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Fusion reaction $$^{48}$$Ca+$$^{249}$$Bk leading to formation of the element Ts (Z=117)

Khuyagbaatar, J.*; Yakushev, A.*; D$"u$llmann, Ch. E.*; Ackermann, D.*; Andersson, L.-L.*; 浅井 雅人; Block, M.*; Boll, R. A.*; Brand, H.*; Cox, D. M.*; et al.

Physical Review C, 99(5), p.054306_1 - 054306_16, 2019/05



Origin of the dramatic change of fission mode in fermium isotopes investigated using Langevin equations

宮本 裕也*; 有友 嘉浩*; 田中 翔也; 廣瀬 健太郎; 西尾 勝久

Physical Review C, 99(5), p.051601_1 - 051601_7, 2019/05

The fission of even-even fermium nuclides $$^{250-260}$$Fm at low excitation energy was studied using Langevin equations of three-dimensional nuclear-shape parametrization. The mass distributions of fission fragments show a dramatic change from an asymmetric shape for the lighter fermium isotopes to sharp symmetric fission for the heavier isotopes. The time evolution of the nuclear shape on the potential surface reveals that the lighter fermium isotopes showing asymmetric fission are trapped in the second minimum for a substantial length of time before overcoming the second saddle point. This behavior changes dramatically for the compact symmetric fission found in the heavier neutron-rich fermium nuclei that disintegrate immediately after overcoming the first saddle point, without feeling the second barrier, resulting in a fission time two orders of magnitude shorter.


Topological characterization of classical waves; The Topological origin of magnetostatic surface spin waves

山本 慧; Thiang, G. C.*; Pirro, P.*; Kim, K.-W.*; Everschor-Sitte, K.*; 齊藤 英治*

Physical Review Letters, 122(21), p.217201_1 - 217201_5, 2019/05

We propose a topological characterization of Hamiltonians describing classical waves. Applying it to the magnetostatic surface spin waves that are important in spintronics applications, we settle the speculation over their topological origin. For a class of classical systems that includes spin waves driven by dipole-dipole interactions, we show that the topology is characterized by vortex lines in the Brillouin zone in such a way that the symplectic structure of Hamiltonian mechanics plays an essential role. We define winding numbers around these vortex lines and identify them to be the bulk topological invariants for a class of semimetals. Exploiting the bulk-edge correspondence appropriately reformulated for these classical waves, we predict that surface modes appear but not in a gap of the bulk frequency spectrum. This feature, consistent with the magnetostatic surface spin waves, indicates a broader realm of topological phases of matter beyond spectrally gapped ones.


Negative Te spin polarization responsible for ferromagnetic order in the doped topological insulator V$$_{0.04}$$(Sb$$_{1-x}$$Bi$$_{x}$$)$$_{1.96}$$Te$$_{3}$$

Ye, M.*; Xu, T.*; Li, G.*; Qiao, S.*; 竹田 幸治; 斎藤 祐児; Zhu, S.-Y.*; Nurmamat, M.*; 角田 一樹*; 石田 行章*; et al.

Physical Review B, 99(14), p.144413_1 - 144413_7, 2019/04

 パーセンタイル:100(Materials Science, Multidisciplinary)

We investigate the microscopic origin of ferromagnetism coupled with topological insulators in V-doped (Sb,Bi)$$_{2}$$Te$$_{3}$$ employing X-ray magnetic circular dichroism and angle-resolved two-photon photoemission spectroscopies, combined with first-principles calculations. We found an magnetic moment at the Te site anti-parallel to that of the V and Sb sites, which plays a key role in the ferromagnetic order. We ascribe it to the hybridization between Te 5${it p}$ and V 3${it d}$ majority spin states at the Fermi energy, consistent with the Zener-type ${it p}$-${it d}$ exchange interaction scenario. The substitution of Bi for Sb suppresses the bulk ferromagnetism by introducing extra electron carriers in the majority spin channel of the Te ${it p}$ states that compensates the antiparallel magnetic moment on the Te site. Our findings reveal important clues to designing magnetic topological insulators with higher Curie temperature that work under ambient conditions.


Probing the quantum phase transition in Mott insulator BaCoS$$_{2}$$ tuned by pressure and Ni substitution

Guguchia, Z.*; Frandsen, B. A.*; Santos-Cottin, D.*; 社本 真一; Gauzzi, A.*; 植村 泰朋*; 他12名*

Physical Review Materials (Internet), 3(4), p.045001_1 - 045001_9, 2019/04



Novel critical behavior of magnetization in URhSi; Similarities to the uranium ferromagnetic superconductors UGe$$_2$$ and URhGe

立岩 尚之; 芳賀 芳範; 山本 悦嗣

Physical Review B, 99(9), p.094417_1 - 094417_12, 2019/03

 パーセンタイル:100(Materials Science, Multidisciplinary)

ウラン系強磁性物質URhSiについて、強磁性転移温度$$T_{rm C}$$近辺で磁気測定を行い、臨界現象の研究を行った。自発磁化の温度依存に関する臨界指数$$beta$$、磁化率の指数$$gamma$$$$T_{rm C}$$における磁化に関する指数$$delta$$を、修正アロットプロットとスケーリング理論等を用いて決定した。URhSiの強磁性状態は一軸磁気異方性が大きいものの、臨界指数は三次元イジングモデルから期待されるもの($$beta$$ = 0.325, $$gamma$$ = 1.241, and $$delta$$ = 4.82)とは異なることが明らかにされた。URhSiの臨界指数($$beta$$ = 0.300 $$pm$$ 0.002, $$gamma$$ = 1.00 $$pm$$ 0.02, and $$delta$$ = 4.32 $$pm$$ 0.04)は、ウラン系強磁性超伝導物質UGe$$_2$$とURhGeと類似している。URhSiの静的磁性と動的磁性をウラン系強磁性超伝導物質と対比させ議論する。


Nucleon and $$Delta$$ isobar in a strong magnetic field

Yakhshiev, U.*; Kim, H.-C.; 岡 眞

Physical Review D, 99(5), p.054027_1 - 054027_11, 2019/03

 パーセンタイル:100(Astronomy & Astrophysics)



High-field phase diagram of the heavy-fermion metal CeIn$$_3$$; Pulsed-field NMR study on single crystals up to 56 T

徳永 陽; Orlova, A.*; Bruyant, N.*; 青木 大*; Mayaffre, H.*; Kr$"a$mer, S.*; Julien, M.-H.*; Berthier, C.*; Horvati$'c$, M.*; 比嘉 野乃花; et al.

Physical Review B, 99(8), p.085142_1 - 085142_5, 2019/02

 パーセンタイル:100(Materials Science, Multidisciplinary)



Manifestation of electron correlation effect in 5$$f$$ states of uranium compounds revealed by 4$$d$$-5$$f$$ resonant photoelectron spectroscopy

藤森 伸一; 小畠 雅明; 竹田 幸治; 岡根 哲夫; 斎藤 祐児; 藤森 淳; 山上 浩志; 芳賀 芳範; 山本 悦嗣; 大貫 惇睦*

Physical Review B, 99(3), p.035109_1 - 035109_5, 2019/01

 パーセンタイル:100(Materials Science, Multidisciplinary)

In the present study, we have elucidated the nature of the electron correlation effect in uranium compounds by imaging the partial $$mathrm{U}~5f$$ density of states (pDOS) of typical itinerant, localized, and heavy fermion uranium compounds by using the $$mathrm{U}$$ 4$$d$$-5$$f$$ resonant photoemission spectroscopy. Obtained $$mathrm{U}~5$$ pDOS exhibit a systematic trend depending on the physical properties of compounds: Although the coherent peak at the Fermi level can be explained by the band-structure calculation, an incoherent peak emerges on the higher binding energy side ($$lesssim 1~mathrm{eV}$$) in the cases of localized and heavy fermion compounds. The intensity and energy position of the incoherent peak is increased and shifted to a higher binding energy as the localization of the $$mathrm{U}~5$$ state increases. These behaviors are consistent with the prediction of the Mott metal-insulator transition, suggesting that the Hubbard-$$U$$ type mechanism takes an essential role in the $$5f$$ electronic structure of actinide materials.


Magnetic and electrical properties of the ternary compound U$$_2$$Ir$$_3$$Si$$_5$$ with one-dimensional uranium zigzag chains

Li, D. X.*; 本多 史憲*; 三宅 厚志*; 本間 佳哉*; 芳賀 芳範; 仲村 愛*; 清水 悠晴*; Maurya, A.*; 佐藤 芳樹*; 徳永 将史*; et al.

Physical Review B, 99, p.054408-1 - 054408-9, 2019/01

Physical properties of the single-crystalline U$$_2$$Ir$$_3$$Si$$_5$$, a new ternary uranium compound with U$$_2$$Co$$_3$$Si$$_5$$-type orthorhombic structure, are investigated by means of magnetic susceptibility, specific heat and electrical resistivity. This compound undergoes an antiferromagnetic transition followed by a first-order phase transition at lower temperature. A possible mechanism of the first-order transition is the occurrence of a magnetic magnetic quadrupolar order, resulting from the quasi-one-dimensional uranium zigzag chain.


$$^{239}$$Pu nuclear magnetic resonance in the candidate topological insulator PuB$$_4$$

Dioguardi, A. P.*; 安岡 弘志*; Thomas, S. M.*; 酒井 宏典; Cary, S. K.*; Kozimor, S. A.*; Albrecht-Schmitt, T. E.*; Choi, H. C.*; Zhu, J.-X.*; Thompson, J. D.*; et al.

Physical Review B, 99(3), p.035104_1 - 035104_6, 2019/01

 パーセンタイル:100(Materials Science, Multidisciplinary)



Spin correlations of quantum spin liquid and quadrupole-ordered states of Tb$$_{2+x}$$Ti$$_{2-x}$$O$$_{7+y}$$

門脇 広明*; 脇田 美香*; F${aa}$k, B.*; Ollivier, J.*; 河村 聖子; 中島 健次; Lynn, J. W.*

Physical Review B, 99(1), p.014406_1 - 014406_12, 2019/01

非弾性中性子散乱を用いてフラストレーションのあるパイロクロア酸化物Tb$$_{2+x}$$Ti$$_{2-x}$$O$$_{7+y}$$ (x = -0.007, 0.000, and 0.003)単結晶試料の磁気相関を測定した。この系は、量子スピン液体と四重極秩序状態を示すものである。実験結果とRPAを使った解析結果を議論する。量子スピン液体状態では対称性の破れが生じており、古典的なRPAの範囲を超えた議論が必要なことが示唆される。


Spectroscopy of strongly deformed $$^{32}$$Ne by proton knockout reactions

Murray, I.*; MacCormick, M.*; Bazin, D.*; Doornenbal, P.*; 青井 考*; 馬場 秀忠*; Crawford, H. L.*; Fallon, P.*; Li, K.*; Lee, J.*; et al.

Physical Review C, 99(1), p.011302_1 - 011302_7, 2019/01

 パーセンタイル:100(Physics, Nuclear)

理化学研究所のRI Beam Factory(RIBF)にて中性子過剰核$$^{32}$$Neの低励起状態を1陽子あるいは2陽子ノックアウト反応によって生成し、そこからの脱励起ガンマ線の測定によって、エネルギー準位を構築した。1410(15)keVのガンマ線を初めて測定し、反応断面積の系統性などから$$4^+_1$$から$$2^+_1$$への遷移に対応すると提案した。既に知られている$$2^+_1$$準位を用いて、$$4^+_1$$$$2^+_1$$の励起エネルギー比2.99(6)が得られた。この値は、回転スペクトルの値に近く、$$^{32}$$Neは強く変形していることがわかった。この実験結果は、大規模殻模型計算の結果とよく一致した。


$$g$$-factor measurement of the 2738 keV isomer in $$^{135}$$La

Laskar, Md. S. R.*; Saha, S.*; Palit, R.*; Mishra, S. N.*; 清水 則孝*; 宇都野 穣; 井手口 栄治*; Naik, Z.*; Babra, F. S.*; Biswas, S.*; et al.

Physical Review C, 99(1), p.014308_1 - 014308_6, 2019/01

 パーセンタイル:100(Physics, Nuclear)

タタ基礎物理学研究所の重イオン加速器にて、$$^{11}$$B($$^{128}$$Te, 4n)$$^{135}$$La反応によって$$^{135}$$Laの励起状態を生成し、2738keVにあるアイソマーの$$g$$因子を時間微分型摂動角分布(TDPAD)法によって測定した。得られた$$g$$因子の値は$$-0.049(3)$$であった。このアイソマーの核構造を理解するため、$$^{135}$$Laに対し、大規模殻模型計算を行った。殻模型計算は低励起状態のバンド構造を非常によく再現し、2738keVのアイソマーのスピンパリティは$$23/2^+$$であることを強く示唆する結果が得られた。このアイソマーは、$$^{134}$$Baの$$10^+_1$$$$d_{5/2}$$軌道にいる陽子が結合してできる配位が主であると解釈された。


Nuclear structure of $$^{76}$$Ni from the ($$p$$,$$2p$$) reaction

Elekes, Z.*; Kripk$'o$, $'A$*; Sohler, D.*; Sieja, K.*; 緒方 一介*; 吉田 数貴; Doornenbal, P.*; Obertelli, A.*; Authelet, G.*; 馬場 秀忠*; et al.

Physical Review C, 99(1), p.014312_1 - 014312_7, 2019/01

 パーセンタイル:100(Physics, Nuclear)

($$p$$,$$2p$$)反応による$$^{76}$$Niの核構造の探索実験を行った。Lenzi, Nowacki, Poves, Sieja相互作用を用いた殻模型計算では実験結果を説明しうる陽子空孔状態が得られており、理論的な断面積計算は実験値とよい一致を与えた。実験で得られたすべての状態を理論的に一意に決定することはできなかったが、過去の実験結果と同様にNi同位体でのZ = 28の大きなshell gapを示す結果が得られた。


Further signatures to support the tetraquark mixing framework for the two light-meson nonets

Kim, H.*; Kim, K. S.*; Cheoun, M.-K.*; 慈道 大介*; 岡 眞

Physical Review D, 99(1), p.014005_1 - 014005_15, 2019/01

 パーセンタイル:100(Astronomy & Astrophysics)



Dipole strength distribution in $$^{206}$$Pb for the evaluation of the neutron capture cross section of $$^{205}$$Pb

静間 俊行; 岩本 信之; 牧永 あや乃*; Massarczyk, R.*; Schwengner, R.*; Beyer, R.*; Bemmerer, D.*; Dietz, M.*; Junghans, A.*; K$"o$gler, T.*; et al.

Physical Review C, 98(6), p.064317_1 - 064317_12, 2018/12

 パーセンタイル:100(Physics, Nuclear)



Radiative transitions of doubly charmed baryons in lattice QCD

Bartiyar, H.*; Can, K. U.*; Erkol, G.*; 岡 眞; 高橋 徹*

Physical Review D, 98(11), p.114505_1 - 114505_14, 2018/12

 被引用回数:2 パーセンタイル:100(Astronomy & Astrophysics)



Measurement of the branching fraction and time-dependent $$CP$$ asymmetry for $$B^0to J/psipi^0$$ decays

Pal, B.*; 谷田 聖; Belle Collaboration*; 他158名*

Physical Review D, 98(11), p.112008_1 - 112008_8, 2018/12

 パーセンタイル:100(Astronomy & Astrophysics)

We measure the branching fraction and time-dependent $$CP$$-violating asymmetry for $$B^0to J/psipi^0$$ decays using a data sample of 711 $${rm fb^{-1}}$$ collected on the $$Upsilon(4S)$$ resonance by the Belle experiment running at the KEKB $$e^+e^-$$ collider. The branching fraction is measured to be $$mathcal{B}(B^0to J/psipi^0) = [1.62,pm 0.11~({rm stat}) pm0.07~({rm syst})]times 10^{-5}$$, which is the most precise measurement to date. The measured $$CP$$ asymmetry parameters are $$mathcal{S} = -0.59,pm 0.19~({rm stat}) pm 0.03~({rm syst})$$ and $$mathcal{A} = -0.15,pm 0.14~({rm stat}),^{+0.04}_{-0.03}~({rm syst})$$. The mixing-induced $$CP$$ asymmetry ($$mathcal{S}$$) differs from the case of no $$CP$$ violation by 3.0 standard deviations, and the direct $$CP$$ asymmetry ($$mathcal{A}$$) is consistent with zero.


Measurement of the decays $$Lambda_cto Sigmapipi$$ at Belle

Berger, M.*; 谷田 聖; Belle Collaboration*; 他197名*

Physical Review D, 98(11), p.112006_1 - 112006_10, 2018/12

 被引用回数:2 パーセンタイル:62.38(Astronomy & Astrophysics)

We report measurements of the branching fractions of the decays $$Lambda^+_ctoSigma^+pi^-pi^+$$, $$Lambda^+_ctoSigma^0pi^+pi^0$$ and $$Lambda^+_ctoSigma^+pi^0pi^0$$ relative to the reference channel $$Lambda^+_cto pK^-pi^+$$. The analysis is based on the full data sample collected at and close to $$Upsilon(4S)$$ resonance by the Belle detector at the KEKB asymmetric-energy $$e^+e^-$$ collider corresponding to the integrated luminosity of 711 fb$$^{-1}$$. We measure $${cal B}(Lambda^+_crightarrowSigma^+pi^-pi^+)/{cal B}(Lambda^+_cto pK^-pi^+) = 0.706~pm 0.003~pm 0.029$$, $${cal B}(Lambda^+_crightarrowSigma^0pi^+pi^0)/{cal B}(Lambda^+_cto pK^-pi^+) = 0.491~pm 0.005~pm 0.028$$ and $${cal B}(Lambda^+_crightarrowSigma^+pi^0pi^0)/{cal B}(Lambda^+_cto pK^-pi^+) = 0.198~pm 0.006~pm 0.016$$. The listed uncertainties are statistical and systematic, respectively.

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