Heterogeneous vortex dynamics in high temperature superconductors

Transcription

1 Heterogeneous vortex dynamics in high temperature superconductors Feng YANG Laboratoire des Solides Irradiés, Ecole Polytechnique, Palaiseau, France. June 18, 2009/PhD thesis defense

2 Outline 1 Introduction Superconductivity Model NMR experiments Shear viscosity of the vortex liquid 2 Methods Experimental procedures Verification: bulk or surface properties? Magneto-optical imaging and transport measurements 3 Results Comparison with 2D melting model Comparison with 3D Bose-glass model 4 Discussions 5 Summary

3 Superconductivity Outline 1 Introduction Superconductivity Model NMR experiments Shear viscosity of the vortex liquid 2 Methods Experimental procedures Verification: bulk or surface properties? Magneto-optical imaging and transport measurements 3 Results Comparison with 2D melting model Comparison with 3D Bose-glass model 4 Discussions 5 Summary

4 Superconductivity Zero resistance and diamagnetism R ( Ω ) T ( K ) Perfect conductivity. Exclusion of magnetic field (known as the Meissner effect). Superconductivity is a thermodynamic state.

5 Superconductivity Zero resistance and diamagnetism R ( Ω ) T ( K ) Perfect conductivity. Exclusion of magnetic field (known as the Meissner effect). Superconductivity is a thermodynamic state.

6 Superconductivity Zero resistance and diamagnetism R ( Ω ) T ( K ) Perfect conductivity. Exclusion of magnetic field (known as the Meissner effect). Superconductivity is a thermodynamic state.

7 Superconductivity Superconducting materials Many materials become superconducting at low temperatures or high pressures. "New" discoveries: cuprate family: YBCO (1987), BSCCO (1988),... boron-doped group-iv semiconductors (diamond, silicon,...) (since 2001) FeAs-based superconductors (2006) SiH 4 (2008, under high pressure) Future: new forms of superconductivity?

8 Superconductivity Superconducting materials Many materials become superconducting at low temperatures or high pressures. "New" discoveries: cuprate family: YBCO (1987), BSCCO (1988),... boron-doped group-iv semiconductors (diamond, silicon,...) (since 2001) FeAs-based superconductors (2006) SiH 4 (2008, under high pressure) Future: new forms of superconductivity?

9 Superconductivity Superconducting materials Many materials become superconducting at low temperatures or high pressures. "New" discoveries: cuprate family: YBCO (1987), BSCCO (1988),... boron-doped group-iv semiconductors (diamond, silicon,...) (since 2001) FeAs-based superconductors (2006) SiH 4 (2008, under high pressure) Future: new forms of superconductivity?

10 Superconductivity Superconducting materials Many materials become superconducting at low temperatures or high pressures. "New" discoveries: cuprate family: YBCO (1987), BSCCO (1988),... boron-doped group-iv semiconductors (diamond, silicon,...) (since 2001) FeAs-based superconductors (2006) SiH 4 (2008, under high pressure) Future: new forms of superconductivity?

11 Superconductivity Superconducting materials Many materials become superconducting at low temperatures or high pressures. "New" discoveries: cuprate family: YBCO (1987), BSCCO (1988),... boron-doped group-iv semiconductors (diamond, silicon,...) (since 2001) FeAs-based superconductors (2006) SiH 4 (2008, under high pressure) Future: new forms of superconductivity?

12 Superconductivity Superconducting materials Many materials become superconducting at low temperatures or high pressures. "New" discoveries: cuprate family: YBCO (1987), BSCCO (1988),... boron-doped group-iv semiconductors (diamond, silicon,...) (since 2001) FeAs-based superconductors (2006) SiH 4 (2008, under high pressure) Future: new forms of superconductivity?

13 Superconductivity Superconducting materials Many materials become superconducting at low temperatures or high pressures. "New" discoveries: cuprate family: YBCO (1987), BSCCO (1988),... boron-doped group-iv semiconductors (diamond, silicon,...) (since 2001) FeAs-based superconductors (2006) SiH 4 (2008, under high pressure) Future: new forms of superconductivity?

14 Superconductivity Two types of superconductors H H c (T) normal state superconducting state (Meissner state) Type-I T c T In general, type-ii superconductors have much higher H c, J c and also T c than type-i superconductors. Here, we study type-ii superconductors.

15 Superconductivity Two types of superconductors H H H c2 (T) H c (T) normal state mixed state normal state superconducting state (Meissner state) Type-I T c T H c1 (T) Meissner state Type-II T c T In general, type-ii superconductors have much higher H c, J c and also T c than type-i superconductors. Here, we study type-ii superconductors.

16 Superconductivity Two types of superconductors H H H c2 (T) H c (T) normal state mixed state normal state superconducting state (Meissner state) Type-I T c T H c1 (T) Meissner state Type-II T c T In general, type-ii superconductors have much higher H c, J c and also T c than type-i superconductors. Here, we study type-ii superconductors.

17 Superconductivity Magnetic flux quantization Magnetic flux quantification in type-ii superconductors vortices B = nφ 0, φ 0 = h 2e = G cm 2. Vortex lattice observed in Bi 2 Sr 2 CaCu 2 O x with micro Hall probes, H //c = 12 Oe, T = 81 K. A. Grigorenko et al., Nature 414, 728 (2001).

18 Superconductivity Vortex distribution in real superconductors An ideal vortex lattice yields j c = 0, R 0. j c is the critical current. Vortex pinning by material defects (pinning centers) Vortex distribution is no longer uniform j c > 0, R = 0. Bean s bulk pinning model (1962). db x dz dbz dx = µ 0j, where j = j c, -j c or 0.

19 Superconductivity Vortex distribution in real superconductors An ideal vortex lattice yields j c = 0, R 0. j c is the critical current. Vortex pinning by material defects (pinning centers) Vortex distribution is no longer uniform j c > 0, R = 0. Bean s bulk pinning model (1962). db x dz dbz dx = µ 0j, where j = j c, -j c or 0.

20 Superconductivity Vortex distribution in real superconductors An ideal vortex lattice yields j c = 0, R 0. j c is the critical current. Vortex pinning by material defects (pinning centers) Vortex distribution is no longer uniform j c > 0, R = 0. Bean s bulk pinning model (1962). db x dz dbz dx = µ 0j, where j = j c, -j c or 0.

21 Superconductivity Vortex distribution in real superconductors An ideal vortex lattice yields j c = 0, R 0. j c is the critical current. Vortex pinning by material defects (pinning centers) Vortex distribution is no longer uniform j c > 0, R = 0. Bean s bulk pinning model (1962). db x dz dbz dx = µ 0j, where j = j c, -j c or 0.

22 Superconductivity Vortex distribution in real superconductors An ideal vortex lattice yields j c = 0, R 0. j c is the critical current. Vortex pinning by material defects (pinning centers) Vortex distribution is no longer uniform j c > 0, R = 0. Bean s bulk pinning model (1962). db x dz dbz dx = µ 0j, where j = j c, -j c or 0.

23 Superconductivity Nonuniform vortex distribution observed by MOI: bulk pinning Magneto-optical imaging (MOI) measures the averaged flux density. Image intensity gradient j c.

24 Superconductivity Nonuniform vortex distribution observed by MOI: bulk pinning Magneto-optical imaging (MOI) measures the averaged flux density. Image intensity gradient j c.

25 Superconductivity Nonuniform vortex distribution observed by MOI: bulk pinning 10 Oe T = 11.6 K, Field increasing 100 Oe full penetration 1 mm Magneto-optical imaging (MOI) measures the averaged flux density. Image intensity gradient j c. Magneto-optical images of a NbN thin film (T c = 14 K) with a thickness of 76 nm (deposited on a 12 nm thick Pt-Co layer with Si as the substrate). Magneto-optical image of a YBa 2 Cu 4 O 8 single crystal, acquired at T = 10 K and H a = 180 Oe.

26 Superconductivity Nonuniform vortex distribution observed by MOI: bulk pinning 10 Oe T = 11.6 K, Field increasing 100 Oe full penetration 1 mm Magneto-optical imaging (MOI) measures the averaged flux density. Image intensity gradient j c. Magneto-optical images of a NbN thin film (T c = 14 K) with a thickness of 76 nm (deposited on a 12 nm thick Pt-Co layer with Si as the substrate). Magneto-optical image of a YBa 2 Cu 4 O 8 single crystal, acquired at T = 10 K and H a = 180 Oe.

27 Superconductivity Nonuniform vortex distribution observed by MOI: bulk pinning 10 Oe T = 11.6 K, Field increasing 100 Oe full penetration 1 mm Magneto-optical imaging (MOI) measures the averaged flux density. Image intensity gradient j c. Magneto-optical images of a NbN thin film (T c = 14 K) with a thickness of 76 nm (deposited on a 12 nm thick Pt-Co layer with Si as the substrate). Magneto-optical image of a YBa 2 Cu 4 O 8 single crystal, acquired at T = 10 K and H a = 180 Oe.

28 Superconductivity Nonuniform vortex distribution observed by MOI: surface barrier BSCCO Even in the absence of bulk pinning, there is still a surface barrier. Once vortices overcome the barrier, they accumulate in the center of the sample, yielding a dome profile. Weak surface pinning, strong bulk pinning Bean s profile. Strong surface pinning, weak bulk pinning Dome profile.

29 Superconductivity Nonuniform vortex distribution observed by MOI: surface barrier BSCCO Even in the absence of bulk pinning, there is still a surface barrier. Once vortices overcome the barrier, they accumulate in the center of the sample, yielding a dome profile. Weak surface pinning, strong bulk pinning Bean s profile. Strong surface pinning, weak bulk pinning Dome profile.

30 Superconductivity Nonuniform vortex distribution observed by MOI: surface barrier BSCCO Even in the absence of bulk pinning, there is still a surface barrier. Once vortices overcome the barrier, they accumulate in the center of the sample, yielding a dome profile. Weak surface pinning, strong bulk pinning Bean s profile. Strong surface pinning, weak bulk pinning Dome profile.

31 Superconductivity Nonuniform vortex distribution observed by MOI: surface barrier BSCCO Even in the absence of bulk pinning, there is still a surface barrier. Once vortices overcome the barrier, they accumulate in the center of the sample, yielding a dome profile. Weak surface pinning, strong bulk pinning Bean s profile. Strong surface pinning, weak bulk pinning Dome profile.

32 Superconductivity Nonuniform vortex distribution observed by MOI: surface barrier BSCCO Even in the absence of bulk pinning, there is still a surface barrier. Once vortices overcome the barrier, they accumulate in the center of the sample, yielding a dome profile. Weak surface pinning, strong bulk pinning Bean s profile. Strong surface pinning, weak bulk pinning Dome profile.

33 NMR Outline 1 Introduction Superconductivity Model NMR experiments Shear viscosity of the vortex liquid 2 Methods Experimental procedures Verification: bulk or surface properties? Magneto-optical imaging and transport measurements 3 Results Comparison with 2D melting model Comparison with 3D Bose-glass model 4 Discussions 5 Summary

34 NMR Influences of bulk pinning and surface barrier to other measurements Example: Nuclear Magnetic Resonance (NMR) Inhomogeneous field distribution! Questions: Is all the sample probed by NMR experiments? Supercurrent affects the density of states and thus the NMR Knight shift data. Is this influence important?

35 NMR Influences of bulk pinning and surface barrier to other measurements Example: Nuclear Magnetic Resonance (NMR) Inhomogeneous field distribution! Questions: Is all the sample probed by NMR experiments? Supercurrent affects the density of states and thus the NMR Knight shift data. Is this influence important?

36 NMR Method to obtain ac current distribution

37 NMR Method to obtain ac current distribution NMR-like field configuration 250 Oe z (axis c) x (axis b) J ac (x) y (axis a) YBa Cu O H ac H dc Differential image acquisition procedure H ac (Oe) direct images 10 direct images averaged averaged M 1 M 2 80 M 1 -M time (s)

38 NMR ac current distribution in YBa 2 Cu 4 O 8 (T c = 82 K) Three regimes negligible screening current (T > 70 K) surface barrier flow (20 K < T < 70 K) bulk pinning flow (T < 20 K)

39 NMR ac current distribution in YBa 2 Cu 4 O 8 (T c = 82 K) K 45 K 50 K 55 K K 60 K 65 K 70 K B z 0.0 B z x (mm) x (mm) Sheet current J y (x) K 45 K 50 K 55 K Sheet current J y (x) K 60 K 65 K 70 K x (mm) Three regimes negligible screening current (T > 70 K) surface barrier flow (20 K < T < 70 K) bulk pinning flow (T < 20 K) x (mm)

40 NMR Results: ac field penetration Only the regions where the ac field penetrates are probed by NMR measurements.

41 NMR Results: ac field penetration Only the regions where the ac field penetrates are probed by NMR measurements. H x /H ac 1 40 K 55 K 650 K 0 35 K T < 20 K x (mm)

42 NMR Discussions Questions: Is all the sample probed by NMR measurements? Supercurrent affects the density of states and thus the NMR Knight shift data. Is this influence important? Answers obtained from our NMR model experiment: At low temperatures (bulk pinning regime), only the sample edges are probed by NMR measurements. For certain materials whose j c is large, the supercurrent may affect the NMR Knight shift data. At intermediate temperatures (surface barrier regime), only the sample bulk is probed. There may be a tiny K s due to the current at the edges only.

43 NMR Discussions Questions: Is all the sample probed by NMR measurements? Supercurrent affects the density of states and thus the NMR Knight shift data. Is this influence important? Answers obtained from our NMR model experiment: At low temperatures (bulk pinning regime), only the sample edges are probed by NMR measurements. For certain materials whose j c is large, the supercurrent may affect the NMR Knight shift data. At intermediate temperatures (surface barrier regime), only the sample bulk is probed. There may be a tiny K s due to the current at the edges only.

44 Shear property Outline 1 Introduction Superconductivity Model NMR experiments Shear viscosity of the vortex liquid 2 Methods Experimental procedures Verification: bulk or surface properties? Magneto-optical imaging and transport measurements 3 Results Comparison with 2D melting model Comparison with 3D Bose-glass model 4 Discussions 5 Summary

45 Shear property High temperature superconductors New paradigm ( 1989): existence of a vortex liquid state.

46 Shear property High temperature superconductors H Abrikosov vortex lattice H c2 (T) normal state H c1 (T) Meissner state Conventional T c T New paradigm ( 1989): existence of a vortex liquid state.

47 Shear property High temperature superconductors H H Abrikosov vortex lattice H c1 (T) H c2 (T) Meissner state normal state Conventional T c T glass or liquid H c2 (T) Abrikosov vortex lattice Meissner state normal state High-T c (YBCO, BSCCO, ) T c T New paradigm ( 1989): existence of a vortex liquid state.

48 Shear property Vortex lattice melting in BSCCO vortex lattice melting: jump in vortex density. R 0. However, pinning centers do not disappear! Why R 0 at the vortex liquid-lattice transition?

49 Shear property Vortex lattice melting in BSCCO vortex lattice melting: jump in vortex density. R 0. However, pinning centers do not disappear! Why R 0 at the vortex liquid-lattice transition?

50 Shear property Vortex lattice melting in BSCCO vortex lattice melting: jump in vortex density. R 0. However, pinning centers do not disappear! Why R 0 at the vortex liquid-lattice transition?

51 Shear property Vortex lattice melting in BSCCO vortex lattice melting: jump in vortex density. R 0. However, pinning centers do not disappear! Why R 0 at the vortex liquid-lattice transition?

52 Shear property Resistance appears at vortex lattice melting Answer: In 2D: by the appearance of free vortex lattice dislocations. Resistance is related to the free dislocation density (Nelson-Halperin theory). In 3D: unclear. Is plastic motion of vortex lines important? Measure the vortex shear properties.

53 Shear property Resistance appears at vortex lattice melting Answer: In 2D: by the appearance of free vortex lattice dislocations. Resistance is related to the free dislocation density (Nelson-Halperin theory). In 3D: unclear. Is plastic motion of vortex lines important? Measure the vortex shear properties.

54 Shear property Resistance appears at vortex lattice melting Answer: In 2D: by the appearance of free vortex lattice dislocations. Resistance is related to the free dislocation density (Nelson-Halperin theory). In 3D: unclear. Is plastic motion of vortex lines important? Measure the vortex shear properties.

55 Shear property Resistance appears at vortex lattice melting Answer: In 2D: by the appearance of free vortex lattice dislocations. Resistance is related to the free dislocation density (Nelson-Halperin theory). In 3D: unclear. Is plastic motion of vortex lines important? Measure the vortex shear properties.

56 Shear property How to measure the shear viscosity? Method Introduce artificial shear flow in weak pinning channel between strong pinning walls. Result ρ = ρ f [1 2δ L tanh( L 2δ )] when δ(t) η/γ >> L, one has: Hydrodynamic description γv + η 2 v + f = 0 Relation between shear viscosity and resistivity: ρ(t) B 2 L2 η(t)

57 Shear property How to measure the shear viscosity? Method Introduce artificial shear flow in weak pinning channel between strong pinning walls. y Result ρ = ρ f [1 2δ L tanh( L 2δ )] x Hydrodynamic description γv + η 2 v + f = 0 when δ(t) η/γ >> L, one has: Relation between shear viscosity and resistivity: ρ(t) B 2 L2 η(t)

58 Shear property How to measure the shear viscosity? Method Introduce artificial shear flow in weak pinning channel between strong pinning walls. y Result ρ = ρ f [1 2δ L tanh( L 2δ )] x Hydrodynamic description γv + η 2 v + f = 0 when δ(t) η/γ >> L, one has: Relation between shear viscosity and resistivity: ρ(t) B 2 L2 η(t)

59 Shear property How to measure the shear viscosity? Method Introduce artificial shear flow in weak pinning channel between strong pinning walls. y Result ρ = ρ f [1 2δ L tanh( L 2δ )] x Hydrodynamic description γv + η 2 v + f = 0 when δ(t) η/γ >> L, one has: Relation between shear viscosity and resistivity: ρ(t) B 2 L2 η(t)

60 Shear property Previous work H. Pastoriza and P. H. Kes, Phys. Rev. Lett. 75, 3525 (1995) Interpretation c 66 = 0 in the vortex liquid state while c 66 > 0 in the vortex solid state (c 66 : shear modulus). But surface barrier problem...

61 Shear property Previous work H. Pastoriza and P. H. Kes, Phys. Rev. Lett. 75, 3525 (1995) Interpretation c 66 = 0 in the vortex liquid state while c 66 > 0 in the vortex solid state (c 66 : shear modulus). But surface barrier problem...

62 Shear property Previous work H. Pastoriza and P. H. Kes, Phys. Rev. Lett. 75, 3525 (1995) Interpretation c 66 = 0 in the vortex liquid state while c 66 > 0 in the vortex solid state (c 66 : shear modulus). But surface barrier problem...

63 Shear property Previous work H. Pastoriza and P. H. Kes, Phys. Rev. Lett. 75, 3525 (1995) Interpretation c 66 = 0 in the vortex liquid state while c 66 > 0 in the vortex solid state (c 66 : shear modulus). But surface barrier problem...

64 Shear property Signature of surface barrier in transport D. T. Fuchs et al., Phys. Rev. Lett. 81, 3944 (1998) Signature of surface barrier Nonlinear resistance in the liquid vortex state. Normalized R(T) of the square and strip crystal in the vicinity of the first order transition at H //c = 300 Oe and with 10 ma current. Measurements performed on Bi 2 Sr 2 CaCu 2 O 8 single crystals.

65 Shear property Signature of surface barrier in transport D. T. Fuchs et al., Phys. Rev. Lett. 81, 3944 (1998) Signature of surface barrier Nonlinear resistance in the liquid vortex state. Normalized R(T) of the square and strip crystal in the vicinity of the first order transition at H //c = 300 Oe and with 10 ma current. Measurements performed on Bi 2 Sr 2 CaCu 2 O 8 single crystals.

66 Shear property Signature of surface barrier in transport D. T. Fuchs et al., Phys. Rev. Lett. 81, 3944 (1998) Signature of surface barrier Nonlinear resistance in the liquid vortex state. Normalized R(T) of the square and strip crystal in the vicinity of the first order transition at H //c = 300 Oe and with 10 ma current. Measurements performed on Bi 2 Sr 2 CaCu 2 O 8 single crystals.

67 Shear property Signature of surface barrier in transport D. T. Fuchs et al., Phys. Rev. Lett. 81, 3944 (1998) Signature of surface barrier Nonlinear resistance in the liquid vortex state. Normalized R(T) of the square and strip crystal in the vicinity of the first order transition at H //c = 300 Oe and with 10 ma current. Measurements performed on Bi 2 Sr 2 CaCu 2 O 8 single crystals.

68 Shear property Our approach Objective Bulk viscosity measurements without surface barrier. Method Contacts and channel structure are remote from the sample edges. Furthermore, the contacts are heavily irradiated in order to attract the current.

69 Shear property Our approach Objective Bulk viscosity measurements without surface barrier. Method Contacts and channel structure are remote from the sample edges. Furthermore, the contacts are heavily irradiated in order to attract the current.

70 Shear property Our approach Objective Bulk viscosity measurements without surface barrier. Method Contacts and channel structure are remote from the sample edges. Furthermore, the contacts are heavily irradiated in order to attract the current.

71 Sample preparation Outline 1 Introduction Superconductivity Model NMR experiments Shear viscosity of the vortex liquid 2 Methods Experimental procedures Verification: bulk or surface properties? Magneto-optical imaging and transport measurements 3 Results Comparison with 2D melting model Comparison with 3D Bose-glass model 4 Discussions 5 Summary

72 Sample preparation Experimental procedures Selection of BSCCO single crystals Realization of channel structure through irradiation Realization of electrical contacts for transport measurements

73 Sample preparation Selection of BSCCO single crystals The channels (weak pinning) should not contain any macroscopic defects. Necessary to select macroscopic defect-free single crystals.

74 Sample preparation Realization of channel structure through irradiation (GANIL) Selective irradiation through nickel masks Thickness of a nickel mask is 6 10 µm. 4 to 5 masks were superposed to block the Pb 56+ ion beam of 1 GeV. Definition of matching field B φ B φ n d φ 0, where n d is the density of columnar defects introduced by ion irradiation.

75 Sample preparation Realization of channel structure through irradiation (GANIL) Selective irradiation through nickel masks Thickness of a nickel mask is 6 10 µm. 4 to 5 masks were superposed to block the Pb 56+ ion beam of 1 GeV. Definition of matching field B φ B φ n d φ 0, where n d is the density of columnar defects introduced by ion irradiation.

76 Sample preparation Realization of channel structure through irradiation (GANIL) Selective irradiation through nickel masks Thickness of a nickel mask is 6 10 µm. 4 to 5 masks were superposed to block the Pb 56+ ion beam of 1 GeV. Definition of matching field B φ B φ n d φ 0, where n d is the density of columnar defects introduced by ion irradiation.

77 Sample preparation Realization of channel structure through irradiation (GANIL) Selective irradiation through nickel masks Thickness of a nickel mask is 6 10 µm. 4 to 5 masks were superposed to block the Pb 56+ ion beam of 1 GeV. Definition of matching field B φ B φ n d φ 0, where n d is the density of columnar defects introduced by ion irradiation.

78 Sample preparation Realization of electrical contacts Plasma etching Photolithography

79 bulk pinning vs. surface pinning Outline 1 Introduction Superconductivity Model NMR experiments Shear viscosity of the vortex liquid 2 Methods Experimental procedures Verification: bulk or surface properties? Magneto-optical imaging and transport measurements 3 Results Comparison with 2D melting model Comparison with 3D Bose-glass model 4 Discussions 5 Summary

80 bulk pinning vs. surface pinning Verification: bulk or surface properties? Mapping of critical current. Current path imaging. Transport measurements.

81 bulk pinning vs. surface pinning Verification: bulk or surface properties? Mapping of critical current. Current path imaging. Transport measurements.

82 Introduction Methods Results Discussions Summary bulk pinning vs. surface pinning Experimental results: MOI Mapping of critical current Field modulated MOI acquired at T = 80.5 K with field modulation of 0.5 Oe, base field = 25 Oe, on BSCCO crystal "iv" (clean 20 µm wide channels). Current path imaging Current modulated differential image acquired at T = 68 K, H//c = 100 Oe, with I = +30 ma, -30 ma, on BSCCO crystal "24-4" (channels + low density of columnar defects (Bφ = 10 G) in the channels).

83 Introduction Methods Results Discussions Summary bulk pinning vs. surface pinning Experimental results: MOI Mapping of critical current Field modulated MOI acquired at T = 80.5 K with field modulation of 0.5 Oe, base field = 25 Oe, on BSCCO crystal "iv" (clean 20 µm wide channels). Current path imaging Current modulated differential image acquired at T = 68 K, H//c = 100 Oe, with I = +30 ma, -30 ma, on BSCCO crystal "24-4" (channels + low density of columnar defects (Bφ = 10 G) in the channels).

84 bulk pinning vs. surface pinning Experimental results: transport measurements R ( Ω ) Present work H //c = 116 Oe BSCCO "iv" 1 ma 4 ma 8 ma T irr CD µm wide channels only (no columnar defects in the channels) T (K) Bulk flow. Signature of shear flow.

85 bulk pinning vs. surface pinning Experimental results: transport measurements R ( Ω ) Present work H //c = 116 Oe BSCCO "iv" 1 ma 4 ma 8 ma T irr CD µm wide channels only (no columnar defects in the channels) T (K) Bulk flow. Signature of shear flow.

86 bulk pinning vs. surface pinning Experimental results: transport measurements R ( Ω ) Present work H //c = 116 Oe BSCCO "iv" 1 ma 4 ma 8 ma T irr CD µm wide channels only (no columnar defects in the channels) T (K) Bulk flow. Signature of shear flow.

87 bulk pinning vs. surface pinning Experimental results: transport measurements R ( Ω ) Present work H //c = 116 Oe BSCCO "iv" 1 ma 4 ma 8 ma T irr CD µm wide channels only (no columnar defects in the channels) T (K) Bulk flow. Signature of shear flow.

88 bulk pinning vs. surface pinning Summary: bulk pinning vs. surface pinning Experimental facts Field modulated differential magneto-optical imaging j c,walls > j surface. Current path imaging current flows through the irradiated structure. Transport measurements: no nonlinear resistance no surface barrier effect in liquid vortex state. Therefore we probe the bulk.

89 bulk pinning vs. surface pinning Summary: bulk pinning vs. surface pinning Experimental facts Field modulated differential magneto-optical imaging j c,walls > j surface. Current path imaging current flows through the irradiated structure. Transport measurements: no nonlinear resistance no surface barrier effect in liquid vortex state. Therefore we probe the bulk.

90 Magneto-optical imaging and transport measurements Outline 1 Introduction Superconductivity Model NMR experiments Shear viscosity of the vortex liquid 2 Methods Experimental procedures Verification: bulk or surface properties? Magneto-optical imaging and transport measurements 3 Results Comparison with 2D melting model Comparison with 3D Bose-glass model 4 Discussions 5 Summary

91 Magneto-optical imaging and transport measurements Signature of shear flow in transport measurements R ( Ω ) Oe BSCCO "iv" 20 µm wide channels only 155 Oe (no columnar defects in the channels) 116 Oe 77 Oe 56 Oe 35 Oe 16 Oe 11 Oe zero-field T irr CD T T irr CD T (K)

92 Magneto-optical imaging and transport measurements Characteristic fields and temperatures H (Oe) shear flow 3 surface pinning effective region homogenous liquid vortex region T (K) 2 1 Only regions 1 and 2 are probed by resistance measurements. Bulk properties of vortex system are probed by resistance measurements.

93 Comparison with 2D melting model Outline 1 Introduction Superconductivity Model NMR experiments Shear viscosity of the vortex liquid 2 Methods Experimental procedures Verification: bulk or surface properties? Magneto-optical imaging and transport measurements 3 Results Comparison with 2D melting model Comparison with 3D Bose-glass model 4 Discussions 5 Summary

94 Comparison with 2D melting model D = 2: Nelson-Halperin model scaling law of resistivity ρ(t) C 1 exp[ 2C 2 ( Tm T T m ) 0.37 ], where C 1 ρ flux flow, C 2 1, and T m is the melting (freezing) temperature. Remarkably, R(T) of our 3D superconductor is well fitted with 2D scaling law...

95 Comparison with 2D melting model D = 2: Nelson-Halperin model 10 0 R ( Ω ) Fit with NH model: R = C 1 exp ( - 2 C 2 T m /(T-T m ) 0.37 ), C 2 = Oe 155 Oe 116 Oe 77 Oe 56 Oe 35 Oe 16 Oe 11 Oe Zero-field scaling law of resistivity ρ(t) C 1 exp[ 2C 2 ( Tm T T m ) 0.37 ], where C 1 ρ flux flow, C 2 1, and T m is the melting (freezing) temperature BSCCO "iv" T (K) Remarkably, R(T) of our 3D superconductor is well fitted with 2D scaling law...

96 Comparison with 2D melting model D = 2: Nelson-Halperin model 10 0 R ( Ω ) Fit with NH model: R = C 1 exp ( - 2 C 2 T m /(T-T m ) 0.37 ), C 2 = Oe 155 Oe 116 Oe 77 Oe 56 Oe 35 Oe 16 Oe 11 Oe Zero-field scaling law of resistivity ρ(t) C 1 exp[ 2C 2 ( Tm T T m ) 0.37 ], where C 1 ρ flux flow, C 2 1, and T m is the melting (freezing) temperature BSCCO "iv" T (K) Remarkably, R(T) of our 3D superconductor is well fitted with 2D scaling law...

97 Comparison with 2D melting model I-V characterization 2D Nelson-Halperin melting property Power law: V = I a, where the exponent a has a universal jump from 1 to 3 at T = T m (characteristic of 2D melting). This jump is observed! Measurements performed on a Bi 2 Sr 2 CaCu 2 O 8 single crystal, containing clean 20 µm wide channels.

98 Comparison with 2D melting model I-V characterization a (critical-exponent) Log 10 V (µv) K K K K K K K K K a (critical-exponent), V = I a. Temperature increasing Log 10 I (µa) BSCCO "iv" H // c = 35 Oe T (K) 2D Nelson-Halperin melting property Power law: V = I a, where the exponent a has a universal jump from 1 to 3 at T = T m (characteristic of 2D melting). This jump is observed! Measurements performed on a Bi 2 Sr 2 CaCu 2 O 8 single crystal, containing clean 20 µm wide channels.

99 Comparison with 2D melting model Possible explanations Current flows only at the top layer. (B. Khaykovich et al., Phys. Rev. B 61, R9261 (2000)) A dimension cross-over takes place nearly simultaneously with the liquid (2D) - solid (3D) transition. Suggestion Multi-terminal transport measurements with electrical contacts on both the top and bottom surfaces. Layered structure of Bi 2 Sr 2 CaCu 2 O 8

100 Comparison with 2D melting model Possible explanations Current flows only at the top layer. (B. Khaykovich et al., Phys. Rev. B 61, R9261 (2000)) A dimension cross-over takes place nearly simultaneously with the liquid (2D) - solid (3D) transition. Suggestion Multi-terminal transport measurements with electrical contacts on both the top and bottom surfaces. Layered structure of Bi 2 Sr 2 CaCu 2 O 8

101 Comparison with 3D Bose-glass model Outline 1 Introduction Superconductivity Model NMR experiments Shear viscosity of the vortex liquid 2 Methods Experimental procedures Verification: bulk or surface properties? Magneto-optical imaging and transport measurements 3 Results Comparison with 2D melting model Comparison with 3D Bose-glass model 4 Discussions 5 Summary

102 Comparison with 3D Bose-glass model D = 3 with columnar defects: Bose-glass model Marchetti and Nelson s proposal Introduce a low density of columnar defects in the channels. A Bose liquid state should be realized in the channels. Prediction Vortex liquid to Bose-glass transition at T BG. Near T BG, ρ(t) L 2 T T BG v z for channel confined vortices. v is the static critical exponent, z is the dynamic critical exponent. Simulations: v 1,z 4.6. Reference: non-confined Bose-liquid Near T BG, ρ(t) T T BG v (z 2)

103 Comparison with 3D Bose-glass model D = 3 with columnar defects: Bose-glass model Marchetti and Nelson s proposal Introduce a low density of columnar defects in the channels. A Bose liquid state should be realized in the channels. Prediction Vortex liquid to Bose-glass transition at T BG. Near T BG, ρ(t) L 2 T T BG v z for channel confined vortices. v is the static critical exponent, z is the dynamic critical exponent. Simulations: v 1,z 4.6. Reference: non-confined Bose-liquid Near T BG, ρ(t) T T BG v (z 2)

104 Comparison with 3D Bose-glass model D = 3 with columnar defects: Bose-glass model Marchetti and Nelson s proposal Introduce a low density of columnar defects in the channels. A Bose liquid state should be realized in the channels. Prediction Vortex liquid to Bose-glass transition at T BG. Near T BG, ρ(t) L 2 T T BG v z for channel confined vortices. v is the static critical exponent, z is the dynamic critical exponent. Simulations: v 1,z 4.6. Reference: non-confined Bose-liquid Near T BG, ρ(t) T T BG v (z 2)

105 Comparison with 3D Bose-glass model Experimental data vs. 3D Bose-glass model R ( Ω ) Fit with Bose-glass model: R = C(T-T BG ) s, s = Oe 116 Oe 77 Oe 35 Oe Zero-field R ( Ω ) Fit with Bose-glass model: R = C(T-T BG ) s 310 Oe 155 Oe 116 Oe 77 Oe 56 Oe BSCCO "24-4" T (K) BSCCO "24-4", containing low density columnar defects (B φ = 10 G) in the 20 µm wide channels. s = BSCCO "10G" T ( K ) BSCCO "10G", uniformly irradiated with a dose of B φ = 10 G. 1.2 < s < 1.8 we find: s = H.

106 Comparison of different types of confinement µ! "!# µ $ % ' (!)*)!# φ & +, - % ' (,,.,/!' (!# φ & 0 % / # H // c = 116 Oe R ( Ω ) µm T / T c Degree of confinement comparison: 20 µm wide channels + B φ = 10 G B φ = 10 G > 20 µm wide clean channels > pristine.

107 Confinement realized in a uniformly irradiated sample Magnetic decoration with B = 8B φ, B φ = 10 G. From: M. Menghini et al., PRL 90, (2003)

108 Summary Bulk vortex properties have been successfully probed. Both of the 2D and 3D models fit with the experimental resistance data approaching zero-resistance. Why? ρ c 0. Surface barrier contribution when it becomes effective. Defects in 3D vortex lattice yield similar contribution to ρ(t) as defects in 2D vortex lattice. Defects in vortex lattice in layered BSCCO resemble 2D defects (i.e., pancake vortices). Field modulated differential magneto-optical imaging can serve as a tool for estimating transport current flow distribution prior to the transport measurements. Outlook Varying channel width: size effect. Establishing electrical contacts on both the top and bottom surfaces: c-axis correlation.

109 Acknowledgment Kees van der Beek Marcin Konczykowski Rozenn Bernard Javier Briatico Panayotis Spathis Tatiana Taurines... Thank you for your attention!