start-ver=1.4
cd-journal=joma
no-vol=81
cd-vols=
no-issue=18
article-no=
start-page=180509-1
end-page=180509-4
dt-received=
dt-revised=
dt-accepted=
dt-pub-year=2010
dt-pub=20100517
dt-online=
en-article=
kn-article=
en-subject=
kn-subject=
en-title=
kn-title=Angle-resolved photoemission observation of the superconducting-gap minimum and its relation to the nesting vector in the phonon-mediated superconductor YNi2B2C
en-subtitle=
kn-subtitle=
en-abstract=
kn-abstract=We have performed ultrahigh-resolution angle-resolved photoemission spectroscopy to directly study the large superconducting (SC) gap anisotropy of YNi2B2C. We succeed in measuring momentum (k) dependence of SC gap for individual Fermi surface (FS) sheets, which demonstrates complexity of SC gap in a phonon-mediated superconductor. Within measured k regions on FS sheets, we find a pointlike minimum of SC gap, whose k positions can be connected by the known nesting vector. This shows close correlation between the nesting vector and node formation.
en-copyright=
kn-copyright=
en-aut-name=BabaT
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kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=1
ORCID=
en-aut-name=YokoyaT
en-aut-sei=Yokoya
en-aut-mei=T
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=2
ORCID=
en-aut-name=TsudaS
en-aut-sei=Tsuda
en-aut-mei=S
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=3
ORCID=
en-aut-name=WatanabeT
en-aut-sei=Watanabe
en-aut-mei=T
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=4
ORCID=
en-aut-name=NoharaM
en-aut-sei=Nohara
en-aut-mei=M
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=5
ORCID=
en-aut-name=TakagiH
en-aut-sei=Takagi
en-aut-mei=H
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=6
ORCID=
en-aut-name=OguchiT
en-aut-sei=Oguchi
en-aut-mei=T
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=7
ORCID=
en-aut-name=ShinS
en-aut-sei=Shin
en-aut-mei=S
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=8
ORCID=
affil-num=1
en-affil=
kn-affil=Institute for Solid State Physics, University of Tokyo
affil-num=2
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=3
en-affil=
kn-affil=Institute for Solid State Physics, University of Tokyo
affil-num=4
en-affil=
kn-affil=Institute for Solid State Physics, University of Tokyo
affil-num=5
en-affil=
kn-affil=Department of Advanced Materials Science, University of Tokyo
affil-num=6
en-affil=
kn-affil=Department of Advanced Materials Science, University of Tokyo
affil-num=7
en-affil=
kn-affil=Department of Quantum Matter, Graduate school of Advanced Sciences of Matter (ADSM), Hiroshima University
affil-num=8
en-affil=
kn-affil=Institute for Solid State Physics, University of Tokyo
END
start-ver=1.4
cd-journal=joma
no-vol=82
cd-vols=
no-issue=19
article-no=
start-page=195114-1
end-page=195114-5
dt-received=
dt-revised=
dt-accepted=
dt-pub-year=2010
dt-pub=20101110
dt-online=
en-article=
kn-article=
en-subject=
kn-subject=
en-title=
kn-title=Electronic structure of pristine and K-doped solid picene: Nonrigid band change and its implication for electron-intramolecular-vibration interaction
en-subtitle=
kn-subtitle=
en-abstract=
kn-abstract=We use photoemission spectroscopy to study electronic structures of pristine and K-doped solid picene. The valence band spectrum of pristine picene consists of three main features with no state at the Fermi level (EF) while that of K-doped picene has three structures similar to those of pristine picene with new states near EF, consistent with the semiconductor-metal transition. The K-induced change cannot be explained with a simple rigid-band model of pristine picene but can be interpreted by molecular-orbital calculations considering electron-intramolecular-vibration interaction. Excellent agreement of the K-doped spectrum with the calculations points to importance of electron-intramolecular-vibration interaction in K-doped picene.
en-copyright=
kn-copyright=
en-aut-name=OkazakiH
en-aut-sei=Okazaki
en-aut-mei=H
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=1
ORCID=
en-aut-name=WakitaT
en-aut-sei=Wakita
en-aut-mei=T
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=2
ORCID=
en-aut-name=MuroT
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kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=3
ORCID=
en-aut-name=KajiY
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en-aut-mei=Y
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=4
ORCID=
en-aut-name=LeeX
en-aut-sei=Lee
en-aut-mei=X
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=5
ORCID=
en-aut-name=MitamuraH
en-aut-sei=Mitamura
en-aut-mei=H
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=6
ORCID=
en-aut-name=KawasakiN
en-aut-sei=Kawasaki
en-aut-mei=N
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=7
ORCID=
en-aut-name=KubozonoY
en-aut-sei=Kubozono
en-aut-mei=Y
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kn-aut-sei=
kn-aut-mei=
aut-affil-num=8
ORCID=
en-aut-name=YamanariY
en-aut-sei=Yamanari
en-aut-mei=Y
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=9
ORCID=
en-aut-name=KambeT
en-aut-sei=Kambe
en-aut-mei=T
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=10
ORCID=
en-aut-name=KatoT
en-aut-sei=Kato
en-aut-mei=T
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=11
ORCID=
en-aut-name=HiraiM
en-aut-sei=Hirai
en-aut-mei=M
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=12
ORCID=
en-aut-name=MuraokaY
en-aut-sei=Muraoka
en-aut-mei=Y
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=13
ORCID=
en-aut-name=YokoyaT
en-aut-sei=Yokoya
en-aut-mei=T
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=14
ORCID=
affil-num=1
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=2
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=3
en-affil=
kn-affil=Japan Synchrotron Radiation Research Institute (JASRI)/SPring-8
affil-num=4
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=5
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=6
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=7
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=8
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=9
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=10
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=11
en-affil=
kn-affil=Institute for Innovative Science and Technology, Graduate School of Engineering, Nagasaki Institute of Applied Science
affil-num=12
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=13
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=14
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
END
start-ver=1.4
cd-journal=joma
no-vol=82
cd-vols=
no-issue=20
article-no=
start-page=205108-1
end-page=205108-6
dt-received=
dt-revised=
dt-accepted=
dt-pub-year=2010
dt-pub=20101108
dt-online=
en-article=
kn-article=
en-subject=
kn-subject=
en-title=
kn-title=Signature of hidden order and evidence for periodicity modification in URu2Si2
en-subtitle=
kn-subtitle=
en-abstract=
kn-abstract=The detail of electronic structures near the Fermi level in URu2Si2 has been investigated employing state-of-art laser angle-resolved photoemission spectroscopy. The observation of a narrow dispersive band near the Fermi level in the ordered state as well as its absence in a Rh-substituted sample strongly suggest that the emergence of the narrow band is a clear signature of the hidden-order transition. The temperature dependence of the narrow band, which appears at the onset of the hidden-order transition, invokes the occurrence of periodicity modification in the ordered state, which is shown for the first time by any spectroscopic probe. We compare our data to other previous studies and discuss possible implications.
en-copyright=
kn-copyright=
en-aut-name=YoshidaRikiya
en-aut-sei=Yoshida
en-aut-mei=Rikiya
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=1
ORCID=
en-aut-name=NakamuraYoshiaki
en-aut-sei=Nakamura
en-aut-mei=Yoshiaki
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=2
ORCID=
en-aut-name=FukuiMasaki
en-aut-sei=Fukui
en-aut-mei=Masaki
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=3
ORCID=
en-aut-name=HagaYoshinori
en-aut-sei=Haga
en-aut-mei=Yoshinori
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=4
ORCID=
en-aut-name=YamamotoEtsuji
en-aut-sei=Yamamoto
en-aut-mei=Etsuji
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=5
ORCID=
en-aut-name=OnukiYoshichika
en-aut-sei=Onuki
en-aut-mei=Yoshichika
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=6
ORCID=
en-aut-name=OkawaMario
en-aut-sei=Okawa
en-aut-mei=Mario
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=7
ORCID=
en-aut-name=ShinShik
en-aut-sei=Shin
en-aut-mei=Shik
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=8
ORCID=
en-aut-name=HiraiMasaaki
en-aut-sei=Hirai
en-aut-mei=Masaaki
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=9
ORCID=
en-aut-name=MuraokaYuji
en-aut-sei=Muraoka
en-aut-mei=Yuji
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=10
ORCID=
en-aut-name=YokoyaTakayoshi
en-aut-sei=Yokoya
en-aut-mei=Takayoshi
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=11
ORCID=
affil-num=1
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=2
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=3
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=4
en-affil=
kn-affil=Advanced Science Research Center, Japan Atomic Energy Agency
affil-num=5
en-affil=
kn-affil=Advanced Science Research Center, Japan Atomic Energy Agency
affil-num=6
en-affil=
kn-affil=Advanced Science Research Center, Japan Atomic Energy Agency
affil-num=7
en-affil=
kn-affil=Institute for Solid State Physics, The University of Tokyo
affil-num=8
en-affil=
kn-affil=Institute for Solid State Physics, The University of Tokyo
affil-num=9
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=10
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=11
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
END
start-ver=1.4
cd-journal=joma
no-vol=86
cd-vols=
no-issue=1
article-no=
start-page=014521-1
end-page=014521-5
dt-received=
dt-revised=
dt-accepted=
dt-pub-year=2012
dt-pub=20120726
dt-online=
en-article=
kn-article=
en-subject=
kn-subject=
en-title=
kn-title=Comparative photoemission studies on the superconducting gap of the filled skutterudite superconductors LaPt4Ge12 and PrPt4Ge12
en-subtitle=
kn-subtitle=
en-abstract=
kn-abstract=We performed a comparative study of the superconducting gap in the new filled skutterudite superconductors LaPt4Ge12 and PrPt4Ge12 using high-resolution photoemission spectroscopy. We succeeded in observing spectral changes across Tc that reflect the opening of the superconducting gap in both compounds and also in observing a noticeable difference in their respective superconducting spectral shapes near the Fermi level, pointing toward a more complex superconducting gap structure in PrPt4Ge12. In addition, we found that the two-gap model is more suitable for describing the superconducting-state spectrum of PrPt4Ge12 than the single-isotropic-gap and single-anisotropic-gap models, which suggests an explanation that multiband effects may possibly induce the anomalous superconducting properties of PrPt4Ge12.
en-copyright=
kn-copyright=
en-aut-name=NakamuraYoshiaki
en-aut-sei=Nakamura
en-aut-mei=Yoshiaki
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=1
ORCID=
en-aut-name=OkazakiHiroyuki
en-aut-sei=Okazaki
en-aut-mei=Hiroyuki
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=2
ORCID=
en-aut-name=YoshidaRikiya
en-aut-sei=Yoshida
en-aut-mei=Rikiya
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=3
ORCID=
en-aut-name=WakitaTakanori
en-aut-sei=Wakita
en-aut-mei=Takanori
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=4
ORCID=
en-aut-name=TakeyaHiroyuki
en-aut-sei=Takeya
en-aut-mei=Hiroyuki
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=5
ORCID=
en-aut-name=HirataKazuto
en-aut-sei=Hirata
en-aut-mei=Kazuto
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=6
ORCID=
en-aut-name=HiraiMasaaki
en-aut-sei=Hirai
en-aut-mei=Masaaki
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=7
ORCID=
en-aut-name=MuraokaYuji
en-aut-sei=Muraoka
en-aut-mei=Yuji
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=8
ORCID=
en-aut-name=YokoyaTakayoshi
en-aut-sei=Yokoya
en-aut-mei=Takayoshi
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=9
ORCID=
affil-num=1
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=2
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=3
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=4
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=5
en-affil=
kn-affil=National Institute for Materials Science (NIMS)
affil-num=6
en-affil=
kn-affil=National Institute for Materials Science (NIMS)
affil-num=7
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=8
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
affil-num=9
en-affil=
kn-affil=The Graduate School of Natural Science and Technology, Okayama University
END
start-ver=1.4
cd-journal=joma
no-vol=88
cd-vols=
no-issue=9
article-no=
start-page=
end-page=
dt-received=
dt-revised=
dt-accepted=
dt-pub-year=2012
dt-pub=20120930
dt-online=
en-article=
kn-article=
en-subject=
kn-subject=
en-title=
kn-title=Superconductivity in (NH3)(y)Cs0.4FeSe
en-subtitle=
kn-subtitle=
en-abstract=
kn-abstract=Alkali-metal-intercalated FeSe materials, (NH3)(y)M0.4FeSe (M: K, Rb, and Cs), have been synthesized using the liquid NH3 technique. (NH3)(y)Cs0.4FeSe shows a superconducting transition temperature (T-c) as high as 31.2 K, which is higher by 3.8 K than the T-c of nonammoniated Cs0.4FeSe. The T(c)s of (NH3)(y)K0.4FeSe and (NH3)(y)Rb0.4FeSe are almost the same as those of nonammoniated K0.4FeSe and Rb0.4FeSe. The T-c of (NH3)(y)Cs0.4FeSe shows a negative pressure dependence. A clear correlation between T-c and lattice constant c is found for ammoniated metal-intercalated FeSe materials, suggesting a correlation between Fermi-surface nesting and superconductivity.
en-copyright=
kn-copyright=
en-aut-name=ZhengLu
en-aut-sei=Zheng
en-aut-mei=Lu
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=1
ORCID=
en-aut-name=IzumiMasanari
en-aut-sei=Izumi
en-aut-mei=Masanari
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=2
ORCID=
en-aut-name=SakaiYusuke
en-aut-sei=Sakai
en-aut-mei=Yusuke
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=3
ORCID=
en-aut-name=EguchiRitsuko
en-aut-sei=Eguchi
en-aut-mei=Ritsuko
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=4
ORCID=
en-aut-name=GotoHidenori
en-aut-sei=Goto
en-aut-mei=Hidenori
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=5
ORCID=
en-aut-name=TakabayashiYasuhiro
en-aut-sei=Takabayashi
en-aut-mei=Yasuhiro
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=6
ORCID=
en-aut-name=KambeTakashi
en-aut-sei=Kambe
en-aut-mei=Takashi
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=7
ORCID=
en-aut-name=OnjiTaiki
en-aut-sei=Onji
en-aut-mei=Taiki
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=8
ORCID=
en-aut-name=ArakiShingo
en-aut-sei=Araki
en-aut-mei=Shingo
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=9
ORCID=
en-aut-name=KobayashiTatsuo C.
en-aut-sei=Kobayashi
en-aut-mei=Tatsuo C.
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=10
ORCID=
en-aut-name=KimJungeun
en-aut-sei=Kim
en-aut-mei=Jungeun
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=11
ORCID=
en-aut-name=FujiwaraAkihiko
en-aut-sei=Fujiwara
en-aut-mei=Akihiko
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=12
ORCID=
en-aut-name=KubozonoYoshihiro
en-aut-sei=Kubozono
en-aut-mei=Yoshihiro
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=13
ORCID=
affil-num=1
en-affil=
kn-affil=Okayama Univ, Res Lab Surface Sci
affil-num=2
en-affil=
kn-affil=Okayama Univ, Res Lab Surface Sci
affil-num=3
en-affil=
kn-affil=Okayama Univ, Res Lab Surface Sci
affil-num=4
en-affil=
kn-affil=Okayama Univ, Res Lab Surface Sci
affil-num=5
en-affil=
kn-affil=Okayama Univ, Res Lab Surface Sci
affil-num=6
en-affil=
kn-affil=Okayama Univ, Res Lab Surface Sci
affil-num=7
en-affil=
kn-affil=Okayama Univ, Dept Phys
affil-num=8
en-affil=
kn-affil=Okayama Univ, Dept Phys
affil-num=9
en-affil=
kn-affil=Okayama Univ, Dept Phys
affil-num=10
en-affil=
kn-affil=Okayama Univ, Dept Phys
affil-num=11
en-affil=
kn-affil=RIKEN, SPring Ctr 8, Japan Synchrotron Radiat Res Inst
affil-num=12
en-affil=
kn-affil=RIKEN, SPring Ctr 8, Japan Synchrotron Radiat Res Inst
affil-num=13
en-affil=
kn-affil=Okayama Univ, Res Lab Surface Sci
END
start-ver=1.4
cd-journal=joma
no-vol=90
cd-vols=
no-issue=22
article-no=
start-page=
end-page=
dt-received=
dt-revised=
dt-accepted=
dt-pub-year=2014
dt-pub=20141222
dt-online=
en-article=
kn-article=
en-subject=
kn-subject=
en-title=
kn-title=Proximity to Fermi-surface topological change in superconducting LaO0.54F0.46BiS2
en-subtitle=
kn-subtitle=
en-abstract=
kn-abstract=The electronic structure of nearly optimally doped novel superconductor LaO1−xFxBiS2(x = 0.46) was investigated using angle-resolved photoemission spectroscopy (ARPES). We clearly observed band dispersions from 2 to 6 eV binding energy and near the Fermi level (EF), which are well reproduced by first-principles calculations when the spin-orbit coupling is taken into account. The ARPES intensity map near EF shows a squarelike distribution around the (Z) point in addition to electronlike Fermi-surface (FS) sheets around the X(R) point, indicating that FS of LaO0.54F0.46BiS2 is in close proximity to the theoretically predicted topological change.
en-copyright=
kn-copyright=
en-aut-name=TerashimaKensei
en-aut-sei=Terashima
en-aut-mei=Kensei
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=1
ORCID=
en-aut-name=SonoyamaJunki
en-aut-sei=Sonoyama
en-aut-mei=Junki
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=2
ORCID=
en-aut-name=WakitaTakanori
en-aut-sei=Wakita
en-aut-mei=Takanori
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=3
ORCID=
en-aut-name=SunagawaMasanori
en-aut-sei=Sunagawa
en-aut-mei=Masanori
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=4
ORCID=
en-aut-name=OnoKanta
en-aut-sei=Ono
en-aut-mei=Kanta
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=5
ORCID=
en-aut-name=KumigashiraHiroshi
en-aut-sei=Kumigashira
en-aut-mei=Hiroshi
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=6
ORCID=
en-aut-name=MuroTakayuki
en-aut-sei=Muro
en-aut-mei=Takayuki
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=7
ORCID=
en-aut-name=NagaoMasanori
en-aut-sei=Nagao
en-aut-mei=Masanori
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=8
ORCID=
en-aut-name=WatauchiSatoshi
en-aut-sei=Watauchi
en-aut-mei=Satoshi
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=9
ORCID=
en-aut-name=TanakaIsao
en-aut-sei=Tanaka
en-aut-mei=Isao
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=10
ORCID=
en-aut-name=OkazakiHiroyuki
en-aut-sei=Okazaki
en-aut-mei=Hiroyuki
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=11
ORCID=
en-aut-name=TakanoYoshihiko
en-aut-sei=Takano
en-aut-mei=Yoshihiko
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=12
ORCID=
en-aut-name=MiuraOsuke
en-aut-sei=Miura
en-aut-mei=Osuke
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=13
ORCID=
en-aut-name=MizuguchiYoshikazu
en-aut-sei=Mizuguchi
en-aut-mei=Yoshikazu
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=14
ORCID=
en-aut-name=UsuiHidetomo
en-aut-sei=Usui
en-aut-mei=Hidetomo
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=15
ORCID=
en-aut-name=SuzukiKatsuhiro
en-aut-sei=Suzuki
en-aut-mei=Katsuhiro
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=16
ORCID=
en-aut-name=KurokiKazuhiko
en-aut-sei=Kuroki
en-aut-mei=Kazuhiko
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=17
ORCID=
en-aut-name=MuraokaYuji
en-aut-sei=Muraoka
en-aut-mei=Yuji
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=18
ORCID=
en-aut-name=YokoyaTakayoshi
en-aut-sei=Yokoya
en-aut-mei=Takayoshi
kn-aut-name=
kn-aut-sei=
kn-aut-mei=
aut-affil-num=19
ORCID=
affil-num=1
en-affil=
kn-affil=Graduate School of Natural Science and Technology and Research Laboratory for Surface Science, Okayama University
affil-num=2
en-affil=
kn-affil=Graduate School of Natural Science and Technology and Research Laboratory for Surface Science, Okayama University
affil-num=3
en-affil=
kn-affil=Graduate School of Natural Science and Technology and Research Laboratory for Surface Science, Okayama University
affil-num=4
en-affil=
kn-affil=Graduate School of Natural Science and Technology and Research Laboratory for Surface Science, Okayama University
affil-num=5
en-affil=
kn-affil=High Energy Accelerator Research Organization (KEK), Photon Factory
affil-num=6
en-affil=
kn-affil=High Energy Accelerator Research Organization (KEK), Photon Factory
affil-num=7
en-affil=
kn-affil=Japan Synchrtron Radiation Research Institute (JASRI)/SPring-8
affil-num=8
en-affil=
kn-affil=Center for Crystal Science and Technology, University of Yamanashi
affil-num=9
en-affil=
kn-affil=Center for Crystal Science and Technology, University of Yamanashi
affil-num=10
en-affil=
kn-affil=Center for Crystal Science and Technology, University of Yamanashi
affil-num=11
en-affil=
kn-affil=National Institute for Materials Science
affil-num=12
en-affil=
kn-affil=National Institute for Materials Science
affil-num=13
en-affil=
kn-affil=Department of Electrical and Electronic Engineering, Tokyo Metropolitan University
affil-num=14
en-affil=
kn-affil=Department of Electrical and Electronic Engineering, Tokyo Metropolitan University
affil-num=15
en-affil=
kn-affil=Department of Physics, Osaka University
affil-num=16
en-affil=
kn-affil=Department of Physics, Osaka University
affil-num=17
en-affil=
kn-affil=Department of Physics, Osaka University
affil-num=18
en-affil=
kn-affil=Graduate School of Natural Science and Technology and Research Laboratory for Surface Science, Okayama University
affil-num=19
en-affil=
kn-affil=1Graduate School of Natural Science and Technology and Research Laboratory for Surface Science
END