Pressure effect on the superconductivity of HgBa 2 Ca 2 Cu 3 O 8+  2010.11.17 Shimizu Lab. M1 KAMADA Yukihiro.

Slides:



Advertisements
Similar presentations
Modulation of conductive property in VO 2 nano-wires through an air gap-mediated electric field Tsubasa Sasaki (Tanaka-lab) 2013/10/30.
Advertisements

M1 colloquium Shimizu-group M1 Daiki Hayashi Possibility of metallic phase and three-dimensional conductance of graphite.
Pressure-Induced Polymerization of Dehydro[24]annulenes Derivative Shimizu-group M1 NAKASE Tomoya 1.
Acknowledgements: Our research is sponsored by DFG SPP planet magnetisms project G1712 7/1. Special thanks are given to Prof. Dr. Wolfgang. Schmahl and.
Pressure-Induced Hydrogen-dominant metallic state in Aluminum Hydride HAGIHARA Toshiya Shimizu-group Igor Goncharenko et al., Phy. Rev. Lett. 100,
Superconductivity in Diamond
1 High Pressure Study on MgB 2 B.Lorenz, et al. Phys. Rev.B 64,012507(2001) Shimizu-group Naohiro Oki.
1 Raman spectra and X-ray diffraction of Boron Triiodide at high pressure SHIMIZU Group ONODA Suzue Ref: A. Anderson and L. Lettress J. Raman Spectrosc.
Kitaoka lab Itohara Keita
Kitaoka Lab. M1 Yusuke Yanai Wei-Qiang Chen et al., EPL, 98 (2012)
Pressure-Induced Polymerization of 24NHBn(Dehydro[24]annulenes) Shimizu-group M1 NAKASE Tomoya 1.
Doping and Disorder in the Oxygenated, Electron-doped High-temperature Superconductor Pr 2-x Ce x CuO 4±  The building blocks of the high-temperature.
Specific heat Blue=olivine, green=MgO, orange=forsterite, black=Al2O3, brown=grossular, purple=pyrope, red=CaO.
Electronic structure of La2-xSrxCuO4 calculated by the
M. Hücker Manipulating Competing Order with High Pressure Neutron Scattering Group (CMPMS) Correlated Electron Systems ( Superconductivity, Magnetism,
Search for high temperature superconductivity of Sr 2 VO 4 under high pressure Shimizu Lab Kaide Naohiro.
Rinat Ofer Supervisor: Amit Keren. Outline Motivation. Magnetic resonance for spin 3/2 nuclei. The YBCO compound. Three experimental methods and their.
The Three Hallmarks of Superconductivity
Pressure Calibration in DAC -- Challenges for Increasing Accuracy and Precision Ho-kwang Mao Carnegie Institution of Washington Pressure Calibration Workshop.
Shimizu-lab M-1 Kubota Kazuhisa
Investigating the mechanism of High Temperature Superconductivity by Oxygen Isotope Substitution Eran Amit Amit Keren Technion- Israel Institute of Technology.
Hall Effect in Sr 14−x Ca x Cu 24 O 41 E. Tafra 1, B. Korin-Hamzić 2, M. Basletić 1, A. Hamzić 1, M. Dressel 3, J. Akimitsu 4 1.Department of Physics,
What are the key ingredients for a successful laser heating experiment at the synchrotron? Guoyin Shen CARS, University of Chicago GeoSoilEnviroCARS The.
Investigation of fluid- fluid phase transition of hydrogen under high pressure and high temperature 2014/11/26 Shimizu laboratory SHO Kawaguchi.
1 Superconductivity  pure metal metal with impurities 0.1 K Electrical resistance  is a material constant (isotopic shift of the critical temperature)
M1 Colloquium Presentation Arora Varun 29A13106 (Shimizu Lab) High Pressure Study of Na x TiNCl and CeFe 2.
How does Superconductivity Work? Thomas A. Maier.
M1 Colloquium Presentation Arora Varun 29A13106 (Shimizu Lab) Superconductivity in MNX type compounds ( TiNCl ) Superconducting Nitride Halides (MNX),
MgB2 Since 1973 the limiting transition temperature in conventional alloys and metals was 23K, first set by Nb3Ge, and then equaled by an Y-Pd-B-C compound.
Electrical conduction property of solid iodine in the molecular phase Shimizu Group Yu TANAKA.
Hydrostaticity of Pressure Transmitting Medium of 4:1 Methanol: Ethanol at High Pressure and Low Temperature Christopher Salvo 1, Andrew Cornelius 2 1.
Colossal Magnetoresistance of Me x Mn 1-x S (Me = Fe, Cr) Sulfides G. A. Petrakovskii et al., JETP Lett. 72, 70 (2000) Y. Morimoto et al., Nature 380,
Pressure effect on electrical conductivity of Mott insulator “Ba 2 IrO 4 ” Shimizu lab. ORII Daisuke 1.
Calorimetric Investigation under High Pressure Shimizu-Group M1 Shigeki TANAKA F. Bouquet et al., Solid State Communications 113 (2000)
High Pressure Studies of Titanium Hydride Up to 50 GPa with Synchrotron X-ray Diffraction Greg Harding 1, Patricia Kalita 2, Stanislav Sinogeikin 3, Andrew.
Superconductivity in electron-doped C 60 crystals 電子ドープされたフラーレン結晶 における超伝導 Kusakabe Lab Kei Kawashima.
An Introduction to Fe-based superconductors
H. Giefers, University of Paderborn Introduction XAFS 12 in Malmö 24. June 2003 High-pressure EXAFS and XRD investigation of unit cell parameters of SnO.
Search for superconductivity in CrB 2 under pressure 29A13025 Shimizu Lab Kaide Naohiro.
会社名など E. Bauer et al, Phys. Rev. Lett (2004) M. Yogi et al. Phys. Rev. Lett. 93, (2004) Kitaoka Laboratory Takuya Fujii Unconventional.
The Nb 5 Si 3 sample was prepared by Dr. Ravhi Kumar at the University of Nevada, Las Vegas. A stainless steel gasket with a 130 μm centered circular hole.
Shimizu Lab. M1 Takuya Yamauchi
Giorgi Ghambashidze Institute of Condensed Matter Physics, Tbilisi State University, GE-0128 Tbilisi, Georgia Muon Spin Rotation Studies of the Pressure.
Reduced-adiabat Isotherms of Metals and Hard Materials at 100 GPa Pressures and Finite Temperatures W. J. Nellis Department of Physics Harvard University.
High Pressure study of Bromine Shimizu Lab M2 Hayashi Yuma.
High Pressure study of Bromine
Phase diagram of solid oxygen at low temperature and high pressure
Recent Progress in High-Pressure Studies on Plastic Properties of Earth Materials COMPRES meeting at lake Tahoe June, 2004.
Nanoscale imaging and control of resistance switching in VO 2 at room temperature Jeehoon Kim, Changhyun Ko, Alex Frenzel, Shriram Ramanathan, and Jennifer.
Competing Orders, Quantum Criticality, Pseudogap & Magnetic Field-Induced Quantum Fluctuations in Cuprate Superconductors Nai-Chang Yeh, California Institute.
Pressure Scales & Hydrostaticity National Institute for Materials Science (NIMS), Tsukuba, Japan TAKEMURA Kenichi COMPRES workshop on pressure scales,
1 SHIMIZU Group ONODA Suzue Metallization and molecular dissociation of SnI 4 under pressure Ref: A.L. Chen, P.Y. Yu, M.P. Pasternak, Phys. Rev. B. 44,
Superconductivity in HgBa 2 Ca m-1 Cu m O 2m+2+δ (m=1,2, and 3) under quasihydrostatic pressures L. Gao et al., Phys. Rev. B 50, 4260 (1994) C. Ambrosch-Draxl.
Growing and Patterning Thin Films of Pr 2 –x Ce x CuO 4-Y Justin Sousa Marco Salvaggio Matthew C. Sullivan Department of Physics, Ithaca College, Ithaca.
Superconductivity and Superfluidity PHYS3430 Professor Bob Cywinski “Superconductivity is perhaps the most remarkable physical property in the Universe”
Fe As A = Ca, Sr, Ba Superconductivity in system AFe 2 (As 1-x P x ) 2 Dulguun Tsendsuren Kitaoka Lab. Division of Frontier Materials Sc. Department of.
Structural Determination of Solid SiH 4 at High Pressure Russell J. Hemley (Carnegie Institution of Washington) DMR The hydrogen-rich solids are.
Pressure Dependence of Superconductivity of Iron Chalcogenides
High pressure study on superconductor K x Fe 2-y Se 2 M1 Hidenori Fujita Shimizu group.
Superconductivity and magnetism in iron-based superconductor
Search and Characterization of Novel Superhard Phases in the B-C-N System Under Extreme Conditions L. C. Ming, P. V. Zinin, and M. H. Manghnani, U niversity.
High pressure phase diagram of Beryllium Phys.Rev.B 86,174118(2012) Shimizu Lab. Takuya Yamauchi.
Why Make Holes in Superconductors? Saturday Morning Physics December 6, 2003 Dr. Sa-Lin Cheng Bernstein.
 = -1 Perfect diamagnetism (Shielding of magnetic field) (Meissner effect) Dynamic variational principle and the phase diagram of high-temperature superconductors.
Superconductivity in CuxBi2Se3 and its Implications for the Undoped Topological Insulator Garrett Vanacore, Sean Vig, Xiaoxiao Wang, Jiang Wang, University.
25th International Conference on Low Temperature Physics
Superconductivity in Bismuth Oxide Compounds
Yoshida Lab Tatsuo Kano
2019/4/16 Search for liquid-metallic hydrogen under high temperature and high pressure Shimizu group M1 SHO Kawaguchi V. Dzyabura et al. PNAS, 110, 20,
Pressure generation of toroidal anvil cell for physical property investigation under ultra-high pressure 2019/5/29 Shimizu Lab Kara Yusuke.
Presentation transcript:

Pressure effect on the superconductivity of HgBa 2 Ca 2 Cu 3 O 8+  Shimizu Lab. M1 KAMADA Yukihiro

Contents Introduction –The world record of the T c –Pressure effect on HgBa 2 Ca 2 Cu 3 O 8+  (previous work) –T c depends on… –Motivation Experiment –About diamond-anvil cell (DAC) –High purity of the samples –The amount of the doping carriers –Method of measuring electrical resistance under high pressure with DAC –Method of cooling & determination of the pressure –Experimental result –Discussion Summary

The world record of the T c Introduction T c = GPa World record of high-T c ! ※ Superconductivity ・ Electrical resistance is Zero ・ Meissner effect (perfect diamagnetism) Its superconductivity can’t be explained with BCS theory. The mechanism of superconductivity still has many mysteries.

Pressure effect on HgBa 2 Ca 2 Cu 3 O 8+  (previous work) The electrical resistivity of Hg-1223 under high pressure Pressure dependence of the T c of Hg-series cuprate L. Gao et al., Phys. Rev. B 50, 4260 (1994) Introduction

SC AFM quasi- gap SC under dope over dope optimal dope Temperature ~ 0.20 electronhole T c depends on…  >0, supplying holes into the CuO 2 layers HgBa 2 Ca m-1 Cu m O 2m+2+  m = 3 is the best for high-T ambient pressure. a a c The carrier concentration Pressure effect is not only changing lattice constant but also changing hole distribution between CuO 2 layers etc… Introduction

T c depends on… F.Nakamura, J.Hori, T.Goko, Y.Uno, N.Kikugawa and T.Fujita, Journal of Low Temperature Physics, Vol Nos. 5/6, 1999 Xiao-Jia Chen, Viktor V. Struzhkin, Yong Yu, Alexander F. Goncharov, Cheng-Tian Lin, Ho-kwang Mao & Russell J. Hemley, Nature 466, (2010) 950–953 La 2-x Sr x CuO 4 Bi 2 Sr 2 Ca 2 Cu 3 O 10+  Introduction

Motivation Try to make a new world record! – High purity of the sample – The amount of the doping carriers – To control the pressure condition – Higher pressure – And so on… Introduction

About diamond-anvil cell (DAC) gasket pressure medium sample Diamond Anvil Cell (DAC) 6 cm 3 cm diamond To explain easily, this picture is the DAC which keeps the pressure by screw. In this experiment, I used the DAC which apply the pressure by gas-pressure system. ※ Experiment

SC AFM quasi- gap SC under dopeover dope optimal dope Temperature ~ 0.20 electronhole High purity of the samples Sample 1 (S1) & Sample 2 (S2) – Purity (Hg-1223 : 90%~) Sample 1 (S1) : T c = 134 ambient pressure –To control a little under doped (annealing in a vacuum) Sample 2 (S2) : T c = 130 ambient pressure –Not to control doping carriers Experiment The amount of the doping carriers

To control the pressure condition Sample 2 (S2) –Hydrostatic With pressure medium (NaCl) –Non-hydrostatic Without pressure medium Experiment

Method of measuring electrical resistance under high pressure with DAC Gasket (SUS310S) Electrical probe (Pt foil) Pressure Medium (NaCl) sample Pressure marker (Ruby chip) Insulator (c-BN powder + epoxy) Electrical probe (Au wire) 300  m 100  m 1.8 GPa Sample 2 Hydrostatic (with NaCl) (Sample 1, Sample 2) ※ with microscope. AC four probe method ※ S1:pserud four probe method Experiment

Method of measuring electrical resistance under high pressure with DAC Gasket (SUS310S) Electrical probe (Pt foil) sample Pressure marker (Ruby chip) Insulator (c-BN powder + epoxy) 300  m Non-hydrostatic (without pressure medium) (Sample 2) Sample  m 0.85 GPa ※ with microscope. AC four probe method Experiment

Method of cooling & determination of the pressure Low temperature generator : Pulse Tube refrigerator (low vibration) Gas type DAC different type Gas type DAC can change the pressure at low temperature. (DAC in the refrigerator) Measured with PC Camera Pressure determination: Ruby fluorescence method Raman shift of diamond Experiment

Experimental result Hg-1223 (S1) with NaCl Hg-1223 (S2) with NaCl Experiment Hydrostatic (with NaCl) (Sample 1, Sample 2)

Experimental result Hg-1223 (S2) with no pressure medium T co TcTc Hg-1223 (S1) at 0.7 GPa The T c was defined by same method of the world record Definition of the T c Experiment Non-hydrostatic (without pressure medium) (Sample 2)

Experimental result Pressure dependence of T c about Sample 1 (carrier controlled) and Sample 2 (non-controlled) Hg-1223 (S1 and S2) with NaCl The pressure effect of the T c depends on the sample Experiment

Experimental result Pressure dependence of T c with pressure medium and without pressure medium about Sample 2 ? The pressure effect of the T c depends on the way how to apply the pressure Hg-1223 (S2) Experiment

Discussion L. Gao et al., Phys. Rev. B 50, 4260 (1994) Comparing the previous work to my work Hg-1223 (S1 and S2) with NaCl Carrier density? But, can’t find any clear reasons.

Discussion Phase transition? The change of the T c by applying the pressure is not continuous The other discussion… Hg-1223 (S1 and S2) with NaCl

Summary From this experiment –Can’t make the new world record… –Phase transition? Future –1. Higher pressure –2. X-ray diffraction measurement –3. Uniaxial pressure –4. Best condition of the pressure The new world record of the T c !?