Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4...
-
Upload
elvin-little -
Category
Documents
-
view
221 -
download
9
Transcript of Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4...
![Page 1: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/1.jpg)
Lecture schedule October 3 – 7, 2011
• #1 Kondo effect• #2 Spin glasses• #3 Giant magnetoresistance• #4 Magnetoelectrics and multiferroics• #5 High temperature superconductivity• #6 Applications of superconductivity• #7 Heavy fermions• #8 Hidden order in URu2Si2• #9 Modern experimental methods in correlated electron systems• #10 Quantum phase transitions
Present basic experimental phenomena of the above topics
![Page 2: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/2.jpg)
Some Spectroscopy Studies of the HO State of URu2Si2
J. A. Mydosh
Kamerlingh Onnes Laboratory, Leiden University, The Netherlands
Introduction
Inelastic neutron scattering (spin)
Optical conductivity (charge)
Ultrasonic velocity (thermo.) [and attenuation (transp.)]
ARPES (charge)
STM/STS (charge and spin)
[But not PCS, & QO]
![Page 3: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/3.jpg)
What is “Hidden Order” (HO)?
[See, e.g. N. Shah, P. Chandra, P. Coleman and JAM, PRB 6I, 564(2000).]
Now quite common usage of HO. Or as some theorists call it “Dark Quantum Matter” or as others call it “Novel Forms of Order” and “Novel Phases” {Reserve for high-field phases} or ‘‘Dark Order’’.
A clear, from bulk thermodynamic and transport measurements, phase transition at T0 where the order parameter (OP) and elementary excitations (EE) are unknown, i.e., cannot be determined from microscopic experiments.
Ψ is primary, unknown OP; m is antiferromagnetic, secondary OP
![Page 4: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/4.jpg)
Key Unsolved Problems/Questions of HO in URu2Si2
• Local, dual or itinerant?• OP’s primary / secondary?• Mediator of phase transition?• INS resonance mode causing HO: Q0 or Q1 ?• How to probe OP experimental?• Relation of HO to LMAF (Adiabatic Continuity)?• Symmetry breaking in HO vs. LMAF?• Spin – charge duality?• HF Liq.(hybridization) or Kondo Liq. at coherence T*?• Kondo effect in (Th1-xUx)Ru2Si2?• Generic HO in other materials? Or is URu2Si2 unique?• Missing link experiments?(Hall effect under pressure, etc.)• Many theories/models -- which one is solution to HO?
![Page 5: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/5.jpg)
Spin: Inelastic neutron scattering - “resonances” at Qo =(1,0,0) and Q1 =(1.4,0,0)
• Broholm et al. PRL & PRB(1987 – 1991)
• Wiebe et al. NP(2007)
• Bourdarot et al. JPSJ(2010) ?(2011)?
• Niklowitz et al. to be published(2011)
![Page 6: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/6.jpg)
Excitation spectrum of URu2Si2 at 1.5K along (H,0,0)
Cones of excitations persist to higher T>To and E~10meV. Well-correlated itinerant-like spin excitations at Q1(incomm). Strongly coupled spin and charge degrees of freedom.
gapping
![Page 7: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/7.jpg)
Resonance at E0 for magnetic response at Qo
Longitudinal mode at 1.5K with continuum of Q-E scattering persisting to higher energies.
![Page 8: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/8.jpg)
Resonance at E1 for magnetic response at Q1
Longitudinal mode at 1.5K with continuum of Q-E scattering persisting to higher energies.
![Page 9: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/9.jpg)
T-dependence of Qo resonance
Growth of intensity below To = 17.8K with Q-E continuum
![Page 10: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/10.jpg)
T-dependence of resonance gap E0 at Qo
E0 represents a long lifetime (small decreasing half-width) collective mode rapidly reaching its final value 1.7 meV.
![Page 11: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/11.jpg)
Integrated intensity of dynamical spin susceptibilityWhat about at Q1 incommensurate resonance?
Red line is a BCS-type gap fit giving T-dependence of HO-OP. No divergence of static spin susceptibility, i.e, HO non-magnetic.
![Page 12: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/12.jpg)
Low energy excitations scanned through HO transition Niklowitz et al.(unpublished,2011)
Note peak at To for commensurate mode and step for incommen. mode
![Page 13: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/13.jpg)
Pressure – temperature phase diagram
Collection of results by Niklowitz et al. PRL(2010).
KL
![Page 14: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/14.jpg)
Pressure dependences of E0, E1 and bulk gap vaules
E0 disappears in LMAF phase, others persist. Note similar energy scales comparable to theoretical models.
LMAF Bragg peaks
HO
![Page 15: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/15.jpg)
Charge: Optical Conductivity
• Bonn et al. PRL(1988)
• van der Marel et al. unpublished(2010 - 2011)
• Lobo et al. unpublished(2010)
• Timusk et al. cond-mat.(2011)
![Page 16: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/16.jpg)
![Page 17: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/17.jpg)
HO-gap in URu2Si2 measured through optical conductivity, D. A. Bonn et al. PRL (1988).
Preliminary data in a – a plane, gapping(~45cm-1) into HO phase. Strong phonons. Missing Drude peak and correlation gap
![Page 18: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/18.jpg)
Van der Marel et al., private communication, 2011
![Page 19: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/19.jpg)
Reflectivity to optical conductivity along a and c
Clear but slow crossover (opening) of hybridization gap at 44K, persisting into HO gapping regime (not seen here).
![Page 20: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/20.jpg)
Extracting of scattering rate -1 as function of T & ωvia extended Drude model
Note decrease of -1 into hyb. gap
![Page 21: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/21.jpg)
Optical conductivity along a and c-axes
Opening of correlation gap ~15meV(125cm-1), clearer along a. Note low energy Drude peak and phonon modes.
![Page 22: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/22.jpg)
Optical conductivity 20 – 70K in hybridization gap region extrapolated to ω 0 via Drude peak analysis
Note opening of hydridization gap below 50K
W(ω) is loss of spectra weight accumulation
![Page 23: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/23.jpg)
Relaxation rate governing the frequency dependent scattering in hybribization gap region
As T increases scattering becomes incoherent
![Page 24: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/24.jpg)
Lower frequency (E) optical conductivity above To
Labo et al., private communication, 2010.
0 20 40 60 80 1000
1000
2000
3000
4000
5000
1 (-1
cm
-1)
Energy (meV)
20 K 25 K 30 K 50 K 100 K
Clear onset of hybridization gapping(~15 meV) below 50K. Drude peak forming at 2 meV(15 cm-1). Note phonons.
![Page 25: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/25.jpg)
Low T, low E optical conductivity probing HO
0 5 10 15 200
1000
2000
3000
4000
5000
6000
7000
8000
1 (
-1cm
-1)
Energy (meV)
5 K 7.5 K 10 K 12.5 K 15 K 20 K
HO gapping ~5meV with transfer of spectral wt. to just above gap and shifting of Drude peak to smaller E. Need lower E & T!
![Page 26: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/26.jpg)
Some conclusions
![Page 27: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/27.jpg)
![Page 28: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/28.jpg)
T – E dependences of optical conductivity
Note lack of intensity(conductivity) above To – correlation gap. No clear sign of HO gap. Need lower T and E.
![Page 29: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/29.jpg)
Low E, high T
0 2 4 6 8 100
2000
4000
6000
8000
10000
1 (-1
cm
-1)
Energy (meV)
20 K 25 K 30 K 50 K 100 K
![Page 30: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/30.jpg)
Low E, low T
0 2 4 6 8 100
2000
4000
6000
8000
10000
1 (-1
cm
-1)
Energy (meV)
5 K 20 K 50 K
![Page 31: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/31.jpg)
Thermodynamics: Ultrasonics velocity (attenuation as transport prop.) Determination of elastic constants, c ij
• Lüthi et al. JLTP (1994)
• Kuwahara et al. JPSJ (1997)
![Page 32: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/32.jpg)
Elastic constants (c = ρv2 ): c11, c33, c44; c66
Note c11 only longitudinal mode showing softening for T < 80K, min. 30K and HO shoulder.
![Page 33: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/33.jpg)
Analysis of elastic constant cij behavior of URu2Si2
Need new interpretation here: softening due to slow opening of hybridization gap. No CDW?
![Page 34: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/34.jpg)
Charge: ARPES
•J. Denlinger et al. JES&RP(2001)
•A. Santander-Syro et al. NP(2009)
•R. Yoshida et al. PRB(2010)
•Kawasaki et al. PRB(2011)
•G. Dakovski et al. PRB(to be published, 2011)
•XXX et al. ??? (2012)
![Page 35: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/35.jpg)
Among the many difficulties of ARPES: URu2Si2 is 3D thus depending upon the energy tuning one scans an arc through the BZ (or changing detector angle).
Note in bct the high symmetry directions Γ, Z; X
![Page 36: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/36.jpg)
Denlinger et al.(2001) – pioneering work
• Synchrotron scans 14 - 230 eV with ΔE > 50 meV at T > 20K.• Good resolution and DFT comparisons of 4d (Ru); 5d (U) lower
bands. Poor agreement with “old” LDA bands near EF.
• But Fermi surface mapping.• Insufficient resolution for near FS and qp studies.• Surface states/bands difficulties!• X hole pocket observed in FS, not confirmed!!!• Local 5f2 model!• Awaiting new results at SCES-2011.
![Page 37: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/37.jpg)
Fermi energy intensity maps off(85ev) / on(112eV)-resonance, 5f enhancement
DFT-LDA calculations bold=hole; fine=electron
X-point descrepancy: distinct hole pocket; LDA : small elec. pocket, also pts. vs large contours
Comparisons ARPES vs (old) LDA
![Page 38: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/38.jpg)
Santander Syro et al. (2009) – T dependences
• Temperature scan into HO state• He lamp low energy (21 eV), high resolution ARPES• Surface states, poor vacuum• Two k space directions: [100] and [110]
• Band of heavy quasi-particles drops below EF upon entering the
HO state• Large restructuring of FS in HO• Many difficulties with data and analyses• Reproducible?
![Page 39: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/39.jpg)
Integrated photoemission spectra along <110> Note quasiparticle peak that moves below To: Dispersing band of heavy
QP, new electron pocket in HO state
Surface state Surface state
![Page 40: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/40.jpg)
Heavy qp band hybridized with light hole conduction band along <110> at 13 K
ARPES intensity
EDC
MDCAverging of 2nd derivatives along E and k
![Page 41: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/41.jpg)
Heavy qp band hybridized with light hole conduction band along <100> at 15 K
ARPES intensity EDC
![Page 42: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/42.jpg)
Yoshida et al.(2010) – Laser Arpes
• Low energy (7 eV) Laser ARPES, high resolution (2 meV), good vacuum technique
• Narrow, dispersive band in HO only, few meV from FS• Yet non-FS crossing• Destroyed with Rh doping on Ru sites• Another hole-like dispersive crossing band and surface
states at ~35 meV• “Periodicity modification“: HO doubling of unit-cell, band
backfolding, predicted by Oppeneer et al. • Low energy ARPES is only sensitive to d-bands, cannot
detect 5f-U bands. Seeing broad (partially hybridized) 4d-Ru bands which appear in HO state
![Page 43: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/43.jpg)
Laser ARPES intensity at 7K for [110] and [100]
Surface state
Hole-like dispersion
![Page 44: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/44.jpg)
Temperature evolution of ARPES intensity integrated over different k cuts
![Page 45: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/45.jpg)
Kawasaki et al.(2011) Soft X-ray ARPES
• Energy 760 eV with resolution 140 meV• Vary energy or detector angle to scan BZ• Spanning vast k-space, all of high symmetry BZ• Bands below 0.6 eV are Ru-4d states, agreeing with previous ARPES
• Band above 0.6 eV to EF disagree with previous ARPES, e.g.,surface band at not observed here. No hole band at X.
• All U-based 5f bands are itinerant!!! • Quasiparticle bands clearly observed at Z(large hole FS and at (large
electron FS) with some nesting• APRES bands consistent with LDA of Oppeneer et al.
![Page 46: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/46.jpg)
BZ with orange and blue scanning planes. Spectral image comparison with LDA band structure
Measured spectral weight along hi-sym.
Calculated BS Agreement with LDA of Oppeneer
Bands 4, 5; 6 cross EF
![Page 47: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/47.jpg)
Photoemission intensity with FS crossings and LDA comparison
Intensity around EF
Indicated band crossings
Calculated band crossings: 6, 5; 4 with C, B; A, and 4; 5 with D; E
![Page 48: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/48.jpg)
Fermi surface images compared with LDA
Integrated intensity Estimated Fermi surfaces with nesting vectors
Band structure FS’’s
![Page 49: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/49.jpg)
Dakovski et al.(2011) Time Resolved ARPES • Pump (1.55 eV)– Probe (29.5 eV) method. First for SCES
• Tune ARPES on URu2Si2 to focus on “hot spots” (maximium gap) in k-space, i.e., below Z in <110> plane as determined from band structure
• Excite quasiparticles via pump, probe their fs decay
• Measurements above To rapid fs decay within hybridization gap
• Measurements below To qp excited above HO gap have longer fs decay times
• Momentum (k) dependent interactions at hot spots causing HO gapping
• Energy resolution: tr-ARPES ≈100meV; ARPES ≈10meV
![Page 50: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/50.jpg)
Femto second spectroscopy at hot spot in HO(12 K)
![Page 51: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/51.jpg)
Comparison spectral intensity above and below To
Note q <110> = 0.56 separating two hot spots in <110>
ARPES (34eV,12K) at Z. Note flat band above EF and agree-ment with Kawasaki for lower bands.
![Page 52: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/52.jpg)
Cartoon model for T evolution of hybrid. and HO gaps
Hot Spots
3D FS with hot spots
See Oppeneer et al. PRB(2010)
![Page 53: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/53.jpg)
Conclusions drawn from ARPES
• Cleaving problem solved, requires ultra high vacuum• Surface states – solved?• Need better resolution at higher E-scans for FS mapping• Inconsistencies among measurements • Present data pushed too far• Yet striving towards efficacious solution of this difficult
technique (note 1990’s ARPES in HTS)• HO gapping not clearly found or hybridization gap seen• First tr-ARPES on heavy fermion material
Stop Thanks
![Page 54: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/54.jpg)
![Page 55: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/55.jpg)
Charge and Spin: Charge and Spin: Visualizing the HO in URuVisualizing the HO in URu22SiSi22
Aynajian, Yazadani et al. PNAS(2010)Aynajian, Yazadani et al. PNAS(2010)
Pegor Aynajian, Eduardo H. da Silva Neto, Colin V. ParkerDepartment of Physics, Princeton University
Yingkai Huangvan der Walls-Zeeman Institute, University of Amsterdam
Abhay PasupathyDepartment of Physics, Columbia University, New York
John MydoshKamerlingh Onnes Laboratory, Leiden University
Ali YazdaniDepartment of Physics, Princeton University
Supported by
![Page 56: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/56.jpg)
![Page 57: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/57.jpg)
![Page 58: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/58.jpg)
Kondo-Fano resonance in URuKondo-Fano resonance in URu22SiSi22
Reminiscent of Fano lineshape in single Kondo impurities
2
2
)/)((1
)/)(()(
o
o
EV
qEVVG
Fano Lineshape
TK=120±10K
q : Ratio of tunneling probability to the descrete level and the continuum.
0 20 40 60 80 100
16
20
24
28
32
36
[m
eV]
Temperature [K]
2 (kBT )2 2(kBTK )2
q=1.3±0.3 ; Eo=5±2meV
![Page 59: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/59.jpg)
![Page 60: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/60.jpg)
![Page 61: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/61.jpg)
D(V) = (V – V0 –iγ) / [(V –V0 –iγ)2 – Δ2]1/2 with γ ~ 1.5 mV
V0
![Page 62: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/62.jpg)
![Page 63: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/63.jpg)
![Page 64: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/64.jpg)
![Page 65: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/65.jpg)
Decomposition
![Page 66: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/66.jpg)
![Page 67: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/67.jpg)
Some ConclusionsSome Conclusions
Recent theoretical work:K. Haule and G. Kotliar, Nature Phys. (2009)M. Maltseva, M. Dzero, and P. Coleman, PRL (2009)Y-f. Yang, PRB(RC) (2009)J. Figgins and D. Morr, PRL (2010)
- Kondo resonance with Fano lineshape.
- Mean field-like T dependence of HO.
- HO asymmetric around EF.
- HO strongest between the surface atoms where the Kondo resonance is enhanced.
-60 -40 -20 0 20 40 60
0.4
0.6
0.8
1
Voltage [mV]
Con
duct
ance
![Page 68: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/68.jpg)
![Page 69: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/69.jpg)
![Page 70: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/70.jpg)
![Page 71: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/71.jpg)
![Page 72: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/72.jpg)
![Page 73: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/73.jpg)
![Page 74: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/74.jpg)
![Page 75: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/75.jpg)
![Page 76: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/76.jpg)
![Page 77: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/77.jpg)
![Page 78: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/78.jpg)
The Hidden Order in URuThe Hidden Order in URu22SiSi22
Palstra et. al, PRL (1985)
Palstra et. al, PRL (1986)
Interplay of the U’s f electrons with the spd electrons and with each other, results in a rich variety of electronic phases.
![Page 79: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/79.jpg)
Variable Temperature STM
Operates between 6K – 180K
Gomes et al. Nature (2007), Pasupathy et al. Science (2008), Pushp et al. Science (2009), Parker et al. PRL (2010)
![Page 80: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/80.jpg)
STM topography on URuSTM topography on URu22SiSi22
Atomically ordered lattice:a~4.2Å corresponding to U or Si
200Å
100Å
0.6
-0.6
![Page 81: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/81.jpg)
STM spectroscopy on URuSTM spectroscopy on URu22SiSi22
Averaged electronic density of states:
Above THO=17.5K Below THO=17.5K
-100 -50 0 50 1000
0.5
1
1.5
2
2.5
Voltage [mV]
Con
duct
ance
[nS
]
-100 -50 0 50 1000
0.5
1
1.5
2
Voltage [mV]
Con
duct
ance
[nS
]
120K
100K
85K
70K
60K
50K
40K
30K
20K
18K
15K
13K
11.7K
10.2K
8.4K
6.6K
-20 -10 0 10 201
2
3
4
5
6
7
8
9
10
Voltage [mV]
Con
duct
ance
[pS
]
6.6K
4K
2K
![Page 82: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/82.jpg)
Entering the hidden order in URuEntering the hidden order in URu22SiSi22
-20 -10 0 10 200
0.5
1
1.5
2
2.5
3
3.5
4
Voltage [mV]
Con
duct
ance
18K
15K
13K
11.7K
10.2K
8.4K
6.6K
4K
2K
A gap in the DOS develops below THO
![Page 83: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/83.jpg)
Entering the hidden order in URuEntering the hidden order in URu22SiSi22
HO turns on with a mean field-like temperature dependece.
Asymmetric gap around EF. Palstra et al. PRL (1985)Maple et al. PRL (1986)Bonn et al. PRL (1998)Wiebe et al. Nature Physics (2009)
0 4 8 12 16 200
1
2
3
4
Normalized by 18KFit to Fano x BCS
[m
eV]
Temperature [K]
![Page 84: Lecture schedule October 3 – 7, 2011 #1 Kondo effect #2 Spin glasses #3 Giant magnetoresistance #4 Magnetoelectrics and multiferroics #5 High temperature.](https://reader034.fdocuments.net/reader034/viewer/2022051019/5697bf921a28abf838c8ecf6/html5/thumbnails/84.jpg)
Kondo lattice in URuKondo lattice in URu22SiSi2 2 ?
Topography Conductance at 6mV q map
1.3
1.2
1.1
1.6
1.4
1.2
nS
- Atomic scale modulations.
- q anti-correlated with topography.
- In single Kondo impurity limit, large q indicates higher tunneling probability to the Kondo resonance.
T=18K