Electronic Liquid Crystal Phases in Strongly Correlated Systems

Transcription

1 Electronic Liquid Crystal Phases in Strongly Correlated Systems Eduardo Fradkin University of Illinois at Urbana-Champaign Talk at the workshop Materials and the Imagination, Aspen Center of Physics, January 4-8, 2011

2 Collaborators S. Kivelson, V. Emery, E. Berg, D. Barci, E.-A. Kim, M. Lawler, T. Lubensky, V. Oganesyan, K. Sun, C. Wu, S. C. Zhang, J. Eisenstein, A. Kapitulnik, A. Mackenzie, J. Tranquada S. Kivelson, E. Fradkin and V. J. Emery, Electronic Liquid Crystal Phases of a Doped Mott Insulator, Nature 393, 550 (1998) S. Kivelson, I. Bindloss, E. Fradkin, V. Oganesyan, J. Tranquada, A. Kapitulnik and C.Howald, How to detect fluctuating stripes in high tempertature superconductors, Rev. Mod. Phys. 75, 1201 (2003) E. Fradkin, S. Kivelson, M. Lawler, J. Eisenstein, and A. Mackenzie, Nematic Fermi Fluids in Condensed Matter Physics, Annu. Rev. Condens. Matter Phys. 1, 153 (2010) E. Berg, E. Fradkin, S. Kivelson, and J. Tranquada, Striped Superconductors: How the cuprates intertwine spin, charge, and superconducting orders, New. J. Phys. 11, (2009). E. Berg, E. Fradkin, and S. Kivelson, Charge 4e superconductivity from pair density wave order in certain high temperature superconductors, Nature Physics 5, 830 (2009). D. Barci and E. Fradkin, Phase Transitions in Superconducting Liquid Crystal Phases, arxiv:

3 Electronic Liquid Crystal phases in doped Mott insulators

4 Electronic Liquid Crystal phases in doped Mott insulators Doping a Mott insulator leads to a system with a tendency to phase separation frustrated by strong correlations

5 Electronic Liquid Crystal phases in doped Mott insulators Doping a Mott insulator leads to a system with a tendency to phase separation frustrated by strong correlations The result are electronic liquid crystal phases: crystals, stripes (smectic), nematic and fluids, with different degrees of breakdown of translation and rotational symmetry

6 Electronic Liquid Crystal phases in doped Mott insulators Doping a Mott insulator leads to a system with a tendency to phase separation frustrated by strong correlations The result are electronic liquid crystal phases: crystals, stripes (smectic), nematic and fluids, with different degrees of breakdown of translation and rotational symmetry In lattice systems these symmetries are discrete

7 Electronic Liquid Crystal phases in doped Mott insulators Doping a Mott insulator leads to a system with a tendency to phase separation frustrated by strong correlations The result are electronic liquid crystal phases: crystals, stripes (smectic), nematic and fluids, with different degrees of breakdown of translation and rotational symmetry In lattice systems these symmetries are discrete Examples: stripe phases in HTSC, nematic phase of the 2DEG in magnetic fields, in YBCO and BSCCO, and in iron pnictides and heavy fermions.

8 Electronic Liquid Crystal phases in doped Mott insulators Doping a Mott insulator leads to a system with a tendency to phase separation frustrated by strong correlations The result are electronic liquid crystal phases: crystals, stripes (smectic), nematic and fluids, with different degrees of breakdown of translation and rotational symmetry In lattice systems these symmetries are discrete Examples: stripe phases in HTSC, nematic phase of the 2DEG in magnetic fields, in YBCO and BSCCO, and in iron pnictides and heavy fermions. In addition to their charge and spin orders, these phases may also be superconducting

9 How Liquid Crystals got an ~ or Soft Quantum Matter

10 Conducting Liquid Crystal Phases and HTSC

11 Conducting Liquid Crystal Phases and HTSC Stripes: unidirectional charge ordered states

12 Conducting Liquid Crystal Phases and HTSC Stripes: unidirectional charge ordered states Nematic: a uniform metallic (or superconducting) state with anisotropic transport

13 Conducting Liquid Crystal Phases and HTSC Stripes: unidirectional charge ordered states Nematic: a uniform metallic (or superconducting) state with anisotropic transport Stripe and nematic ordered states in HTSC: static stripes in LBCO and LNSCO x~1/8, in LSCO and YBCO in magnetic fields. Nematic order in the pseudogap regime of YBCO: INS ~6.45 and anisotropy in Nernst measurements

14 Conducting Liquid Crystal Phases and HTSC Stripes: unidirectional charge ordered states Nematic: a uniform metallic (or superconducting) state with anisotropic transport Stripe and nematic ordered states in HTSC: static stripes in LBCO and LNSCO x~1/8, in LSCO and YBCO in magnetic fields. Nematic order in the pseudogap regime of YBCO: INS ~6.45 and anisotropy in Nernst measurements Fluctuating stripes, in superconducting LSCO, LBCO away from 1/8, and underdoped YBCO

15 Conducting Liquid Crystal Phases and HTSC Stripes: unidirectional charge ordered states Nematic: a uniform metallic (or superconducting) state with anisotropic transport Stripe and nematic ordered states in HTSC: static stripes in LBCO and LNSCO x~1/8, in LSCO and YBCO in magnetic fields. Nematic order in the pseudogap regime of YBCO: INS ~6.45 and anisotropy in Nernst measurements Fluctuating stripes, in superconducting LSCO, LBCO away from 1/8, and underdoped YBCO The high energy electronic states seen in BSCCO by STM/STS have local nematic order

16 Conducting Liquid Crystal Phases and HTSC Stripes: unidirectional charge ordered states Nematic: a uniform metallic (or superconducting) state with anisotropic transport Stripe and nematic ordered states in HTSC: static stripes in LBCO and LNSCO x~1/8, in LSCO and YBCO in magnetic fields. Nematic order in the pseudogap regime of YBCO: INS ~6.45 and anisotropy in Nernst measurements Fluctuating stripes, in superconducting LSCO, LBCO away from 1/8, and underdoped YBCO The high energy electronic states seen in BSCCO by STM/STS have local nematic order Is charge order a friend or a foe of high T c superconductivity?

17 The case of La1-x Bax CuO4

18 The case of La1-x Bax CuO4 LBCO, the original HTSC, is known to exhibit low energy stripe fluctuations in its superconducting state

19 The case of La1-x Bax CuO4 LBCO, the original HTSC, is known to exhibit low energy stripe fluctuations in its superconducting state It has a very low Tc near x=1/8 where it shows static stripe order in the LTT crystal structure

20 The case of La1-x Bax CuO4 LBCO, the original HTSC, is known to exhibit low energy stripe fluctuations in its superconducting state It has a very low Tc near x=1/8 where it shows static stripe order in the LTT crystal structure Experimental evidence for superconducting layer decoupling in LBCO at x=1/8

21 The case of La1-x Bax CuO4 LBCO, the original HTSC, is known to exhibit low energy stripe fluctuations in its superconducting state It has a very low Tc near x=1/8 where it shows static stripe order in the LTT crystal structure Experimental evidence for superconducting layer decoupling in LBCO at x=1/8 Layer decoupling, long range charge and spin stripe order and superconductivity: a novel striped superconducting state, a Pair Density Wave, in which charge, spin, and superconducting orders are intertwined!

22 70 60 Phase Diagram of LBCO LTO LBCO Temperature (K) SC T LT LTT CO SO SC T c hole doping (x) M. Hücker et al (2009)

23 Li et al (2007): Dynamical Layer Decoupling in LBCO

24 Li et al (2007): Dynamical Layer Decoupling in LBCO ARPES: anti-nodal d-wave SC gap is large and unsuppressed at 1/8

25 Li et al (2007): Dynamical Layer Decoupling in LBCO ARPES: anti-nodal d-wave SC gap is large and unsuppressed at 1/8 Static charge stripe order for T< T charge=54 K

26 Li et al (2007): Dynamical Layer Decoupling in LBCO ARPES: anti-nodal d-wave SC gap is large and unsuppressed at 1/8 Static charge stripe order for T< T charge=54 K Static Stripe Spin order T < T spin= 42K

27 Li et al (2007): Dynamical Layer Decoupling in LBCO ARPES: anti-nodal d-wave SC gap is large and unsuppressed at 1/8 Static charge stripe order for T< T charge=54 K Static Stripe Spin order T < T spin= 42K ρab drops rapidly to zero from Tspin to TKT

28 Li et al (2007): Dynamical Layer Decoupling in LBCO ARPES: anti-nodal d-wave SC gap is large and unsuppressed at 1/8 Static charge stripe order for T< T charge=54 K Static Stripe Spin order T < T spin= 42K ρab drops rapidly to zero from Tspin to TKT ρab shows KT behavior for Tspin > T > TKT

29 Li et al (2007): Dynamical Layer Decoupling in LBCO ARPES: anti-nodal d-wave SC gap is large and unsuppressed at 1/8 Static charge stripe order for T< T charge=54 K Static Stripe Spin order T < T spin= 42K ρab drops rapidly to zero from Tspin to TKT ρab shows KT behavior for Tspin > T > TKT ρc as T for T>T ** 35K

30 Li et al (2007): Dynamical Layer Decoupling in LBCO ARPES: anti-nodal d-wave SC gap is large and unsuppressed at 1/8 Static charge stripe order for T< T charge=54 K Static Stripe Spin order T < T spin= 42K ρab drops rapidly to zero from Tspin to TKT ρab shows KT behavior for Tspin > T > TKT ρc as T for T>T ** 35K ρc 0 as T T3D= 10K

31 Li et al (2007): Dynamical Layer Decoupling in LBCO ARPES: anti-nodal d-wave SC gap is large and unsuppressed at 1/8 Static charge stripe order for T< T charge=54 K Static Stripe Spin order T < T spin= 42K ρab drops rapidly to zero from Tspin to TKT ρab shows KT behavior for Tspin > T > TKT ρc as T for T>T ** 35K ρc 0 as T T3D= 10K ρc / ρab for TKT > T > T3D

32 Li et al (2007): Dynamical Layer Decoupling in LBCO ARPES: anti-nodal d-wave SC gap is large and unsuppressed at 1/8 Static charge stripe order for T< T charge=54 K Static Stripe Spin order T < T spin= 42K ρab drops rapidly to zero from Tspin to TKT ρab shows KT behavior for Tspin > T > TKT ρc as T for T>T ** 35K ρc 0 as T T3D= 10K ρc / ρab for TKT > T > T3D Meissner state only below T c= 4K

33

34 Anisotropic Transport Below the Charge Ordering transition Li et al, 2007

35 The 2D Resistive State and 2D Superconductivity Li et al, 2007

36 How Do We Understand This Remarkable Effects?

37 How Do We Understand This Remarkable Effects? Broad temperature range, T3D < T < T2D with 2D superconductivity but not in 3D, as if there is not interlayer Josephson coupling

38 How Do We Understand This Remarkable Effects? Broad temperature range, T3D < T < T2D with 2D superconductivity but not in 3D, as if there is not interlayer Josephson coupling In this regime there is both striped charge and spin order

39 How Do We Understand This Remarkable Effects? Broad temperature range, T3D < T < T2D with 2D superconductivity but not in 3D, as if there is not interlayer Josephson coupling In this regime there is both striped charge and spin order This can only happen if there is a special symmetry of the superconductor in the striped state that leads to an almost complete cancellation of the c-axis Josephson coupling.

40 A Striped Textured Superconducting Phase

41 A Striped Textured Superconducting Phase The stripe state in the LTT crystal structure has two planes in the unit cell.

42 A Striped Textured Superconducting Phase The stripe state in the LTT crystal structure has two planes in the unit cell. Stripes in the 2nd neighbor planes are shifted by half a period to minimize the Coulomb interaction: 4 planes per unit cell

43 A Striped Textured Superconducting Phase The stripe state in the LTT crystal structure has two planes in the unit cell. Stripes in the 2nd neighbor planes are shifted by half a period to minimize the Coulomb interaction: 4 planes per unit cell The AFM spin order suffers a π phase shift accross the charge stripe which has period 4

44 A Striped Textured Superconducting Phase The stripe state in the LTT crystal structure has two planes in the unit cell. Stripes in the 2nd neighbor planes are shifted by half a period to minimize the Coulomb interaction: 4 planes per unit cell The AFM spin order suffers a π phase shift accross the charge stripe which has period 4 We propose that the superconducting order is also striped and also suffers a π phase shift.

45 A Striped Textured Superconducting Phase The stripe state in the LTT crystal structure has two planes in the unit cell. Stripes in the 2nd neighbor planes are shifted by half a period to minimize the Coulomb interaction: 4 planes per unit cell The AFM spin order suffers a π phase shift accross the charge stripe which has period 4 We propose that the superconducting order is also striped and also suffers a π phase shift. The superconductivity resides in the spin gap regions and there is a π phase shift in the SC order across the AFM regions

46 Period 4 Striped Superconducting State E. Berg et al, 2007 (x) x

47 Period 4 Striped Superconducting State E. Berg et al, 2007 (x) x This state has intertwined striped charge, spin and superconducting orders.

48 Period 4 Striped Superconducting State E. Berg et al, 2007 (x) x This state has intertwined striped charge, spin and superconducting orders. A state of this type was found in variational Monte Carlo (Ogata et al 2004) and MFT (Poilblanc et al 2007)

49 How does this state solve the puzzle?

50 How does this state solve the puzzle? If this order is perfect, the Josephson coupling between neighboring planes cancels exactly due to the symmetry of the periodic array of π textures

51 How does this state solve the puzzle? If this order is perfect, the Josephson coupling between neighboring planes cancels exactly due to the symmetry of the periodic array of π textures The Josephson couplings J1 and J2 between planes two and three layers apart also cancel by symmetry.

52 How does this state solve the puzzle? If this order is perfect, the Josephson coupling between neighboring planes cancels exactly due to the symmetry of the periodic array of π textures The Josephson couplings J1 and J2 between planes two and three layers apart also cancel by symmetry. The first non-vanishing coupling J3 occurs at four spacings. It is quite small and it is responsible for the non-zero but very low Tc

53 How does this state solve the puzzle? If this order is perfect, the Josephson coupling between neighboring planes cancels exactly due to the symmetry of the periodic array of π textures The Josephson couplings J1 and J2 between planes two and three layers apart also cancel by symmetry. The first non-vanishing coupling J3 occurs at four spacings. It is quite small and it is responsible for the non-zero but very low Tc Defects and/or discommensurations gives rise to small Josephson coupling J0 neighboring planes

54 Are there other interactions?

55 Are there other interactions? It is possible to have an inter-plane biquadratic coupling involving the product SC of the order parameters between neighboring planes Δ1 Δ2 and the product of spin stripe order parameters also on neighboring planes M1. M2

56 Are there other interactions? It is possible to have an inter-plane biquadratic coupling involving the product SC of the order parameters between neighboring planes Δ1 Δ2 and the product of spin stripe order parameters also on neighboring planes M1. M2 However in the LTT structure M1. M2=0 and there is no such coupling

57 Are there other interactions? It is possible to have an inter-plane biquadratic coupling involving the product SC of the order parameters between neighboring planes Δ1 Δ2 and the product of spin stripe order parameters also on neighboring planes M1. M2 However in the LTT structure M1. M2=0 and there is no such coupling In a large enough perpendicular magnetic field it is possible (spin flop transition) to induce such a term and hence an effective Josephson coupling.

58 Are there other interactions? It is possible to have an inter-plane biquadratic coupling involving the product SC of the order parameters between neighboring planes Δ1 Δ2 and the product of spin stripe order parameters also on neighboring planes M1. M2 However in the LTT structure M1. M2=0 and there is no such coupling In a large enough perpendicular magnetic field it is possible (spin flop transition) to induce such a term and hence an effective Josephson coupling. Thus in this state there should be a strong suppression of the 3D SC Tc but not of the 2D SC Tc

59 Away from x=1/8

60 Away from x=1/8 Away from x=1/8 there is no perfect commensuration

61 Away from x=1/8 Away from x=1/8 there is no perfect commensuration Discommensurations are defects that induce a finite Josephson coupling between neighboring planes J1 ~ x-1/8 2, leading to an increase of the 3D SC Tc away from 1/8

62 Away from x=1/8 Away from x=1/8 there is no perfect commensuration Discommensurations are defects that induce a finite Josephson coupling between neighboring planes J1 ~ x-1/8 2, leading to an increase of the 3D SC Tc away from 1/8 Similar effects arise from disorder which also lead to a rise in the 3D SC Tc

63 Landau-Ginzburg Theory of the striped SC: Order Parameters Striped SC: Δ(r)=ΔQ(r) e i Q.r + Δ-Q(r) e -iq.r, complex charge 2e singlet pair condensate with wave vector, (i.e. an FFLO type state at zero magnetic field) Nematic: detects breaking of rotational symmetry: N, a real neutral pseudo-scalar order parameter Charge stripe: ρk, unidirectional charge stripe with wave vector K Spin stripe order parameter: S Q, a neutral complex spin vector order parameter, K=2Q

64 Ginzburg-Landau Free Energy Functional

65 Ginzburg-Landau Free Energy Functional F=F2+ F3 + F4 +...

66 Ginzburg-Landau Free Energy Functional F=F2+ F3 + F The quadratic and quartic terms are standard

67 Ginzburg-Landau Free Energy Functional F=F2+ F3 + F The quadratic and quartic terms are standard F3= γs ρk * SQ. SQ + π/2 rotation + c.c.

68 Ginzburg-Landau Free Energy Functional F=F2+ F3 + F The quadratic and quartic terms are standard F3= γs ρk * SQ. SQ + π/2 rotation + c.c. +γδ ρk * Δ-Q * ΔQ + π/2 rotation + c.c.

69 Ginzburg-Landau Free Energy Functional F=F2+ F3 + F The quadratic and quartic terms are standard F3= γs ρk * SQ. SQ + π/2 rotation + c.c. +γδ ρk * Δ-Q * ΔQ + π/2 rotation + c.c. +gδ N (ΔQ * ΔQ+ Δ-Q * Δ-Q -π/2 rotation) + c.c.

70 Ginzburg-Landau Free Energy Functional F=F2+ F3 + F The quadratic and quartic terms are standard F3= γs ρk * SQ. SQ + π/2 rotation + c.c. +γδ ρk * Δ-Q * ΔQ + π/2 rotation + c.c. +gδ N (ΔQ * ΔQ+ Δ-Q * Δ-Q -π/2 rotation) + c.c. +gs N (SQ *. SQ -π/2 rotation)

71 Ginzburg-Landau Free Energy Functional F=F2+ F3 + F The quadratic and quartic terms are standard F3= γs ρk * SQ. SQ + π/2 rotation + c.c. +γδ ρk * Δ-Q * ΔQ + π/2 rotation + c.c. +gδ N (ΔQ * ΔQ+ Δ-Q * Δ-Q -π/2 rotation) + c.c. +gs N (SQ *. SQ -π/2 rotation) +gc N (ρk * ρk -π/2 rotation)

72 Some Consequences of the GL theory

73 Some Consequences of the GL theory The symmetry of the term coupling charge and spin order parameters requires the condition K= 2Q

74 Some Consequences of the GL theory The symmetry of the term coupling charge and spin order parameters requires the condition K= 2Q Striped SC order implies charge stripe order with 1/2 the period, and of nematic order

75 Some Consequences of the GL theory The symmetry of the term coupling charge and spin order parameters requires the condition K= 2Q Striped SC order implies charge stripe order with 1/2 the period, and of nematic order Charge stripe order with wave vector 2Q and/or nematic order favors stripe superconducting order which may or may not occur depending on the coefficients in the quadratic part

76 Some Consequences of the GL theory The symmetry of the term coupling charge and spin order parameters requires the condition K= 2Q Striped SC order implies charge stripe order with 1/2 the period, and of nematic order Charge stripe order with wave vector 2Q and/or nematic order favors stripe superconducting order which may or may not occur depending on the coefficients in the quadratic part Coupling to a charge 4e SC order parameter Δ4

77 Some Consequences of the GL theory The symmetry of the term coupling charge and spin order parameters requires the condition K= 2Q Striped SC order implies charge stripe order with 1/2 the period, and of nematic order Charge stripe order with wave vector 2Q and/or nematic order favors stripe superconducting order which may or may not occur depending on the coefficients in the quadratic part Coupling to a charge 4e SC order parameter Δ4 F 3=g4 [Δ4 * (ΔQ Δ-Q+ rotation)+ c.c.]

78 Some Consequences of the GL theory The symmetry of the term coupling charge and spin order parameters requires the condition K= 2Q Striped SC order implies charge stripe order with 1/2 the period, and of nematic order Charge stripe order with wave vector 2Q and/or nematic order favors stripe superconducting order which may or may not occur depending on the coefficients in the quadratic part Coupling to a charge 4e SC order parameter Δ4 F 3=g4 [Δ4 * (ΔQ Δ-Q+ rotation)+ c.c.] Striped SC order (PDW) uniform charge 4e SC order

79 Coexisting uniform and striped SC order

80 Coexisting uniform and striped SC order PDW order ΔQ and uniform SC order Δ0

81 Coexisting uniform and striped SC order PDW order ΔQ and uniform SC order Δ0 F3,u=ϒΔ Δ0 * ρq Δ-Q+ρ-Q ΔQ+gρ ρ-2q ρq 2 +rotation +c.c.

82 Coexisting uniform and striped SC order PDW order ΔQ and uniform SC order Δ0 F3,u=ϒΔ Δ0 * ρq Δ-Q+ρ-Q ΔQ+gρ ρ-2q ρq 2 +rotation +c.c. If Δ0 0 and ΔQ 0 there is a ρq component of the charge order!

83 Coexisting uniform and striped SC order PDW order ΔQ and uniform SC order Δ0 F3,u=ϒΔ Δ0 * ρq Δ-Q+ρ-Q ΔQ+gρ ρ-2q ρq 2 +rotation +c.c. If Δ0 0 and ΔQ 0 there is a ρq component of the charge order! The small uniform component Δ0 removes the sensitivity to quenched disorder of the PDW state

84 Topological Excitations of the Striped SC

85 Topological Excitations of the Striped SC ρ(r)= ρk cos [K r+ Φ(r)]

86 Topological Excitations of the Striped SC ρ(r)= ρk cos [K r+ Φ(r)] Δ(r)= ΔQ exp[i Q r + i θq(r)]+ Δ-Q exp[-i Q r + i θ-q(r)]

87 Topological Excitations of the Striped SC ρ(r)= ρk cos [K r+ Φ(r)] Δ(r)= ΔQ exp[i Q r + i θq(r)]+ Δ-Q exp[-i Q r + i θ-q(r)] F3,ϒ=2ϒΔ ρk ΔQ Δ-Q cos[2 θ-(r)-φ(r)]

88 Topological Excitations of the Striped SC ρ(r)= ρk cos [K r+ Φ(r)] Δ(r)= ΔQ exp[i Q r + i θq(r)]+ Δ-Q exp[-i Q r + i θ-q(r)] F3,ϒ=2ϒΔ ρk ΔQ Δ-Q cos[2 θ-(r)-φ(r)] θ±q(r)=[θ+(r) ± θ-(r)]/2

89 Topological Excitations of the Striped SC ρ(r)= ρk cos [K r+ Φ(r)] Δ(r)= ΔQ exp[i Q r + i θq(r)]+ Δ-Q exp[-i Q r + i θ-q(r)] F3,ϒ=2ϒΔ ρk ΔQ Δ-Q cos[2 θ-(r)-φ(r)] θ±q(r)=[θ+(r) ± θ-(r)]/2 θ±q single valued mod 2π θ± defined mod π

90 Topological Excitations of the Striped SC ρ(r)= ρk cos [K r+ Φ(r)] Δ(r)= ΔQ exp[i Q r + i θq(r)]+ Δ-Q exp[-i Q r + i θ-q(r)] F3,ϒ=2ϒΔ ρk ΔQ Δ-Q cos[2 θ-(r)-φ(r)] θ±q(r)=[θ+(r) ± θ-(r)]/2 θ±q single valued mod 2π θ± defined mod π ϕ and θ- are locked topological defects of ϕ and θ+

91

92 Topological Excitations of the Striped SC

93 Topological Excitations of the Striped SC SC vortex with Δθ+ = 2π and Δϕ=0

94 Topological Excitations of the Striped SC SC vortex with Δθ+ = 2π and Δϕ=0 Bound state of a 1/2 vortex and a dislocation

95 Topological Excitations of the Striped SC SC vortex with Δθ+ = 2π and Δϕ=0 Bound state of a 1/2 vortex and a dislocation Δθ+ = π, Δϕ= 2π

96 Topological Excitations of the Striped SC SC vortex with Δθ+ = 2π and Δϕ=0 Bound state of a 1/2 vortex and a dislocation Δθ+ = π, Δϕ= 2π Double dislocation, Δθ+ = 0, Δϕ= 4π

97 Topological Excitations of the Striped SC SC vortex with Δθ+ = 2π and Δϕ=0 Bound state of a 1/2 vortex and a dislocation Δθ+ = π, Δϕ= 2π Double dislocation, Δθ+ = 0, Δϕ= 4π All three topological defects have logarithmic interactions

98 Half-vortex and a Dislocation

99 Double Dislocation

100

101 Thermal melting of the PDW state

102 Thermal melting of the PDW state Three paths for thermal melting of the PDW state

103 Thermal melting of the PDW state Three paths for thermal melting of the PDW state Three types of topological excitations: (1,0) (SC vortex), (0,1) (double dislocation), (±1/2, ±1/2) (1/2 vortex, single dislocation bound pair)

104 Thermal melting of the PDW state Three paths for thermal melting of the PDW state Three types of topological excitations: (1,0) (SC vortex), (0,1) (double dislocation), (±1/2, ±1/2) (1/2 vortex, single dislocation bound pair) Scaling dimensions: p,q=π(ρsc p 2 +κcdw q 2 )/T=2 (for marginality)

105 Thermal melting of the PDW state Three paths for thermal melting of the PDW state Three types of topological excitations: (1,0) (SC vortex), (0,1) (double dislocation), (±1/2, ±1/2) (1/2 vortex, single dislocation bound pair) Scaling dimensions: p,q=π(ρsc p 2 +κcdw q 2 )/T=2 (for marginality) Phases: PDW, Charge 4e SC, CDW, and normal (Ising nematic)

106 Schematic Phase Diagram

107

108 Effects of Disorder

109 Effects of Disorder The striped SC order is very sensitive to disorder: disorder pinned charge density wave coupling to the phase of the striped SC SC gauge glass with zero resistance but no Meissner effect in 3D

110 Effects of Disorder The striped SC order is very sensitive to disorder: disorder pinned charge density wave coupling to the phase of the striped SC SC gauge glass with zero resistance but no Meissner effect in 3D Disorder induces dislocation defects in the stripe order

111 Effects of Disorder The striped SC order is very sensitive to disorder: disorder pinned charge density wave coupling to the phase of the striped SC SC gauge glass with zero resistance but no Meissner effect in 3D Disorder induces dislocation defects in the stripe order Due to the coupling between stripe order and SC, ±π flux vortices are induced at the dislocation core.

112 Effects of Disorder The striped SC order is very sensitive to disorder: disorder pinned charge density wave coupling to the phase of the striped SC SC gauge glass with zero resistance but no Meissner effect in 3D Disorder induces dislocation defects in the stripe order Due to the coupling between stripe order and SC, ±π flux vortices are induced at the dislocation core. Strict layer decoupling only allows for a magnetic coupling between randomly distributed ±π flux vortices

113 Effects of Disorder The striped SC order is very sensitive to disorder: disorder pinned charge density wave coupling to the phase of the striped SC SC gauge glass with zero resistance but no Meissner effect in 3D Disorder induces dislocation defects in the stripe order Due to the coupling between stripe order and SC, ±π flux vortices are induced at the dislocation core. Strict layer decoupling only allows for a magnetic coupling between randomly distributed ±π flux vortices Novel glassy physics and fractional flux

114 Effects of Disorder The striped SC order is very sensitive to disorder: disorder pinned charge density wave coupling to the phase of the striped SC SC gauge glass with zero resistance but no Meissner effect in 3D Disorder induces dislocation defects in the stripe order Due to the coupling between stripe order and SC, ±π flux vortices are induced at the dislocation core. Strict layer decoupling only allows for a magnetic coupling between randomly distributed ±π flux vortices Novel glassy physics and fractional flux the charge 4e SC order is unaffected by the Bragg glass of the pinned CDW

115 Phase Sensitive Experiments I=J2 sin(2δθ)

116 Role of Nematic Fluctuations in PDW Melting?

117 Role of Nematic Fluctuations in PDW Melting? If nematic fluctuations become strong, orders that break translational symmetry become progressively suppressed

118 Role of Nematic Fluctuations in PDW Melting? If nematic fluctuations become strong, orders that break translational symmetry become progressively suppressed In the absence of a lattice in 2D smectic order is not possible (at T>0) (Toner & Nelson, 1980)

119 Role of Nematic Fluctuations in PDW Melting? If nematic fluctuations become strong, orders that break translational symmetry become progressively suppressed In the absence of a lattice in 2D smectic order is not possible (at T>0) (Toner & Nelson, 1980) Coupling to the lattice breaks continuous rotational invariance to the point group of the lattice

120 Role of Nematic Fluctuations in PDW Melting? If nematic fluctuations become strong, orders that break translational symmetry become progressively suppressed In the absence of a lattice in 2D smectic order is not possible (at T>0) (Toner & Nelson, 1980) Coupling to the lattice breaks continuous rotational invariance to the point group of the lattice For a square lattice the point group is C4 and the nematicisotropic transition is 2D Ising

121 Role of Nematic Fluctuations in PDW Melting? If nematic fluctuations become strong, orders that break translational symmetry become progressively suppressed In the absence of a lattice in 2D smectic order is not possible (at T>0) (Toner & Nelson, 1980) Coupling to the lattice breaks continuous rotational invariance to the point group of the lattice For a square lattice the point group is C4 and the nematicisotropic transition is 2D Ising As the coupling to the lattice is weakened the structure of the phase diagram changes and the nematic transition is pushed to lower temperatures

122

123 PDW melting as a McMillan-de Gennes theory The electronic nematic order parameter is an antisymmetric traceless tensor N ij = N(ˆn iˆn j ij /2) Its presence amounts to a local change of the geometry, the local metric, seen by the charge 4e SC order parameter 4e the CDW order parameter and the PDW order K ±Q Metric tensor: g ij = ij + N ij Novel derivative couplings in the free energy F d = Z dx 2 p detg g ij n D cdw i K D cdw j K + +(Di sc ±Q) Dj sc ±Q + Di 4e 4e Dj 4e 4e o D sc i = i i2ea i ± iq n i D cdw i = i + i2q n i D 4e i = i i4ea i

124 Deep in the PDW phase the amplitude of the SC, CDW and nematic order parameters are fixed but their phases are not Z n F = d 2 s x 2 gij ( i 2eA i )( j 2eA j ) + 2 gij ( i + Q n i )( j + Q n j ) + K 1 ( n) 2 + K 3 ( n) 2 + h n 2o s = ±Q 2 + 4e 2 apple = ±Q 2 + K 2 Effective CDW stiffness reduced by gapped nematic fluctuations e = 1+ Q2 /h

125 Deep in the charge 4e nematic superconducting phase F = Z d 2 x K 2 + s 2 + sn 2 (n )2 and are the orientational nematic fluctuations and SC phase fluctuations in the absence of orientational pinning SC (half) vortices and nematic disclinations attract each other due to the fluctuations of the local geometry (nematic fluctuations): the only topological excitations are disclinations bound to half vortices If the nematic fluctuations are gapped by lattice effects there is a crossover to the pinned case discussed before Fermionic SC quasiparticles couple to the pair field which is uncondensed in the charge 4e SC. This leads to a pseudogap in the quasiparticle spectrum

126 Conclusions The static stripe order seen in LBCO and other LSCO related materials can be understood in terms of the PDW, a state in which charge, spin and superconducting orders are intertwined rather than competing This state competes with the uniform d-wave state Several predictions can be tested experimentally The observed nematic order is a state with fluctuating stripe order, i.e. it is a state with melted stripe order. Is the nematic state a melted PDW? Is the PDW peculiar to LBCO? If so why? If it is generic, why? A microscopic theory of the PDW is needed. This state is not accessible by a weak coupling BCS approach. Strong evidence in 1d Kondo-Heisenberg chain.