立命館大学理工学研究所紀要: 第74号

立   命   館   大   学

理 工 学 研 究 所 紀 要

第74号

MEMOIRS

OF THE

INSTITUTE

OF

SCIENCE & ENGINEERING

RITSUMEIKAN UNIVERSITY

KUSATSU, SHIGA, JAPAN

NO. 74

2015

ISSN 0370-4254 CODEN:RDRKAJ

理工学研究所紀要 第74号 2015 目次

＜一般論文＞

1. A NOTE ON UNIFORM RESOLVENT ESTIMATES OF DIRAC OPERATORS

……… Hubert Kalf・大鍛治隆司・山田 修宣 …… 1

2. プラグマティストとしての漱石の可能性─グローバル化に対峙する日本人論への含意を探って─

……… 山中  司 …… 11

3. Oxide Layer Formation on Fe Ultrafine Grain Particles and Characteristic formation of ultrafine Ca particles

……… 墻内 千尋・齊藤 嘉夫 …… 25

大型研究装置成果報告書 ……… 49

理工学研究所記事 ……… 99

1

A note on uniform resolvent estimates of Dirac operators

Hubert Kalf, Takashi Okaji and Osanobu Yamada

Abstract.

A standard trace theorem can be used to estimate

(1)

x

−s

(α

· p − z)

−1

x

−s



uniformly for non-real z if s > 1/2. In contrast, it is shown that

such an estimate holds for

(2)

x

−s

(α

· p + mβ − z)

−1

x

−s



if s = 1, but not for s < 1. However, with the help of a slightly

refined trace theorem it is possible to replace the weight

x

−s

by

|x|

−t

_x

−s

₍₀

_{≤ t < 1/2, t + s > 1/2) in (1) and by |x|}

−t

_x

−1+t

(0 < t < 1/2) in (2).

2000 Mathematics Subject Classification:

Primary, 35 J 45, Secondly, 47 A 45

Keywords and Phrases:

Dirac operators, Uniform resolvent estimates

立 命 館 大 学 理 工 学 研 究 所 紀 要 第74号 2015年

Memoirs of the Institute of Science and Engineering, Ritsumeikan University, Kusatsu, Shiga, Japan. No. 74, 2015

−1−

2

Kalf, Okaji and Yamada

1

Introduction

Let

H

₀

= α

· p =

3



j=1

α

_j

p

_j

H = H

₀

+ mβ (m > 0), p

_j

=

∂

∂x

_j

,

where x = (x

₁

, x

₂

, x

₃

)

∈ R

3

and α

_j

and β are 4

× 4 Dirac matrices

satisfying α

_j

α

_k

+ α

_k

α

_j

= 2δ

_jk

I

₄

(1

≤ j, k ≤ 4 ) with α4

:= β. We

regard H

₀

and H as selfadjoint operators acting in the Hilbert space

L

2

_{:= L}

2

₍

_R

3

₎

4

_{. We use the norm}

_{ ·  and the inner product (· , ·)}

in

L

2

. In the present note we investigate the weighted estimate of the

resolvents

R

₀

(z) = (H

₀

− z)

−1

,

R(z) = (H

− z)

−1

,

uniformly for Im z

= 0. Simple uniform resolvent estimates for Dirac

operators are the starting point of the investigations in [Ka].

For

Schr¨

odinger operators a typical uniform resolvent estimate

|x|

α−1

|D|

α

(

−Δ − z)

−1

|D|

α

|x|

α−1

 ≤ const. (Im z = 0)

(1.1)

is shown as Theorem 1 in [KY] for each 0

≤ α < 1/2 (see also [RS1],

[RS2]), where

x =



1 +

|x|

2

,

|x| =



x

2₁

+ x

2₂

+ x

2₃

for x = (x

₁

, x

₂

, x

₃

)

∈ R

3

and

T  is the operator norm of a bounded operator T on L

2

. Here we

use also the weighted Hilbert space for s

∈ R

L

2_s

= L

2_s

(

R

3

)

4

:=

{f(x) | f

_s

:=

x

s

f (x)

 < ∞}

and the Sobolev space

H

s

= H

s

(

R

3

)

4

:=

{f(x) | f

_Hs

=

ξ

s

f (ξ)

ˆ

 < ∞},

where

ˆ

f (ξ) = (2π)

−3/2



R3

e

−iξ,x

_{f (x) dx.}

Uniform resolvent estimates

3

2

The massless case

Theorem

2.1

.

For any s > 1/2 there exists a positive constant C

_s

such

that

x

−s

R

₀

(z)

x

−s

 = x

−s

(α

· p − z)

−1

x

−s

 ≤ C

_s

for any non-real z.

Outline of the proof. Let

(α

· p)u − zu = f,

z = λ + iε, ε

= 0,

for

x

s

f

∈ L

2

(s > 1/2). Let

P

_±

(ξ) =

1

2



I

±

α

· ξ

|ξ|



=

1

2



I

±

₃ j=1

ξ

j

α

j

|ξ|

,

which satisfies

(α

· ξ)P

_±

(ξ) =

±|ξ|P

_±

(ξ)

in view of (α

· ξ)

2

=

|ξ|

2

I

₄

. Therefore we obtain

ˆ

u(ξ) =

1

|ξ| − z

P

+

(ξ) ˆ

f (ξ)

−

1

|ξ| + z

P

−

(ξ) ˆ

f (ξ)

and

(u, f ) = (ˆ

u, ˆ

f ) =



R3



P+

(ξ) ˆ

f (ξ), ˆ

f (ξ)



|ξ| − z

−

P

−

(ξ) ˆ

f (ξ), ˆ

f (ξ)



|ξ| + z



dξ.

(2.1)

Let 1/2 < s < 3/2. For any f

∈ L

2_s

, that is, ˆ

f

∈ H

s

we can define the

trace operator γ(k) from

H

s

to Σ := L

2

(S

2

)

4

for each k > 0 by means

of

(γ(k) ˆ

f )(ω) = k ˆ

f (kω) (ω

∈ S

2

),

such that

γ(k) ˆ

f



_Σ

≤ C min{k

θ

, 1

} f

_s

(k > 0),

(2.2)

γ(k1

) ˆ

f

− γ(k2

) ˆ

f



_Σ

≤ C|k1

− k2|

θ

f

_s

(

|k1

− k2| ≤ 1) (2.3)

with θ = s

− (1/2) > 0 (see [Ku, §2.4 and Chapter IV]). Then (2.1)

above implies

(u, f ) = (ˆ

u, ˆ

f ) =



_∞ 0

(P

₊

(

·)γ(k) ˆ

f , γ(k) ˆ

f )

_Σ

k

− z

dk

−



_∞ 0

(P

₋

(

·)γ(k) ˆ

f , γ(k) ˆ

f )

_Σ

k + z

dk.

A NOTE ON UNIFORM RESOLVENT ESTIMATES OF DIRAC OPERATORS

−3−

4

Kalf, Okaji and Yamada

Privalov’s theorem and the trace theorem guarantee that there is a

pos-itive constant C such that

|(u, f)| ≤ Cf

s

which shows

u

−s

≤ Cf

s

,

or by setting g =

x

s

f ,

x

−s

R

₀

(z)

x

−s

g

 ≤ Cg.



Corollary

2.2

.

Let s > 1/2 and

C

_s

:= sup

Im z=0

x

−s

_R

0

(z)

x

−s

.

Let Q(x) be a measurable 4

× 4 Hermitian matrix-valued function Q(x)

satisfying

sup

x∈R3

x

2s

_{|Q(x)| < 1/C}

. s

Then H

₀

+ Q is purely absolutely continuous on

R.

The proof follows directly from the resolvent equation

x

−s

(H

₀

+ Q

− z)

−1

x

−s

=

1 +

x

−2s

Q(x)

x

−s

R

₀

(z)

x

−s



x

−s

R

₀

(z)

x

−s

.

Remark

2.3

.

It is shown in [KOY] that, if

sup

x∈R3

|x||Q(x)| < 1.

Then zero is not an eigenvalue of H

₀

+ Q.

Remark

2.4

.

In contrast to the Schr¨

odinger case it is shown in [Y] that

x

−s

(α

· p − λ ± i0)

−1

x

−s



with s > 1/2 does not decay as

|λ| → ∞.

Uniform resolvent estimates

5

3

The massive case

The following property was proved in [IM] by the method of weakly

conjugate operators. The idea of proof given here was stimulated by [O]

and [BG].

Theorem

3.1

.

Let m > 0. Then there exists a positive constant C such

that

x

−1

(α

· p + mβ − z)

−1

x

−1

 ≤ C

for any non-real z.

Outline of the proof. Since

(α

· p + mβ − z)

−1

= (α

· p + mβ + z)(p

2

+ m

2

− z

2

)

−1

,



α

· p ∓



z

2

− m

2



₋₁

=



α

· p ±



z

2

− m

2



(p

2

+ m

2

− z

2

)

−1

,

we have

x

−1

(α

· p + mβ − z)

−1

x

−1

=

x

−1

(α

· p ±



z

2

− m

2

)

−1

x

−1

(3.1)

+(mβ + z

∓



z

2

− m

2

)

x

−1

(p

2

+ m

2

− z

2

)

−1

x

−1

. (3.2)

The first term (3.1) can be estimated by Theorem 2.1, while the second

term (3.2) is given by (1.1) of [KY].



Corollary

3.2

.

Let

C

₁

:= sup

Im z=0

x

−1

_R(z)

_x

−1

_.

Let Q(x) be a measurable 4

× 4 Hermitian matrix-valued function Q(x)

satisfying

sup

x∈R3

x

2

_{|Q(x)| < 1/C1}

_.

Then H + Q is purely absolutely continuous on

R.

The non-existence of eigenvalues

±m is obtained in Theorem 1.2 by [BG]

under a similar condition..

Proposition

3.3

.

Theorem 3.1 does not hold for s < 1, that is, we cannot

expect

x

−s

(α

· p + mβ − z)

−1

x

−s

 ≤ C

(3.3)

for any non-real z.

A NOTE ON UNIFORM RESOLVENT ESTIMATES OF DIRAC OPERATORS

−5−

6

Kalf, Okaji and Yamada

For the proof we prepare

Proposition

3.4

.

For s < 1 we cannot expect a uniform resolvent

esti-mate

(−Δ − z)

−1

f



_−s

≤ C

_s

f

_s

for any non-real z and f

∈ L

2_s

.

Proof. Although the proposition is wellknown, we give a simple proof.

Let us assume the uniform resolvent estimate

(−Δ − z)

−1

f



_−s

≤ C

_s

f

_s

(s < 1)

for any f

∈ L

2_s

and z

∈ C such that Im z = 0. Let u ∈ C

₀∞

and put

f = (

−Δ − z)u into the above inequality. we then have

u

−s

≤ C

s

(−Δ − z)u

−s

≤ C

s

Δu

−s

+ C

s

|z|u

−s

for any u

∈ C

₀∞

and z

∈ C such that Im z = 0. In the limit z → 0 we

obtain

u

−s

≤ C

s

Δu

s

for any u

∈ C

₀∞

. Now we can prove

Lemma

3.5

.

Let s < 1. Then there is not any positive constant C

_s

such

that

u

_−s

≤ C

_s

Δu

_s

for any u

∈ C

₀∞

.

Proof. Let g =

t

(r

−α

, 0, 0, 0) and ϕ

∈ C

∞

such that ϕ = 1 (r

≤ 1), = 0

(r

≥ 2). Take R > 0 as sufficiently large and put ϕ

_R

(x) := ϕ(x/R)(1

−

ϕ(x)). Then,

ϕ

R

g



2−s

=



R3

(1 +

|x|)

−2s

_|ϕ

R

(x) g(x)

|

2

dx

≥ C0



_R 2

r

−2s−2α+2

_dr

is divergent as R

→ ∞, if −2s − 2α + 3 ≥ 0. On the other hand,

Δ(ϕ

R

g)



s

is convergent as R

→ ∞, if 2s − 2α − 1 < 0. Therefore there

is a contradiction, if we find α such that

s

−

1

2

< α

≤ −s +

3

2

,

that is, if s < 1.



Uniform resolvent estimates

7

Proof of Proposition 3.3. Let us write

α

_j

=



0 σ

j

σ

_j

0



,

where σ

_j

are Pauli matrices and

H = H

₀

+ mβ =



mI

₂

σ

· p

σ

· p −mI2



(m > 0).

Suppose (3.3) for some s < 1. Then

u

−s

≤ C

s

(H ± mI4

)u



s

for any u

∈ C

₀∞

. Let us consider the case

H + mI

₄

=



2mI

₂

σp

σp

0



.

If u =

t

(v, w) satisfies

v

−s

+

w

−s

≤ C

s

(

2mv + (σp)w

s

+

(σp)v

s

)

and by putting v =

−(1/2m)(σp)w, we have

w

−s

≤ v

−s

+

w

−s

≤ C

s

(

2mv + (σp)w)

s

+

(σp)v

s

)

=

C

 s

2m

Δw

s

.

Therefore we have a contradiction by the same reason as in Lemma 3.5.



4

A refined trace theorem with non-smooth weight functions

In the trace theorem (2.2) and (2.3) we propose that the condition

s > 1/2 for the weight function ρ(r) :=

r

s

is necessary mainly to

the integrability condition



_∞

0

ρ(r)

−2

_{dr <}

_∞.

Recently we noticed that the trace theorem can be proved by replacing

ρ(r) = r

t

r

s

with 0 < t < 1/2 and t + s > 1/2. If we use the result we obtain in the

massless case

A NOTE ON UNIFORM RESOLVENT ESTIMATES OF DIRAC OPERATORS

−7−

8

Kalf, Okaji and Yamada

Proposition

4.1

.

For any 0

≤ t < 1/2, t+s > 1/2 there exists a positive

constant C

_s,t

such that

|x|

−t

x

−s

R

₀

(z)

x

−s

|x|

−t



=

x

−s

|x|

−t

(α

· p − z)

−1

x

−s

|x|

−t

 ≤ C

_ρ

for any non-real z.

In the massive case we have

Proposition

4.2

.

Let m > 0. For any 0 < t < 1/2 there exists a positive

constant C such that

|x|

−t

x

−1+t

(α

· p + mβ − z)

−1

x

−1+t

|x|

−t

 ≤ C

for any non-real z.

The detailed proofs will be given in our forthcoming paper.

Acknowledgement. This work was partially supported by JSPS

KAK-ENHI Grant Number 15K04956.

References

[BG]

N. Boussaid and S. Gol´

enia, Limiting absorption principle for

some long range perturbations of Dirac systems of threshold

energies, Comm. Math. Phys.,

299

(2010), 677–708.

[IM]

A. Iftimovici and Mˇ

antoiu, M., Limiting absorption principle

at critical values for the Dirac operator, Letters Math. Phys.,

49

(1999), 235–243.

[KOY]

H. Kalf, T. Okaji and O. Yamada, The Dirac operator with

mass m

₀

≥ 0: Non-existence of zero-modes and of threshold

eigenvalues, Documenta Math.,

20

(2015), 37–64.

[Ka]

T. Kato, Holomorphic families of Dirac operators, Math. Z.,

183

(1983), 399–406.

[KY]

T. Kato and K. Yajima, Some examples of smooth

opera-tors and the associated smoothing effect, Rev. Math. Phys.,

1

(1989), 481–496.

Uniform resolvent estimates

9

[Ku]

S.T. Kuroda, An Introduction to Scattering Theory, Lecture

Note Series No. 51, Aarhus University, Denmark, 1978.

[O]

T. ¯

Okaji, On the spectrum of Dirac operators, K¯

oky¯

uroku,

RIMS, Kyoto Univ.,

1607

(2008), 65–76.

[RS1]

M. Ruzhansky and M. Sugimoto, Smoothing properties of

evo-lution equations via canonical transforms and comparison

prin-ciple, Proc. London Math. Soc. (3),

105

(2012), 393–423.

[RS2]

M. Ruzhansky and M. Sugimoto, Trace theorems: Critical cases

and best constants, Proc. Amer. Math. Soc.,

143

(2015), 227–

237.

[Y]

O. Yamada, A remark on the limiting absorption method for

Dirac operators, Proc. Japan Acad., Ser. A.,

69

(1993), 243–

246.

Hubert Kalf

Mathematisches Institut

der Universit¨

at M¨

unchen

Theresienstr. 39

D-80333 M¨

unchen,

Germany

hubert.kalf@mathematik.

uni-muenchen.de

Takashi Okaji

Department

of

Mathe-matics, Graduate school

of Science,

Kyoto University

Kyoto 606-8502

Japan

[email protected]

Osanobu Yamada

Faculty of Science and

Engineering

Ritsumeikan University

Kusatsu, Shiga 525-8577

Japan

[email protected].

ac.jp

A NOTE ON UNIFORM RESOLVENT ESTIMATES OF DIRAC OPERATORS

−9−

⌮ᕤᏛ◊✲ᡤ⣖せ  ₁

ࣉࣛࢢ࣐ࢸ࢕ࢫࢺ࡜ࡋ࡚ࡢₙ▼ࡢྍ⬟ᛶ㸫ࢢ࣮ࣟࣂࣝ໬࡟ᑐᓖࡍࡿ

᪥ᮏேㄽ࡬ࡢྵពࢆ᥈ࡗ࡚㸫

ᒣ ୰  ྖ

=======================================================================

A Possibility of Soseki Natsume as a Pragmatist: Exploring the

implications in Theories of Japanese People directing Globalization

Tsukasa Yamanaka

 This paper attempts to reinterpret Soseki Natsume’s theory of civilization from the perspective of pragmatism, and stand out in relief as a pragmatist. Besides it argues that his thought has a significant implication to current Japanese society which is at the mercy of gloablization. According to Sato (2014), acceptance of pragmatism by Soseki has been hardly discussed except for some pointings from Hideyo Yamada (1983) and Shunsuke Tsurumi (2007: 182-185), therefore the approach of these considerations seem to be thought to have novelty. Picking up especially “Gendainihon-no-kaika” and “Watashi-no-kojinshugi” among his criticisms, the paper explores Soseki’s pragmatism and his suggestions for how to behave in the global society.

Keywords; Soseki Natsume, Pragmatism, Globalization, “Jiko-honi”, Theories of Japanese People

E-mail: [email protected] (T. Yamanaka)

=================================================================================

❧࿨㤋኱Ꮫ⏕࿨⛉Ꮫ㒊

College of Life Sciences, Ritsumeikan University, Kusatsu, Shiga 525-8577, Japan

立 命 館 大 学 理 工 学 研 究 所 紀 要 第74号 2015年

Memoirs of the Institute of Science and Engineering, Ritsumeikan University, Kusatsu, Shiga, Japan. No. 74, 2015

−11−

プラグマティストとしての漱石の可能性

−13−

プラグマティストとしての漱石の可能性

−15−

プラグマティストとしての漱石の可能性

−17−

プラグマティストとしての漱石の可能性

−19−

プラグマティストとしての漱石の可能性

−21−

プラグマティストとしての漱石の可能性

−23−

立 命 館 大 学 理 工 学 研 究 所 紀 要 第74号 2015年

Memoirs of the Institute of Science and Engineering, Ritsumeikan University, Kusatsu, Shiga, Japan. No. 74, 2015

−25−

The shape of the smoke is also shown in the left.

Chihiro Kaito, Yoshio Saito

(a )

Oxide Layer Formation on Fe Ultrafine Grain Particles and Characteristic formation of ultrafine Ca particles

−27−

Oxide Layer Formation on Fe Ultrafine Grain Particles and Characteristic formation of ultrafine Ca particles

−29−

Oxide Layer Formation on Fe Ultrafine Grain Particles and Characteristic formation of ultrafine Ca particles

−31−

crystallizations are smaller than 10 nm.

Oxide Layer Formation on Fe Ultrafine Grain Particles and Characteristic formation of ultrafine Ca particles

−33−

Oxide Layer Formation on Fe Ultrafine Grain Particles and Characteristic formation of ultrafine Ca particles

−35−

Oxide Layer Formation on Fe Ultrafine Grain Particles and Characteristic formation of ultrafine Ca particles

−37−

Oxide Layer Formation on Fe Ultrafine Grain Particles and Characteristic formation of ultrafine Ca particles

−39−

Oxide Layer Formation on Fe Ultrafine Grain Particles and Characteristic formation of ultrafine Ca particles

−41−

Oxide Layer Formation on Fe Ultrafine Grain Particles and Characteristic formation of ultrafine Ca particles

−43−

Oxide Layer Formation on Fe Ultrafine Grain Particles and Characteristic formation of ultrafine Ca particles

−45−

Oxide Layer Formation on Fe Ultrafine Grain Particles and Characteristic formation of ultrafine Ca particles

−47−

኱ᆺ◊✲⿦⨨ᡂᯝሗ࿌᭩

−49−

኱ᆺ◊✲⿦⨨ᡂᯝሗ࿌᭩

⿦⨨ྡ _{ࣄ࣮࣐࣮࣓࣮ࣗࣥ࢝ࣟࣜࢱ࣮࣭ேᕤ⎔ቃヨ㦂ᐊ㸦ప㓟⣲ࢳࣕࣥࣂ࣮㸧} ◊✲㈐௵⪅ 㸦ᡤᒓ࣭ᙺ⫋࣭Ặྡ㸧 ┿⏣ ᶞ⩏㸦ࢫ࣏࣮ࢶ೺ᗣ⛉Ꮫ㒊࣭ᩍᤵ㸧 ◊✲ࢸ࣮࣐  㧗ᙉᗘ㐠ື⤊஢ᚋ࡟࠾ࡅࡿ࢚ࢿࣝࢠ࣮ᾘ㈝㔞ࡢኚ໬ࡢືែ㸦ࣄ࣮࣐ࣗࣥ࢝ ࣮࣓࣮ࣟࣜࢱ࣮ࢆ౑⏝ࡋࡓ◊✲㸧  ప㓟⣲⎔ቃୗ࡛ࡢ㐠ືࡀ⢾௦ㅰࡸ㣗ḧㄪ⠇࡟ཬࡰࡍᙳ㡪㸦ప㓟⣲ࢳࣕࣥࣂ ࣮ࢆ౑⏝ࡋࡓ◊✲㸧  ప㓟⣲⎔ቃୗ࡛⾜࠺㧗ᙉᗘࢺ࣮ࣞࢽࣥࢢࡢຠᯝ㸦ప㓟⣲ࢳࣕࣥࣂ࣮ࢆ౑⏝ ࡋࡓ◊✲㸧  ⎔ቃ ࡢ┦㐪ࡀ㐠ື࡟క࠺௦ㅰ࣭ෆศἪືែ࡟ཬࡰࡍᙳ㡪㸦ప㓟⣲ࢳࣕࣥ ࣂ࣮ࢆ౑⏝ࡋࡓ◊✲㸧 ◊✲ࡢᴫせ  ࣄ࣮࣐࣮࣓࣮ࣗࣥ࢝ࣟࣜࢱ࣮ෆ࡛ᐇ᪋ࡍࡿ୍㐣ᛶࡢ▷᫬㛫࣭㧗ᙉᗘ㐠ືࡀࠊ 㐠ືᚋࡢᏳ㟼᫬࡟࠾ࡅࡿ࢚ࢿࣝࢠ࣮ᾘ㈝㔞㸦㓟⣲ᦤྲྀ㔞ࠊ஧㓟໬Ⅳ⣲⏘⏕ 㔞࠿ࡽ⟬ฟ㸧࡟ཬࡰࡍᙳ㡪ࢆ㐠ືᚋᩘ᫬㛫࡟ࢃࡓࡾ㐃⥆ⓗ࡟ゎᯒࡋ࡚࠸ࡿࠋ ࣄ࣮࣐࣮࣓࣮ࣗࣥ࢝ࣟࣜࢱ࣮ࢆ౑⏝ࡍࡿࡇ࡜࡛ࠊ㐠ືᚋࡢ᪥ᖖ⏕άෆ࡟࠾ ࡅࡿ࢚ࢿࣝࢠ࣮ᾘ㈝㔞ࡢኚ໬ࢆ㛗᫬㛫㸦㐠ືᚋ  ᫬㛫㸧࡟ࢃࡓࡾ㧗⢭ᗘ࡟ ᳨ウࡍࡿࡇ࡜ࡀྍ⬟࡜࡞ࡿࠋ  ୰⛬ᗘࡢప㓟⣲⎔ቃୗ࡛⾜࠺୍㐣ᛶࡢ᭷㓟⣲㐠ືࡀ⢾௦ㅰᣦᶆ㸦⾑୰ࢢࣝ ࢥ࣮ࢫࡸ࿧Ẽ࢞ࢫᣦᶆ࠿ࡽ⟬ฟࡋࡓⅣỈ໬≀㓟໬㔞ࠊ⾑୰࢖ࣥࢫࣜࣥ⃰ᗘ ࡞࡝㸧ࡸ㣗ḧㄪ⠇࡟㛵㐃ࡋࡓෆศἪᣦᶆ㸦⾑୰ࢢࣞࣜࣥࠊ3<<ࠊ*/3 ࡞࡝㸧 ࡟ཬࡰࡍᙳ㡪ࢆ᳨ウࡋ࡚࠸ࡿࠋࡲࡓࠊప㓟⣲⎔ቃୗ࡛⾜࠺  㐌㛫⛬ᗘࡢࢺ ࣮ࣞࢽࣥࢢࡀ࢖ࣥࢫࣜࣥឤཷᛶࡢཬࡰࡍᙳ㡪࡟ࡘ࠸࡚ࡶ᳨ウࢆࡋ࡚࠸ࡿࠋ ࡇࡢ㝿࡟ࡣࠊࢺ࣮ࣞࢽࣥࢢᮇ㛫๓ᚋࡢ✵⭡Ᏻ㟼᫬࡟ J ࡢࣈࢻ࢘⢾ࢆ⤒ཱྀ ᦤྲྀࡋࠊ⾑୰ࢢࣝࢥ࣮ࢫࡸ࢖ࣥࢫࣜࣥ⃰ᗘࡢኚ໬ࡢືែࢆホ౯ᣦᶆ࡜ࡋ࡚ ࠸ࡿࠋ  ప㓟⣲⎔ቃୗ࡛⾜࠺㧗ᙉᗘࢺ࣮ࣞࢽࣥࢢࡀࠊ↓㓟⣲ᛶ㐠ືࣃࣇ࢛࣮࣐ࣥࢫ ࡸ㦵᱁➽ෆ࡟࠾ࡅࡿ࢚ࢿࣝࢠ࣮ᇶ㉁㸦ࢡࣞ࢔ࢳࣥࣜࣥ㓟㔞࡞࡝㸧࡟ཬࡰࡍ ᙳ㡪ࢆ᳨ウࡋ࡚࠸ࡿࠋ≉࡟ࠊ 㐌㛫⛬ᗘ࡛᏶⤖ࢆࡍࡿࡁࢃࡵ࡚▷ᮇ㛫࡛ࡢప 㓟⣲ࢺ࣮ࣞࢽࣥࢢࡢຠᯝ࡟╔┠ࢆࡋ࡚࠸ࡿࠋࡲࡓࠊᮏᏛ㐠ື㒊ဨ㸦ዪᏊ㝣 ୖ㒊㛗㊥㞳㑅ᡭ࡞࡝㸧ࡢయຊᙉ໬࡟࠾࠸࡚ࡶࠊ✚ᴟⓗ࡟ά⏝ࡋ࡚࠸ࡿࠋᖺ 㛫ᩘᅇ࡟ࢃࡓࡾࠊ୺せ࡞➇ᢏ఍ࡢ๓࡟᭷㓟⣲ᛶ⬟ຊࡸங㓟௦ㅰ⬟ࡢᨵၿࢆ ࡡࡽ࠸࡜ࡋ࡚ࠊప㓟⣲ᐊෆ࡛ࡢ㧗ᙉᗘࢺ࣮ࣞࢽࣥࢢࢆᐇ᪋ࡋ࡚࠸ࡿࠋ  ప ࡲࡓࡣ㧗 ⎔ቃୗ࡛ࡢ㐠ືࡀ࢚ࢿࣝࢠ࣮௦ㅰࡸ㣗ḧㄪ⠇ࠊ㦵᱁➽⏤᮶ ࡢ⏕⌮άᛶ≀㉁ࡢ⏘⏕࡟ཬࡰࡍᙳ㡪ࢆ᳨ウࡋ࡚࠸ࡿࠋ≉࡟ࠊప ⎔ቃୗ࡛

ࡢ୍㐣ᛶࡢ㐠ືࡀ㦵᱁➽⏤᮶ࡢ⏕⌮άᛶ≀㉁㸦࢖ࣜࢩࣥ㸧ࡢ⏘⏕࡟ཬࡰࡍ ᙳ㡪࡟╔┠ࢆࡋ࡚࠸ࡿࠋࡲࡓࠊ㣗ḧㄪ⠇࡟㛵ࢃࡿ◊✲࡛ࡣࠊ⎔ቃ ࡸ㓟⣲ ⃰ᗘࡢኚ໬ࡀ㣗ḧㄪ⠇࡟㛵㐃ࡍࡿෆศἪᣦᶆࡸ㐠ືᚋ࡟࠾ࡅࡿ㣗஦㔞࡟ཬ ࡰࡍᙳ㡪ࢆ᳨ウࡋ࡚࠸ࡿࠋ ฼⏝ᡂᯝ 1. ▷᫬㛫࣭㧗ᙉᗘ㐠ືᚋ࡟ࡣᩘ᫬㛫࡟ࢃࡓࡾᏳ㟼᫬࡛ࡢ࢚ࢿࣝࢠ࣮ᾘ㈝㔞ࡸ 㣗ᚋ࡟࠾ࡅࡿ࢚ࢿࣝࢠ࣮ᾘ㈝㔞ࡀஹ㐍ࡍࡿࡇ࡜ࢆㄆࡵ࡚࠸ࡿࠋ 2. ప㓟⣲⎔ቃୗ࡛⾜࠺㐠ື࡛ࡣ⢾௦ㅰࡀஹ㐍ࡍࡿ୍᪉࡛ࠊ㣗ḧㄪ⠇࡟㛵㐃ࡍ ࡿෆศἪᣦᶆ࡟ࡣ኱ࡁ࡞ᙳ㡪ࡣࡳࡽࢀ࡞࠸ࡇ࡜ࢆㄆࡵ࡚࠸ࡿࠋ 3. ప㓟⣲⎔ቃୗ࡛⾜࠺㧗ᙉᗘࢺ࣮ࣞࢽࣥࢢࡣ▷᫬㛫࡛ࡢ㐠ື᫬ࡢ᭱኱Ⓨ᥹ࣃ ࣮࣡ࡢᨵၿ࡟᭷ຠ࡛࠶ࡿࡇ࡜ࠊ➽ࢡࣞ࢔ࢳࣥࣜࣥ㓟㔞ࡢቑຍࢆࡶࡓࡽࡍࡇ ࡜ࢆㄆࡵ࡚࠸ࡿࠋࡲࡓࠊᮏᏛዪᏊ㝣ୖ㒊㛗㊥㞳㑅ᡭ࡟ᑐࡋ࡚ᐃᮇⓗ࡟ప㓟 ⣲ࢺ࣮ࣞࢽࣥࢢࢆᑟධࡋࠊ඲᪥ᮏ኱ᏛዪᏊ㥐ఏ5 㐃ぞࠊ඲᪥ᮏ኱ᏛዪᏊ㑅 ᢤ㥐ఏ㸦ᐩኈᒣዪᏊ㥐ఏ㸧3 㐃ぞ࡞࡝ࡢᡂᯝ࡟㈉⊩ࢆࡋ࡚࠸ࡿࠋ 4. ప ⎔ቃ࡛ࡣࠊ୍㐣ᛶࡢ㐠ື࡟క࠺㣗ḧῶ㏥ࡢ⛬ᗘࡀ㍍ῶࡉࢀࡿࡇ࡜ࢆㄆ ࡵ࡚࠸ࡿࠋ ࠙ㄽᩥ㸦2015ࠥ2016 ᖺ㸧ࠚ

1. Morisihma T, Goto K. Ghrelin, GLP-1 and Leptin Responses during Exposure to Moderate Hypoxia. Appl Physiol Nutr Metab, 2016 (in press)

2. Goto K, Morishima T, Kurobe K, Huang Z, Ogita F. Augmented carbohydrate oxidation under moderate hypobaric hypoxia equivalent to simulated altitude of 2500m. Tohoku J Exp Med. 36 (3): 163-168, 2015

3. Kasai N, Mizuno S, Ishimoto S, Sakamoto E, Maruta M, Goto K. Effect of training in hypoxia on repeated sprint performance in female athletes. Springerplus, 4: 310, 2015

4. Kojima C, Sasaki H, Tsuchiya Y, Goto K. The influence of environmental temperature on appetite-related hormonal responses. J Physiol Anthropol. 34 (1):22, 2015

5. Morishima T, Kurihara T, Hamaoka T, Goto K. Effects of different periods of hypoxic training on glucose metabolism and insulin sensitivity. Clin Physiol Funct Imaging, 35 (2): 104-109, 2015 ࠙ᅜෆᏛ఍ࠚ 1. ➟஭ಙ୍, ᑠᓥ༓ᑜ, 㧗ᶫⱥᖾ, ᚋ⸨୍ᡂ, 㕥ᮌᗣᘯ, 㝣ୖ➇ᢏ▷㊥㞳㑅ᡭ ࡟࠾ࡅࡿ▷ᮇ㛫ࡢప㓟⣲ࢺ࣮ࣞࢽࣥࢢࡀ㦵᱁➽࢚ࢿࣝࢠ࣮ᇶ㉁㔞࡟ཬࡰࡍ ᙳ㡪, ➨ 70 ᅇయຊ་Ꮫ఍኱఍, ࿴ḷᒣ┴Ẹᩥ໬఍㤋 ࿴ḷᒣ, 2015 −51−

࠙ಟኈㄽᩥࠚ 1. ప㓟⣲⎔ቃୗ࡟࠾ࡅࡿࢫࣉࣜࣥࢺࢺ࣮ࣞࢽࣥࢢࡢຠᯝ࡟㛵ࡍࡿ◊✲, 2016 ᖺ 1 ᭶ᥦฟ ࠙༤ኈㄽᩥࠚ 1. ▷ᮇ㛫ࡢ㌟యάື࡜㣗஦ෆᐜࡢኚᐜࡀ㐠ື᫬࡟࠾ࡅࡿᡂ㛗࣍ࣝࣔࣥࡢศἪ ᛂ⟅࡟ཬࡰࡍᙳ㡪࡟㛵ࡍࡿ◊✲㸪2016 ᖺ 1 ᭶ᥦฟ 2. ୍㐣ᛶࡢ㐠ື࡟ᑐࡍࡿ࢖ࣜࢩࣥࡢศἪᛂ⟅࡟㛵ࡍࡿ◊✲ࠊ2016 ᖺ 1 ᭶ᥦฟ

⿦⨨ྡ㸹 ㉸㧗ศゎ⬟ศᯒࢩࢫࢸ࣒    



◊✲㈐௵⪅ ᶵᲔᕤᏛ⛉ ᩍᤵ 䭯ᒣ᝴ 㸦⟶⌮ጤဨ㛗㸧 㒊㛛ྡ  ◊✲ࢸ࣮࣐  ㄪ࿴⤌⧊ไᚚ࡟ࡼࡿ㧗ᶵ⬟ᮦᩱࡢ๰〇  」┦ྜ㔠࡟࠾ࡅࡿ➨  ┦ࡢᙧែ࡜⤖ᬗᏛⓗ≉ᚩ  㧗 ࡟࠾ࡅࡿከ㍈పࢧ࢖ࢡࣝ⑂ປ࠾ࡼࡧࢡ࣮ࣜࣉ◚᩿ᑑ࿨ホ౯ἲࡢ◊✲  㟁Ꮚࢹࣂ࢖ࢫ⏝ᶞ⬡ⷧ⭷ࡢ≀ᛶ್ホ౯ἲࡢ᳨ウ  㟁Ꮚ㢧ᚤ㙾࡟ࡼࡿ㓟໬≀࡟ᢸᣢࡋࡓ㔠ᒓゐ፹ᮦᩱࡢ⾲㠃ほᐹ  ୕ḟඖࣇ࢛ࢺࢽࢵࢡ⤖ᬗࡢᙧᡂ  ❅໬≀༙ᑟయࡢᴟᚤᵓ㐀ホ౯  Cu(InࠊGa)Se2⣔ከ⤖ᬗⷧ⭷ኴ㝧㟁ụࡢ⏺㠃ᵓ㐀ไᚚ  ᶵ⬟ᛶࢼࣀᮦᩱࡢᙧែࡸᵓ㐀ࠊ࠾ࡼࡧࡑࡢㅖ≀ᛶホ౯ ◊✲ࡢᴫせ ㉸㧗ศゎ⬟ศᯒࢩࢫࢸ࣒ࡣࠊຍ㏿㟁ᅽ N9 ࡢ ('6 ศᯒ⿦⨨௜ᒓᆺ㉮ᰝᆺ㟁 Ꮚ㢧ᚤ㙾㸦6(0㸧ࠊN9ࠊ87:('6 ศᯒ⿦⨨௜ᒓ㧗ศゎ⬟ 7(0 ࠿ࡽᵓᡂࡉࢀ࡚ ࠾ࡾࠊ≀㉁⛉Ꮫศ㔝ࢆ୰ᚰ࡟ᗈ࠸㡿ᇦ࡛ά⏝ࡉࢀ࡚࠸ࡿ㸬ά⏝౛࡜ࡋ࡚ࠊ◊ ✲ࢸ࣮࣐㸯ࢆ௨ୗ࡟⤂௓ࡍࡿ㸬   㔠ᒓᮦᩱࡣࠊຊᏛ≉ᛶࡢࡳ࡞ࡽࡎຍᕤᛶࡸ⪏㣗ᛶ࡞࡝ࠊඃࢀࡓᛶ㉁ࢆᩘከ ࡃഛ࠼࡚࠾ࡾࠊ᭷⏝࡞⣲ᮦ࡛࠶ࡿࠋ࡜ࡾࢃࡅࠊᘓ⠏ᵓ㐀యࡸ㍺㏦ᶵჾ࡞࡝ࡢ 㠃࠿ࡽ♫఍ᇶ┙ࢆᨭ࠼ࡿᵓ㐀⏝ᮦᩱ࡟࡜ࡾᙉᗘࡣ㔜せ࡞ᛶ㉁࡛࠶ࡾࠊࡇࢀࡲ ࡛ᵝࠎ࡞ᡭἲ࡟ࡼࡾ㧗ᙉᗘᮦᩱࡢ㛤Ⓨࡀ㐍ࡵࡽࢀ࡚ࡁࡓࠋࡑࡢ୰࡛ࡶ≉࡟ࠊ ⤖ᬗ⢏ᚤ⣽໬ἲࡣ㧗ᙉᗘ໬࡟ᴟࡵ࡚᭷ຠ࡛࠶ࡿࡇ࡜࠿ࡽ኱ࡁ࡞㛵ᚰࢆ㞟ࡵ࡚ ࡁࡓࠋ⤖ᬗ⢏ࡀᚤ⣽໬ࡍࡿ࡜ +DOO3HWFK ࡢ㛵ಀ ࡛▱ࡽࢀࡿࡼ࠺࡟ࠊ⤖ᬗ⢏ ᚄࡢᖹ᪉᰿ࡢ㏫ᩘ࡟ẚ౛ࡋ࡚ᙉᗘࡀୖ᪼ࡍࡿࠋࡋ࠿ࡋࠊ୍᪉࡛ࠊ㧗ᙉᗘᮦᩱ ࡛ࡣ㝆అᚋࠊ᪩ᮇ࡟ረᛶ୙Ᏻᐃࡀ⏕ࡌ࡚ࢿࢵ࢟ࣥࢢࢆ㉳ࡇࡋ◚᩿࡟⮳ࡾᘏᛶ ࡀᦆ࡞ࢃࢀࡿ࡜࠸࠺ၥ㢟ࡀ࠶ࡿࠋࡇࡢࠕᙉᗘࠖ࡜ࠕᘏᛶࠖࡢࢺ࣮ࣞࢻ࢜ࣇࡢ 㛵ಀࡣࠊ㔠ᒓᮦᩱࡢ㧗ᙉᗘ໬࡟࠾࠸࡚㔜せ࡞ㄢ㢟࡜࡞ࡗ࡚࠸ࡿࠋࡇࢀ࡟ᑐࡋ ࡚ࠊ኱ࡁ࡞ረᛶࡦࡎࡳࢆᚓࡿࡓࡵ࡟ࠊኚែㄏ㉳ረᛶ㸦7UDQVIRUPDWLRQ,QGXFHG 3ODVWLFLW\75,3㸧ࡸ཮ᬗㄏ㉳ረᛶ㸦7ZLQQLQJ,QGXFHG3ODVWLFLW\7:,3㸧 ࡢ฼⏝ࡀ᳨ウࡉࢀ࡚࠸ࡀࠊࡇࢀࡽࡢ 75,3ࠊ7:,3 ⌧㇟ࡣⓎ⌧ࡍࡿᮦᩱࡀ㝈ᐃࡉ ࢀ࡚࠸ࡿࠋ୍᪉࡛ࠊ⢊ᮎ෬㔠ἲࢆᛂ⏝ࡋࡓㄪ࿴⤌⧊ไᚚἲ㸦+DUPRQLF6WUXFWXUH 'HVLJQ㸧ࡣ⣧㔠ᒓࠊྜ㔠࡟㝈ࡽࡎ㔠ᒓᮦᩱࡢ㧗ᘏᛶ໬࡟᭷ຠ࡞ᡭἲ࡛࠶ࡾࠊ ㏆ᖺࠊ✀ࠎࡢ㔠ᒓᮦᩱ࡟㐺⏝ࡋࡓ◊✲ࡀሗ࿌ࡉࢀ࡚࠸ࡿࠋᚑ᮶࠿ࡽࡢ࣑ࢡࣟ ࡞ᙉ໬ἲ࡜ᵓ㐀⏤᮶ࡢ࣐ࢡࣟ࡞㧗ᘏᛶ໬࡜ࢆ⤌ࡳྜࢃࡏࡓ᪂ࡋ࠸ᮦ㉁タィᡭ ἲ࡛࠶ࡿࠋᮏ◊✲࡛ࡣㄪ࿴⤌⧊ไᚚἲ࡟ࡘ࠸࡚ヲ⣽࡞᳨ウࡋࡓࠋ −53−

 ฼⏝ᡂᯝ

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㸺ㄽᩥ㸼

㸦㸯㸧InN NanoColumns Grown by Molecular Beam Epitaxy and Their Luminescence Properties, K. Wang, T. Araki, T. Yamaguchi, Y.T. Chen, E. Yoon, Y. Nanishi, J. Cryst. Growth, 430 (2015) 93-97.

㸦㸰㸧Masao Sakane, Takamoto Itoh, Hideyuki Kanayama; “Effect of Multiaxial Stress on Low Cycle Fatigue”, Bulletin of JSME, Mechanical Engineering Reviews, Vol.2, No.1, (2015), pp.1-15. DOI: 10.1299/mer.14-00214

㸦㸱㸧Takahiro Morishita, Takamoto Itoh, Masao Sakane, Hiroshi Nakamura, Masahiro Takanashi; “Multiaxial Fatigue Property of Ti-6Al-4V using Hollow Cylinder Specimen under Push-pull and Cyclic Inner Pressure Loading Article reference”, International Journal of Fatigue,

DOI:10.1016/j.ijfatigue.2016.02.019

㸦㸲㸧Takahiro Morishita, Takamoto Itoh, “Evaluation of multiaxial low cycle fatigue life for type 316L stainless steel notched specimen under non-proportional loading”, Theoretical and Applied Fracture Mechanics, DOI: 10.1016/j.ijpvp.2016.02.024

㸦㸳㸧Controlled back slope of Ga/(In+Ga) profile in Cu(In,Ga)Se2 absorber fabricated by multi layer precursor method for improvement of its photovoltaic performance J. Chantana, D. Hironiwa, T. Watanabe, S. Teraji, K. Kawamura, T. Minemoto Sol. Energy Mater. Sol. Cells 133 (2015) 223-228.

㸦㸴㸧Estimation of open-circuit voltage of Cu(In,Ga)Se2 solar cells before cell fabrication J. Chantana, D. Hironiwa,T. Watanabe, S. Teraji, K. Kawamura, T. Minemoto Renewable Energy 76 (2015) 575-581.

㸦㸵㸧Application of Multi-Buffer Layer of (Zn,Mg)O/CdS in Cu2ZnSn(S,Se)4 Solar Cells D. Hironiwa, J. Chantana, N. Sakai, T. Katou, H. Sugimoto, T. Minemoto Curr. Appl. Phys. 15 (2015) 383-388.

㸦㸶㸧Evaluation of sputtering damage in Cu2ZnSn(S,Se)4 solar cells with CdS and (Cd, Zn)S buffer layers by photoluminescence N. Matsuo, D. Hironiwa, J. Chantana, N. Sakai, T. Kato, H. Sugimoto, T. Minemoto Jpn. J. Appl. Phys. 54 (2015) 042302-1-5.

㸦㸷㸧Raman Peak Position of Cu(In,Ga)Se2 Film for Predication of Ga/(In+Ga) Content near Its Surface and Open-Circuit Voltage J. Chantana, D. Hironiwa,T. Watanabe, S. Teraji, K. Kawamura, T. Minemoto Thin Solid Films 582 (2015) 7-10.

㸦㸯㸮㸧 Impact of Annealing Treatment Before Buffer Layer Deposition on Cu2ZnSn(S,Se)4 Solar Cell D. Hironiwa, N. Sakai, T. Katou, H. Sugimoto, Z.Tang, J. Chantana, T. Minemoto Thin Solid Films 582 (2015) 151-153.

㸦㸯㸯㸧 Impact of growth temperature on the properties of SnS film prepared by thermal evaporation and its photovoltaic performance Y. Kawano, J. Chantana, T. Minemoto Curr.

Appl. Phys. 15 (2015) 897-901.

㸦㸯㸰㸧 Effect of ammonia etching on structural and electrical properties of Cu2ZnSn(S,Se)4 absorbers D. Hironiwa, R. Takai, J. Chantana, N. Sakai, T. Katou, H. Sugimoto, T. Minemoto Appl. Surf. Sci. 335 (2015) 209-213.

㸦㸯㸱㸧 Bismuth-doped Cu(In,Ga)Se2 absorber prepared by multi-layer precursor method and its solar cell J. Chantana, D. Hironiwa, T. Watanabe, S. Teraji, K. Kawamura, T. Minemoto Phys. Status Solidi C 12 (2015) 680-683.

㸦㸯㸲㸧 Reaction path for formation of Cu2SnSe3 film by selenization of Cu-Sn precursor Z. Tang, K. Aoyagi, Y. Nukui, K. Kosaka, H. Uegaki, J. Chantana, D. Hironiwa, T. Minemoto Sol. Energy Mater. Sol. Cells 143 (2015) 311-318.

㸦㸯㸳㸧 Physical properties of Cu(In,Ga)Se2 film on flexible stainlesssteel substrate for solar cell application : A multi-layer precursor method J. Chantana, D. Hironiwa, T. Watanabe, S. Teraji, T. Minemoto Sol. Energy Mater. Sol. Cells 143 (2015) 510-516.

㸦㸯㸴㸧 Investigation on evaporation and supression of SnS during fabrication of Cu2SnS3 thin films Z. Tang, K. Kosaka, H. Uegaki, J. Chantana, Y. Nukui, D. Hironiwa, T. Minemoto Phys. Status Solidi A 212 (2015) 2289-2296.

㸦㸯㸵㸧 Annealing effect on Cu2ZnSn(S,Se)4 solar cell with Zn1-xMgxO buffer layer D. Hironiwa, N. Matsuo, J. Chantana, N. Sakai, T. Katou, H. Sugimoto, T. Minemoto Phys. Status Solidi A 212 (2015) 2766-2771.

㸦㸯㸶㸧 Takashi Nakamura, Misaki Katayama, Toshiki Watanabe, Yasuhiro Inada, Takeo Ebina, Aritomo Yamaguchi, “Stability of Copper Nitride Nanoparticles under High Humidity and in Solutions with Different Acidity”, Chem. Lett., 2015, 44(6), 755-757.

㸦㸯㸷㸧 ∦ᒣ┿⚈, ✄⏣ᗣᏹ, ᑎᮧㅬኴ㑻, ⏣୰ᗤ⿱㸪͆ศᏊ≧㓟⣲ࡢάᛶ໬ᶵ⬟ࢆ᭷ࡍࡿ ᢸᣢࣂࢼࢪ࣒࢘㓟໬≀ගゐ፹࡟㛵ࡍࡿගບ㉳≧ែࡢXAFS ゎᯒ͇㸪 SPring-8/SACLA ฼⏝◊ ✲ᡂᯝ㞟㸪2015, 3(2), 609-612.

㸦㸰㸮㸧 Misaki Katayama, Ryota Miyahara, Toshiki Watanabe, Hirona Yamagishi, Shohei Yamashita, Terue Kizaki, Toshimi Sugawara, Yasuhiro Inada, “Development of Dispersive XAFS System for Analysis of Time-Resolved Spatial Distribution of Electrode Reaction”, J. Synchrotron Rad., 2015, 22(5), 1227-1232.

㸦㸰㸯㸧 ∦ᒣ┿⚈, ✄⏣ᗣᏹ㸪͆X ⥺྾཰ᚤ⣽ᵓ㐀ἲ࡟ࡼࡿࣜࢳ࣒࢘ศᕸࡢ࢖࣓࣮ࢪࣥࢢ͇㸪 J. Vac. Soc. Jpn., 2015, 58(10), 375-378.

㸦㸰㸰㸧 Shohei Yamashita, Yusaku Yamamoto, Misaki Katayama, and Yasuhiro Inada, “Kinetic Study on Solid-Phase Reduction of Silica-Supported Nickel Oxide Species”, Bull. Chem. Soc. Jpn., 2015, 88(12), 1629-1635.

㸦㸰㸱㸧 G. Dirras, M. Ota, D. Tingaud, K. Ameyama and T. Sekiguchi; “Microstructure evolution during direct impact loading of commercial purity Į-titanium with harmonic structure design”, Mat´eriaux & Techniques 103, 311 (2015), DOI: 10.1051/mattech/2015031,

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www.mattech-journal.org 㸦㸰㸲㸧 ኴ⏣ ⨾⤮ࠊ䭯ᒣ ᝴㸹ࠗ㸫⢊ᮎ෬㔠ࡢ᪂ࡋ࠸ྍ⬟ᛶ㸫ㄪ࿴⤌⧊ไᚚἲ࡟ࡼࡿ㧗 ᙉᗘ࣭㧗ᘏᛶᮦᩱࡢ๰〇࠘ࠊ⢊య⢊ᮎ෬㔠༠఍ࠊvol.62(2015)ࠊNo.6ࠊpp297-301. 㸦㸰㸳㸧 ኴ⏣ ⨾⤮ࠊ⳥ụ ᑗ୍ࠊୖ㔝 ᫂ࠊ䭯ᒣ ᝴㸹ࠗㄪ࿴⤌⧊ไᚚἲ࡟ࡼࡿ㧗ᙉᗘ࣭ 㧗ࡌࢇᛶࢆ᭷ࡍࡿ㔠ᒓᮦᩱࡢ๰〇࠘ࠊ໬ᏛᕤᏛ఍ࠊvol.79(2015)ࠊNo.5ࠊpp.372-374. 㸦㸰㸴㸧 ᰘ⏣ 㥴, ኳ㇂ ㅍ, ᮡᒣ 㐍, Ᏻ⸨ ጁᏊ, 㟼㟁ᐜ㔞ᆺ᣺ືᏊࢆ⏝࠸ࡓ PMMA ࡢ⑂ ປヨ㦂, 㟁ẼᏛ఍ㄽᩥㄅ E㸦ࢭࣥࢧ࣭࣐࢖ࢡ࣐ࣟࢩࣥ㒊㛛ㄅ㸧, 135/7, 257, (2015).

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㸦㸯㸧Kusaka, T., "Toughening Mechanisms in Composite Materials", 2015 ᖺ 9 ᭶, Woodhead Publishing, ➨9 ❶.

㸺ᅜ㝿఍㆟࣭ㄽᩥ㸼

㸦㸯㸧RF-MBE Growth of InN on Mist-CVD Grown ǂ-In2O3/Sapphire, T. Araki, N. Masuda, A. Buma, Y. Nanishi, M. Oda and T. Hitora, The 3rd International Conference on Light-Emitting Devices and Their Industrial Applications (LEDIA '15), Yokohama, Japan (2015.4)

㸦㸰㸧Growth and Characterization of InN on ǂ-In2O3/Sapphire by RF-MBE, N. Masuda, A. Buma, T. Araki, Y. Nanishi, M. Oda, and T. Hitora, The 7th _{Asia-Pacific Workshop on}

Widegap Semiconductors (APWS 2015), Seoul, Korea (2015.5)

㸦㸱㸧RF-MBE Growth and Structural Characterization of InN on Mist-CVD-grown alpha-In2O3/Sapphire, A. Buma, N. Masuda, T. Araki, Y. Nanishi, M. Oda, and T. Hitora, The 6th International Symposium on Growth of Ϫ-nitrides, Hamamatsu, Japan (2015.11)

㸦㸲㸧Growth and Characterization of Thin InN Films Grown by RF-MBE, A. Usuda, K. Komura, M. Aranami, T. Araki, and Y. Nanishi, The 6th International Symposium on Growth of Ϫ-nitrides, Hamamatsu, Japan (2015.11)

㸦㸳㸧Takamoto Itoh, Takahiro Morishita, Masao Sakane; “Evaluation and Visualization of Multiaxial Stress and Strain States under Non-proportional Loading”, First International Workshop on Challenges in Multiaxial Fatigue Urbino, Italy, 22-24 April 2015

㸦㸴㸧Takahiro Morishita, Takamoto Itoh, Zhenlong Bao; “Fatigue Life of Type 316 Stainless Steel under Wide Ranged Multiaxial Loading”, 14th International Conference on Pressure Vessel Technology Proceedings of ICPVT̺14, 23–26 September, 2015, Shanghai, China

㸦㸵㸧Takamoto Itoh, Masao Sakane, Takahiro Morishita, Hiroshi Nakamura, Masahiro Takanashi; “Crack mode and life of Ti-6Al-4V under multiaxial low cycle fatigue”, The 5th International Conference on CRACK PATHS (CP 2015), Ferrara, Itally 16-18 September 2015

miniature specimens”, Thirty-Second Spanish Conference on Fracture and Structural Integrity (32 SCFSI) ESIS TC-10 Workshop Enviromentaly Assisted Cracking & Hydorogen Embriilement, Zamora, Spain, 27-29 April 2015

㸦㸷㸧Muhammad, A.B.A.H., Kusaka, T, Tanageshima, R., "Effect of Loading Frequency on Mixed Mode Fatigue Crack Growth Behavior in CFRP Adhesive Joints", International Conference on Advanced Technology in Experimental Mechanics 2015, October 4-8, 2015, (Toyohashi, Japan).

㸦㸯㸮㸧 Zailani, S., Kawamura, Y., Kusaka, T., Tanegashima, R., Takahashi, J., "Effect of Materials Composition on Progressive Crashing Behavior of Composite Laminates", International Conference on Advanced Technology in Experimental Mechanics 2015, October 4-8, 2015, (Toyohashi, Japan).

㸦㸯㸯㸧 Oka, N., Kusaka, T, Tanageshima, R., "Mixed Mode Fracture Behavior of CFRP Adhesive Joints under Static and Impact Loading", International Conference on Advanced Technology in Experimental Mechanics 2015, October 4-8, 2015, (Toyohashi, Japan).

㸦㸯㸰㸧 Miyawaki, A., Kitai, Y., Kusaka, T., Tanegashima, R., Tanaka, Y., Hineno, Y., "Numerical Analysis of Sealing Mechanism in Triple Offset Butterfly Valves", 5th International Symposium on Functionalization and Applications of Soft/Hard Materials, January 21-24, 2016, (Kusatsu, Japan). 㸦㸯㸱㸧 Ohara, M., Han, X., Tanegashima, R., Kusaka, T., "Application of Fine Blanking

Technique to Precision Punching of CFRP Plates", 5th International Symposium on Functionalization and Applications of Soft/Hard Materials, January 21-24, 2016, (Kusatsu, Japan). 㸦㸯㸲㸧 Honda, H., Seike, N., Tanegashima, R., Kusaka, T., "A Novel Joining Technique for

Composite Laminates by Termal Decomposition Process Using Cr2O3 Catalyst", 5th International Symposium on Functionalization and Applications of Soft/Hard Materials, January 21-24, 2016, (Kusatsu, Japan).

㸦㸯㸳㸧 Yusop, H., Oka, N., Tanegashima, R., Kusaka, T., "Experimental Characterization of Impact Fracture Toughness of CFRP Adhesive Joints Using SHPB Technique", 5th International Symposium on Functionalization and Applications of Soft/Hard Materials, January 21-24, 2016, (Kusatsu, Japan).

㸦㸯㸴㸧 Syafiq, M., Aqmal, M., Fujita, M., Tanegashima, R, Kusaka, T., "Effect of Loading Rate on Fatigue Crack Growth Behavior in CFRP Adhesive Joints", 5th International Symposium on Functionalization and Applications of Soft/Hard Materials, January 21-24, 2016, (Kusatsu, Japan). 㸦㸯㸵㸧 Misaki Katayama, Taro Uenoyama, Ryota Miyahara, Yasuhiro Inada, “Reaction

distribution in LiNiO2 positive electrode of lithium ion battery”, 16th International Conference on

X-Ray Absorption Fine Structure, Karlsruhe, Germany, Aug. 2015.

㸦㸯㸶㸧 Shohei Yamashita, Yusaku Yamamoto, Misaki Katayama, Yasuhiro Inada, “Clarification of redox mechanism of nickel species supported on silica”, 16th International Conference on X-Ray Absorption Fine Structure, Karlsruhe, Germany, Aug. 2015.

㸦㸯㸷㸧 Yusaku Yamamoto, Shohei Yamashita, Nik Afiza Binti, Misaki Katayama, Yasuhiro

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Inada, “Microscopic investigations for preparation and redox processes of supported Ni catalyst prepared by sol-gel method”, 16th International Conference on X-Ray Absorption Fine Structure, Karlsruhe, Germany, Aug. 2015.

㸦㸰㸮㸧 Siwaruk Chotiwan, Hiroki Tomiga, Shohei Yamashita, Misaki Katayama, Yasuhiro Inada, “Time-resolved study on dynamic chemical state conversion of supported metal species on silica by means of dispersive XAFS technique”, 16th International Conference on X-Ray Absorption Fine Structure, Karlsruhe, Germany, Aug. 2015.

㸦㸰㸯㸧 Kiyohiko Ikeda, Toshiki Watanabe, Misaki Katayama, Yasuhiro Inada, “XAFS analysis of calcination process for Cr catalysts supported on Ȗ-Al2O3 and SiO2”, 16th International

Conference on X-Ray Absorption Fine Structure, Karlsruhe, Germany, Aug. 2015.

㸦㸰㸰㸧 Misaki Katayama, Ryota Miyahara, Hirona Yamagishi, Shohei Yamashita, Yasuhiro Inada, “Time-resolved spatial distribution analysis of electrode reaction by means of vertically dispersive XAFS technique”, PacifiChem 2015, Honolulu, USA, Dec. 2015.

㸦㸰㸱㸧 hota Kikuzaki, Chihiro Yogi, Tomoe Sanada, Kazuo Kojima, Misaki Katayama, Yasuhiro Inada, Toshiaki Ohta, “Effects of sulfur electrolyte additives on solid electrolyte interfaces of lithium-ion batteries”, PacifiChem 2015, Honolulu, USA, Dec. 2015.

㸦㸰㸲㸧 Ryota Miyahara, Misaki Katayama, Yasuhiro Inada, “Development of in-situ battery cell for X-ray absorption spectroscopy”, PacifiChem 2015, Honolulu, USA, Dec. 2015.

㸦㸰㸳㸧 Mie Ota, Sanjay Kumar Vajpai, Han Yu, Hidenori Maezawa and Kei Ameyama; “Novel Microstructure Design for High Mechanical Performance Pure Titanium”, 5th International Symposium on Functionalization and Applications of Soft/Hard materials, Jan. 21-24, 2016, Kusatsu, Japan.

㸦㸰㸴㸧 Sanjay Kumar Vajpai, Mie Ota, Kei Ameyama, Tomoyuki Watanabe, Ryo Maeda, David Tingaud and Guy Dirras; “HARMONIC STRUCTURE: AN EFFECTIVE TAILORED HETEROGENEOUS MICROSTRUCTURAL DESIGN TO STRENGTHEN TI-6AL-4V ALLOY”, The 13th World conference on Titanium, Aug. 16-20, 2015, San Diego, USA.

㸦㸰㸵㸧 Mie Ota, Sanjay Kumar Vajpai, Hidenori Maezawa, Hikaru Kawabata and Ameyama; “Innovative Materials Design for High Performance Pure Titanium”, The 13th World conference on Titanium, Aug. 16-20, 2015, San Diego, USA.

㸦㸰㸶㸧 Kei Ameyama, Mie Ota and Sanjay Kumar Vajpai; “Deformation Mechanism of Harmonic Structure Materials with High Strength and High Ductility”, International Workshop on Giant Straining Process for Advanced Materials in 2015 (GSAM2015), Sep. 3-6, 2015, Fukuoka, Japan.

㸦㸰㸷㸧 R. Maeda, T. Watanabe, Shota Yokoyama, M. Ota, S. K. Vajpai and K. Ameyama, “Unique mechanical properties of Harmonic Structure Designed Ti-6Al-4V compact produced by High Pressure Gas Milling”, Nov. 8-10, 2015, Kyoto, Japan.

Harmonic Structure Pure Al by Extrusion”, Nov. 8-10, 2015, Kyoto, Japan.

㸦㸱㸯㸧 Kiichi Sawai, Daiki Ueda, Sanjay K. Vajpai, Mie Ota and Kei Ameyama; “Unique Deformation Behavior in Harmonic Structure Designed Pure Iron Compacts”, Nov. 8-10, 2015, Kyoto, Japan.

㸦㸱㸰㸧 Yamato Suto, Takato Yamada, Mie Ota, Sanjay K. Vajpai and Kei Ameyama; “Strain Rate Dependence of Harmonic Structure Designed Pure Cu”, Nov. 8-10, 2015, Kyoto, Japan.

㸦㸱㸱㸧 Sanjay Kumar Vajpai, Mie Ota, Kei Ameyama; “HIGH PERFORMANCE ADVANCED STRUCTURAL MATERIALS THROUGH AN INNOVATIVE GRADIENT MICROSTRUCTURE HARMONIC STRUCTURE DESIGN”, 5th International Symposium on Functionalization and Applications of Soft/Hard materials, Jan. 21-24, 2016, Kusatsu, Japan.

㸦㸱㸲㸧 Bhupendra Sharma, Sanjay Kumar Vajpai and Kei Ameyama; “A Novel Powder Metallurgy Processing Approach to Prepare Fine-Grained ȕ Ti-Nb alloy from Titanium Hydride Powder”, 5th International Symposium on Functionalization and Applications of Soft/Hard materials, Jan. 21-24, 2016, Kusatsu, Japan.

㸦㸱㸳㸧 Shimin Chen, C. -H. Chuang and K. Ameyama; “PORTABLE IMPEDANCE-BASED IMMUNOASSAY DEVICE FOR DETECTION OF BLADDER CANCER”, 5th International Symposium on Functionalization and Applications of Soft/Hard materials, Jan. 21-24, 2016, Kusatsu, Japan.

㸦㸱㸴㸧 Satoshi Matsuda, Mie Ota, Kei Ameyama, Pierre O Renault, Pierre Godard, Damien Faurie, Tarik Sadat, David Tingaud and Guy Dirras; “In situ X-ray diffraction study of mechanical behavior of harmonic structure design Ti-6Al-4V alloy”, 5th International Symposium on Functionalization and Applications of Soft/Hard materials, Jan. 21-24, 2016, Kusatsu, Japan.

㸦㸱㸵㸧 H. Maezawa, R. Maeda, M. Ota, S. K. Vajpai and K. Ameyama; “Unique Deformation Behavior on Strain Rate Sensitivity of Harmonic Structure Designed Ti-6Al-4V Alloy”, 5th International Symposium on Functionalization and Applications of Soft/Hard materials, Jan. 21-24, 2016, Kusatsu, Japan.

㸦㸱㸶㸧 Tomoyuki Kageyama, Nur Zalikha Binti Khalil, Takayuki Sahara, Mie Ota, Kei Ameyama, Chaoli Ma; “The creation of harmonic structured composite with pure aluminum and Silicon”, 5th International Symposium on Functionalization and Applications of Soft/Hard materials, Jan. 21-24, 2016, Kusatsu, Japan.

㸦㸱㸷㸧 Daiki Ueda, A. Hocini, Mie Ota, Sanjay K. Vajpai, D Tingaud, K. Ameyama and G. Dirras; “Microstructure evolution and Mechanical behavior under shear loadings of Ti-25Nb-25Zr alloy processed by Mechanical Milling”, 5th International Symposium on Functionalization and Applications of Soft/Hard materials, Jan. 21-24, 2016, Kusatsu, Japan.

㸦㸲㸮㸧 Masashi Nakatani, Yuya Fujiki, Mie Ota, Sanjay. K. Vajpai and Kei. Ameyama; “Mechanical properties of harmonic structure designed SUS304L austenitic stainless steel”, 5th International Symposium on Functionalization and Applications of Soft/Hard materials, Jan. 21-24,

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2016, Kusatsu, Japan.

㸦㸲㸯㸧 Zhang Yitan, Zheng Ruixiao, Bhupendra Sharma, Cao-li and Kei Ameyama; “Microstructure and Mechanical properties of Al-5083/ B4C composites synthesized through spark plasma sintering and rolling”, 5th International Symposium on Functionalization and Applications of Soft/Hard materials, Jan. 21-24, 2016, Kusatsu, Japan.

㸦㸲㸰㸧 Shota Yokoyama, Ryo Maeda, Azziz Hocini, Ota Mie, Sanjay K.Vajpai, avid Tingaud, K Ameyama and Guy Dirras; “Influence of thermo-mechanical treatments on the mechanical behavior under shear loadings of Ti-15V-3Cr-3Sn-3Al alloy processed by High Pressure Gas Jet Milling”, 5th International Symposium on Functionalization and Applications of Soft/Hard materials, Jan. 21-24, 2016, Kusatsu, Japan.

㸦㸲㸱㸧 K. Ueno and T. Ando, Effect of Temperature and Scale on Plastic Deformation of Single Crystal Si, 28th International Microprocesses and Nanotechnology Conference㸪 㸦2015/11㸪ᐩᒣ㸧 

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㸺ᅜෆᏛ఍㸼

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ࣜࢳ࣒࢘࢖࢜ࣥ㟁ụࡢṇᴟά≀㉁ࡢຎ໬ᣲືほᐹࠖ㸪ᨺᑕගᏛ఍➨  ᅇⱝᡭ◊✲఍㸪ᒸᓮ㸪  ᖺ  ᭶ 㸦㸰㸲㸧 ᒣୗ⩧ᖹᒣᮏᝆ⟇∦ᒣ┿⚈✄⏣ᗣᏹ㸪ࠕࢩࣜ࢝ᢸᣢࢽࢵࢣࣝゐ፹ࡢືែ࡟ ᑐࡍࡿ⢏Ꮚࢧ࢖ࢬຠᯝࠖ㸪➨  ᅇゐ፹ウㄽ఍㸪ὠ㸪 ᖺ  ᭶ 㸦㸰㸳㸧 㟷ᾏᬛ኱∦ᒣ┿⚈✄⏣ᗣᏹ㸪ࠕࢩࣜ࢝ᢸᣢ 0Q ゐ፹ࡢ↝ᡂ㐣⛬࡬ࡢ๓㥑యࡢຠ ᯝࠖ㸪➨  ᅇ &6- ໬Ꮫࣇ࢙ࢫࢱ 㸪ᮾி㸪 ᖺ  ᭶ 㸦㸰㸴㸧 Ώ㑔⛱ᶞ∦ᒣ┿⚈✄⏣ᗣᏹ㸪ࠕ&(< ἲ࡜㏱㐣ἲࡢྠ᫬ ᐃ࡟ࡼࡿ LQVLWX;$)6 ࢭࣝࡢ㛤Ⓨࠖ㸪➨  ᅇ &6- ໬Ꮫࣇ࢙ࢫࢱ 㸪ᮾி㸪 ᖺ  ᭶ 㸦㸰㸵㸧 ⳥ᓮᑗኴ୚൤༓ᑜ┾⏣ᬛ⾨ᑠᓥ୍⏨∦ᒣ┿⚈✄⏣ᗣᏹኴ⏣ಇ᫂㸪 ࠕࣜࢳ࣒࢘࢖࢜ࣥ㟁ụ࡟ᑐࡍࡿ◲㯤⣔㟁ゎᾮῧຍ๣ࡢຠᯝࠖ㸪➨  ᅇ &6- ໬Ꮫࣇ࢙ࢫࢱ 㸪 ᮾி㸪 ᖺ  ᭶ 㸦㸰㸶㸧 బ஭ᏹᙲᒣୗ⩧ᖹ∦ᒣ┿⚈✄⏣ᗣᏹ㸪ࠕ⾲㠃ࢆࢩࣜ࢝ಟ㣭ࡋࡓ࢔࣑ࣝࢼ࡟ ᢸᣢࡋࡓࢽࢵࢣࣝゐ፹ࡢ ;$)6 ゎᯒࠖ㸪➨  ᅇ ; ⥺ศᯒウㄽ఍㸪ጲ㊰㸪 ᖺ  ᭶ 㸦㸰㸷㸧 ∦᱒೺㈗▼஭㥴ᖹᒣᮏᝆ⟇∦ᒣ┿⚈✄⏣ᗣᏹ㸪ࠕࢩࣜ࢝ᢸᣢ &R ⢏Ꮚࡢ㓟 ໬㑏ඖ≉ᛶ࡟ཬࡰࡍ⢏Ꮚࢧ࢖ࢬຠᯝࠖ㸪➨  ᅇ ; ⥺ศᯒウㄽ఍㸪ጲ㊰㸪 ᖺ  ᭶ 㸦㸱㸮㸧 ୰஭┿⌮ዉ୰ᮧ⪃ᚿᒣཱྀ᭷᭸Ώ㑔⛱ᶞ∦ᒣ┿⚈✄⏣ᗣᏹ㸪ࠕ❅໬㖡ࢼ ࣀ⢏Ꮚࡢ᪼ 㑏ඖ㐣⛬ࡢ LQVLWX;$)6 ゎᯒࠖ㸪➨  ᅇ ; ⥺ศᯒウㄽ఍㸪ጲ㊰㸪 ᖺ  ᭶ 㸦㸱㸯㸧 ᒣ㔜ᑑኵ኱ᮾ⌶἞∦ᒣ┿⚈✄⏣ᗣᏹ㸪ࠕ㉮ᰝᆺ㏱㐣㌾ ; ⥺㢧ᚤ㙾ࢆ⏝࠸ࡓ ྜ๣㟁ᴟෆ࡟࠾ࡅࡿṇᴟά≀㉁ࡢຎ໬ᣲືほᐹࠖ㸪➨  ᅇ㟁ụウㄽ఍㸪ྡྂᒇ㸪 ᖺ  ᭶ 㸦㸱㸰㸧 ᒣᓊᘯዉᐑཎⰋኴ∦ᒣ┿⚈✄⏣ᗣᏹ㸪ࠕࣜࢳ࣒࢘࢖࢜ࣥ஧ḟ㟁ụ࣐ࣥ࢞ࣥ 㓟ࣜࢳ࣒࢘ṇᴟ㠃ෆ࡟࠾ࡅࡿ୙ᆒ୍㟁ᴟ཯ᛂࡢືⓗゎᯒࠖ㸪➨  ᅇ᪥ᮏᨺᑕගᏛ఍ᖺ఍࣭ᨺ ᑕග⛉Ꮫྜྠࢩ࣏ࣥࢪ࣒࢘㸪᯽㸪 ᖺ  ᭶ 㸦㸱㸱㸧 ሯ㉺ᾏΏ∦ᒣ┿⚈✄⏣ᗣᏹ㸪ࠕࣜࢳ࣒࢘࢖࢜ࣥ஧ḟ㟁ụ /L0Q[1L[2 ṇᴟࡢ ඘ᨺ㟁㐣⛬࡟࠾ࡅࡿ LQVLWX;$)6 ゎᯒࠖ㸪➨  ᅇ᪥ᮏᨺᑕගᏛ఍ᖺ఍࣭ᨺᑕග⛉Ꮫྜྠࢩ ࣏ࣥࢪ࣒࢘㸪᯽㸪 ᖺ  ᭶ 㸦㸱㸲㸧 Ლᒣ㞝㈗∦ᒣ┿⚈✄⏣ᗣᏹ㸪ࠕࢰࣝࢤࣝἲࢆ⏝࠸ࡓ࢞ࣛࢫ≧ࢩࣜ࢝ᢸᣢࣂࢼ ࢪ࣒࢘ගゐ፹ࡢ↝ᡂ㐣⛬࡟㛵ࡍࡿ ;$)6 ࡟ࡼࡿ≧ែゎᯒࠖ㸪➨  ᅇ᪥ᮏᨺᑕගᏛ఍ᖺ఍࣭ᨺ ᑕග⛉Ꮫྜྠࢩ࣏ࣥࢪ࣒࢘㸪᯽㸪 ᖺ  ᭶

㸦㸱㸳㸧 ᶓᒣ ᑗኴࠊ๓⏣ ுࠊΏ㑔 ᬛஅࠊSanjay Kumar Vajpaiࠊኴ⏣ ⨾⤮ࠊ䭯ᒣ ᝴㸹ࠗ㧗ᅽ࢞ࢫࢪ࢙ࢵࢺ࣑ࣜࣥࢢἲ࡟ࡼࡾㄪ࿴⤌⧊ไᚚࡉࢀࡓTi-6Al-4V ྜ㔠ࡢኚᙧᣲື࠘ࠊ ⢊య⢊ᮎ෬㔠༠఍ᖹᡂ27 ᖺᗘ᫓Ꮨ኱఍ࠊ2015 ᖺ 5 ᭶ 26-28 ᪥ࠊ᪩✄⏣኱Ꮫᅜ㝿఍㆟ሙࠊ ᮾி 㸦㸱㸴㸧 ୖ⏣ ኱グࠊ⃝஭ ㈗୍ࠊኴ⏣ ⨾⤮ࠊ䭯ᒣ ᝴㸹ࠗㄪ࿴⤌⧊ไᚚࡉࢀࡓ⣧㕲ࡢ ⤌⧊ᙧᡂ࡜≉␗࡞ኚᙧᣲື࠘ࠊ⢊య⢊ᮎ෬㔠༠఍ᖹᡂ27 ᖺᗘ᫓Ꮨ኱఍ࠊ2015 ᖺ 5 ᭶ 26-28 ᪥ࠊ᪩✄⏣኱Ꮫᅜ㝿఍㆟ሙࠊᮾி

㸦㸱㸵㸧 ๓ἑ ⱥ඾ࠊᕝ⏿ ගࠊ㯮ᕝ ࿴᫭ࠊSanjay Kumar Vajpaiࠊኴ⏣ ⨾⤮ࠊ䭯ᒣ ᝴㸹ࠗᕤᴗ⏝⣧ࢳࢱࣥ⢊ᮎࢆ⏝࠸ࡓ㧗ᅽ࢞ࢫࢪ࢙ࢵࢺ࣑ࣜࣥࢢἲ࡟ࡼࡿㄪ࿴⤌⧊ไᚚ࠘ࠊ⢊య ⢊ᮎ෬㔠༠఍ᖹᡂ27 ᖺᗘ᫓Ꮨ኱఍ࠊ2015 ᖺ 5 ᭶ 26-28 ᪥ࠊ᪩✄⏣኱Ꮫᅜ㝿఍㆟ሙࠊᮾி 㸦㸱㸶㸧 ቑ⏣ ୍ᶞࠊᒸ⏣ 㥴ࠊୗᇛ ၨ♸ࠊSanjay Kumar Vajpaiࠊኴ⏣ ⨾⤮ࠊ䭯ᒣ

᝴㸹ࠗ↓㟁ゎࢽࢵࢣࣝࡵࡗࡁἲ࡟ࡼࡿ⣧ࢽࢵࢣࣝࡢㄪ࿴⤌⧊ᙧᡂ࡜ᶵᲔⓗ≉ᛶ࠘ࠊ⢊య⢊ᮎ෬ 㔠༠఍ᖹᡂ27 ᖺᗘ᫓Ꮨ኱఍ࠊ2015 ᖺ 5 ᭶ 26-28 ᪥ࠊ᪩✄⏣኱Ꮫᅜ㝿఍㆟ሙࠊᮾி 㸦㸱㸷㸧 䭯ᒣ ᝴ࠊኴ⏣ ⨾⤮ࠊGuy DirrasࠊDavid Tingaud㸹ࠗ⣧ࢳࢱࣥㄪ࿴⤌⧊ᮦᩱ

ࡢ㧗㏿ኚᙧ࡟ࡼࡿ⤌⧊ኚ໬࠘ࠊ᪥ᮏ㕲㗰༠఍➨170 ᅇ⛅Ꮨㅮ₇኱఍ࠊ2015 ᖺ 9 ᭶ 16-18 ᪥ࠊ ஑ᕞ኱Ꮫఀ㒔࢟ࣕࣥࣃࢫࠊ⚟ᒸ

㸦㸲㸮㸧 Sanjay Kumar Vajpai, Choncharoen Sawangrat and Kei Ameyama; “Effect of bimodal harmonic structure design on the deformation behavior and mechanical properties of Co-Cr-Mo alloys” ࠊ᪥ᮏ㕲㗰༠఍➨ 170 ᅇ⛅Ꮨㅮ₇኱఍ࠊ2015 ᖺ 9 ᭶ 16-18 ᪥ࠊ஑ᕞ኱Ꮫఀ㒔࢟ࣕࣥࣃࢫࠊ⚟ᒸ

㸦㸲㸯㸧 Han YuࠊΏ㑔 ⫱ክࠊ䭯ᒣ ᝴㸹࣐ࠗࣝࢳࢫࢣ࣮ࣝ FEM ࡟ࡼࡿㄪ࿴⤌⧊ᮦᩱࡢ ≉␗࡞ኚᙧᣲື࠘ࠊ᪥ᮏ㕲㗰༠఍➨170 ᅇ⛅Ꮨㅮ₇኱఍ࠊ2015 ᖺ 9 ᭶ 16-18 ᪥ࠊ஑ᕞ኱Ꮫ ఀ㒔࢟ࣕࣥࣃࢫࠊ⚟ᒸ

㸦㸲㸰㸧 ᑠⳢ ಟྖࠊ䭯ᒣ᝴㸹ࠗ⣧ Ni ㄪ࿴⤌⧊ᮦᩱࡢ⤌⧊࡜ຊᏛ≉ᛶ࠘ࠊ᪥ᮏ㕲㗰༠఍➨ 42 ᅇᏛ⏕࣏ࢫࢱ࣮ࢭࢵࢩࣙࣥⓎ⾲ࠊ9 ᭶ 17 ᪥ࠊ஑ᕞ኱Ꮫఀ㒔࢟ࣕࣥࣃࢫ I2_{CNERࠊ⚟ᒸ}

㸦㸲㸱㸧 ᒸ⏣ 㥴ࠊቑ⏣ ୍ᶞࠊኴ⏣ ⨾⤮ࠊSanjay Kumar Vajpaiࠊ䭯ᒣ ᝴ࠊCinzia Menapace㸹ࠗ⣧Ni ㄪ࿴⤌⧊ᮦᩱࡢ㧗 ኚᙧᣲື࠘ࠊ⢊య⢊ᮎ෬㔠༠఍ᖹᡂ 27 ᖺᗘ⛅Ꮨ኱఍ࠊ 2015 ᖺ 11 ᭶ 11-13 ᪥ࠊி㒔኱Ꮫⓒ࿘ᖺ᫬ィྎグᛕ㤋ࠊி㒔

㸦㸲㸲㸧 బཎ ㈗⾜ࠊᒸ⏣ 㥴ࠊ㛗㔝 ᬛோࠊኴ⏣ ⨾⤮ࠊ䭯ᒣ ᝴㸹ࠗAZ91D ࣐ࢢࢿࢩ ࣒࢘ྜ㔠ㄪ࿴⤌⧊ไᚚᮦᩱࡢ⤌⧊࡜ᶵᲔⓗ≉ᛶ࠘ࠊ⢊య⢊ᮎ෬㔠༠఍ᖹᡂ27 ᖺᗘ⛅Ꮨ኱఍ࠊ 2015 ᖺ 11 ᭶ 11-13 ᪥ࠊி㒔኱Ꮫⓒ࿘ᖺ᫬ィྎグᛕ㤋ࠊி㒔

㸦㸲㸳㸧 㡲⸨ ኱࿴ࠊᒣ⏣ ᓫ኱ࠊኴ⏣ ⨾⤮ࠊSanjay Kumar Vajpaiࠊ䭯ᒣ ᝴㸹ࠗㄪ࿴ ⤌⧊ࢆ᭷ࡍࡿ⣧㖡ࡢ㧗 ኚᙧᣲື࠘ࠊ⢊య⢊ᮎ෬㔠༠఍ᖹᡂ 27 ᖺᗘ⛅Ꮨ኱఍ࠊ2015 ᖺ 11 ᭶11-13 ᪥ࠊி㒔኱Ꮫⓒ࿘ᖺ᫬ィྎグᛕ㤋ࠊி㒔 㸦㸲㸴㸧 ๓⏣ ுࠊΏ㑔 ᬛஅࠊΏᏲ ㈗኱ࠊኴ⏣ ⨾⤮ࠊ䭯ᒣ ᝴㸹ࠗTi-6Al-4V ྜ㔠ࡢ 㧗ᅽ࢞ࢫࢪ࢙ࢵࢺ࣑ࣜࣥࢢἲ࡟ࡼࡿㄪ࿴⤌⧊ไᚚ࠘ࠊ⢊య⢊ᮎ෬㔠༠఍ᖹᡂ 27 ᖺᗘ⛅Ꮨ኱ ఍ࠊ2015 ᖺ 11 ᭶ 11-13 ᪥ࠊி㒔኱Ꮫⓒ࿘ᖺ᫬ィྎグᛕ㤋ࠊி㒔 㸦㸲㸵㸧 ୰㇂ ோࠊ⸨ᮌ ‪ஓࠊኴ⏣ ⨾⤮ࠊ䭯ᒣ ᝴㸹ࠗSUS304L ㄪ࿴⤌⧊ᮦᩱࡢኚᙧ ࡟ཬࡰࡍ⤌⧊ࡢᙳ㡪࠘ࠊ⢊య⢊ᮎ෬㔠༠఍ᖹᡂ27 ᖺᗘ⛅Ꮨ኱఍ࠊ2015 ᖺ 11 ᭶ 11-13 ᪥ࠊ ி㒔኱Ꮫⓒ࿘ᖺ᫬ィྎグᛕ㤋ࠊி㒔 㸦㸲㸶㸧 ⃝஭ ㈗୍ࠊኴ⏣ ⨾⤮ࠊ䭯ᒣ ᝴㸹ࠗ⣧㕲ࡢㄪ࿴⤌⧊ไᚚᮦᩱࡢኚᙧᣲື࠘ࠊ⢊ య⢊ᮎ෬㔠༠఍ᖹᡂ27 ᖺᗘ⛅Ꮨ኱఍ࠊ2015 ᖺ 11 ᭶ 11-13 ᪥ࠊி㒔኱Ꮫⓒ࿘ᖺ᫬ィྎグᛕ 㤋ࠊி㒔 㸦㸲㸷㸧 䭯ᒣ ᝴ࠊబཎ㈗⾜ࠊኴ⏣ ⨾⤮㸹ࠗ⣧Al ࣂࣝࢡᮦࡢຍᕤ⇕ฎ⌮࡟ࡼࡿㄪ࿴⤌⧊ −63−