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 en-aut-sei=Baba en-aut-mei=T 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 en-aut-sei=Muro en-aut-mei=T kn-aut-name= kn-aut-sei= kn-aut-mei= aut-affil-num=3 ORCID= en-aut-name=KajiY en-aut-sei=Kaji 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 kn-aut-name= 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