Js denoting the jumps in X. Without loss of generality, we let t= 1 and we omit the indext. For instance, we writeIV =IV1 and J V =J V1.

We assume that prices are observed within the fixed time interval [0,1] (which we think of as a given day) and that the log-prices Xt are recorded at regular time points ti =i/n, for i= 0, . . . , n, from which we compute nintraday returns at frequency 1/n,

ri ≡Xi/n−X(i1)/n, i= 1, . . . , n, where we omit the index ninri to simplify the notation.

Our focus is on testing for “no jumps” using the bootstrap. In particular, following A¨ıt-Sahalia and Jacod (2009), we would like to decide on the basis of the observed intraday returns {ri :i= 1, . . . , n}

in which of the two following complementary sets the path we actually observed falls:

0 = :t7−→Xt(ω) is continuous on [0,1]}1 = :t7−→Xt(ω) is discontinuous on [0,1]},

where Ω = Ω0 1 and Ω01 = ∅.Formally, our null hypothesis can be defined as H0 : ω 0

whereas the alternative hypothesis isH1 :ω∈1. LetRVn=∑n

i=1r2i denote the realized volatility and let BVn= 1

k12

n i=2

|ri1| |ri| be the bipower variation, where we let k1 E(χ211/2)

= E(|Z|) = 2/

π, where Z N(0,1).

This is a special case ofkq=E(χ21q/2)

=E(|Z|q) = 2q/2 Γ(1+q2 )

Γ(12) , q >0.

The class of statistics we consider is based on the comparison between RVn and BVn. It is now well known that under certain regularity conditions including the assumption that X is continuous (see BN-S (2006) and Barndorff-Nielsen, Graversen, Jacod, and Shephard (2006)) the following joint CLT holds:

√n

( RVn−IV BVn−IV

)

−→st N(0,Σ), (4)

where −→st denotes stable convergence and Σ =

( 2 2 2 θ

)

IQ, (5)

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withIQ≡1

0 σ4uduand θ=(

k141) + 2(

k121)

2.6090.

An implication of (4) is that under “no jumps”, i.e. in restriction to Ω0,

√n(RVn−BVn)

√V

−→st N(0,1), whereV ≡τ·IQis the asymptotic variance of

n(RVn−BVn) andτ =θ−2.Hence, a linear version of the test is given by

Tn=

√n(RVn−BVn)

Vˆn

, (6)

where

Vˆn≡τ·IQcn with IQcn= n (k4/3)3

n i=3

|ri|4/3|ri−1|4/3|ri−2|4/3.

Choosing the tripower realized quarticity ensures that IQcn−→P IQ on both Ω0 and Ω1.Thus,Tn

−→st

N(0,1), in restriction to Ω0, and the test that rejects the null of “no jumps” at significance level α whenever Tn > z1α, where z1α is the 100 (1−α) % percentile of the N(0,1) distribution has asymptotically correct strong size, i.e. the critical region Cn = {Tn> z1α} is such that for any measurable setS 0 such thatP(S)>0,

nlim→∞P∈ Cn|S) =α.

Under the alternative hypothesis, we can show that Tn is alternative-consistent, i.e. the probability that we make the incorrect decision of “accepting the null” when this is false goes to zero:

nlim→∞P(

1∩C¯n

) = 0,

where ¯Cn is the complement ofCn. Since the above condition implies that P(C¯n|1

) 0, as n→ ∞, we have thatP(Cn|1)1 asn→ ∞, which we can interpret as saying that the test has asymptotic power equal to 1.

3 The bootstrap

When bootstrapping hypothesis tests, imposing the null hypothesis on the bootstrap data generating process is not only natural, but may be important to minimize the probability of a type I error.

In particular, Davidson and MacKinnon (1999) (see also MacKinnon (2009)) show that in order to minimize the error in rejection probability under the null (type I error) of a bootstrap test, we should estimate the bootstrap DGP as efficiently as possible. This entails imposing the null hypothesis on the bootstrap DGP.

In this paper, we follow this rule and impose the null hypothesis of no jumps when generating the bootstrap intraday returns. Specifically, we let

ri=√ ˆ

vni ·ηi, i= 1, . . . , n, (7)

for some variance measure ˆvinbased on{ri:i= 1, . . . , n}, and where ηi is generated independently of the data as an i.i.d. N(0,1) random variable. For simplicity, we again write ri instead ofri,n.

According to (7), bootstrap intraday returns are conditionally (on the original sample) Gaussian with mean zero and volatility ˆvni, and therefore do not contain jumps. This bootstrap DGP is motivated

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by the simplified modelXt=∫t

0σsdWs, whereσ is independent ofW and there is no drift nor jumps1. Under these assumptions, conditionally on the path of volatility,ri∼N(0, vin),independently across i, wherevin=∫i/n

(i1)/nσu2du. Thus, we can think of ˆvinas the sample analogue ofvin. The main goal of Section 3.1 is to provide a set of general conditions on ˆvinunder which the bootstrap is asymptotically valid. In practice, we need to choose ˆvin and our recommendation is to use a thresholding estimator that we define formally in Section 3.2.

The bootstrap analogues ofRVn and BVn are RVn =

n i=1

ri2 and BVn = 1 k21

n i=2

ri1|ri|.

The first class of bootstrap statistics we consider is described as Tn=

√n(RVn−BVn−E(RVn−BVn))

Vˆn

, (8)

where

E(RVn−BVn) =

n i=1

ˆ vni

n i=2

(vˆin1)1/2

vin)1/2, and

Vˆn =τ ·IQcn with IQcn= n (k4/3)3

n i=3

|ri|4/3ri14/3ri24/3.

Thus,Tn is exactly as Tn except for the recentering ofRVn−BVn around the bootstrap expectation E(RVn−BVn). This ensures that the bootstrap distribution ofTn is centered at zero, as is the case forTn under the null hypothesis of no jumps whennis large.

Nevertheless, and as we will study in Section 4, Tn has a higher order bias under the null which is not well mimicked by Tn, implying that this test does not yield asymptotic refinements. For this reason, we consider a second class of bootstrap statistics based on

T¯n=

√n(RVn−BVn−E(RVn−BVn))

Vˆn

+1 2

√nv1n+ ˆvnn)

Vˆn

, (9)

where the second term accounts for the higher-order bias inTn. This correction has an impact in finite samples, as our simulation results show. In particular, ¯Tn has lower size distortions than Tn under the null , especially for the smaller sample sizes.

Next, we provide general conditions on ˆvin under whichTn −→d N(0,1),in prob-P independently of whether ω 0 orω 1. The consistency of the bootstrap then follows by verifying these high level conditions for a particular choice of ˆvin.We verify them for a thresholding-based estimator, but other choices of ˆvin could be considered. For instance, we could rely on local multipower realized volatility estimators of vin, following the approach of Mykland, Shephard and Sheppard (2012)) (see also Mykland and Zhang (2009)). Asymptotic refinements of the bootstrap based on ¯Tn will be discussed in Section 4.

1Although (7) is motivated by this very simple model, as we will prove below, this does not prevent the bootstrap method to be valid more generally. In particular, its validity extends to the case where there is a leverage effect and the drift is non-zero.

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3.1 Bootstrap validity under general conditions on vˆni

We first provide a set of conditions under which a joint bootstrap CLT holds for (RVn, BVn). In particular, we would like to establish that

Σn1/2 n

( RVn−E(RVn) BVn−E(BVn)

)

d

−→N(0, I2), in prob-P, where

Σn≡V ar (

n

( RVn BVn

))

=

( V ar(

nRVn) Cov(

nRVn,√ nBVn) V ar(

nBVn)

) ,

is such that Σn −→P Σ. The following result gives the first and second order bootstrap moments of (RVn, BVn).Note that since ri =√

ˆ

vni ·ηi, we can write RVn =

n i=1

ˆ

vin·ui and BVn = 1 k12

n i=2

(vˆin1)1/2

vni)1/2·wi

where ui ≡η2i and wi ≡ |ηi1| |ηi|, with ηi i.i.d. N(0,1). The bootstrap moments of (RVn, BVn) depend on the moments and dependence properties of (ui, wi).The proof is trivial and is omitted for brevity.

Lemma 3.1 If ri =√ ˆ

vin·ηi, i= 1, . . . , n, where ηi ∼i.i.d. N(0,1), then (a1) E(RVn) =

n i=1

ˆ vin. (a2) E(BVn) =

n i=2

(vˆin1)1/2

vni)1/2. (a3) V ar(

nRVn) = 2n

n i=1

vin)2. (a4) V ar(

nBVn) =(

k141) n

n i=2

vni)( ˆ vin1)

+ 2(

k121) n

n i=3

vin)1/2( ˆ vin1) (

ˆ vin2)1/2

. (a5) Cov(

nRVn,√

nBVn) =n

n i=2

vin)3/2( ˆ vin1)1/2

+n

n i=2

vin)1/2( ˆ vin1)3/2

.

Lemma 3.1 shows that the bootstrap moments ofRVn and BVn depend on multipower variation measures of {vˆin}. In particular, they depend onn1+q/2

n i=K

K k=1

(vˆink+1)qk/2

, where K is a positive integer and q K

k=1qk,withqk 0.

The following assumption imposes a convergence condition on these measures as well as other additional high level conditions on ˆvni that are sufficient for a bootstrap CLT to hold. Note that this is a high level condition that does not depend on specifying whether we are on Ω0 or on Ω1.

Condition A Suppose that {vˆin} satisfies the following conditions:

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(i) For any K N and any sequence {qk R+ : k = 1, . . . , K} of nonnegative numbers such that 0≤q K

k=1qk8,

n−1+q/2

n i=K

K k=1

(vˆnik+1)qk/2 P

−→

1

0

σuqdu >0, asn→ ∞.

(ii) There exists α [0,37) such that n[n/(Ln+1)]

j=1

( ˆ vnj(L

n+1)

)2

= oP (1), where Ln nα and [x]

denotes the largest integer smaller or equal tox.

Condition A(i) requires the multipower variations of ˆvni to converge to∫1

0 σuqdufor anyq 8.Under this condition, the probability limit of Σn, the bootstrap covariance matrix of

n(RVn, BVn),is equal to Σ (for this result, convergence of the multipower variations of ˆvinwithq= 4 suffices). Together with Condition A(i), Condition A(ii) is used to show that a CLT holds for

n(RVn−E(RVn), BVn−E(BVn)) in the bootstrap world. In particular, since the vector (ui, wi) is lag-one dependent, we adopt a large-block-small-block argument, where the large blocks are made of Ln consecutive observations and the small block is made of a single element. Part (ii) ensures that the contribution of the small blocks is asymptotically negligible. The proof of Theorem 3.1 then follows by showing that Vˆn =τ ·IQcn −→P V =τ ·IQ under Condition A(i) (this follows from the convergence of the multi- power variations of ˆvni of eighth order, explaining why we require q 8).

Under this high level condition, we can prove the following result.

Theorem 3.1 Under Condition A, if n→ ∞, Tn−→d N(0,1), in prob-P.

Since Tn st

−→ N(0,1) on Ω0, the fact that Tn −→d N(0,1), in prob-P, ensures that the test has correct size asymptotically. Under the alternative (i.e. on Ω1) since Tn diverges at rate

n, but we still have that Tn −→d N(0,1), the test has power asymptotically. More formally, let the bootstrap critical region be defined as follows,

Cn ={

ω:Tn(ω)> qn,1 α(ω)} , where qn,1α(ω) is such that

P(

Tn(·, ω)≤qn,1α(ω))

= 1−α.

The bootstrap test rejects H0 : ω 0 against H1 : ω 1 whenever ω ∈ Cn. The following theorem follows from Theorem 3.1 and the asymptotic properties of Tn underH0 and under H1. Theorem 3.2 Suppose Tn −→st N(0,1), in restriction to Ω0, and Tn −→P + on1. If Condition A holds, then the bootstrap test based on Tn controls the asymptotic strong size and is alternative- consistent.

3.2 Bootstrap validity when ˆvin is based on thresholding

The results of the previous subsection ensure the consistency of the bootstrap distribution of Tn for any choice of ˆvin that verifies Condition A. In this section, we verify this condition for the following choice of ˆvin:

ˆ

vj+(in 1)kn = 1 kn

kn

m=1

r2(i1)kn+m1(r(i1)kn+m≤un

),

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wherei= 1, . . . ,kn

n andj= 1, . . . , kn. Here, kn is an arbitrary sequence of integers such thatkn→ ∞ and kn/n→0 and un is a sequence of threshold values defined as

un=αnϖ for some constantα >0 and 0< ϖ <1/2.

We will maintain these assumptions on kn and un throughout. The estimator ˆvin is equal to n1 times a “spot volatility” estimator that is popular in the high-frequency econometrics literature under jumps (see e.g. Mancini (2001) and A¨ıt-Sahalia and Jacod (2009)). By excluding all returns containing jumps over a given threshold when computing ˆvin,we guarantee that the bootstrap distribution ofTn converges to a N(0,1) random variable, independently of whether there are jumps or not. This is crucial for the bootstrap test to control asymptotic size and at the same time have power.

The following lemma is auxiliary in verifying Condition A.

Lemma 3.2 Assume that X satisfies (1), (2) and (3) such that Assumption H-2 holds. Let q =

K

k=1qk withqk0 and K N. If either of the following conditions holds:

(a) q >0 and X is continuous;

(b) q <2 ;

(c) q 2, Assumption H-r holds for somer [0,2),and 2qq−1r ≤ϖ < 12; then n1+q/2

n i=K

K k=1

(vˆni−k+1)qk/2 P

−→

1

0

σuqdu >0.

Lemma 3.2 follows from Theorem A.1 in Appendix A, a result that is of independent interest and can be seen as an extension of Theorem 9.4.1 of Jacod and Protter (2012) (see also Jacod and Rosenbaum (2013)). In particular, Theorem A.1 provides a law of large numbers for smooth functions of consecutive truncated local realized volatility estimators defined on non-overlapping time intervals.

Instead, Theorem 9.4.1 of Jacod and Protter (2012) only allows for functions that depend on a sin- gle local realized volatility estimate even though they are possibly based on overlapping intervals.

Recently, Li, Todorov and Tauchen (2016) focus on single local realized volatility estimate based on non-overlapping intervals and extend the limit results of Theorem 9.4.1 of Jacod and Protter (2012) to a more general class of volatility functionals that do not have polynomial growth. Here we restrict our attention to functions that have at most polynomial growth, which is enough to accommodate the blocked multipower variations measures of Lemma 3.2.

Given this result, we can state the following theorem.

Theorem 3.3 Assume that X satisfies (1), (2), (3) such that Assumption H-2 holds. If in addition, either of the two following conditions holds:

(a) X is continuous; or

(b) Assumption H-r holds for some r [0,2) and 167r ≤ϖ < 12;

then the conclusion of Theorem 3.1 holds for the thresholding-based bootstrap testTn.

Theorem 3.3 shows that the thresholding-based statistic Tn is asymptotically distributed as a standard normal random variable independently of whether the null of no jumps is true or not. This guarantees that the bootstrap jump test has the correct asymptotic size and is consistent under the alternative of jumps. Note that under the null, whenX is continuous, the result holds for any level of

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truncation, including the case where un = , which corresponds to no truncation. Nevertheless, to ensure thatTnis also asymptotically normal under the alternative hypothesis of jumps some truncation is required. Part (b) of Theorem 3.3 shows that we should choose un =αnϖ with 167r ≤ϖ < 12, a condition that is more stringent than the usual condition on ϖ (which is 0 < ϖ < 1/2). The lower bound on ϖis an increasing function of r, a number that is related to the degree of activity of jumps as specified by Assumption H-r. For finite activity jumps where r = 0, ϖ should be larger or equal than 7/16 but strictly smaller than 1/2.Asr increases towards 2 (allowing for an increasing number of small jumps), the range of values ofϖbecomes narrower, implying that we need to choose a smaller level of truncation in order to be able to separate the Brownian motion from the jumps contributions to returns.

The following result is a corollary to Theorem 3.3.

Corollary 3.1 Assume that X satisfies (1), (2), (3) such that Assumption H-r holds for some r [0,2) and let un=αnϖ with 167r ≤ϖ < 12. Then, the conclusions of Theorem 3.2 are true for the thresholding-based bootstrap test Tn.

This result shows that the thresholding-based bootstrap jump test has the correct asymptotic size and is consistent under the alternative of jumps provided we choose a truncation levelun=αnϖwith

7

16r ≤ϖ < 12,wherer is [0,2). In particular, if we chooseϖin the vicinity of 1/2, as commonly done in applications, the bootstrap test is consistent under the alternative of jumps for a wide spectrum of jump activities including finite activity. For example, ifϖ= 0.45, the set ofrsuch thatϖ≥7/(16−r) is [0,0.444] and whenϖ= 0.48, this set becomes [0,1.417].

4 Second-order accuracy of the bootstrap

In this section, we investigate the ability of the bootstrap test based on the thresholding local realized volatility estimator to provide asymptotic higher-order refinements under the null hypothesis of no jumps. Our analysis is based on the following simplified model for Xt,

Xt=

t

0

σsdWs, (10)

where σ is c`adl`ag locally bounded away from 0 and ∫t

0 σs2ds < for all t [0,1]. In addition, we assume thatσ is independent of W.Thus, we not only impose the null hypothesis of no jumps under which Jt= 0,but we also assume that there is no drift nor leverage effects. Under these assumptions, conditionally on the path of volatility, ri N(0, vni) independently across i, a result that we will use throughout this section. Allowing for the presence of drift and leverage effects would complicate substantially our analysis. In particular, we would not be able to condition on the volatility path σ when deriving our expansions if we relaxed the assumption of independence between σ and W. Allowing for the presence of a drift would require a different bootstrap method, the main reason being that the effect of the drift on the test statistic is of order O(

n1/2)

and our bootstrap returns have mean zero by construction (see Gon¸calves and Meddahi, 2009). We leave these important extensions for future research.

To study the second-order accuracy of the bootstrap, we rely on second-order Edgeworth expansions of the distribution of our test statisticsTnandTn. As is well known, the coefficients of the polynomials entering a second-order Edgeworth expansion are a function of the first three cumulants of the test statistics (cf. Hall, 1992). In order to derive these higher-order cumulants, we make the following additional assumption. We rely on it to obtain the limit of the first order cumulant of Tn (cf. κ1,1 below).

(11)

Assumption V The volatility process σ2u is pathwise continuous, bounded away from zero and Holder-continuous inL2(P) on [0,1] of order δ >1/2,i.e., E((

σu2−σ2s)2)

=O(|u−s|).

Thus, we not only impose that the volatility path is continuous, but we also rule out stochastic volatility models driven by a Brownian motion. Examples of processes that satisfy Assumption V include fractional Brownian motion with Hurst parameter H >1/2.

4.1 Second-order expansions of the cumulants of Tn

Next we provide asymptotic expansions for the cumulants ofTn. For any positive integeri,letκi(Tn) denote the ith cumulant of Tn. In particular, recall that κ1(Tn) = E(Tn), κ2(Tn) = V ar(Tn) and κ3(Tn) =E(Tn−E(Tn))3.In addition, for anyq >0,we let σq=∫1

0 σuqdu.

Theorem 4.1 Assume that X satisfies (10) and Assumption V holds, where σ is independent ofW. Then, conditionally on σ, we have that

κ1(Tn) = 1

√n

 1 2

τ

σ02+σ12

σ4 −a1 2

σ6 (

σ4 )3/2



| {z }

κ11,11,2

+O (1

n )

;

κ2(Tn) = 1 +O (1

n )

; and κ3(Tn) = 1

√n (

a2+3

2(a1−a3)

) σ6 (

σ4 )3/2

| {z }

κ3

+O (1

n )

,

where τ = θ−2 = (

k141) + 2(

k121)

2 and the constants a1, a2 and a3 also depend on kq =E|Z|q, Z ∼N(0,1), for certain values of q >0; their specific values are given in Lemma S2.5 in the Appendix.

Theorem 4.1 shows that the first and third order cumulants ofTnare subject to a higher order bias of order O(

n1/2)

, given by the constants κ1 and κ3. Since the asymptotic normal approximation assumes that the values of these cumulants are zero, this induces an error of order O(

n1/2)

for the asymptotic normal approximation when approximating the null distribution ofTn.

The bootstrap is asymptotically second-order accurate if the bootstrap first and third order cumu- lants mimicκ1 and κ3. As it turns out, this is not true for the bootstrap test based onTn. The main reason is that it fails to capture κ1,1, a bias term that is due to the fact that bipower variation is a biased (but consistent) estimator ofIV. To understand how this bias impacts the first order cumulant of Tn, note that we can write

Tn=

√n(RVn−BVn)

Vˆn

= (Sn+An) (

1 + 1

√n(Un+Bn) )1/2

, (11)

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