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Dive into the distinct features of cuprates among materials with strong correlations, analyzing recent experimental advances, theoretical challenges, and novel quantum behaviors. Discover the breakdown of band theory, unconventional superconductivity, multiple electronic phases, and more theoretical insights. Understand the significance of clean versus dirty cuprates and the impact of disorder on our understanding of these materials. Explore the intricacies of cuprates' quantum behavior, their electron phases, and theoretical models. Unveil the secrets of cuprates through theoretical and experimental investigations.
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Whither Strongly Correlated Electron Physics ? T.M.Rice ETHZ & BNL • What`s so unique about the cuprates among the many materials with strongly correlated physics : e.g. transition metal oxides, heavy fermions, organic conductors.... • Recent Experimental Advances & Surprises: Clean vs. Dirty Cuprates • Experiments and Materials I would like to see
Special Features of Strongly Correlated Electrons • Breakdown of Band Theory & Landau Theory of Fermi Liquids e.g. Mott insulators ,pseudogap metallic phase etc • Unconventional Superconductivty e.g. p- & d- wave and heavy fermion superconductors ? • Novel Quantum Critical Points e.g. heavy fermion <-> RKKY metal • Multiple Electronic Phases in Close Proximity to each other e.g. magnetism & superconductivity etc. - - - - - - - - - - - Theoretical Challenges • Strong Interactions => breakdown of perturbation theory etc • Many Phases close by in energy e.g. AF,Stripe,d-SC &SF(?) order • Microscopic Modelling can be difficult e.g. U compounds etc
What‘s so unique about cuprates ? They are the most quantum of the conducting oxides !
x2-y2 3z2-r2 yz zx xy O eg t2g Cu Cuprates => CuO2 plane electronically relevant CuO2-plane e.g. Parent compound: La2CuO4 Cu2+3d9 Cu2+ 1 hole in 3d-eg O-octahedra spin S = 1/2 square lattice of Cu2+-ions Strong Coulomb interaction Mott Insulator, S = 1/2 2D Heisenberg Antiferromagnet => A Highly Quantum System !
2px 2py singlet 3dx2- y2 doped holes enter the O-2p orbitals and formZ-R singlets t-J-model:motion of holes in AF background Holes in a CuO2 plane : Cu3+ CuO2-plane s-hybridization O Cu doped hole 2p Cu2+ 3dx2- y2 Same Symmetry for Cu2+ & Cu3+ => highly mobile holes
Are there other planar S = 1/2 AF systems with larger values of (t,J) and so larger Tc ? Nickelates ? Favored valence is Ni2+ with S =1 [2 holes,octa. coord. Cannot be doped with mobile holes & Hund`s Rule] Can we force a different Ni valence with S= 1/2 ? • Ni3+: No Good! 3 holes favor a 3d82p5 config. => metallic behavior e.g. LaSrNiO4 • Ni+ : Rare! Needs planar coordination as in LaNiO2
Differing Results in LDA + U • Anisimov,Bukvalov & Rice PRB `99 • get AFIsimilar to CaCuO2 • Lee & Pickett PRB `04 • get weakly AFM unlike CaCuO2 • Expt. Hayward et al J.Am.Chem. • insulator with Curie -Weiss • S=1/2 & = - 257K; no AF order • Nonstoichiometric Mott • Insulator? LaNiO2 Conclusion Nickelates are not promising !
Cuprates : Clean vs. Dirty Is our view of the cuprates strongly influenced by the disorder intrinsic to many of the cuprates ?
Disorder in Cuprates Eisaki et al PRB 69,064512 (`04) Site of Disorder (a) Most Damage & (c) Least Damage Single Layer Bilayer Trilayer N.B. Cuprates with good surfaces are in (a) Hg & Tl Cuprates BSCCO & Na-CCOC
Ultra Clean Underdoped Cuprates ( No Intrinsic Disorder ) a) YBCO6.5 Ortho II - UBC group Alternate Chains with & without O b) YBa2Cu4O8 - Karpinski Double Cu-O-Cu Chains
T TN T* strange metal spin gap Spin glass AF Tc SC x under optimally over doped Standard Phase Diagram of the High-Tc Superconductors doping holes 0 Is this the correct phase diagram for clean cuprates ?
Zero Field NMR on Multilayer Hg & Tl cuprates - Osaka group(Mukuda et al 06) Hole density largest on outer planes least on inner planes
Coexisting uniform AF & SC order Phase Diagram with overlaopping AF & SC regions => VMC Results by Ogata,TK Lee etc
STM Patterns on Na-CCOCKohsaka et al Science 315,1380 `07 + Cu sites 2 Features a) Rotational Symmetry of Cu4O4-square locally broken when tip is above O-sites but not Cu-sit b) Short Range Order with 4a0 Domains Is the Pseudogap phase in underdoped cuprates an Intrinsic Electronic Glass?
No Sign of Charge Modulation on O - sites in an underdoped ultraclean cuprate NMR on O(2,3) planar sites Tomeno et al PRB (1994)
Theory of the STMY Chen,TMR & FCZhang PRL`07 Na-CCOC STM tip couples to the outermost orbitals => 3pz Cl When tip is above O-sites there can be interference between tunneling paths depending on relative phase to inject electrons thru’ nn Cl - ions. 1 hole bound to Na+ acceptor can have a degenerate groundstate => Rotational symmetry breaking in STM pattern .
Quantum Oscillations in ultraclean underdoped Cuprates YBCO6.5 Ortho II Doiron-Leyraud et al `07 YBa2Cu4O8 - Yelland et al `07 • Small Fermi Pockets How many pockets in the BZ? In a Paramagnet ARPES predicts 4 => Too Many Holes ( x= 0.15 & 0.2) Underdoped Na-CCOC 1/4 of BZ M — Yang,TMR & Zhang`06
If magnetic field induces AF long range order which reduces the Brillouin Zone ? => 2 Pockets => x= 0.075 & 0.1 Paramagnet Chen et al `07 ARPES AF order
Experiments I would like to see: ARPES & STM on clean and ultraclean cuprates Structured Cuprates => doped chains,ladders,islands, layered . . . New S=1/2 Materials with mobile carriers and different lattices : Organics ?
2-Leg Ladder Compounds with Cu2O3 - planes SrCu2O3 Sr14Cu24O41 — Tel. No. Compound <— CuO2 chains <— Cu2O3 planes — | 180º O-Cu-O Bonds form 2-leg ladders • 2-leg AF S=1/2 Ladders form short range RVB spin liquids • Holes form more stable pairs but 1D nature of ladders leads to competition between `d-SC and CDW ( hole pair xtals) • Only doped example is Sr14Cu24O41 which forms a hole pair xtal. • Are there compounds with doped Cu2O3 - planes similar to the many cuprates with doped CuO2 planes and would this enhance Tc ?
Pattern CuO2 with ZnO2 —> weakly coupled CuO2 islands Can it lead to a U<0 Hubbard model when hole doped ? • Cu • Zn • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • Interisland Hopping ≈ t’/4 U ≈ -J + Coulomb + el. ph Energy gain from singlet groundstate of an island may be possible?
Cuprates after 20 years are still producing surprises and fascinating puzzles. => John Tranquada