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Contents lists available atScienceDirect

Journal of Multivariate Analysis

journal homepage:www.elsevier.com/locate/jmva

Likelihood ratio order of the second order statistic from independent

heterogeneous exponential random variables

I

Peng Zhao

a

, Xiaohu Li

a,∗

, N. Balakrishnan

b

aSchool of Mathematics and Statistics, Lanzhou University, Lanzhou 730000, China

bDepartment of Mathematics and Statistics, McMaster University, Hamilton, Ontario, Canada L8S 4K1

a r t i c l e i n f o Article history:

Received 5 February 2008 Available online 24 September 2008

AMS subject classifications:

primary 60E15 secondary 60K10

Keywords:

Majorization order Weakly majorization order

p-larger order

Hazard rate order

a b s t r a c t

Let X1, . . . ,Xnbe independent exponential random variables with respective hazard rates

λ1, . . . , λn, and let Y1, . . . ,Ynbe independent exponential random variables with common hazard rateλ. This paper proves that X2:n, the second order statistic of X1, . . . ,Xn, is larger than Y2:n, the second order statistic of Y1, . . . ,Yn, in terms of the likelihood ratio order if and only if λ ≥ 1 2n−1  2Λ1+Λ 3−Λ1Λ2 Λ2 1−Λ2 

withΛk=Pni=1λki,k=1,2,3. Also, it is shown that X2:nis smaller than Y2:nin terms of the likelihood ratio order if and only if

λ ≤ n P i=1 λi−max 1≤inλi n−1 .

These results form nice extensions of those on the hazard rate order in Pˇaltˇanea [E. Pˇaltˇanea, On the comparison in hazard rate ordering of fail-safe systems, Journal of Statistical Planning and Inference 138 (2008) 1993–1997].

© 2008 Elsevier Inc. All rights reserved. 1. Introduction

Order statistics play an important role in statistics, reliability theory, and many applied areas. Let X1:n

X2:n

≤ · · · ≤

Xn:n

denote the order statistics of random variables X1

,

X2

, . . . ,

Xn. It is well known that the kth order statistic Xk:nis the lifetime

of an

(

n

k

+

1

)

-out-of-n system, which is a very popular structure of redundancy in fault-tolerant systems and has been applied in industrial and military systems. In particular, the lifetimes of parallel and series systems correspond to the order statistics, Xn:nand X1:n. Order statistics have been extensively investigated in the case when the observations are independent

and identically distributed (i.i.d). However, in some practical situations, observations are non-i.i.d. Due to the complicated expression of the distribution in the non-i.i.d case, only limited results are found in the literature. One may refer to [1–3] for comprehensive discussions on this topic, and the recent review article of [4] for results on the independent and non-identically distributed (i.ni.d) case.

Due to the nice mathematical form and the unique memoryless property, the exponential distribution has widely been applied in statistics, reliability, operations research, life testing and other areas. Readers may refer to [5,6] for an encyclopedic

ISupported by the National Natural Science Foundation of China (10771090).

Corresponding author.

E-mail addresses:xhli@lzu.edu.cn,mathxhli@hotmail.com(X. Li). 0047-259X/$ – see front matter©2008 Elsevier Inc. All rights reserved. doi:10.1016/j.jmva.2008.09.010

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treatment to developments on the exponential distribution. Here, we will focus on the second order statistic, which characterizes the lifetime of the

(

n

1

)

-out-of-n system (referred as the fail-safe system) in reliability theory and yields the winner’s price for the bid in the second price reverse auction; see, for example, [7,8]. Pledger and Proschan [9] were among the first to compare stochastically the order statistics of non-i.i.d exponential random variables with corresponding order statistics from i.i.d exponential random variables. Since then, many researchers followed up this topic including [10–18]. It is also worth noting that some stochastic comparison results on order statistics from two i.ni.d. (not necessarily exponential) samples are closely related to the subject matter of this paper. For instance, [19] proved that the order statistics from two different collections of random variables are ordered in the likelihood ratio order if the underlying random variables are so ordered. Similar results were also given by [20].

For ease of reference, let us first recall some stochastic orders which are closely related to the main results to be developed here in this paper. Throughout, the term increasing stands for monotone non-decreasing and the term decreasing stands for

monotone non-increasing.

Definition 1.1. For two random variables X and Y with their densities f , g and distribution functions F , G, letF

¯

=

1

F and

¯

G

=

1

G. As the ratios in the statements below are well defined, X is said to be smaller than Y in the:

(i) likelihood ratio order (denoted by X

lrY ) if g

(

x

)/

f

(

x

)

is increasing in x; (ii) hazard rate order (denoted by X

hrY ) ifG

¯

(

x

)/¯

F

(

x

)

is increasing in x; (iii) stochastic order (denoted by X

stY ) ifG

¯

(

x

) ≥ ¯

F

(

x

)

.

For a comprehensive discussion on stochastic orders, one may refer to [21,22].

Suppose X1

, . . . ,

Xnare independent exponential random variables with Xi having hazard rate

λ

i, i

=

1

, . . . ,

n. Let

Y1

, . . . ,

Ynbe a random sample of size n from an exponential distribution with common hazard rate

λ

. Bon and Pˇaltˇanea [16]

showed, for 1

k

n, Xk:n

stYk:n

⇐⇒

λ ≥

"



n k



−1

X

1≤i1<···<ikn

λ

i1

. . . λ

ik

#

1k

.

(1.1)

Recently, [18] further proved

X2:n

hrY2:n

⇐⇒

λ ≥ ˇλ =

s



n 2



−1

X

1≤i<jn

λ

i

λ

j (1.2) and X2:n

hrY2:n

⇐⇒

λ ≤

n

P

i=1

λ

i

max 1≤in

λ

i n

1

.

(1.3)

These two results partially improve(1.1)in the case with k

=

2.

This paper investigates the likelihood ratio order instead. In this regard, it is proved that

X2:n

lrY2:n

⇐⇒

λ ≥ ˆλ =

1 2n

1



2Λ1

+

Λ3

Λ1Λ2 Λ2 1

Λ2



(1.4) withΛk

=

P

ni=1

λ

ki, k

=

1

,

2

,

3. Also, X2:n

lrY2:n

⇐⇒

λ ≤

n

P

i=1

λ

i

max 1≤in

λ

i n

1

.

(1.5)

These two results form nice extensions of(1.2)and(1.3). Some examples of special cases are given for illustrating the performance of our main results.

2. Preliminaries

This section presents some useful lemmas, which are not only helpful for proving our main results in what follows, but are also of independent interest.

Definition 2.1. Suppose two vectors x

=

(

x1

, . . . ,

xn

)

and y

=

(

y1

, . . . ,

yn

)

. Let x(1)

≤ · · · ≤

x(n)and y(1)

≤ · · · ≤

y(n)be

(3)

(i) x

=

(

x1

, . . . ,

xn

) ∈

Rnis said to majorize y

=

(

y1

, . . . ,

yn

) ∈

Rn(written as x m



y) if j

X

i=1 x(i)

j

X

i=1 y(i)

,

for j

=

1

, . . . ,

n

1

,

and

P

n i=1x(i)

=

P

n i=1y(i);

(ii) x

Rnis said to weakly majorize y

Rn(written as x



w y) if j

X

i=1 x(i)

j

X

i=1 y(i)

,

for j

=

1

, . . . ,

n

;

(iii) x

Rn

+is said to be p-larger than y

Rn+(written as x

p



y) if j

Y

i=1 x(i)

j

Y

i=1 y(i)

,

for j

=

1

, . . . ,

n

.

Clearly, x



m y implies x



w y, and x



p y is equivalent to log

(

x

)



w log

(

y

)

. Here log

(

x

)

is the vector of logarithms of the coordinates of x. Khaledi and Kochar [14] proved that x



m y implies x



p y for x

,

y

Rn+. The converse is, however, not true. Those functions that preserve the majorization ordering are said to be Schur-convex. For more discussions on majorization orders and their applications, see [23,13,15].

Boland et al. [24] proved that, for X1

,

X2

,

Y1

,

Y2, independent exponential random variables with respective hazard rates

λ

1

, λ

2

, λ

∗1

, λ

∗ 2,

1

, λ

2

)

m



1

, λ

2

) H⇒

X1

+

X2

lrY1

+

Y2

.

(2.1)

As the first result,Theorem 2.2presents a characterization of X1

+

X2

lrY1

+

Y2and hence improves(2.1). It should

be remarked here that [25] built this result in a completely different but lengthy way, and also that it is only a one-way implication. Here, we present a simple and brief proof and summarize it in terms of the weakly majorization order, and moreover it is a two-way implication result.

Theorem 2.2. For independent exponential random variables X1

,

X2

,

Y1

,

Y2with respective hazard rates

λ

1

, λ

2

, λ

∗1

, λ

2,

X1

+

X2

lrY1

+

Y2

⇐⇒

1

, λ

2

)

w



1

, λ

2

).

Proof. Without loss of generality, let us assume

λ

1

λ

2and

λ

∗1

λ

2.

⇐H

If

λ

1

λ1+λ2

2 , let Z and W be two independent exponential random variables with common hazard rate

λ1+λ2 2 . Obviously, we have λ1+λ2 2

λ

∗ 1

λ

2. Since the exponential distribution has log-concave density, from Theorem 1.C.9 of

[21], it follows that Z

+

W

lrY1

+

Y2. On the other hand, we also have



λ1+λ2 2

,

λ1+λ2 2



m



1

, λ

2

)

. By Example 1.C.50 of [21], we have X1

+

X2

lrZ

+

W . Now, we reach the required result by transitivity.

If

λ

1

<

λ1+λ2

2 , it is easy to observe that

λ

1

λ

∗1

<

λ

1

+

λ

2 2

< λ

1

+

λ

2

λ

∗ 1

min

2

, λ

∗2

).

Since

1

, λ

2

)

m



1

, λ

1

+

λ

2

λ

1

)

, we have X1

+

X2

lrX10

+

X 0 2, where X 0 1and X 0

2are independent exponentials having

respective hazard rates

λ

1and

λ

1

+

λ

2

λ

∗1. On the other hand, as discussed above, it also holds that X

0

1

+

X

0

2

lrY1

+

Y2.

Hence, we reach the required result again.

H⇒

Denote by f12)and f∗ 1,λ

2)the density functions of X1

+

X2and Y1

+

Y2, respectively. If

λ

1

> λ

∗ 1, then lim t→∞ f12)

(

t

)

f∗ 1,λ ∗ 2)

(

t

)

=

lim t→∞ λ1λ2 λ2−λ1

·

e −λ1t

e−λ2t



λ∗ 1λ ∗ 2 λ∗ 2−λ∗1

·



e−λ∗1t

e−λ∗2t



=

lim t→∞

λ

1

λ

2

∗2

+

λ

∗ 1

)

λ

∗ 1

λ

∗ 2

2

λ

1

)

·

1

e (λ1−λ2)t 1

e(λ∗1−λ∗2)t

·

e(λ∗1−λ1)t

=

0

.

This contradicts the fact that f(λ1,λ2)(t) f(λ∗1,λ∗2)(t)

(4)

On the other hand, by Taylor’s expansion at the origin, we have, for t

>

0, f12)

(

t

) = λ

1

λ

2



t

λ

1

+

λ

2 2 t 2



+

o t2



,

and its derivative

f0 1,λ2)

(

t

) = λ

1

λ

2

λ

1

λ

2

1

+

λ

2

)

t

+

o

(

t

).

As a result, f0 (λ1,λ2)

(

t

)

f12)

(

t

)

=

λ

1

λ

2

λ

1

λ

2

1

+

λ

2

)

t

+

o

(

t

)

λ

1

λ

2t

+

o

(

t

)

=

1 t

1

+

λ

2

) +

o

(

1

).

Similarly, f0∗ 1,λ ∗ 2)

(

t

)

f∗ 1,λ ∗ 2)

(

t

)

=

1 t

∗ 1

+

λ

∗ 2

) +

o

(

1

).

By X1

+

X2

lrY1

+

Y2, we have, for t

>

0, f0 1,λ2)

(

t

)

f12)

(

t

)

f0∗ 1,λ ∗ 2)

(

t

)

f∗ 1,λ ∗ 2)

(

t

)

,

and this implies

λ

1

+

λ

2

λ

∗1

+

λ

2. 

The following lemma will be used to proveLemma 2.4.

Lemma 2.3 ([23], p. 57). Let I

R be an open interval. A continuously differentiable function

ϕ :

In

R is Schur-convex on In

if and only if, for all i

6=

j and z

In,

(

zi

zj

) ϕ

(i)

(

z

) − ϕ

(j)

(

z

) ≥

0

,

where

ϕ

(i)

(

z

)

is the partial derivative with respect to its ith argument.

The lemma below will be useful to prove the main result in the next section. For brevity, let us first introduce the notation

Λk

=

P

n i=1

λ

k i

,

k

=

1

,

2

,

3 andΛ

(

m

) = P

n i=1

λ

i

λ

m

,

m

=

1

, . . . ,

n. Lemma 2.4. Let

λ = (λ

1

, . . . , λ

n

)

be a positive vector. Then

¯

λ ≥ ˆλ =

1 2n

1



2Λ1

+

Λ3

Λ1Λ2 Λ2 1

Λ2



,

(2.2) where

λ =

¯

1n

P

n

i=1

λ

iis the arithmetic mean of

λ

0s. Proof. The right side of(2.2)may be rewritten as

ˆ

λ =

1 2n

1



2Λ1

+

Λ3

Λ1Λ2 Λ2 1

Λ2



=

1 2n

1

2Λ1

n

P

i=1

λ

2 iΛ

(

i

)

n

P

i=1

λ

iΛ

(

i

)

.

To reach the required result, we need to prove

ˆ

λ =

1 2n

1

2Λ1

n

P

i=1

λ

2 iΛ

(

i

)

n

P

i=1

λ

iΛ

(

i

)

Λ1 n

= ¯

λ,

which is in fact equivalent to

n

X

i=1

λ

i Λ1

λ

iΛ

(

i

) ≥

n

X

i=1 1 n

λ

iΛ

(

i

).

(5)

Note that, for any i

6=

j,

λ

iΛ

(

i

) − λ

jΛ

(

j

) = (λ

i

λ

j

)[

Λ1

i

+

λ

j

)]

sgn

=

λ

i

λ

j

,

and so it suffices to prove that, under the restriction pi

pj sgn

=

yi

yjfor i

6=

j, the function g

(

p1

, . . . ,

pn

) = P

ni=1piyiis

Schur-convex in

(

p1

, . . . ,

pn

)

, where

P

n

i=1pi

=

1 and yi

>

0 for i

=

1

, . . . ,

n. It is easy to verify that, for i

6=

j,

(

pi

pj

)



g

(

p1

, . . . ,

pn

)

pi

g

(

p1

, . . . ,

pn

)

pj



=

(

pi

pj

)(

yi

yj

) ≥

0

.

Then, the desired result follows immediately fromLemma 2.3. 

3. Main results

In this section, we present the main results. The first one is an analogue of Lemma 2.1 in [18].

Lemma 3.1. Let X be an exponential random variable with hazard rate a and Y be a mixture of exponential random variables, with the distribution function FY

=

P

n

i=1piFaisuch that

P

n

i=1pi

=

1 and Faiis the distribution function of a exponential random variable with hazard rate ai

>

0. Then

X

lrY

⇐⇒

a

n

P

i=1 pia2i n

P

i=1 piai (3.1) and X

lrY

⇐⇒

a

min 1≤inai

.

(3.2)

Proof. It is well known that log-convexity is preserved under mixing (see [26]), which implies that the ratiof

0

Y(t)

fY(t)is increasing

in t

0. Note that, for t

0

Y

(

t

) =

f0 Y

(

t

)

fY

(

t

)

= −

n

P

i=1 pia2ie −ait n

P

i=1 piaie−ait

,

and we have

min 1≤in ai

=

lim t→∞∆Y

(

t

) ≥

Y

(

t

) ≥

Y

(

0

) = −

n

P

i=1 pia2i n

P

i=1 piai

.

Assume X

lrY , it holds that

n

P

i=1 pia2i n

P

i=1 piai

=

Y

(

0

) ≥

X

(

0

) = −

a

,

which implies the right-hand side of(3.1).

Conversely, if the right-hand side of(3.1)holds, then

X

(

t

) = −

a

≤ −

n

P

i=1 pia2i n

P

i=1 piai

=

Y

(

0

) ≤

Y

(

t

),

which is actually an equivalent characterization for X

lrY .

(6)

Theorem 3.2. Let X1

, . . . ,

Xn be independent exponential random variables with respective hazard rates

λ

1

, . . . , λ

n, and

Y1

, . . . ,

Ynbe a random sample of size n from an exponential population with hazard rate

λ

. Then, X2:n

lrY2:nif and only if

λ ≥ ˆλ =

1 2n

1



2Λ1

+

Λ3

Λ1Λ2 Λ2 1

Λ2



withΛk

=

P

n i=1

λ

k i, k

=

1

,

2

,

3.

Proof. Sufficiency X2:nhas its density function as, for t

0,

fX2:n

(

t

) = −(

n

1

)

Λ1e −Λ1t

+

n

X

i=1 Λ

(

i

)

e−Λ(i)t

.

Applying Taylor’s expansion at the origin, we get

fX2:n

(

t

) = −

"

n

X

i=1 Λ2

(

i

) − (

n

1

)

Λ2 1

#

t

+

1 2

"

(

n

1

)

Λ31

n

X

i=1 Λ3

(

i

)

#

t2

+

o

(

t2

),

and the derivative of the density function

fX02:n

(

t

) = −

"

n

X

i=1 Λ2

(

i

) − (

n

1

)

Λ21

#

+

"

(

n

1

)

Λ31

n

X

i=1 Λ3

(

i

)

#

t

+

o

(

t

).

Thus, ∆X2:n

(

t

) =

fX0 2:n

(

t

)

fX2:n

(

t

)

=

1 t

+

(

n

1

)

Λ3 1

n

P

i=1 Λ3

(

i

)

n

P

i=1 Λ2

(

i

) − (

n

1

)

Λ2 1

+

o

(

1

).

Likewise, ∆Y2:n

(

t

) =

f0 Y2:n

(

t

)

fY2:n

(

t

)

=

1 t

(

2n

1

)λ +

o

(

1

).

Since X2:n

lrY2:nimplies∆X2:n

(

t

) ≥

Y2:n

(

t

)

for all t

0, we have

λ ≥

(

n

1

)

Λ31

n

P

i=1 Λ3

(

i

)

(

2n

1

)



(

n

1

)

Λ21

n

P

i=1 Λ2

(

i

)



=

1 2n

1



2Λ1

+

Λ3

Λ1Λ2 Λ2 1

Λ2



= ˆ

λ.

Necessity. According to [27], the first sample spacing X1:nis independent of the second sample spacing X2:n

X1:n. Let T1be

an exponential random variable with hazard rateΛ1, and T2be a mixture of exponential random variables with distribution

function FT2

=

P

n

i=1Λλi1FΛ(i), which is independent of T1. Then, X2:n st

=

T1

+

T2. Likewise, Y2:n st

=

U1

+

U2, where U1and U2are

independent exponential random variables with respective hazard rates n

λ

and

(

n

1

. Consider the other exponential random variable T3with hazard rate

n

P

i=1

λ

iΛ2

(

i

)

n

P

i=1

λ

iΛ

(

i

)

=

n

P

i=1 λi Λ1Λ 2

(

i

)

n

P

i=1 λi Λ1Λ

(

i

)

,

which is independent of T1. From equivalence(3.1)inLemma 3.1, it follows immediately that

T2

lrT3

.

Since T1has a log-concave density, by Theorem 1.C.9 of [21], we have

T1

+

T2

lrT1

+

T3

.

To reach the desired conclusion, we need to prove

(7)

Due toTheorem 2.2, it suffices to show

Λ1

,

n

P

i=1

λ

iΛ2

(

i

)

n

P

i=1

λ

iΛ

(

i

)

w



(

n

λ, (

n

1

)λ).

Since n

P

i=1

λ

iΛ2

(

i

)

n

P

i=1

λ

iΛ

(

i

)

=

Λ1

n

P

i=1

λ

2 i n

P

i=1

λ

i

<

Λ1

,

it is enough to prove the following two statements:

n

P

i=1

λ

iΛ2

(

i

)

n

P

i=1

λ

iΛ

(

i

)

(

n

1

(3.3) and Λ1

+

n

P

i=1

λ

iΛ2

(

i

)

n

P

i=1

λ

iΛ

(

i

)

(

2n

1

)λ.

(3.4) Note that

ˆ

λ =

1 2n

1



2Λ1

+

Λ3

Λ1Λ2 Λ2 1

Λ2



=

1 2n

1

Λ1

+

n

P

i=1

λ

iΛ2

(

i

)

n

P

i=1

λ

iΛ

(

i

)

,

(3.5) and so n

P

i=1

λ

iΛ2

(

i

)

n

P

i=1

λ

iΛ

(

i

)

=

(

2n

1

)ˆλ −

Λ1

(

2n

1

)ˆλ −

n

λ = (

ˆ

n

1

)ˆλ ≤ (

n

1

)λ,

and hence(3.3)holds byLemma 2.4. By using(3.5), inequality(3.4)can be directly derived fromLemma 2.4. 

As pointed out earlier in Section1, Pˇaltˇanea [18] built characterization(1.2)on hazard rate order under the setup in

Theorem 3.2. Since the likelihood ratio order implies the hazard rate order, it may be concluded that

˜

λ ≤ ˇλ ≤ ˆλ ≤ ¯λ,

(3.6)

where

λ

˜

is the geometric mean of

λ

0s. The following example is an illustration of the above assertion.

Example 3.3. For an independent exponential random vector

(

X1

,

X2

,

X3

)

with hazard rate vector

1

, λ

2

, λ

3

) =

(

5

.

5

,

5

.

5

,

40

)

, it can be easily evaluated that

ˆ

λ ≈

16

.

0719

,

λ ≈

˜

10

.

656

,

λ ≈

ˇ

12

.

52

,

λ =

¯

17

.

Clearly,(3.6)holds.

Consider independent and identical exponential random variables

(

Y1

,

Y2

,

Y3

)

with the common hazard rate

λ = ˇλ

.

By equivalence(1.2), we have X2:3

hrY2:3. However, with fX2:3 and fY2:3 denoting the density functions of X2:3and Y2:3,

respectively, we have fX2:3

(

0

.

02

)

fY2:3

(

0

.

02

)

0

.

8604

>

0

.

788055

fX2:3

(

0

.

04

)

fY2:3

(

0

.

04

)

.

Thus, the ratiofX2:3(x)

(8)

Theorem 3.4. Let X1

, . . . ,

Xn be independent exponential random variables with respective hazard rates

λ

1

, . . . , λ

n, and

Y1

, . . . ,

Ynbe a random sample of size n from an exponential population with hazard rate

λ

. Then, X2:n

lrY2:nif and only if

λ ≤

n

P

i=1

λ

i

max 1≤in

λ

i n

1

.

Proof. Pˇaltˇanea [18] proved that X2:n

hrY2:nif and only if

λ ≤

Pn i=1λi−max1≤inλi n−1

=

min1≤inΛ(i) n−1 withΛ

(

m

) = P

n i=1

λ

i

λ

m

,

m

=

1

, . . . ,

n. Since the likelihood ratio order implies the hazard rate order, it suffices to prove that

λ ≤

min1≤inΛ(i)

n−1

implies X2:n

lrY2:n.

Suppose T1is exponential with hazard rateΛ1, T2is a mixture of exponential random variables with distribution function

FT2

=

P

n

i=1

λi

Λ1FΛ(i), and T4is an exponential random variable with hazard rate min1≤inΛ

(

i

)

, both of which are independent

of T1. According to(3.2), it follows from

λ ≤

min1≤inΛ(i)

n−1 that T2

lrT4. Also, by Theorem 1.C.9 of [21], we have

X2:n st

=

T1

+

T2

lrT1

+

T4

.

Suppose U1and U2are independent exponential random variables with respective hazard rates n

λ

and

(

n

1

. Now, we

only need to prove

T1

+

T4

lrU1

+

U2 st

=

Y2:n

.

ByTheorem 2.2again, this inequality is equivalent to



Λ1

,

min 1≤inΛ

(

i

)



w



(

n

λ, (

n

1

)λ).

(3.7)

It is easy to verify that

min



Λ1

,

min 1≤inΛ

(

i

)



=

min 1≤inΛ

(

i

) ≥ (

n

1

)λ =

min

{

n

λ, (

n

1

)λ}

and Λ1

+

min 1≤inΛ

(

i

) =

1 n

1 n

X

i=1 Λ

(

i

) +

min 1≤inΛ

(

i

) ≥ (

2n

1

)

min 1≤inΛ

(

i

)

n

1

(

2n

1

)λ,

which guarantees inequality(3.7). This completes the proof. 

As a consequence ofTheorems 3.2 and 3.4, we immediately obtain the following corollary, which compares the corresponding second order statistics in terms of the likelihood ratio order for the case when both exponential samples are heterogeneous.

Corollary 3.5. Let X1

, . . . ,

Xn be independent exponential random variables with respective hazard rates

λ

1

, . . . , λ

n, and

Y1

, . . . ,

Ynbe another set of exponential random variables with respective hazard rates

µ

1

, . . . , µ

n. If

1 2n

1



2Λ1

+

Λ3

Λ1Λ2 Λ2 1

Λ2



n

P

i=1

µ

i

max 1≤in

µ

i n

1 withΛk

=

P

n i=1

λ

k i, k

=

1

,

2

,

3, then X2:n

lrY2:n

.

Proof. Let Z1

, . . . ,

Znbe a random sample of size n from an exponential population with hazard rate

λ

such that

1 2n

1



2Λ1

+

Λ3

Λ1Λ2 Λ2 1

Λ2



λ ≤

n

P

i=1

µ

i

max 1≤in

µ

i n

1

.

FromTheorems 3.2and3.4, it follows that

(9)

Upon applying an argument similar to that used by Pˇaltˇanea [18] to prove(1.2)and(1.3), an analogue ofCorollary 3.5on the hazard rate order can also be established.

Corollary 3.6. Let X1

, . . . ,

Xn be independent exponential random variables with respective hazard rates

λ

1

, . . . , λ

n, and

Y1

, . . . ,

Ynbe another set of exponential random variables with respective hazard rates

µ

1

, . . . , µ

n. If

v

u

u

u

t

P

1≤i<jn

λ

i

λ

j n 2



n

P

i=1

µ

i

max 1≤in

µ

i n

1

,

then X2:n

hrY2:n

.

Under the setup of the above corollary, Dykstra et al. [12] showed with the help of a counterexample that

1

, . . . , λ

n

)

m



1

, . . . , µ

n

)

does not imply X2:n

hrY2:n, and so is the likelihood ratio order between X2:nand Y2:n. Here,Corollaries 3.5

and3.6provide, respectively, the sufficient conditions for the likelihood ratio order and the hazard rate order between X2:n

and Y2:n.

4. Examples

In order to illustrate the performance of our main results established in Section3, we present here some interesting special cases. Let X1

, . . . ,

Xnbe independent exponential random variables with respective hazard rates

λ

1

, . . . , λ

n, and

Y1

, . . . ,

Ynbe a random sample of size n from an exponential population with hazard rate

µ

. For the sake of convenience,

let us denote

`

λ =

n

P

i=1

λ

i

max 1≤in

λ

i n

1

.

Example 4.1. Suppose that

λ

1

= · · · =

λ

n

=

λ

. In this case, it is easy to check

ˆ

λ =

1 2n

1



2Λ31

3Λ1Λ2

+

Λ3 Λ2 1

Λ2



=

1 2n

1 n

(

n

1

)(

2n

1

3 n

(

n

1

2

=

λ

and

`

λ =

n

P

i=1

λ

i

max 1≤in

λ

i n

1

=

λ.

Due toTheorems 3.2and3.4, it immediately follows that X2:n

lrY2:n

⇐⇒

µ ≥ λ

and X2:n

lrY2:n

⇐⇒

µ ≤ λ

, which

actually are well known in the literature. 

Example 4.2. Suppose that

λ

1

= · · · =

λ

n−1

=

λ

and

λ

n

=

λ

0

6=

λ

. This case is of special interest in the modelling of a

single outlier. Note that

Λ1

=

(

n

1

)λ + λ

0

,

Λ2

=

(

n

1

2

+

λ

20

,

Λ3

=

(

n

1

3

+

λ

30

.

After some simplifications, it is easy to see that

ˆ

λ =

1 2n

1



2Λ31

3Λ1Λ2

+

Λ3 Λ2 1

Λ2



=

(

n

2

)(

2n

3

3

+

3

(

2n

3

2

λ

0

+

3

λλ

20 2

(

2n

1

)λλ

0

,

and fromTheorem 3.2, we have

X2:n

lrY2:n

⇐⇒

µ ≥ ˆλ =

(

n

2

)(

2n

3

3

+

3

(

2n

3

2

λ

0

+

3

λλ

20

2

(

2n

1

)λλ

0

.

On the other hand, byTheorem 3.4, if

λ > λ

0, then

X2:n

lrY2:n

⇐⇒

µ ≤ `λ =

(

n

2

)λ + λ

0

(10)

and if

λ < λ

0, then

X2:n

lrY2:n

⇐⇒

µ ≤ `λ = λ.



Example 4.3. For n

=

2m

+

1, let X1

, . . . ,

Xn be independent exponential random variables with X1

, . . . ,

Xmhaving

respective hazard rates

(

1

i

n

)λ,

i

=

1

, . . . ,

m, Xm+1having its hazard rate

λ

, and Xm+2

, . . . ,

Xnhaving respective hazard

rates

h

1

+

l−(m+1)

n

i λ

, l

=

m

+

2

, . . . ,

n. In this case, it can be readily calculated that Λ1

=

n

λ,

Λ2

=

n

λ

2

+

2

λ

2 m

X

i=1 i2 n2

,

Λ3

=

n

λ

3

+

6

λ

3 m

X

i=1 i2 n2

.

We then get

ˆ

λ =

1 2n

1



2Λ31

3Λ1Λ2

+

Λ3 Λ2 1

Λ2



=



2n3

3n2

+

n

6

(

n

1

)

P

m i=1 i2 n2



λ

(

2n

1

)



n2

n

2 m

P

i=1 i2 n2



and

`

λ =



1

m n

(

n

1

)



λ.

Upon applyingTheorems 3.2and3.4once again, we arrive at

X2:n

lrY2:n

⇐⇒

µ ≥ ˆλ =



2n3

3n2

+

n

6

(

n

1

)

P

m i=1 i2 n2



λ

(

2n

1

)



n2

n

2 m

P

i=1 i2 n2



and X2:n

lrY2:n

⇐⇒

µ ≤ `λ =



1

m n

(

n

1

)



λ.

 Acknowledgments

This work was initiated while Peng Zhao was visiting the Department of Mathematics and Statistics, McMaster University, Canada, and he is grateful to China Scholarship Council (CSC) for providing the financial support for this visit. The authors would also like to thank a referee for useful comments on the original version of this paper.

References

[1] H.A. David, H.N. Nagaraja, Order Statistics, 3rd ed., Wiley, Hoboken, New Jersey, 2003.

[2] N. Balakrishnan, C.R. Rao, Handbook of Statistics, in: Order Statistics: Theory and Methods, vol. 16, Elsevier, Amsterdam, 1998. [3] N. Balakrishnan, C.R. Rao, Handbook of Statistics, in: Order Statistics: Applications, vol. 17, Elsevier, Amsterdam, 1998. [4] N. Balakrishnan, Permanents, order statistics, outliers, and robustness, Revista Matemática Complutense 20 (2007) 7–107.

[5] R.E. Barlow, F. Proschan, Statistical Theory of Reliability and Life Testing: Probability Models, Holt, Rinehart and Winston Inc., New York, 1975. [6] N. Balakrishnan, A.P. Basu, The Exponential Distribution: Theory, Methods and Applications, Gordon and Breach Publishers, Newark, New Jersey, 1995. [7] A. Paul, G. Gutierrez, Mean sample spacings, sample size and variability in auction-theoretic framework, Operations Research Letters 32 (2004)

103–108.

[8] X. Li, A note on the expected rent in auction theory, Operations Research Letters 33 (2005) 531–534.

[9] P. Pledger, F. Proschan, Comparisons of order statistics and of spacings from heterogeneous distributions, in: J.S. Rustagi (Ed.), Optimizing Methods in Statistics, Academic Press, New York, 1971, pp. 89–113.

[10] F. Proschan, J. Sethuraman, Stochastic comparisons of order statistics from heterogeneous populations, with applications in reliability, Journal of Multivariate Analysis 6 (1976) 608–616.

[11] S.C. Kochar, J. Rojo, Some new results on stochastic comparisons of spacings from heterogeneous exponential distributions, Journal of Multivariate Analysis 59 (1996) 272–281.

[12] R. Dykstra, S.C. Kochar, J. Rojo, Stochastic comparisons of parallel systems of heterogeneous exponential components, Journal of Statistical Planning and Inference 65 (1997) 203–211.

[13] J.L. Bon, E. Pˇaltˇanea, Ordering properties of convolutions of exponential random variables, Lifetime Data Analysis 5 (1999) 185–192. [14] B. Khaledi, S.C. Kochar, Some new results on stochastic comparisons of parallel systems, Journal of Applied Probability 37 (2000) 1123–1128.

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[15] B. Khaledi, S.C. Kochar, Stochastic orderings among order statistics and sample spacings, in: J.C. Misra (Ed.), Uncertainty and Optimality-Probability, Statistics and Operations Research, World Scientific Publishers, Singapore, 2002, pp. 167–203.

[16] J.L. Bon, E. Pˇaltˇanea, Comparisons of order statistics in a random sequence to the same statistics with i.i.d. variables, ESAIM: Probability and Statistics 10 (2006) 1–10.

[17] S.C. Kochar, M. Xu, Stochastic comparisons of parallel systems when components have proportional hazard rates, Probability in the Engineering and Informational Science 21 (2007) 597–609.

[18] E. Pˇaltˇanea, On the comparison in hazard rate ordering of fail-safe systems, Journal of Statistical Planning and Inference 138 (2008) 1993–1997. [19] R.E. Lillo, A.K. Nanda, M. Shaked, Preservation of some likelihood ratio stochastic orders by order statistics, Statistics and Probability Letters 51 (2001)

111–119.

[20] F. Belzunce, J.M. Ruiz, M.C. Ruiz, On preservation of some shifted and proportional orders by systems, Statistics and Probability Letters 60 (2002) 141–154.

[21] M. Shaked, J.G. Shanthikumar, Stochastic Orders, Springer, New York, 2007.

[22] A. Müller, D. Stoyan, Comparison Methods for Stochastic Models and Risks, Wiley, New York, 2002.

[23] A.W. Marshall, I. Olkin, Inequalities: Theory of Majorization and its Applications, Academic Press, New York, 1979.

[24] P.J. Boland, E. EL-Neweihi, F. Proschan, Schur properties of convolutions of exponential and geometric random variables, Journal of Multivariate Analysis 48 (1994) 157–167.

[25] K. Chang, Stochastic orders of the sums of two exponential random variables, Statistics and Probability Letters 51 (2001) 389–396. [26] M.Y. An, Logconcavity versus logconvexity: A complete characterization, Journal of Economic Theory 80 (1998) 350–369.

[27] S.C. Kochar, R. Korwar, Stochastic orders for spacings of heterogeneous exponential random variables, Journal of Multivariate Analysis 57 (1996) 69–83.

References

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