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(1)

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/kyzT{|FO5}~mD[q!"ST'(./ƒh,*•€•./I ,*./+!"#+!„i…opCDnF….†Dh„‡xIMcDonald and Xu 1995ˆNadarajah and Gupta 2004, p.127, Crooks 2019, pp.102–107I 672019‰ŠiW‹E2O5I,*./kyzT{|FO5}~mD$%

&./ˆWeibull./2fg'()*2ZO5j+,*)-kl‚xI!

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1

一般化ガンマ確率変数の指数変換の分布の形状について(鍵原)

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一般化ガンマ確率変数の指数変換の 分布の形状について

鍵 原 理 人*

(2)

!"#$%&'()*+,-./012345'67"#893!"#:

34;:3<=>?@A0B*>"C0DEFGHIJ"#:()KLM NHIJ"#9OPHIJ"#*QRSA0=>?@A9<TSGConsul and Jain 1971 UGrassia 1977, Johnson, Kotz and Balakrishnan 1994, pp.383–384GCrooks 2019 pp.67–71VW=GWeibull"#:()KLMN Weibull"#9OPWeibull"#*QRSA0=>?@A09Mazucheli, Menezes, Fernandes, de Oliveira and Ghitany 2019VW=D%KGGrassia (1977)*Mazucheli, Menezes, Fernandes, de Oliveira and Ghitany (2019) LGXAYA:"#KZ[,\N*]^:_`:ab$cd5Kef/0D

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(  )2

−   −148

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2 !"#$%&'()*+,*)-./+01

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Γ(α) :=

0 xα−1e−xdx, α >0. (1)

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g(u|α) := 1

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%ƒ+α >0CΓ(α)>0'B"12C+!"#$#%&u∈(0,∞)'()

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. 3

一般化ガンマ確率変数の指数変換の分布の形状について(鍵原)

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−   −149

(4)

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0BC=23#V )DE<(g0$G0)F<(3"AGHI2J g0(v|α, β) = d

dvG0(v|α, β) = 1 βg

v1βα vβ1−1.

K@A#0 < v < 12 v 0L"A#V )DE<( g0$MN312 O0< α, β <∞PJ

g0(v|α, β) = 1

βΓ(α)vαβ−1e−vβ1. (3) γ:= 1/β12Q('R8S=3#V :=Uβ=U1/γ)DE<(g0)T9+

-GHI2O0< α, γ <∞PJ g0(v|α, γ) = γ

Γ(α)vγα−1e−vγ, 0< v <∞. (4) (3)NU"V$(4)NWXYZI[DE<(g08\]%&:;8^_`

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G(W|α, γ, σ) :=P(W ≤w) =P V w

σ

=

wσ

0 g0(v|α, γ)dv

(  )4

−   −150

(5)

!"#$%&'()*g+G&,)*-./,01234 g(w|α, γ, σ) = d

dwG(w|α, γ, σ) = 1 σg0w

σα, γ .

56/$w >073w89./$W&'()*g+:;-./<=234

g(w|α, γ, σ) = γ σΓ(α)

w

σ γα−1

e(wσ)γ. (5)

>.$?(@*σ-2A&BC@*α-γ+D/EF!"34σ, α, γ∈(0,∞).

σ= 1&GH$IJKLMNOP&'()*(5);+QRIJKLMNOP

&'()*(4);8STU34g(w|α, γ,1) =g0(w|α, γ), w >0.

1/$QRIJKLMNOP&'()*(4);+$γ= 1&GH$QRL MNOP&'()*8STg0(v|α,1) =g(v|α).$%&?(OPVWX8 LMNOP-YZ[-\]^_LMNOP&'()*+$IJKLMNO P&'()*(5);8`^/γ= 1-U3[-8a6/<=234

g(w|α,1, σ) = 1 σΓ(α)

w

σ α−1

ewσ, 0< w <1.

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&'()*+$IJKLMNOP&'()*(5);8`^/α= 1-U3 [-8a6/<=234

g(w|1, γ, σ) = γ σ

w

σ γ−1

e(wσ)γ, 0< w <1.

f8$QRIJKLMNOP&'()*(4);+$α=γ= 1&GH$QR g*OP&'()*g0(v|1,1) =e−v8ST.$%&?(OPVWX8g*

OP-YZ[-\]^_g*OP&'()*+$IJKLMNOP&'(

)*(5);8`^/α=γ= 1-U3[-8a6/<=234 g(w|1,1, σ) = 1

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5

一般化ガンマ確率変数の指数変換の分布の形状について(鍵原)

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F0(z|α, γ) :=P(Z≤z) =P(V ≥ −logz) = 1−G0(−logz|α, γ).

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0 g0(v|α, γ)dv

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zΓ(α)

log1 z

γα−1

e(log1z)γ, z∈(0,1). (6)

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−   −152

(7)

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&'IJKLMN*[email protected],IJKUF09BZXU.noYZOp 2.3aqrT[Fj%&'LMN*+$stLMN*+UVuvZ-wxZ O-yu%Crooks 2019\Mazucheli, Menezes, Fernandes, de Oliveira and

Ghitany 2019qrT[

z9%&'IJKLMN*+,QRS,;<='(6):$%α=γ= 1, {|%Γ(1) = 1.noYZU%

f0(z|1,1) = 1

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H%QRIJKLMN*+,;<='(4):]α=γ= 1,€.•G‚ƒ (0,∞)„,QRd'*+.}~YZXU.noYZU%QRd'@A`' ,…,d'`e.•09QRIc*+]†gzvZXU]@m.‡ˆzv Z[Fj%(6):$%γ = 1,{|.&'LMN*+,QRS,;<='%

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`'5‰`eYZXU.•09P,*+5IJKYZ[•Ž%(6):.•0 9••zvZQR&'IJKLMN*+,;<='f0UZ∼f0.&89%

X:=Zδ ,*+5ghYZOδ >0T[

7

一般化ガンマ確率変数の指数変換の分布の形状について(鍵原)

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−   −153

(8)

X!"#$%&f'()*+,-.2.1/'01!23&456*7' 89:;-<!(=&>?@x∈(0,1)AB

f(x|α, γ, δ) =1 δf0

x1δα, γ xδ1−1.

9:;-0< x <1C?x8DE;-X!"#$%'E;<FG>H+?

@0< α, γ, δ <∞AB

f(x|α, γ, δ) = γ δγαΓ(α)x

log1

x

γα−1

exp

1 δγ

log1

x

γ

. (7)

η := 1/δC?I%JK&L*'-X :=Zδ =Z1/η!"#$%f !M(=

G>H+?@0< α, γ, η <∞AB f(x|α, γ, η) = γηγα

Γ(α)x

log1 x

γα−1

exp

−ηγ

log 1 x

γ

. (8)

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f(x|α, γ, σ) = γ σγαΓ(α)x

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−   −154

(9)

!"#$%&'()*+,-./01%(8)23#η = 1.45#67 89:$%&'()*+,-./01%(6)28;<=>?f(x|α, γ,1) = f0(x|α, γ). @A#γ= 1BCDE#$%)*+,-./01%

f(x|α,1, η) =ηαxη−1 Γ(α)

log1

x α−1

FGHIJConsul and Jain 1971KGrassia 1977, Crooks 2019, p.67L MN#α= 1BCDE#$%Weibull,-./01%FGHI>JMazucheli, Menezes, Fernandes, de Oliveira and Ghitany 2019LMN?

f(x|1, γ, η) = γηγ x

log 1

x γ−1

exp

−ηγ

log1 x

γ

.

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η = 1.458_I`I.,-.9:aBbEIPc]@A#Mazucheli, Menezes, Fernandes, de Oliveira and Ghitany (2019)3$%Weibull,- RdeWeibull,-Bbfgh>OB8ij=>]

kl8#(8)2gmn!IA/01%f8oc6pq%X ∼f 8$U"#

_.1rqsY :=µ+σX, µ∈(−∞,∞), σ∈(0,∞).,-Rtu>O B8Pv"#dewx(0,1)y8mn!IA/01%f Rzj.{|wx (µ, µ+σ)8}~=>OBFg•>]OI3$%&'()*+,-.eC€

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Jα, γ >0N]OOg#V BZ.,-.‡3_I`Iˆ|wx(0,∞)Bde

wx(0,1)g‰>OB8ij=>]X^#Š‹8^h"3#r.PcXŒ

9

一般化ガンマ確率変数の指数変換の分布の形状について(鍵原)

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−   −155

(10)

!"#$%&'()*+v∈(0,∞), z∈(0,1),-

g0(v) :=g0(v|α, γ), f0(z) :=f0(z|α, γ).

./0123z∈(0,1)&45/0 f0(z) = 1

zg0(−logz)

67*89&:2)*90;3<=#z6>?)*89&@A0B3CD EFGHI*-

f0(z) =1

z2{g0(−logz) +g0(−logz)}. 8860123v∈(0,∞)&45/

g0(v) = (γα1)−γvγ

v g0(v)

67*89&:2)*90

g0(v) +g0(v) =(γα1) +v−γvγ

v g0(v)

67*360B3JK#G*- f0(z) = g0(−logz)

z2logz {(γα−1)logz−γ(−logz)γ}, z∈(0,1).

8860123z∈(0,1)&45/0z2>09logz <0, g0(−logz)>0 67*89&:2)*90B3LMCD#G*+z∈(0,1),-

f0(z)≶0 ⇐⇒ (γα1) +

log1 z −γ

log1

z

γ

≷0

⇐⇒ log1 z −γ

log1

z γ

≷1−γα.

83LMCD&NO/04P&@*z3QRSTUV#v:=logz∈(0,∞) 9J!)*90B3JK#G*-

f0(z)≶0 ⇐⇒ v−γvγ ≷1−γα (9)

W50 v=logz, z∈(0,1).

(  )1010

−   −156

(11)

!"#$%&'(γ= 1)*+,γ= 1)*+#-./&0123456 78(γ= 1)*+((9)9':);<#=>?@A5B

f0(z)≶0 ⇐⇒ α≷1.

;C&((6)9DEF@A5GHIJKL?MNOPQ)RSTJf0(z|α, γ) )UVW'W2#XYZA5[\,]56^A#;\(γ= 1)*+(R STJf0)_`#a%&:)bc2d5B

!" 1 (GHIJKL?MNOPQ)_`Bγ= 1)*+). γ= 1)*+(

(6)9DEF@A5RSTJf0)efg{(z, f0(z|α, γ))|z∈(0,1)})_`

'(hi)jJα#kl&!");<#Em5no5pqr6s/(!"

D'f0(z) :=f0(z|α, γ),tuv56 1. 0< α <1)*+B>wUxy

RSTJf0(z)'z)>wUxTJDz\({)efg'|}\) _`2~v6

2. α= 1)*+BK•PQ

RSTJf0(z)'€•)z∈(0,1)#I/&EJ12‚\({)e fg'ƒ„y)_`2~vnK•PQr6

3. α >1)*+B>wV…y

RSTJf0(z)'z)>wV…TJDz\({)efg'|"\) _`2~v6

:#(γ= 1)*+(

v−γvγ = 0 ⇐⇒ (1−γvγ−1)v= 0

⇐⇒ v= 0m†'1−γvγ−1= 0

#;\(

1−γvγ−1= 0 ⇐⇒ v=γ1−γ1

11

一般化ガンマ確率変数の指数変換の分布の形状について(鍵原)

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−   −157

(12)

!"#$%&'(#)v∈[0,∞)!*+,-)./0123%4

v−γvγ = 0 ⇐⇒ v= 0567v=γ1−γ1 . (10) 889'0 < γ <1):;'1/(1−γ)>1!<='0< γ1/(1−γ)< γ <1 9>='γ >1):;'1/(1−γ)<0!<='0< γ1/(1−γ)<1< γ9>

%8&!"#$%?@A!BC,7'γ1/(1−γ)2DE!v0&FG$%HI 2'I3JKL4

v0:=γ1−γ1 , 0< v0<min{1, γ}. (11) 56'v=logz ⇐⇒ z =e−vM%01!"#+,'DE!-)FG2 NO$%He−1= 0.367879· · ·'I1JKL4

z0:=e−v0= exp

−γ1−γ1

, max{e−1, e−γ}< z0<1. (12)

0 1 2 3 4 5

0.00.20.40.60.81.00.30.70.9

O

I1: z=z0H(12)PL&z=zH(18)PL)QRSHTUz'VUγL4W X· · · z=z0 = exp[−γ1/(1−γ)]'YX· · · z=z = exp[−γ2/(1−γ)]'ZW X· · · z= exp[−γ]'ZYX· · · z= exp[−1] = 0.367879. . .

(  )1212

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(13)

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;6<=>-α?γ@ABC)DE6FG?>-69H:#γ= 16IJ#

K@LM1%NOP@!(QDRS"#TU@VW":#γ = 16IJ@

;W"#γ >16IJXY3.1Z[?γ <16IJXY3.2Z[@4\"]

^C)DE6_%#`O(QabcdM?e"fgC)XY3.3Z[D

3.1 !"#$%& γ > 1 #'(

γ >16IJ#(9)$@V\)v−γvγ6<h@;W"i69HjklC )m?@noC)Xp2qrDTU#m69Hc9H(∗)?e"stC)[u

1. v= 0 (⇐⇒ z=e−v= 1)6v#v−γvγ = 0.

2. 0< v < v06vX0< v0=γ1/(1−γ)<1[#0< v−γvγ < v0. 3. v=v0 (⇐⇒ z=z0=e−v0)6v#v−γvγ = 0.

4. v0< v <∞6v#v−γvγ<0.

5. v→ ∞(⇐⇒ z→0)6v#v−γvγ → −∞.

1 γ 1

γ

γ1−γ1 γ1−γ1

0 γ1+γ1−γ

γ1−γ2

p 2: u = γvγ ?u = v6wxyXγ > 16IJuz{u#|{v[u}

~· · · u=γvγ#•~· · · u=v

13

一般化ガンマ確率変数の指数変換の分布の形状について(鍵原)

(  )13

−   −159

(14)

!"#$%(∗)&'()*+γ >1#,-(./*+(6)01234567 8$9f0(z|α, γ)#:;(</*=>?6@A#B+α >1#,-Cα= 1

#,-+α <1#,-#3<#,-(DE*=>?6@

3.1.1 α >1!"#

α >1#,-+FG#γ >0(H)*1−γα <1−γ1I6@JK+LL 1M+N(γ >11I6LC(OG?6C+1−γα <1−γ <0&P6@QR

*+STUV(WX)K$%(∗)(OG?6C+YZ[v1> v0=γ1−γ1 \]

^)*v1−γvγ1 = 1−αγC1_6@LL1+z1:=e−v1C`a?5b+(9) 0(cd+(6)012345678$9f0(z|α, γ)#ef`M`31ghi5 6@LL1+zCvMj/(klfmno#$%z=e−v ⇐⇒ v=logz (I6LC(OG?6@L5(cd+γ >1p<α >1#,-+78$9 f0(z|α, γ)#:;M+

z=z1=e−v1

&qrstquvwC?6kxy1I6LC\z{?6@|)+v1M$%

0v1−γvγ1 = 1−αγ&}K)+v1> v0 =γ1/(1−γ)<11I6@L5(

cR*+quvz1Mz0cd~4[v1I6LC\Dp6•

z1=e−v1 < e−v0 =z0.

3.1.2 α= 1!"#

α= 1#,-+1−γα= 1−γ1Id+LL1+γ >11I6LC(O G?6C+1−γα = 1−γ < 0&P6@QR*+STUV(WX)K$

%(∗)(OG?6C+YZ[v1> v0\]^)*+v1−γvγ1 = 1−γ ⇐⇒

(1−γvγ−11 )v1 = 1−γ C1_6@LL1+v−γvγ \v > v01klfm 1Id+p<+v0<1()*v0−γvγ0 = 01Id+1−γ <01I6LC (OG?6C+v1−γvγ1 = 1−γ ⇐⇒ v1= 11I6LC\Dp6@cR

*+z1 :=e−v1 = 1/e&P*+(9)0(cd+(6)012345678$9 f0(z|α, γ)#ef`M`41ghi56@|)+zCvMj/(klfmn

(  )1414

−   −160

(15)

!"#$z =e−v ⇐⇒ v =logz%&'()%*+,'-(.%/01 γ >123α= 1"45167#8f0(z|1, γ)"9:;1

z=1

e = 0.367879· · ·

<=>?@=ABC),'DEFG&'()HIJ,'-KL1v0<1G

&'()%*+,')1=AB1/e;z0/0MNOKBG&'()HP 2'Q

e−1< e−v0 =z0.

3.1.3 α <1!"#

α <1"451R+"γ >0%STU1−γα >1−γG&'-((G1 γ >1G&'()%*+,')1−γ <0<V'"G11−γα"WX;Y Z%;[\)K'-]^U1_`G;11−γα <0"45)1−γα= 0"

4511−γα >0"45"33"45%PaUbc,'-

dY%11−γα <0"45%3eUbc,'-((G1γ >1)α <1

%*+,')1f"gB#$<V'Q 1−γα <0 ⇐⇒ 0< 1

γ < α <1.

("h1ijkl%mnTo#$(∗)%*+,')1pqKv1> v0HrsT Uv1−γv1γ = 1−γα)Gt'-((G1z1:=e−v1)uv,.w1(9)x%/

01(6)xG\yO.'67#8f0(z|α, γ)"z{u;u5@|}~uCG•€

•.'-‚T1z)v;ƒe%D„{…†!"#$z=e−v ⇐⇒ v=logz

%&'()%*+,'-(.%/011< γ <∞231/γ < α <1"451 67#8f0(z|α, γ)"9:;1

z=z1=e−v1

<=>?@=ABC),'DEFG&'-‚T1v1;#$xv1−γv1γ = 1−αγ

<‡oT1v1> v0=γ1/(1−γ)<1G&'-(.%/^U1=ABz1;z0

15

一般化ガンマ確率変数の指数変換の分布の形状について(鍵原)

(  )15

−   −161

(16)

!"#$%&'()*+,-.)/

z1=e−v1 < e−v0 =z0.

01231−γα= 04562789:;<)=**'3γ >1+α <1 2>?<)+3@4A&BCDE)/

1−γα= 0 ⇐⇒ 0< 1

γ =α <1.

*4F3GHIJ2KLMNBC(∗)2>?<)+3v= 0ONPv=v0= γ1/(1−γ)<12Q89v−γvγ = 0'().R3(9)S2!"3(6)S'T U$V)WXBYf0(z|α, γ)4Z[\P\5]^_`\a'bcRV)=d M3z+vPe82fg[hij4BCz=e−v ⇐⇒ v=logz2()

*+2>?<)=*V2!"3γ >1.7α= 1/γ <14563WXBY f0(z|α, γ)4klP3

z=z0=e−v0=e−γ1−γ1 >1

e = 0.367879· · · Dmno]mp&a+<)fqr'()=

0s231−γα >04562789:;<)=**'3γ >1+α <1 2>?<)+3@4A&BCDE)/

1−γα >0 ⇐⇒ 0< α < 1 γ <1.

$93t?4γ >12uM93v−γvγ P3v4BY+M9vwxyz [0, v0]'{|%4'3mn&D})]0< v0=γ1/(1−γ)<1a/

v:= arg max

v∈[0,v0]v−γvγ. (13) ON3GHIJ2KLMNBC(∗)2!"3v∈(0, v0)2Q890< v−γvγ <

v0<1'("3.73v= 0ONPv=v02Q89v−γvγ = 0'()*

+2>?<)+3mnovP~o•3€•3v(0, v0)2M9 0 < v−γvγ = max

v∈[0,v0]v−γvγ < v0=γ1−γ1 < 1

(  )1616

−   −162

(17)

!"#$%&'"()*+,-./γ >1012+,1−γα%α/34$

2+5602+789:;<=,'>,0< α <1/γ <1012+,

α→0lim1−γα= 1, lim

α→γ11−γα= 0

;<"#$0?.@"$,AB!α(0,1/γ)%C.0DE2+

1−γα=v−γvγ = max

v∈[0,v0]v−γvγ (14)

$;F"(#G0H=,-./γ >1012+I/JK3LMN"O

v−γvγ ≶1−γα ⇐⇒ αα. (15)

P2,0< α <1/γ;<"#$0?.@"(

QR/ST0UVW+,XY/Z[\1−γα >0 ⇐⇒ α <1/γ/Z[]

0>W+^,γ >1!"_`/a,0< α < α/Z[$α=α/Z[, α< α <1/γ/Z[/3>/Z[0&b+ST@"(

cd,0< α < α/Z[,(15)e0H=

1−γα > max

v∈[0,v0]v−γvγ

;<=,'>,fghi0jk2l3L(∗)$(9)e0?.@"$,-./

v >0012+I/JK3LMN"O

1−γα > v−γvγ ⇐⇒ f0(z)>0, ∀z∈(0,1).

H*+,(6)e;mnoG"pq34f0(z|α, γ)/r9s^s5\atus]

;vwxG"(##;,z$v^yW0789:z{/3Lz=e−v ⇐⇒

v=logz0<"#$0?.@"()*+,pq34f0(z|α, γ)/|}^

78!uQ=\78r~•];<"(

I0,α=α/Z[,(15)e0H=

1−γα= max

v∈[0,v0]v−γvγ =v−γvγ

17

一般化ガンマ確率変数の指数変換の分布の形状について(鍵原)

(  )17

−   −163

(18)

!"#$

1−γα > v−γvγ, ∀v=v

%&'()*+$(9),!-./')$(6),%0123'4567f0(z|α, γ) 89:;<;5=>?@;A%BC+3'D((%$z)v<EF!GH:

IJK86Lz =e−v ⇐⇒ v =logz!&M$z :=e−v);N/'D OP$v8QRS.T!UF#<VW28XYZ[\23]FD(3!^

M$4567f0(z|α, γ)8_`<GHOabM=GH9cdA)O'()e fY/'D

gh!$α< α <1/γ8ij$(15),!^M 1−γα < max

v∈[0,v0]v−γvγ =v−γvγ>0

%&M$*U$veS.!0k'()$l"#$v= 0k]<v=v0!P F#v−γvγ = 0%&'()!-./')$v−γvγ ev867)"#m n%&'()!^M$0< v1< v< v2< v0<1Zo]/v1)v2epq

"#$

1−γα=v1−γvγ1 =v2−γv2γ )/'()e%r'D((%$

z2:=e−v2 < z:=e−v < z1:=e−v1 (16) );N/')$stuv!wx"]6L(∗))(9),!^M$(6),%01 23'4567f0(z|α, γ)89:;<;5=y?;A%BC+3'D((%$

z)v<EF!GH:IJK86Lz=e−v ⇐⇒ v=logz!&'()

!-./'DOP$z1)z2<l3z3v1)v28S.T8{|)"#S.

!0kM$v1)v28S.T!UF#<VW28XYZ[\23]FD;5

=y?;A!^M$4567f0(z|α, γ)8_`<$9c}:I}9c)F~3

•67€OabM8_`$•FKC3‚$GH%<OFƒ88abM8„

…Zx/()e†*'Ds‡%<$(3ZˆGH9cd)‰Š()!/'D

18(  )18

−   −164

(19)

3.1.4 !"#$%

!"#$3.1"%&'()*+,-.&/012γ >1,342(6)56 789:);<=>?@ABCDEF,GHI>f0,JK&LM1N,O PQR)S

&'2 (;<=>?@ABCDEF,JKSγ >1,34). γ >1,342 (6)56789:)GHI>f0,TUV{(z, f0(z|α, γ))|z∈(0,1)},JK W2XY,Z>α&[\1]^,/_&7`)abc2

α= 1 γ−

11

γ

γ1+γ1−γ, 0< α< 1 γ 6d)a`e2]^6Wf0(z) :=f0(z|α, γ)fghi)a 1. 0< α≤α,34Sjklmn#o62o7pq%

GHI>f0(z)Wz,jklmI>6dr2s,TUVWjktu

*r,JKQvia

2. α< α <1/γ,34Swjklmn#o72o8pq%

GHI>f0(z),TUVW2wjktu*r,JK#lmxyzx lmfM_JK2{5|}{pq%Qvia

3. 1/γ ≤α <∞,34Sj~n#o6pq%

GHI>f0(z),TUVW2z=z1Q•€•#•‚Y%fi)j~

n,JKQviS

z1=e−v1.

bc2v1WIƒ5v1−γvγ1 = 1−αγQ„ec2v1≥v0=γ1/(1−γ) 6d)a`e2…:&/r2z1=e−v1 ≤z0=e−v06d)a

v1Wα,jklmI>fc17`r2s,OPfc12•‚Yz1W α,jkyzI>fc17`)a†&2α= 1/γ,‡2z1 =e−v0 = z0> e−16dr2α= 1,‡2z1=e−1= 0.367879· · · 6d)a (). γ >1,‡2ˆ‰tα (0,1/γ)Š‹Œc1(6)56789:)G HI>f0,JKŠ0 < α≤α,34&jklmn2α < α <1/γ,3

19

一般化ガンマ確率変数の指数変換の分布の形状について(鍵原)

(  )19

−   −165

(20)

!"#$%&'()1/γ < α <*+!"$,(-./0-"1234) 53.16"78/9:*;<"=>3?"@AB"CDEF=>3)GH I4)γ"JK3LM/α*NOPQ/0-"R/F

α*N4(14)S"TU23LM/F=>3)α4v"VWX)v4 (13)S"=>3LYCD/FZ>3)GH"7234)vOPQE9Iα O[\R/F]*9I)z*NOPQ/0-"R/F

^_)(13)S*`abcd"723)`aevfgheIi/0-v (0, v0), v0=γ1/(1−γ)-`ab*1jkl"=m)v4n*=o"pq"

LM/rs2tuvw

1−γ2vγ−1 = 0 ⇐⇒ v=γ1−γ2 =v02. (17) 00I)0< v0 <1"xqR/-)0< v =v02< v0<1"=m)yB"

v(0, v0)Ii/FME)`ab*2jkl4)γ >1"=m)(13)S*

`abcd"723yB"zECD32/0-"xqR/w

−γ21)vγ−2<0, ∀v∈[0, v0].

.7)1−γ2vγ−1 ≶0 ⇐⇒ vγ1−γ2 =v"=m)v−γvγ4)v*{

|-X3)v < vI$%&')v > vI$%}~Ii/F0D"=>3) (16)S"•D/v1-v2fpq"LM/-€B/F

n")PQADEv"JK3)(14)S"Z>3αf•AD/w α= 1

γ

1

γv−vγ

= 1

γ+γ1−γ −γ1+γ1−γ = 1 γ−

11

γ

γ1+γ1−γ. 00I)(13)S"123?"9:XE‚m)ƒq*v (0, v0)"„X3) 0< v−γvγ < v0<1"xqR/-)

0< 1

γv−vγ < 1 γ

Ii/BA)v=v02< v0"xqR/-)0< α<1/γO•/F

`…")z:=e−v, v=v204n*=o"†CD/rs1tuvw z=e−v02= exp

−γ1−γ2

. (18)

(  )2020

−   −166

(21)

3.2 !"#$%& γ < 1 #'(

γ <1!"#$(9)%&'()v−γvγ!*+&,-./!012345) 67&895):;3<=>?@$6!01A01(∗∗)7B.CD5)EF

1. v= 0 (⇐⇒ z= 1)!G$v−γvγ= 0.

2. 0< v < v0!G:0< v0=γ1/(1−γ)< γE$−v0< v−γvγ<0.

3. v=v0 (⇐⇒ z=e−v0)!G$v−γvγ = 0.

4. v0< v <∞!G$v−γvγ>0.

5. v→ ∞(⇐⇒ z→0)!G$v−γvγ → ∞.

1 1

γ γ

γ1−γ1 γ1−γ1

0 γ1+γ1−γ

γ1−γ2

; 3: u = γvγ 7u = v!HIJ:γ < 1!"#FKLu$MLvEFN O· · · u=γvγ$PO· · · u=v

QR!01(∗∗)AS&B.$T3.1U7VW!XYAZ[\]^$(6)% _`abc)de0ff0!ghi7B.$γ <1!"#$i67i7$i 82jkc)>6c&lm.$γ <1!"#$(6)%_`abc)nopf qrstuvwx!de0ff0!yz&,-./!{|Aj)F

21

一般化ガンマ確率変数の指数変換の分布の形状について(鍵原)

(  )21

−   −167

(22)

!"3 (!"#$%&'()*+,-./0γ <1-12). γ <1-123 (6)456789:;<=$f0->?@{(z, f0(z|α, γ))|z∈(0,1)}-./

A3BC-D$αEFGHIJ-KLE6M:NOP3 α= 1

γ +

1

γ−1

γ1+γ1−γ, α> 1 γ 5Q:NMR3IJ5Af0(z) :=f0(z|α, γ)STUV:N

1. 0< α≤1/γ-120UWXYZ9[\]

;<=$f0(z)->?@A3z=z1^_`aSV:UWX-./^

bV0

z1=e−v1.

OP3v1A=c4v1−γvγ1 = 1−γα^dRP3v1≥v0=γ1/(1−γ) 5Q:NMR3e9EKf3z1=e−v1 ≤z0=e−v05Q:N

gE3α= 1/γ-h3z1 =e−v0 =z05Qf3α= 1-h3z1 = e−1= 0.367879· · · 5Q:N

2. 1/γ < α < α-120ijklmXYZ10[\]

;<=$f0(z)->?@A3ijknoJf-./Ylmpqrp lmSsL./3t8uvt[\]^bVN

3. α≤α <∞-120jklmXYZ93Z10[\]

;<=$f0(z)Az-jklm=$5Qf3w->?@Ajkno Jf-./^bVN

#$. xyz-{|E}sHA3yz2-{|S~•-€•^‚ƒ„…KsN OP3γ <1-12Eα†1/γKf‡ˆ‰n:eSE}sHA30< γ <1 EŠ‹V:S31/γ1>0Œ}γ1+γ1−γ >05Q:Œ•3α>1/γ^Ž:N

e-a3•Eα<2/γ5Q:eS•‘’89:Nw-“3 α= 1

γ +

1

γ 1

γ1−γ1+γ = 1 γ

1

γv−vγ

(  )2222

−   −168

(23)

!"#$%&'()#*+,-v =v20 < v0, v0 =γ1/(1−γ) <1!"#*

$$!-./01&23,456(∗∗)&78-9(:v∈(0, v0)&;,<

−1<−v0< v−γvγ <0!"#$%&'()#%-

1 γ < 1

γv−vγ <0

!"#=>-v =v20 < v0&'()#%-?=&1/γ < α <2/γ!"#

$%@A=#*

3.3 !"#$%&'()*+,*)-+./+01

BC1%BC2-BC3:DEFGH)#$%&7I<-(6)J!KLM N#OP;QRSTUVWAX:YZ5Qf0:[\&]^<_:`abc C1dFe#*fg-cC1Fh%,<23,4:@h1!"8-i%,<

23,4:@i4!"#*

23 1 (OP;QRSTUVWAX:[\). (6)J!KLMN#YZ5Q f0:jkl{(z, f0(z|α, γ))| z∈(0,1)}:[\m-no:pQα%γ&q r<st:7u&Kv#bh1-i4-BwBxyd*+,-

α= 1 γ−

11

γ

γ1+γ1−γ = 1 γ+

1

γ 1

γ1+γ1−γ (19)

!"#bγ= 1d*v4-st!mf0(z) :=f0(z|α, γ)%z{)#*

1. 0< γ <1:|Hb}~&]^<mBC3xyd•α>1/γFe#*

(a) 0< α≤1/γ:|H•

YZ5Qf0:jklm-Uۥ:[\F3)*

(b) 1/γ < α < α:|H•

YZ5Qf0:jklm-‚ƒ„…†•b‡ˆ‰fŠt8d:

[\F3)*

(c) α≤α <∞:|H•

YZ5Qf0:jklm-ƒ„…†•bŠt8d:[\F3)*

23

一般化ガンマ確率変数の指数変換の分布の形状について(鍵原)

(  )23

−   −169

(24)

2. γ= 1!"#$%&'()*+,-1./01 (a) 0< α <1/γ!"#1

2345f0!678+9:;<=>$?@A0!BCDEFG (b) α= 1/γ!"#$HIJK01

2345f0!678+9LM>!BCDEFG (c) 1/γ < α <!"#1

2345f0!678+9:;NO>$?@A0!BCDEFG

3. 1< γ <∞!"#$%&'()*+,-2./01α<1/γDPQ. (a) 0< α≤α!"#1

2345f0!678+9:;<=>$?@A0!BCDEFG (b) α< α <1/γ!"#1

2345f0!678+9R:;<=>$STUV?@A0!

BCDEFG

(c) 1/γ≤α <∞!"#1

2345f0!678+9:W>!BCDEFG

X 1: 2345f0(z|α, γ)!BC!JY$0< α, γ <∞9Z-1./0

0 · · · α · · · 1/γα · · · α · · ·

γ <1 ... U [> R:;NO> :;NO> ...

γ= 1 ... :;<=> HIJK :;NO> ...

γ >1 ... :;<=> R:;<=> :W> ...

∗γ <1!"#+α>1/γ >1\VA, γ >1!"#+α<1/γ <1\VQ.

(  )2424

−   −170

(25)

!4: "#$%f0(z|α, γ)&'(&)*+,-α./-γ.01123456 7· · · α=α= 1/γ(11/γ)γ(1+γ)/(1−γ).87· · · α= 1/γ

4 !"

9:;<(0,∞)=>?@ABCDEF%)G>HIJKL%>MNOP

&F%LQRSTUV>WXOYZBCJKL%&)G[.\];<(0,1)

=>?@ABCDE^_)G`aCbcd[.U&e6Rf>NO.F%

)GRghVNOijk)GlWeibull)GRmnopqVNOrsTC

^tuijk)G>HIJKL%>MNOP&F%LQRSTUV>WX O.^_)GRghVNOM%ijk)GlM%Weibull)GRmnop qVNOrsTCWv^twoJK)Gx+M%^tuijk)G4Ry zN{b|&"#$%[(8)}.|NO.|&DE~&"#$%[(6)}>

•€ZBCbm>.DE~&pq+(6)}4>•‚O[.|&ƒ%V"#&

25

一般化ガンマ確率変数の指数変換の分布の形状について(鍵原)

(  )25

−   −171

(26)

!"#$%&'()*+,-./#012-3456789&:;12- 3<=-7>[email protected]#CDE(8)FG*HI3J./#KLM&NOC

*P=QRS./#TU2VW#!"#$%*HI3#'()?+,JX

;2-3YZ63IR>

[\*@I3]^Z67VW$U(6)F&_H`abcEdefUAB ghijbcGJ.2H#TU&_k.lH.Ambc#ABg2?n3 IR>Ambc#ABg2-3op)?PJqrsbctuvw>qrs bcxy72H#TU&_k./#2H#TU*z{3qrsbcJ/#

VW#!"&|}*~gZ•R>€•‚')*J.qrsbc#VW#!

"J./#2H#TU*z{3.ƒ„…5†‡EAmbcˆ‰Š‡ˆU‹

‡ˆ‰Œ•އˆ‰Œ••‡G*b†Z6REP‘’.Johnson, Kotz and Balakrishnan 1995, p.219“”•2018–—G>/6*f-3.[\*€n 3]^Z67defUABghijbc#VW$U(6)F#!"J./#2 H#TU*z{3.ƒ„…7†‡EAmbcˆ‰Š‡ˆU‹‡ˆ‰Œ•Ž

‡ˆ‰Œ••‡ˆ˜‰Œ•އˆ˜‰Œ••‡G*b†Z6R™2Sš›

-7E:;1.p1–—G>

œ•*€•.[\*@I3]^Z67defUABghijbcJ.qr sbctJpžZ64?I˜‰Œ•އ2˜‰Œ••‡2Iw!"&=- 4R™2S›5l*?n7>™#˜‰Œ‡#!"&=Q#J.(6)F*ž6 RTUα2γ#Ÿ567 ¡.¢k.γ <1lH1/γ < α < α#CDE˜

‰Œ••‡G2γ >1lHα< α <1/γ#CDE˜‰Œ•އG*£¤

?IEp1.¥4–—G>-l-.•?…2x™#¦*@I3.[\*€n 3]^Z67defUABghijbc#VWJqrsbc#VW€•x

|}?!"&=Q™2S›5l*Z67>

(  )2626

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!"#$

[1] !"#$%1962&'()*+,-./01

[2] 2345%2018&6789:;<=>?@ABC'DEFGHIGJK, L62ML1N2OPpp.51–76.

[3] 2345%2019&6789QRS+<T+SU<:;<=>?@ABC 'DEFGHIGJK,L63ML2OPpp.195–224.

[4] VWXY%1980&'Z[\]I,^_FG`ab1

[5] Balakrishnan, N. and V. B. Nevzorov (2003)A Primer on Statistical Distributions, John Wiley & Sons.

[6] Consul, P. C. and G. C. Jain (1971) “On the log-gamma distribution and its properties”,Statistisch Hefte, 12, pp.100–106.

[7] Crooks, G. E. (2019) Field Guide to Continuous Probability Distri- butions, Berkeley Institute for Theoretical Sciences.

[8] Grassia A. (1977) “On a family of distributions with argument be- tween 0 and 1 obtained by transformation of the gamma and de- rived compound distributions”, Australian Journal of Statistics, 19, pp.108–114.

[9] Johnson, N. L., S. Kotz and N. Balakrishnan (1994)Continuous Uni- variate Distributions, Volume 1, 2nd edition, John Wiley & Sons.

[10] Johnson, N. L., S. Kotz and N. Balakrishnan (1995)Continuous Uni- variate Distributions, Volume 2, 2nd edition, John Wiley & Sons.

[11] Leemis, M. L. and J. T. McQueston (2008) “Univariate distribution relationships”,The American Statistician, 62, 45–53.

27

一般化ガンマ確率変数の指数変換の分布の形状について(鍵原)

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−   −173

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[12] Mazucheli, J., A. F. B. Menezes, L. B. Fernandes, R. P. de Oliveira and M. E. Ghitany (2019) “The unit-Weibull distribution as an alter- native to the Kumaraswamy distribution for the modeling of quan- tiles conditional on covariates”,Journal of Applied Statistics, (to be appeared), DOI: 10.1080/02664763.2019.1657813.

[13] McDonald, J.B. and Y.J. Xu (1995) “A generalization of the beta distribution with applications”,Journal of Econometrics, 66, pp.133–

152.

[14] Nadarajah, S. and A. Gupta (2004) “Generalizations and related uni- variate distributions”, InHandbook of Beta Distribution and Its Ap- plications, edited by A.K. Gupta and S. Nadarajah, Marcel Dekker, pp.97–163.

[15] Rinne, H. (2009) The Weibull Distribution: A Handbook, Taylor &

Francis Group.

(  )2828

−   −174

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A !"#$%&'()*+,*)-+./+012 345*+678

!"#$%&'()*+,-./012345678(6)9:;<)*=

>?@/f0(z|α, γ), z∈(0,1)ABCD!EF8G>?@/f0(z|α, γ), z∈ (0,1)HIJKALMN=DO*#PQG2CHRST/α, γ >0U>?@

/f0HVWXHRSUH@YZ[\]#^=D_H`aUb&GEc 1U Ec2GEc3Zd\*Ge%&8Gfc1Zd\*=D^$GghHK

#$%&Gz0Uz, αH;<#C%&8_*i*(12)9U(18)9G(19) 9:jk\*=lm1Gm4nopDq+Gz1Uz2H;<#C%&8G_

*i*Hrs#tu&!vwHxFyEcAno)*+%D

A.1 γ = 1 +9:

K2: >?@/f0(z| α, γ)HIJKz{Klα <1HrspGwKlα= 1 Hrsz0|67pG}Klα >1Hrsp

z 0 · · · 1

f0 +

f0

z 0 · · · 1

f0 0

f0

z 0 · · · 1

f0

f0

29

一般化ガンマ確率変数の指数変換の分布の形状について(鍵原)

(  )29

−   −175

(30)

A.2 γ > 1 !"#

! 3: "#$%f0(z| α, γ)&'(!)α >1&*+, z 0 · · · z1 · · · 1

f0 + 0

f0

! 4: "#$%f0(z| α, γ)&'(!)α= 1&*+, z 0 · · · 1/e · · · 1

f0 + 0

f0

!5:"#$%f0(z|α, γ)&'(!)α <1&*+,-./0!)1/γ < α <1

&*+,1./2!)α= 1/γ&*+,13/!)α < α <1/γ&*+,1 4/0!)α=α&*+,14/2!)0< α < α&*+,

z 0 · · · z1 · · · 1

f0 + 0

f0

z 0 · · · z0 · · · 1

f0 + 0 0

f0

z 0 · · · z2 · · · z1 · · · 1

f0 + 0 0 +

f0 0

z 0 · · · z · · · 1

f0 + 0 +

f0

z 0 · · · 1

f0 +

f0

(  )3030

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(31)

A.3 γ < 1 !"#

! 6: "#$%f0(z| α, γ)&'(!)α <1&*+, z 0 · · · z1 · · · 1

f0 0 +

f0

! 7: "#$%f0(z| α, γ)&'(!)α= 1&*+, z 0 · · · 1/e · · · 1

f0 0 +

f0

!8:"#$%f0(z|α, γ)&'(!)α >1&*+,-./0!)1< α <1/γ

&*+,1./2!)α= 1/γ&*+,13/!)1/γ < α < α&*+,1 4/0!)α=α&*+,14/2!)α< α <∞&*+,

z 0 · · · z1 · · · 1

f0 0 +

f0

z 0 · · · z0 · · · 1

f0 0 + 0

f0

z 0 · · · z2 · · · z1 · · · 1

f0 0 + 0

f0 0

z 0 · · · z · · · 1

f0 0

f0

z 0 · · · 1

f0

f0

31

一般化ガンマ確率変数の指数変換の分布の形状について(鍵原)

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(32)

B !"#$%&'()*+,*)-+./+012 345*+678

!"#$%(6)&'()*+,-./0f0(z|α, γ), z(0,1)12345 678,9:;<f0(z|α, γ)%=;<z>?

B.1 γ = 1 +9:

0 1 2 3 4 5

0.2 0.4 0.6 0.8 1

6 5: -./0f0(z|α, γ)12349γ = 11@A><α= 0.39BCD>%

α= 0.69BED>%α= 19CD>%α= 29ED>%α= 39FCD>

B.2 γ > 1 +9:

0 0.5 1 1.5 2 2.5 3 3.5

0.2 0.4 0.6 0.8 1

6 6: -./0f0(z|α, γ)12349γ = 21@A><α= 0.19BCD>%

α= 0.259BED>%α= 1/γ= 0.59CD>%α= 0.759ED>%α= 19F CD>%α= 29FED>

(  )3232

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(33)

0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8

0.2 0.4 0.6 0.8 1

! 7: "#$%f0(z|α, γ)&'()*γ = 2&+,-.α= 0.4*/01-2 α = α = 0.4375*/31-2α = 0.45*01-2α = 0.47*31-2 α= 0.49*401-2α= 1/γ = 0.5*431-

0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2

0.2 0.4 0.6 0.8 1

!8: "#$%f0(z|α, γ)&'()*γ= 5&+,-.α= 0.12< α0.128

*/01-2α = 0.13*/31-2α = 0.15*01-2α = 0.17*31-2 α= 0.19*401-2α= 1/γ = 0.2*431-

33

一般化ガンマ確率変数の指数変換の分布の形状について(鍵原)

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