the wellspring of all phases on the kagome lattice
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THE WELLSPRING OF ALL PHASES ON THE KAGOME LATTICE University of - PowerPoint PPT Presentation

THE WELLSPRING OF ALL PHASES ON THE KAGOME LATTICE University of Illinois at Urbana Champaign with Hitesh Changlani, Dmitrii Kochkov, Krishna Kumar, Eduardo Fradkin Blue Waters Symposium Talk Frustrated Quantum Magnets.. Insulator -


  1. THE WELLSPRING OF ALL PHASES ON THE KAGOME LATTICE University of Illinois at Urbana Champaign with Hitesh Changlani, Dmitrii Kochkov, Krishna Kumar, Eduardo Fradkin Blue Waters Symposium Talk

  2. Frustrated Quantum Magnets….. Insulator - Electrons don’t move Interaction between electron spins spins want to anti-align Quantum ? Materials: Frustration from triangles Herbertsmithite Vesigniette Kapellasite Volborthite

  3. Quantum Mechanics is hard

  4. B9XicbZBNS8NAEIYnftb6VfXoZbEInkpSBD0WvXisYD+gTctmu2mXbjZhd6KU0P/hxYMiXv0v3vw3btsctPWFhYd3ZpjZN0ikMOi6387a+sbm1nZhp7i7t39wWDo6bpo41Yw3WCxj3Q6o4VIo3kCBkrcTzWkUSN4Kxrezeu RayNi9YCThPsRHSoRCkbRWr1qT5EuiogbYrFfKrsVdy6yCl4OZchV75e+uoOYpRFXyCQ1puO5CfoZ1SiY5N iNzU8oWxMh7xjUVG7yM/mV0/JuXUGJIy1fQrJ3P09kdHImEkU2M6I4sgs12bmf7VOiuG1nwmVpMgVWywKU0kwJrMIyEBozlBOLFCmhb2VsBHVlKENqmhD8Ja/vArNasVzK979Zbl2k8dRgFM4gwvw4ApqcAd1aA D c/wCm/Ok/PivDsfi9Y1J585gT9yPn8AWRSRwA= </latexit> <latexit sha1_base64="/y4tLtKLjmEqIkYaWgSzQlzhnQw=">A B9XicbZBNS8NAEIYnftb6VfXoZbEInkpSBD0WvXisYD+gTctmu2mXbjZhd6KU0P/hxYMiXv0v3vw3btsctPWFhYd3ZpjZN0ikMOi6387a+sbm1nZhp7i7t39wWDo6bpo41Yw3WCxj3Q6o4VIo3kCBkrcTzWkUSN4Kxrezeu RayNi9YCThPsRHSoRCkbRWr1qT5EuiogbYrFfKrsVdy6yCl4OZchV75e+uoOYpRFXyCQ1puO5CfoZ1SiY5N iNzU8oWxMh7xjUVG7yM/mV0/JuXUGJIy1fQrJ3P09kdHImEkU2M6I4sgs12bmf7VOiuG1nwmVpMgVWywKU0kwJrMIyEBozlBOLFCmhb2VsBHVlKENqmhD8Ja/vArNasVzK979Zbl2k8dRgFM4gwvw4ApqcAd1aA D c/wCm/Ok/PivDsfi9Y1J585gT9yPn8AWRSRwA= </latexit><latexit sha1_base64="/y4tLtKLjmEqIkYaWgSzQlzhnQw=">A B9XicbZBNS8NAEIYnftb6VfXoZbEInkpSBD0WvXisYD+gTctmu2mXbjZhd6KU0P/hxYMiXv0v3vw3btsctPWFhYd3ZpjZN0ikMOi6387a+sbm1nZhp7i7t39wWDo6bpo41Yw3WCxj3Q6o4VIo3kCBkrcTzWkUSN4Kxrezeu RayNi9YCThPsRHSoRCkbRWr1qT5EuiogbYrFfKrsVdy6yCl4OZchV75e+uoOYpRFXyCQ1puO5CfoZ1SiY5N iNzU8oWxMh7xjUVG7yM/mV0/JuXUGJIy1fQrJ3P09kdHImEkU2M6I4sgs12bmf7VOiuG1nwmVpMgVWywKU0kwJrMIyEBozlBOLFCmhb2VsBHVlKENqmhD8Ja/vArNasVzK979Zbl2k8dRgFM4gwvw4ApqcAd1aA D c/wCm/Ok/PivDsfi9Y1J585gT9yPn8AWRSRwA= </latexit><latexit sha1_base64="/y4tLtKLjmEqIkYaWgSzQlzhnQw=">A B9XicbZBNS8NAEIYnftb6VfXoZbEInkpSBD0WvXisYD+gTctmu2mXbjZhd6KU0P/hxYMiXv0v3vw3btsctPWFhYd3ZpjZN0ikMOi6387a+sbm1nZhp7i7t39wWDo6bpo41Yw3WCxj3Q6o4VIo3kCBkrcTzWkUSN4Kxrezeu RayNi9YCThPsRHSoRCkbRWr1qT5EuiogbYrFfKrsVdy6yCl4OZchV75e+uoOYpRFXyCQ1puO5CfoZ1SiY5N iNzU8oWxMh7xjUVG7yM/mV0/JuXUGJIy1fQrJ3P09kdHImEkU2M6I4sgs12bmf7VOiuG1nwmVpMgVWywKU0kwJrMIyEBozlBOLFCmhb2VsBHVlKENqmhD8Ja/vArNasVzK979Zbl2k8dRgFM4gwvw4ApqcAd1aA D c/wCm/Ok/PivDsfi9Y1J585gT9yPn8AWRSRwA= </latexit><latexit sha1_base64="/y4tLtKLjmEqIkYaWgSzQlzhnQw=">A Quantum Mechanics is computationally hard Even at this scaling, if we wanted There is an exponential scaling to do 50 spins, would need one million nodes for a day. ~50 years of numerics in quantum mechanics Algorithm: Find lowest eigenvector of matrix 2 n × 2 n Today: State of the art: 36 spins (many calculations) ~8 hours on Blue Waters 50 spins (1 calculation) (Lauchli on German supercomputers) The quantum mechanical problem hits a wall even with Blue Waters scale. Approximate algorithms or better exponential scaling a route forward. Blue Waters still critical. This is an exploratory and iterative science. The story I’m going to tell involved calculations we didn’t know we were going to be doing at the beginning of the project. Thousands of iterative simulations needed.

  5. What we found? Hamiltoniain (i.e. matrix) with exponentially many ground states. Why it’s interesting? Each ground state represents a phase of matter (liquid, solid, gas, anti-ferromagnet, etc) This means that there is a special Hamiltonian where all phases meet. This means that it sources all interesting phases on a class of materials. Including a particularly interesting (and useful for quantum computing) phase: a spin-liquid.

  6. In strongly correlated systems like frustrated magnets… there are a menagerie of competing phases. Z2 (or Dirac) Spin Liquid Heisenberg (White/Huse) Chiral Spin Liquid 2/3 Plateau (this work) 1/3 Plateau (Donna Sheng) Chiral Term (Bela Bauer, Andreas Ludwig) J1, J2, J3 (Donna Sheng) q=0 magnetic order √ √ 3 order 3 × Ferromagnetism … Is this a cosmic coincident or is their a deep reason behind this?

  7. Aside: Spin Liquids are really interesting. Phil Anderson suggested that the n.n. Heisenberg model on the triangular lattice wasn’t a neel state (frustration!) J z 1 0 ∞ instead, he suggested it was a RVB state. (today we would call such a thing a spin-liquid). | "#i � | #"i

  8. Aside: Spin Liquids are really interesting. Phil Anderson suggested that the n.n. Heisenberg model on the triangular lattice wasn’t a neel state (frustration!) J z 1 0 ∞ instead, he suggested it was a RVB state. (today we would call such a thing a spin-liquid). | "#i � | #"i + + Like Benzene

  9. Aside: Spin Liquids are really interesting. Phil Anderson suggested that the n.n. Heisenberg model on the triangular lattice wasn’t a neel state (frustration!) J z 1 0 ∞ instead, he suggested it was a RVB state. (today we would call such a thing a spin-liquid). | "#i � | #"i + + Not actually a spin liquid - years of numerics (1970-1990) Like Benzene

  10. Aside: Spin Liquids are really interesting. + + Beyond the Landau theory of phases - no broken symmetries! Long Range Entanglement - Can’t be produced from a product state via a short quantum circuit Fractionalized Excitations - Electron breaks into multiple emergent pieces. Topological Degeneracy - Manifold dependent geometry The search for spin liquids is truly a hunt. We haven’t had any good story for what sort of lattices should support spin liquids. The hunt for spin liquids is one of the forefront areas of condensed matter research! Would be useful for storing quantum information and topological quantum computing!

  11. An interesting discovery…. (amazing it hasn’t been known for 30 years) X j + S y i S y X S x i S x S z i S z H = j − 0 . 5 j ij ij J z 0 -0.5 1 ∞ On the kagome: massive exact degeneracy in the XXZ model! exactly -J/4 Finding this was only possible because we could afford to explore many points on Blue Waters. What’s going on? Who ordered this?

  12. Who ordered that? X j + S y i S y X S x i S x S z i S z H = j − 0 . 5 j ij ij These are all the ground states of a single triangle. Define 3 “colors”

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