Magnetic Excitations of Stripes
- E. W. Carlson
- D. X. Yao
- D. K. Campbell
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
Superconductivity from a non-Fermi liquid High pairing scale despite strong repulsion
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”
superconductivity
T
Josephson coupling Pairing
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”
Unidirectional modulation in charge and spin Charge: quasi-one-dimensional (rivers of charge) Spin: 2D Magnetic texture
Reciprocal Lattice Vectors
2D spin waves disperse out of the reciprocal lattice vector positions
Disappearance of (,) peak with doping Appearance of satellite peaks
AFM signal averages to zero
antiphase domain walls
OR site-centered site-centered bond-centered bond-centered
OR site-centered site-centered bond-centered bond-centered
Charge Peaks related by X2
Charge Peaks Antiphase Domain Walls in Antiferromagnetism Spin Peaks in Wrong Direction!
Hoffman et al., Science (2002) Vershinin et al., Science (2004)
Bond-centered
Reciprocal Lattice Vectors
Bond-centered
Bond-centered
weight here rules out site-centered stripes
Magnetic Reciprocal Lattice Vectors
Bond-centered Site-centered
Intensities
Bond-centered Site-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
site-centered bond-centered
1 2 3 1 2 3 1 1
Site-centered, p=3 Bond-centered, p=3
6
5
Jb= 0.4 Ja Jb= - 1.0 Ja
Batista et al., PRB (2001) EC, Yao, et al., PRB (2004)
YBCO6.6, S. Hayden et al., Nature 429, 531 (2004) Stripe-ordered LBCO, S. Hayden et al., Nature 429, 534 (2004)
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
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
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
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
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
Smooth transition from diagonal to vertical peaks Fermi Surface Arcs
Globally diagonal Locally vertical Antiphase domain walls
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
2D magnetic texture
but not from a pure antiferromagnet. Resonance peak
Bond-centered stripes:
forbidden for site-centered stripes
Comparison to Recent Cuprate Data