Magnetic Excitations of Stripes E. W. Carlson D. X. Yao D. K. - - PowerPoint PPT Presentation

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Magnetic Excitations of Stripes E. W. Carlson D. X. Yao D. K. - - PowerPoint PPT Presentation

Magnetic Excitations of Stripes E. W. Carlson D. X. Yao D. K. Campbell Stripes: Why? HTSC Dilemmas Superconductivity from a non-Fermi liquid High pairing scale despite strong repulsion Metallic Charge Stripes: Spin-Charge Separation


slide-1
SLIDE 1

Magnetic Excitations of Stripes

  • E. W. Carlson
  • D. X. Yao
  • D. K. Campbell
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SLIDE 2

Stripes: Why?

HTSC Dilemmas

Superconductivity from a non-Fermi liquid High pairing scale despite strong repulsion

Metallic Charge Stripes: Spin-Charge Separation

Non-Fermi liquid normal state (Luttinger liquid) Pair the spin degrees of freedom, and avoid the Coulomb repulsion.

EC, V. Emery, S. Kivelson, D. Orgad in “Physics of Unconventional Superconductors”

  • ed. Bennemann and Ketterson, (2004)
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SLIDE 3

superconductivity

T

Josephson coupling Pairing

Inherent Competition

stripe fluctuations Static Stripes Good pairing Bad phase coherence Fluctuating Stripes Bad pairing Good phase coherence think think “ “stripe phonon stripe phonon” ” think local stripe order think local stripe order

EC, V. Emery, S. Kivelson, D. Orgad in “Physics of Unconventional Superconductors”

  • ed. Bennemann and Ketterson, (2004)
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SLIDE 4

Unidirectional modulation in charge and spin Charge: quasi-one-dimensional (rivers of charge) Spin: 2D Magnetic texture

Stripes

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SLIDE 5

Stripes Have 2D Magnetic Texture

  • Real Space

Reciprocal Lattice Vectors

2D spin waves disperse out of the reciprocal lattice vector positions

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SLIDE 6

Neutron Scattering in Cuprates and Nickelates

Disappearance of (,) peak with doping Appearance of satellite peaks

AFM signal averages to zero

antiphase domain walls

  • OR

OR site-centered site-centered bond-centered bond-centered

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SLIDE 7

Neutron Scattering in Cuprates and Nickelates

  • OR

OR site-centered site-centered bond-centered bond-centered

Charge Peaks related by X2

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SLIDE 8

Checkerboards and Plaids?

Charge Peaks Antiphase Domain Walls in Antiferromagnetism Spin Peaks in Wrong Direction!

Hoffman et al., Science (2002) Vershinin et al., Science (2004)

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SLIDE 9

Odd Spacing

Bond-centered

  • Site-centered
  • Magnetic

Reciprocal Lattice Vectors

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SLIDE 10

Odd Spacing

Bond-centered

  • Site-centered
  • Intensities
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SLIDE 11

Odd Spacing

Bond-centered

  • Site-centered
  • Observing

weight here rules out site-centered stripes

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SLIDE 12

Magnetic Reciprocal Lattice Vectors

Even Spacing

Bond-centered Site-centered

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SLIDE 13

Intensities

Even Spacing

Bond-centered Site-centered

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SLIDE 14

Inelastic Response: Spin Waves

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SLIDE 15

Site or Bond-Centered

Ja > 0 (AFM) Jb > 0 (AFM)

Jb Ja Jb

Ja > 0 (AFM) Jb < 0 (FM)

Ja

Site-centered p=3 Bond-centered p=3

Semiclassical Spin Waves

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SLIDE 16

Low Energy Velocities

Spin wave cones may remain rather isotropic for bond-centered stripes, despite microscopic anisotropy.

site-centered bond-centered

1 2 3 1 2 3 1 1

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SLIDE 17

Spin Wave Dispersions

  • Bond-centered has one more band
  • Bond-centered has weight at (0,π)
  • Bands repel, do not cross

Resonance unlikely from crossings

Site-centered, p=3 Bond-centered, p=3

6

π π

5

Jb= 0.4 Ja Jb= - 1.0 Ja

Batista et al., PRB (2001) EC, Yao, et al., PRB (2004)

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SLIDE 18

Data

YBCO6.6, S. Hayden et al., Nature 429, 531 (2004) Stripe-ordered LBCO, S. Hayden et al., Nature 429, 534 (2004)

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SLIDE 19

Symmetrize

E=0.5J E=0.5Ja

a

E=1.5J E=1.5Ja

a

E=2.5J E=2.5Ja

a

E=3.5J E=3.5Ja

a

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SLIDE 20

VB4 Jb = -.1 Ja

E=0.5J E=0.5Ja

a

E=1.0J E=1.0Ja

a

E=1.5J E=1.5Ja

a

E=2.0J E=2.0Ja

a

E=3.5J E=3.5Ja

a

E=4.0J E=4.0Ja

a

E=3.0J E=3.0Ja

a

E=2.5J E=2.5Ja

a

Vertical, Bond-centered, Spacing = 4

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SLIDE 21

E=0.5J E=0.5Ja

a

E=1.0J E=1.0Ja

a

E=1.5J E=1.5Ja

a

E=2.0J E=2.0Ja

a

E=3.5J E=3.5Ja

a

E=4.0J E=4.0Ja

a

E=3.0J E=3.0Ja

a

E=2.5J E=2.5Ja

a

VB4 Jb = -.56 Ja

Vertical, Bond-centered, Spacing = 4

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SLIDE 22

VS4 Jb = Ja

E=0.5J E=0.5Ja

a

E=1.0J E=1.0Ja

a

E=1.5J E=1.5Ja

a

E=2.0J E=2.0Ja

a

E=3.5J E=3.5Ja

a

E=4.0J E=4.0Ja

a

E=3.0J E=3.0Ja

a

E=2.5J E=2.5Ja

a

Vertical, Site-centered, Spacing = 4

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SLIDE 23

Other Stripe Patterns

Diagonal

“DB4”

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SLIDE 24

DB2 Jb= -.1 Ja

E=0.25J E=0.25Ja

a

E=0.5J E=0.5Ja

a

E=0.75J E=0.75Ja

a

E=1 J E=1 Ja

a

E=1.75J E=1.75Ja

a

E=2 J E=2 Ja

a

E=1.5 J E=1.5 Ja

a

E=1.25 J E=1.25 Ja

a

Diagonal, Bond-centered, Spacing = 2

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SLIDE 25

Other Stripe Patterns

Staircase

  • M. Granath, PRB (2004)

Smooth transition from diagonal to vertical peaks Fermi Surface Arcs

Globally diagonal Locally vertical Antiphase domain walls

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SLIDE 26

SB2 Jb = -.1 Ja

E=0.4J E=0.4Ja

a

E=0.7J E=0.7Ja

a

E=1J E=1Ja

a

E=1.6 J E=1.6 Ja

a

E=3.6J E=3.6Ja

a

E=4.0 J E=4.0 Ja

a

E=2.6J E=2.6Ja

a

E=2.0 J E=2.0 Ja

a

Staircase, Bond-centered, Spacing = 2

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SLIDE 27

Conclusions

2D magnetic texture

  • Stripes produce 2D spin waves.
  • Finite energy weight at (π, π) is natural from stripes,

but not from a pure antiferromagnet. Resonance peak

  • Unlikely from crossing (bands repel)

Bond-centered stripes:

  • Ferromagnetic coupling across domain wall
  • One more band than site-centered
  • Odd spacing has new elastic peaks,

forbidden for site-centered stripes

  • Isotropic spin wave cones
  • “Legs” of scattering

Comparison to Recent Cuprate Data

  • Low energy could be semiclassical spin waves
  • High energy is not