Quantum theory of vortices in d-wave superconductors

Transcription

1 Quantum theory of vortices in d-wave superconductors Physical Review B 71, and (2005), Annals of Physics 321, 1528 (2006), Physical Review B 73, (2006), cond-mat/ Leon Balents (UCSB) Lorenz Bartosch (Harvard) Anton Burkov (Harvard) Predrag Nikolic (Harvard) Subir Sachdev (Harvard) Krishnendu Sengupta (HRI, India) Talk online at

2 BCS theory of vortices in d-wave superconductors + periodic potential + strong Coulomb interactions Vortices in BCS superconductors near a superconductor-mott insulator transition at finite doping

3 The cuprate superconductor Ca 2-x Na x CuO 2 Cl 2 T. Hanaguri, C. Lupien, Y. Kohsaka, D.-H. Lee, M. Azuma, M. Takano, H. Takagi, and J. C. Davis, Nature 430, 1001 (2004). Closely related modulations in superconducting Bi 2 Sr 2 CaCu 2 O 8+δ observed first by C. Howald, H. Eisaki, N. Kaneko, and A. Kapitulnik, cond-mat/ and Physical Review B 67, (2003).

4 The cuprate superconductor Ca 2-x Na x CuO 2 Cl 2 Evidence that holes can form an insulating state with period 4 modulation in the density T. Hanaguri, C. Lupien, Y. Kohsaka, D.-H. Lee, M. Azuma, M. Takano, H. Takagi, and J. C. Davis, Nature 430, 1001 (2004). Closely related modulations in superconducting Bi 2 Sr 2 CaCu 2 O 8+δ observed first by C. Howald, H. Eisaki, N. Kaneko, and A. Kapitulnik, cond-mat/ and Physical Review B 67, (2003).

5 STM around vortices induced by a magnetic field in the superconducting state J. E. Hoffman, E. W. Hudson, K. M. Lang, V. Madhavan, S. H. Pan, H. Eisaki, S. Uchida, and J. C. Davis, Science 295, 466 (2002). Differential Conductance (ns) Local density of states (LDOS) Regular QPSR Vortex 1Å spatial resolution image of integrated LDOS of Bi 2 Sr 2 CaCu 2 O 8+δ ( 1meV to 12 mev) at B=5 Tesla Sample Bias (mv) I. Maggio-Aprile et al. Phys. Rev. Lett. 75, 2754 (1995). S.H. Pan et al. Phys. Rev. Lett. 85, 1536 (2000).

6 Vortex-induced LDOS of Bi 2 Sr 2 CaCu 2 O 8+δ integrated from 1meV to 12meV at 4K 7 pa 0 pa b Vortices have halos with LDOS modulations at a period 4 lattice spacings 100Å J. Hoffman et al., Science 295, 466 (2002). G. Levy et al., Phys. Rev. Lett. 95, (2005). Prediction of periodic LDOS modulations near vortices: K. Park and S. Sachdev, Phys. Rev. B 64, (2001).

7 Questions on the cuprate superconductors What is the quantum theory of the ground state as it evolves from the superconductor to the modulated insulator? What happens to the vortices near such a quantum transition?

8 Outline The superfluid-insulator transition of bosons The quantum mechanics of vortices near the superfluidinsulator transition Dual theory of superfluid-insulator transition as the proliferation of vortex-anti-vortex pairs Influence of nodal quasiparticles on vortex dynamics in a d-wave superconductor

9 I. The superfluid-insulator transition of bosons

10 Bosons at filling fraction f = 1 Weak interactions: superfluidity Strong interactions: Mott insulator which preserves all lattice symmetries M. Greiner, O. Mandel, T. Esslinger, T. W. Hänsch, and I. Bloch, Nature 415, 39 (2002).

11 Bosons at filling fraction f = 1 Ψ 0 Weak interactions: superfluidity

12 Bosons at filling fraction f = 1 Ψ 0 Weak interactions: superfluidity

13 Bosons at filling fraction f = 1 Ψ 0 Weak interactions: superfluidity

14 Bosons at filling fraction f = 1 Ψ 0 Weak interactions: superfluidity

15 Bosons at filling fraction f = 1 Ψ = 0 Strong interactions: insulator

16 Bosons at filling fraction f = 1/2 or S=1/2 XXZ model Ψ 0 Weak interactions: superfluidity

17 Bosons at filling fraction f = 1/2 or S=1/2 XXZ model Ψ 0 Weak interactions: superfluidity

18 Bosons at filling fraction f = 1/2 or S=1/2 XXZ model Ψ 0 Weak interactions: superfluidity

19 Bosons at filling fraction f = 1/2 or S=1/2 XXZ model Ψ 0 Weak interactions: superfluidity

20 Bosons at filling fraction f = 1/2 or S=1/2 XXZ model Ψ 0 Weak interactions: superfluidity

21 Bosons at filling fraction f = 1/2 or S=1/2 XXZ model Ψ = 0 Strong interactions: insulator

22 Bosons at filling fraction f = 1/2 or S=1/2 XXZ model Ψ = 0 Strong interactions: insulator

23 Bosons at filling fraction f = 1/2 or S=1/2 XXZ model Ψ = 0 Strong interactions: insulator Insulator has density wave order

24 Bosons at filling fraction f = 1/2 or S=1/2 XXZ model? Superfluid Insulator Charge density wave (CDW) order Interactions between bosons

25 Bosons at filling fraction f = 1/2 or S=1/2 XXZ model? Superfluid Insulator Charge density wave (CDW) order Interactions between bosons

26 Bosons at filling fraction f = 1/2 or S=1/2 XXZ model = 1 2 ( + )? Superfluid Insulator Valence bond solid (VBS) order Interactions between bosons N. Read and S. Sachdev, Phys. Rev. Lett. 62, 1694 (1989).

27 Bosons at filling fraction f = 1/2 or S=1/2 XXZ model 12 ( = + )? Superfluid Insulator Valence bond solid (VBS) order Interactions between bosons N. Read and S. Sachdev, Phys. Rev. Lett. 62, 1694 (1989).

28 Bosons at filling fraction f = 1/2 or S=1/2 XXZ model 12 ( = + )? Superfluid Insulator Valence bond solid (VBS) order Interactions between bosons N. Read and S. Sachdev, Phys. Rev. Lett. 62, 1694 (1989).

29 Bosons at filling fraction f = 1/2 or S=1/2 XXZ model 12 ( = + )? Superfluid Insulator Valence bond solid (VBS) order Interactions between bosons N. Read and S. Sachdev, Phys. Rev. Lett. 62, 1694 (1989).

30 The superfluid-insulator quantum phase transition Key difficulty: Multiple order parameters (Bose- Einstein condensate, charge density wave, valencebond-solid order ) not related by symmetry, but clearly physically connected. Standard methods only predict strong first order transitions (for generic parameters).

31 The superfluid-insulator quantum phase transition Key difficulty: Multiple order parameters (Bose- Einstein condensate, charge density wave, valencebond-solid order ) not related by symmetry, but clearly physically connected. Standard methods only predict strong first order transitions (for generic parameters). Key theoretical tool: Quantum theory of vortices

32 Outline The superfluid-insulator transition of bosons The quantum mechanics of vortices near the superfluidinsulator transition Dual theory of superfluid-insulator transition as the proliferation of vortex-anti-vortex pairs Influence of nodal quasiparticles on vortex dynamics in a d-wave superconductor

33 II. The quantum mechanics of vortices near a superfluid-insulator transition Dual theory of the superfluid-insulator transition as the proliferation of vortex-anti-vortex-pairs

34 Excitations of the superfluid: Vortices and anti-vortices Central question: In two dimensions, we can view the vortices as point particle excitations of the superfluid. What is the quantum mechanics of these particles?

35 In ordinary fluids, vortices experience the Magnus Force F M F = mass density of air i velocity of ball i circulation M ( ) ( ) ( )

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37 Dual picture: The vortex is a quantum particle with dual electric charge n, moving in a dual magnetic field of strength = h (number density of Bose particles) C. Dasgupta and B.I. Halperin, Phys. Rev. Lett. 47, 1556 (1981); D.R. Nelson, Phys. Rev. Lett. 60, 1973 (1988); M.P.A. Fisher and D.-H. Lee, Phys. Rev. B 39, 2756 (1989)

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40 Bosons on the square lattice at filling fraction f=p/q

41 Bosons on the square lattice at filling fraction f=p/q

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48 Vortex theory of the superfluid-insulator transition As a superfluid approaches an insulating state, the decrease in the strength of the condensate will lower the energy cost of creating vortex-antivortex pairs.

49 Vortex theory of the superfluid-insulator transition Proliferation of vortex-anti-vortex pairs.

50 Vortex theory of the superfluid-insulator transition Proliferation of vortex-anti-vortex pairs.

51 Vortex theory of the superfluid-insulator transition Proliferation of vortex-anti-vortex pairs.

52 N. Read and S. Sachdev, Phys. Rev. Lett. 62, 1694 (1989). C. Lannert, M.P.A. Fisher, and T. Senthil, Phys. Rev. B 63, (2001) S. Sachdev and K. Park, Annals of Physics, 298, 58 (2002) T. Senthil, A. Vishwanath, L. Balents, S. Sachdev and M.P.A. Fisher, Science 303, 1490 (2004).

53 N. Read and S. Sachdev, Phys. Rev. Lett. 62, 1694 (1989). C. Lannert, M.P.A. Fisher, and T. Senthil, Phys. Rev. B 63, (2001) S. Sachdev and K. Park, Annals of Physics, 298, 58 (2002) T. Senthil, A. Vishwanath, L. Balents, S. Sachdev and M.P.A. Fisher, Science 303, 1490 (2004).

54 Vortex-induced LDOS of Bi 2 Sr 2 CaCu 2 O 8+δ integrated from 1meV to 12meV at 4K 7 pa 0 pa b Vortices have halos with LDOS modulations at a period 4 lattice spacings 100Å J. Hoffman et al., Science 295, 466 (2002). G. Levy et al., Phys. Rev. Lett. 95, (2005). Prediction of periodic LDOS modulations near vortices: K. Park and S. Sachdev, Phys. Rev. B 64, (2001).

55 Outline The superfluid-insulator transition of bosons The quantum mechanics of vortices near the superfluidinsulator transition Dual theory of superfluid-insulator transition as the proliferation of vortex-anti-vortex pairs Influence of nodal quasiparticles on vortex dynamics in a d-wave superconductor

56 III. Influence of nodal quasiparticles on vortex dynamics in a d-wave superconductor P. Nikolic

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59 A finite effective mass m v ~ Λ v where Λ~ Δ is a high energy cutoff 2 F

60 C 1 sub-ohmic damping with 2 v = v F Universal function of Δ v F

61 C Bardeen-Stephen viscous drag with 2 2 v = v F Universal function of Δ v F

62 C Bardeen-Stephen viscous drag with 2 2 v = v F Universal function of Δ v F Effect of nodal quasiparticles on vortex dynamics is relatively innocuous.

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64 Influence of the quantum oscillating vortex on the LDOS Resonant feature near the vortex oscillation frequency P. Nikolic, S. Sachdev, and L. Bartosch, cond-mat/

65 Influence of the quantum oscillating vortex on the LDOS Resonant feature near the vortex oscillation frequency P. Nikolic, S. Sachdev, and L. Bartosch, cond-mat/ Differential Conductance (ns) Regular QPSR Vortex Sample Bias (mv) I. Maggio-Aprile et al. Phys. Rev. Lett. 75, 2754 (1995) S.H. Pan et al. Phys. Rev. Lett. 85, 1536 (2000).

66 Conclusions Evidence that that vortices in in the the cuprate superconductors carry a flavor index which encodes the the spatial modulations of of a proximate insulator. Quantum zero zero point motion of of the the vortex provides a natural explanation for for LDOS modulations observed in in STM experiments. Size Size of of modulation halo halo allows estimate of of the the inertial mass of of a vortex Direct detection of of vortex zero-point motion may may be be possible in in inelastic neutron or or light-scattering experiments The The quantum zero-point motion of of the the vortices influences the the spectrum of of the the electronic quasiparticles, in in a manner consistent with with LDOS spectrum Aharanov-Bohm or or Berry phases lead lead to to surprising kinematic duality relations between seemingly distinct orders. These phase factors allow for for continuous quantum phase transitions in in situations where such transitions are are forbidden by by Landau-Ginzburg-Wilson theory.