20
Pressure effect on the superconductivity of HgBa 2 Ca 2 Cu 3 O 8+ 2010.11.17 Shimizu Lab. M1 KAMADA Yukihiro

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

Embed Size (px)

Citation preview

Page 1: Pressure effect on the superconductivity of HgBa 2 Ca 2 Cu 3 O 8+  2010.11.17 Shimizu Lab. M1 KAMADA Yukihiro

Pressure effect on the superconductivity of HgBa2Ca2Cu3O8+

2010.11.17

Shimizu Lab. M1 KAMADA Yukihiro

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

Contents

• Introduction– The world record of the Tc

– Pressure effect on HgBa2Ca2Cu3O8+ (previous work)– Tc 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

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

The world record of the Tc

Introduction

Tc = 164 K @ 31 GPa

World record of high-Tc!

※ 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.

Page 4: Pressure effect on the superconductivity of HgBa 2 Ca 2 Cu 3 O 8+  2010.11.17 Shimizu Lab. M1 KAMADA Yukihiro

Pressure effect on HgBa2Ca2Cu3O8+ (previous work)

The electrical resistivity of Hg-1223 under high pressure

Pressure dependence of the Tc of Hg-series cuprate

L. Gao et al., Phys. Rev. B   50, 4260 (1994)

Introduction

Page 5: Pressure effect on the superconductivity of HgBa 2 Ca 2 Cu 3 O 8+  2010.11.17 Shimizu Lab. M1 KAMADA Yukihiro

SCAFM AFM

quasi-gap

SC

under dope over dope

optimal dopeoptimal dopeTemperature

00.15 0.15 ~0.20electron hole

Tc depends on…

>0, supplying holes into the CuO2 layers

HgBa2Cam-1CumO2m+2+

m = 3 is the best for high-Tc @ ambient pressure.

aa

c

The carrier concentration

Pressure effect is not only changing lattice constant but also changing hole distribution between CuO2 layers etc…

Introduction

Page 6: Pressure effect on the superconductivity of HgBa 2 Ca 2 Cu 3 O 8+  2010.11.17 Shimizu Lab. M1 KAMADA Yukihiro

Tc depends on…

F.Nakamura, J.Hori, T.Goko, Y.Uno, N.Kikugawa and T.Fujita, Journal of Low Temperature Physics, Vol. 117. 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

La2-xSrxCuO4 Bi2Sr2Ca2Cu3O10+

Introduction

Page 7: Pressure effect on the superconductivity of HgBa 2 Ca 2 Cu 3 O 8+  2010.11.17 Shimizu Lab. M1 KAMADA Yukihiro

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

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

About diamond-anvil cell (DAC)

gasket

pressuremedium

sample

Diamond Anvil Cell(DAC)

6 cm

3 cmdiamond

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

Page 9: Pressure effect on the superconductivity of HgBa 2 Ca 2 Cu 3 O 8+  2010.11.17 Shimizu Lab. M1 KAMADA Yukihiro

SCAFM

quasi-gap

SC

under dope over dope

optimal dopeoptimal dopeTemperature

00.15 0.15 ~ 0.20electron hole

High purity of the samples

• Sample 1 (S1) & Sample 2 (S2)

– Purity (Hg-1223 : 90%~)

• Sample 1 (S1) : Tc = 134 K @ ambient pressure

– To control a little under doped (annealing in a vacuum)

• Sample 2 (S2) : Tc = 130 K @ ambient pressure

– Not to control doping carriers

Experiment

The amount of the doping carriers

Page 10: Pressure effect on the superconductivity of HgBa 2 Ca 2 Cu 3 O 8+  2010.11.17 Shimizu Lab. M1 KAMADA Yukihiro

To control the pressure condition

• Sample 2 (S2)– Hydrostatic

• With pressure medium (NaCl)

– Non-hydrostatic• Without pressure medium

Experiment

Page 11: Pressure effect on the superconductivity of HgBa 2 Ca 2 Cu 3 O 8+  2010.11.17 Shimizu Lab. M1 KAMADA Yukihiro

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 m100 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

Page 12: Pressure effect on the superconductivity of HgBa 2 Ca 2 Cu 3 O 8+  2010.11.17 Shimizu Lab. M1 KAMADA Yukihiro

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 2 100 m

0.85 GPa

※ with microscope.

AC four probe method

Experiment

Page 13: Pressure effect on the superconductivity of HgBa 2 Ca 2 Cu 3 O 8+  2010.11.17 Shimizu Lab. M1 KAMADA Yukihiro

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

CameraPressure determination:• Ruby fluorescence method• Raman shift of diamond

Experiment

Page 14: Pressure effect on the superconductivity of HgBa 2 Ca 2 Cu 3 O 8+  2010.11.17 Shimizu Lab. M1 KAMADA Yukihiro

Experimental result

Hg-1223 (S1) with NaCl

Hg-1223 (S2) with NaCl

Experiment

Hydrostatic (with NaCl) (Sample 1, Sample 2)

Page 15: Pressure effect on the superconductivity of HgBa 2 Ca 2 Cu 3 O 8+  2010.11.17 Shimizu Lab. M1 KAMADA Yukihiro

Experimental result

Hg-1223 (S2) with no pressure medium

Tco

Tc

Hg-1223 (S1) at 0.7 GPa

The Tc was defined by same method of the world record

Definition of the Tc

Experiment

Non-hydrostatic (without pressure medium) (Sample 2)

Page 16: Pressure effect on the superconductivity of HgBa 2 Ca 2 Cu 3 O 8+  2010.11.17 Shimizu Lab. M1 KAMADA Yukihiro

Experimental result

Pressure dependence of Tc about Sample 1 (carrier controlled) and Sample 2 (non-controlled)

Hg-1223 (S1 and S2) with NaCl

The pressure effect of the Tc depends on the sample

Experiment

Page 17: Pressure effect on the superconductivity of HgBa 2 Ca 2 Cu 3 O 8+  2010.11.17 Shimizu Lab. M1 KAMADA Yukihiro

Experimental result

Pressure dependence of Tc with pressure medium and without pressure medium about Sample 2

?

The pressure effect of the Tc depends on the way how to apply the pressure

Hg-1223 (S2)

Experiment

Page 18: Pressure effect on the superconductivity of HgBa 2 Ca 2 Cu 3 O 8+  2010.11.17 Shimizu Lab. M1 KAMADA Yukihiro

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.

Page 19: Pressure effect on the superconductivity of HgBa 2 Ca 2 Cu 3 O 8+  2010.11.17 Shimizu Lab. M1 KAMADA Yukihiro

Discussion

Phase transition?

The change of the Tc by applying the pressure is not continuous

The other discussion…

Hg-1223 (S1 and S2) with NaCl

Page 20: Pressure effect on the superconductivity of HgBa 2 Ca 2 Cu 3 O 8+  2010.11.17 Shimizu Lab. M1 KAMADA Yukihiro

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 Tc!?