Floating Zone Growth of Pure and Pb-Doped Bi-2201 Crystals
Source abstract
Abstract
In this review, we summarize recent progress in crystal growth and understanding of the influence of crystal structure on superconductivity in pure and Pb-doped Bi2Sr2CuOy (Bi-2201) materials belonging to the overdoped region of high-temperature cuprate superconductors. The crystal growth of Bi-2201 superconductors faces challenges due to intricate materials chemistry and the lack of knowledge of corresponding phase diagrams. Historically, a crucible-free floating zone method emerged as the most promising growth approach for these materials, resulting in high-quality single crystals. This review outlines the described methods in the literature and the authors’ synthesis endeavors encompassing Pb-doped Bi-2201 crystals, provides a detailed structural characterization of as-grown and post-growth annealed samples, and highlights optimal growth conditions that yield large-size, single-phase, and compositionally homogeneous Bi-2201 single crystals.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: Physics of Superconductivity and Magnetism · Superconducting Materials and Applications · Magnetic properties of thin films
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Leibniz Institute for Solid State and Materials Research Dresden (IFW Dresden), 01069 Dresden, Germany
References (52)
Show source-provided references
1. Towards a Complete Theory of High Tc10.1038/nphys253 ↗
2. Doping a Mott Insulator: Physics of High-Temperature Superconductivity10.1103/RevModPhys.78.17 ↗
3. From Quantum Matter to High-Temperature Superconductivity in Copper Oxides10.1038/nature14165 ↗
4. Energy Gaps in High-Transition-Temperature Cuprate Superconductors10.1038/nphys3009 ↗
5. Development of Ferromagnetic Fluctuations in Heavily Overdoped (Bi,Pb)2Sr2CuO6+δ Copper Oxides10.1103/PhysRevLett.121.057002 ↗
6. Re-Entrant Charge Order in Overdoped (Bi,Pb)2.12Sr1.88CuO6+δ Outside the Pseudogap Regime10.1038/s41563-018-0108-3 ↗
7. Charge-Density-Wave Origin of Cuprate Checkerboard Visualized by Scanning Tunnelling Microscopy10.1038/nphys1021 ↗
8. Dependence of the Critical Temperature in Overdoped Copper Oxides on Superfluid Density10.1038/nature19061 ↗
9. First Direct Observation of the Van Hove Singularity in the Tunnelling Spectra of Cuprates10.1038/ncomms1229 ↗
10. Disappearance of Superconductivity and a Concomitant Lifshitz Transition in Heavily Overdoped Bi2Sr2CuO6 Superconductor Revealed by Angle-Resolved Photoemission Spectroscopy10.1088/0256-307X/36/1/017402 ↗
11. Observation of Broken Inversion and Chiral Symmetries in the Pseudogap Phase in Single- and Double-Layer Bismuth-Based Cuprates10.1103/PhysRevB.105.155103 ↗
12. Local Noncentrosymmetric Structure of Bi2Sr2CaCu2O8+y by X-ray Magnetic Circular Dichroism at Cu K-Edge XANES10.1007/s10948-017-4418-5 ↗
13. Revealing Hidden Spin-Momentum Locking in a High-Temperature Cuprate Superconductor10.1126/science.aao0980 ↗
14. Doubling of the Bands in Overdoped Bi2Sr2CaCu2O8: Evidence for c-Axis Bilayer Coupling10.1103/PhysRevLett.87.117002 ↗
15. Electron-Tunneling Measurements of Low-Tc Single-Layer Bi2+xSr2−yCuO6+δ: Evidence for a Scaling Disparity between Superconducting and Pseudogap States10.1103/PhysRevB.86.214506 ↗
16. Low Anisotropy of the Upper Critical Field in a Strongly Anisotropic Layered Cuprate Bi2.15Sr1.9CuO6+δ: Evidence for a Paramagnetically Limited Superconductivity10.1103/PhysRevB.89.214516 ↗
17. Chen, D., Lin, C., Maljuk, A., and Zhou, F. (2016). Growth and Characterization of Bulk Superconductor Material, Springer.10.1007/978-3-319-31548-5 ↗
18. Growth of Heavily Pb-Substituted Bi-2201 Single Crystals by a Floating Zone Method10.1016/S0921-4534(97)01680-8 ↗
19. Growth and Properties of Large Area Bi2+xSr2−xCuO6+y Single Crystals10.1016/0921-4534(91)90596-Q ↗
20. Comparative Study of Bi2201 Single Crystalsgrown from Solution Melt and in Cavities Formed in KCl10.1016/S0038-1098(98)00359-7 ↗
21. Growth of Large Superconducting Bi2+xSr2−yCuO6+δ Single Crystals by Travelling Solvent Floating Zone Method10.1016/S0921-4534(01)00414-2 ↗
22. Effects of Oxygen and Strontium Vacancies on the Superconductivity of Single Crystals of Bi2Sr2−xCuOy10.1103/PhysRevB.40.6872 ↗
23. Superconducting Single Crystals10.1038/337021b0 ↗
24. Single Crystal Growth of the Superconductor Bi2.0(Bi0.2Sr1.8Ca1.0)Cu2.0O810.1016/0022-0248(88)90057-7 ↗
25. Preparation of Bi2Sr2CuO6 Single Crystals by the Traveling Solvent Floating Zone Method10.1016/0921-4534(91)92030-F ↗
26. Crystal Growth of the Quasi-One-Dimensional Compound Ca2+xY2−xCu5O1010.1016/S0921-4526(99)02549-1 ↗
27. Crystal Growth and Anisotropic Resistivity of Bi2Sr2−xLaxCuOy10.1103/PhysRevB.54.7449 ↗
28. Growth and Accurate Characterization of Bi2Sr2−xLaxCuO6+δ Single Crystals10.1007/s10948-010-0761-5 ↗
29. New Class of High Tc Structures: Intergrowth of Multiple Copper Oxide Perovskite-like Layers with Double Sheets of BiO10.1016/0038-1098(88)90987-8 ↗
30. New Insight on Bismuth Cuprates with Incommensurate Modulated Structures10.1107/S2052520616005643 ↗
31. Lattice Symmetry Breaking in Cuprate Superconductors: Stripes, Nematics, and Superconductivity10.1080/00018730903122242 ↗
32. Structures of the Superconducting Oxides Tl2Ba2CuO6 and Bi2Sr2CuO610.1103/PhysRevB.38.225 ↗
33. X-ray Investigation of the Incommensurate Modulated Structure of Bi2.08Sr1.84CuO6−δ10.1107/S0108768192002143 ↗
34. Detailed Structure of a Pb-Doped Bi2Sr2CuO6 Superconductor10.1103/PhysRevB.58.2851 ↗
35. New Non-Superconducting Modulation-Free BiPbSr2MOy Phases (M = Co, Mn, Fe) Isotypic with the 10 K Bi2Sr2CuOy Superconductor10.1016/0921-4534(90)90480-3 ↗
36. Incommensurate Modulations in the Lead-Doped Bismuth Strontium Calcium Copper Oxide 221 Superconducting Phase: A Five-Dimensional Superspace Description10.1021/cm00009a026 ↗
37. Crystal Structure of Bi2Sr2CuO6: A Structure Based on Periodic Crystallographic Shear Planes in the “2201” Structure10.1016/0038-1098(93)90493-7 ↗
38. Crystal Chemistry of the Compound Sr2Bi2CuO610.1557/JMR.1990.0046 ↗
39. Bi-2201 Phases Synthesis, Structures and Superconducting Properties10.1016/0921-4534(95)00172-7 ↗
40. The Incommensurate Modulation in the Bi2Sr2−xCaxCuO6 Superconductor, and Its Relation to the Modulation in Bi2Sr2−xCaxCu2O810.1016/0921-4534(89)90416-4 ↗
41. Structural Model for the Incommensurate Bismuth High-Tc Superconductors10.1103/PhysRevB.45.8085 ↗
42. Rietveld Analysis of the Composite Crystal in Superconducting Bi2+xSr2−xCuO6+y10.1016/0921-4534(92)90115-S ↗
43. High-Quality Large-Sized Single Crystals of Pb-Doped Bi2Sr2CuO6+δ High-Tc Superconductors Grown with Traveling Solvent Floating Zone Method10.1088/0256-307X/27/8/087401 ↗
44. Co-Doping Effects of Pb and La in (Bi,Pb)2(Sr,La)2CuOy10.1016/j.physc.2004.01.048 ↗
45. Bi, Pb-Sr-Cu-O System Including a Modulation-Free Superconductor10.1016/0921-4534(90)90167-D ↗
46. (2016). APEX3, SAINT-Plus and SADABS, Bruker AXS Inc.
47. Comparison of Silver and Molybdenum Microfocus X-ray Sources for Single-Crystal Structure Determination10.1107/S1600576714022985 ↗
48. SHELXT—Integrated Space-Group and Crystal-Structure Determination10.1107/S2053273314026370 ↗
49. A Short History of SHELX10.1107/S0108767307043930 ↗
50. The Incommensurate Modulation of the 2212 Bi-Sr-Ca-Cu-O Superconductor10.1126/science.241.4868.954 ↗
51. Single Crystal X-Ray Structure Analysis of Bi2(Sr, Ca)2CuOx and Bi2(Sr, Ca)3Cu2Ox Superconductors10.1143/JJAP.27.L1661 ↗
52. Superconductivity at 27 K in Modulation-Free Bi2−xPbxSr2−yLayCuO6 Phases with X ≅ y + 0.210.1016/0921-4534(90)90637-T ↗