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初貝 安弘 ORCID iD icon
筑波大学
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Web 記事 - 201007のエントリ

時間反転な系特有のクラマース縮退は4元数(Quaternion)により自然に記述されます。[Y. Hatsugai in Focus issue in topological insulators :NJP] [論文直接]

一般に波動関数の位相の不定性はベリー接続に U(1) のゲージ構造をあたえますが、クラマース縮退のある場合、それはSp(1)ゲージ構造となります。また、ベリー接続の特異点を与える偶然縮退は一般にはDirac単磁極を与えますが、時間反転不変な場合、この特異点はYang のSU(2)単磁極となります。この例のように Sp(1)=SU(2)の同値性に基づくと時間反転不変な系でのベリー接続はSU(2)ゲージ理論の一つの実現をあたえることとなります。
ここで通常の複素数を四元数(Quertenion)に読み替えることにより、時間反転を持たない場合と持つ場合がアナロジーを越えてマップとして自然に読み替えられることとなります。ベリー接続のゲージ固定条件を考えることにより、非自明かつ自然な次元は複素数、四元数の基底の数により規定され、それぞれ2次元、4次元となります。対応して位相不変量はそれぞれ、2次元、4次元球面上の第1,第2チャーン数であたえられ、その量子化は1つ次元が下の赤道上、1次元閉曲線上の回転数、3次元球面上のポントリャーギン数の量子化に帰着しますが、これは特定のゲージ固定のもとでの球面上の特異点とみることもできます。この特異点は、自然な次元から1つ次元をあげた、それぞれ3次元、5次元のなかで一般化したDirac stringとなり、その終点がDiracおよびYang 単磁極となるのです。これら2次元、4次元球面上の赤道はカイラル対称な部分空間として特徴付けられ、この赤道上での奇数次元の積分で定義されるベリー位相並びにチャーンサイモン積分は第一、第2チャーン数を整数のゲージ不定性としてのぞけば半整数値に量子化されることとなります。これがZ2量子化です。くわしくはまた!

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今年もやります。まずは量子力学3(遠隔). 冬は 統計力学2 改め物性理論4 (大学院「ベリー接続の理論とバルクエッジ対応」). 令和二年の新年あけましておめでとうございます。今年もあと102日!
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投稿者 : hatsugai 投稿日時: 2020-09-17 11:42:01 (22 ヒット)

As for a topological characterization of a full Liouvillian (including jump term) for the non hermitian fractional quantum Hall states, we are proposing a pseudospin Chern number associated with the Niu-Thouless-Wu type twists in the doubled Hilbert space. Numerical demonstration of the proposal is explicitely given and its validity is discussed. Have a look at "Fate of fractional quantum Hall states in open quantum systems: Characterization of correlated topological states for the full Liouvillian" by Tsuneya Yoshida, Koji Kudo, Hosho Katsura, and Yasuhiro Hatsugai, Phys. Rev. Research 2, 033428 (2020) (open access).


投稿者 : hatsugai 投稿日時: 2020-09-17 11:06:17 (35 ヒット)

The Dirac cone is a typical singular energy dispersion in two dimensions that is a source of various non-trivial topological effects. When realized in real/synthetic materials, it is generically tilted and the equi-energy surface (curve) can be elliptic/hyperbolic (type I/II). The type III Dirac cone is a critical situation between the type I and II that potentially causes various non-trivial physics. As for realization of the type III Dirac cones, we are proposing a generic theoretical scheme without any fine tuning of material parameters . It may also help to synthesize in meta materials. The molecular orbital (MO) construction of the generic flat bands which we are also proposing plays a crutial role. Have a look at "Type-III Dirac Cones from Degenerate Directionally Flat Bands: Viewpoint from Molecular-Orbital Representation" by Tomonari Mizoguchi and Yasuhiro Hatsugai, J. Phys. Soc. Jpn. 89, 103704 (2020) Also arXiv:2007.14643.


投稿者 : hatsugai 投稿日時: 2020-09-08 20:05:59 (44 ヒット)

Motivated by a historical example, the Dirac Hamiltonian as a square-root of the Klein-Gordon Hamiltonian, its lattice analogue has been discussed recently. Zero energy states are shared by the parent and its descendant. The story is more than that. Not necessarily zero energy but its high energy part can also share topological characters. We hereby propose a “square-root higher order topological insulator (square-root HOTI)” when its squared parent is HOTI. Based on the simple observation that square of the decorated honeycomb lattice is given by a decoupled sum of the Kagome and honeycomb lattices, we have demonstrate that the “corner states” of the breezing Kagome lattice with boundaries share topological characters with its descendant as the decorated honeycomb lattice. Have a look at our recent paper, "Square-root higher-order topological insulator on a decorated honeycomb lattice" by Tomonari Mizoguchi, Yoshihito Kuno, and Yasuhiro Hatsugai, to appear in Phys. Rev. A, also arXiv:2004.03235.


投稿者 : hatsugai 投稿日時: 2020-08-16 14:53:28 (171 ヒット)

Adiabatic deformation of gapped systems is a conceptual basis of topological phases. It implies that topological invariants of the bulk described by the Berry connection work as topological order parameters of the phase. This is independent of the well-established symmetry breaking scenario of the phase characterization. Adiabatic heuristic argument for the fractional quantum Hall states is one of the oldest such trials that states the "FRACTIONAL" state is deformed to the “INTEGER”. Although it is intuitive and physically quite natural, there exist several difficulties. How the states with different degeneracy are deformed each other adiabatically? We have clarified the questions and demonstrated this adiabatic deformation on a torus in the paper "Adiabatic heuristic principle on a torus and generalized Streda formula" by Koji Kudo and Yasuhiro Hatsugai , Phys. Rev. B 102, 125108 (2020) (also arXiv:2004.00859) What is deformed continuously is a gap not the states ! This is also sufficient for the topological stability of the Chern number (of the degenerate multiplet) as a topological order parameter. Have a look at.


投稿者 : hatsugai 投稿日時: 2020-07-30 12:47:16 (163 ヒット)

Our article on non-hermitian band touching for strongly correlated systems has been published in PTEP (Progress of Theoretical and Experimental Physics), "Exceptional band touching for strongly correlated systems in equilibrium", by Tsuneya Yoshida, Robert Peters, Norio Kawakami, Yasuhiro Hatsugai. Focusing on the non-hermitian topological phenomena for the equilibrium Green function of correlated electrons, a compact review of the exceptonal band touching that is intrinsic for non-hermitian matrices is described as well. Have a look at.


    検索
    バルク・エッジ対応
    [0] バルクとエッジ
    [1] 集中講義
    [2] 原論文と解説
    [3] トポロジカル秩序とベリー接続:日本物理学会誌 「解説」 [JPS-HP] [pdf]
    [4] "Band gap, dangling bond and spin : a physicist's viewpoint" [pdf] [Web]
    トポロジカル相
    [0]昔の科研費
    科研費 1992年度:電子系スピン系におけるトポロジカル効果
    科研費 1994年度:物性論におけるトポロジーと幾何学的位相
    私の講演ファイルのいくつか
    [1] MIT, Boston (2003)
    [2] APS/JPS March Meeting (2004)
    [3] JPS Fall meeting, JAPAN (2004)
    [4] APS/JPS March meeting (2005)
    [5] JPS Fall meeting (2005):Entanglement
    [6] Superclean workshop, Nasu (2006)
    [7] MPIPKS, Dresden (2006)
    [8] KEK, Tsukuba (2007)
    [9] ETH, Zurich (2008)
    [10] ICREA, Sant Benet (2009)
    [11] JPS Meeting, Kumamoto (2009)
    [12]HMF19, Fukuoka (2010)
    [13] NTU, Singapore (2011)
    [14] ICTP, Trieste (2011)
    [15] Villa conf., Orland (2012)
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