ECRYS-2011, August, 15-27, 2011 at the Institute of Scientific Studies in Cargese, Corse Charge...
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ECRYS-2011, August, 15-27, 2011 at the Institute of Scientific Studies in Cargese, Corse Charge Fluctuation, Charge Ordering and Zero-Gap State in Molecular
ECRYS-2011, August, 15-27, 2011 at the Institute of Scientific
Studies in Cargese, Corse Charge Fluctuation, Charge Ordering and
Zero-Gap State in Molecular Conductors Toshihiro Takahashi
Department of Physics, Gakushuin University, Mejiro 1-5-1,
Toshima-ku, Tokyo 171-8588, Japan
Slide 2
Charge Fluctuation Charge Ordering Zero-Gap State
San-dai-banashi A style of Japanese traditional comic story,
rakugo. Three keywords are given independently by the audience. The
storyteller, rakugo-ka, makes ad lib a consistent comic story using
all the keywords. 3 keywords:
Slide 3
Outline Introduction to NMR technique to probe charge degree of
freedom Charge fluctuation and charge ordering in -phase BEDT-TTF
salts Charge disproportionation in the zero-gap state of -BEDT-TTF
2 I 3 Coupling with the permanent electric dipolar moment of anion
in TMTSF 2 FSO 3 Charge disproportionation in -type BETS salts
Summary & Remarks
Slide 4
Outline Introduction to NMR technique to probe charge degree of
freedom Charge fluctuation and charge ordering in -phase BEDT-TTF
salts Charge disproportionation in the zero-gap state of -BEDT-TTF
2 I 3 Coupling with the permanent electric dipolar moment of anion
in TMTSF 2 FSO 3 Charge disproportionation in -type BETS salts
Summary & Remarks
Slide 5
Simple Picture of Charge Ordering (CO) 1/4-filled system, D 2 A
or DA 2, without large dymerization One carrier per two molecules
Coulomb interaction, U & V, finding a charge arrangement to
minimize Coulomb energy As including transfer =>rich variety of
phenomena
Slide 6
Charge Ordering vs. Charge Disproportionation Long-range Charge
Ordering (CO) vs. Charge Disproportionation (CD) Charge Frustration
Melting of CO Charge Fluctuation/Charge Dynamics Various
Optical/Dielectric responses
Slide 7
How can NMR detect CO/CD? Not detecting charge but spindensity
Not detecting Long Range CO but just the distribution of local
charge (spin) What we observed in CO/CD systems in common were
anomalous broadening of NMR spectrum. How can CO/CD affect NMR
spectrum and other NMR parameters? Note that;
Slide 8
Brief introduction to NMR (Nuclear Magnetic Resonance) Nuclear
spin carries angular momentum, and magnetic moment,. Zeeman
splitting in strong magnetic field: Resonance condition: Magnetic
moment; Angular momentum; Zeeman splitting for I=1/2 Resonance
Condition;
Slide 9
NMR can detect CO/CD Nuclei in material see local fields given
by the environments in addition to the external field. What we
detect with NMR are the information of the local field; Central
shift Local field distribution Local field at each nuclear
site
Slide 10
Interaction with electrons Orbital motion and Chemical shift
Spin interaction and Knight shift Orbital motion Spin Local fields
are produced by surrounding electrons!
Slide 11
Interaction with electrons Orbital motion and Chemical shift
Spin interaction and Knight shift Shielding current Magnetic
shielding current gives local field. Chemists concerns the
isotropic part of the chemical shift tensor. It is usually small
compared with the spin contribution.
Slide 12
Interaction with electrons Orbital motion and Chemical shift
Spin interaction and Knight shift Spin magnetization
Slide 13
Interaction with electrons Orbital motion and Chemical shift
Spin interaction and Knight shift Spin magnetization Lone-pair spin
contribution is also anisotropic and much larger than orbital
contribution in the present systems.
Slide 14
Hyperfine interaction Hyperfine interaction Hyperfine
interaction tensor Knight shift ~ proportional to electron spin
susceptibility ~ anisotropic due to the hyperfine tensor for a pure
-electron with uniaxial symmetry
Slide 15
Hyperfine interaction Inhomogeneity of Knight shift causes
inhomogeneous broadening. Inhomogeneous width should be
proportional to the Knight shift. ~ proportional to electron spin
susceptibility ~ anisotropic due to the hyperfine tensor
Slide 16
Typical Materials, exhibiting CO 1/4-filled Organic molecular
conductors, of the chemical form of A 2 D Q-1D system DI-DCNQI 2 Ag
(K. Hiraki, 1998) TMTTF 2 X (PF 6, AsF 6, ) (D.S. Chow, 2000) 2D ET
salts -ET 2 I 3, (Y. Takano, 2001) -ET 2 RbZn(SCN) 4 (K. Miyagawa,
2000, R. Chiba, 2001) X-ray, Raman & IR spectroscopy also
confirmed CO in various materials
Slide 17
Outline Introduction to NMR technique to probe charge degree of
freedom Charge fluctuation and charge ordering in -phase BEDT-TTF
salts Charge disproportionation in the zero-gap state of -BEDT-TTF
2 I 3 Coupling with the permanent electric dipolar moment of anion
in TMTSF 2 FSO 3 Charge disproportionation in type BETS salts
Summary
Slide 18
-(ET) 2 MZn(SCN) 4 (M=Rb,Cs) H. Mori et al., Phys. Rev. B57, 12
023(1998)
Slide 19
Electric and Magnetic property electric resistivityspin
susceptibility RbZn salt CsZn salt
Slide 20
Charge ordered transition in - (ET) 2 RbZn(SCN) 4 K. Miyagawa
et al., 2000 Charge Order T
p a =2kbar electron hole Ambient Pressure YM X Fermi Surface CP
(p a =4kbar) Contact Point & Zero Gap State (ZGS) Dirac cone p
a > 3kbar CP (contact point) M Zero Gap State under pressure
Kobayashi et al., JPSJ (2005)
Slide 33
The first ZGS in a bulk system was confirmed! All peculiar
ground states are explained on the basis of unified band
parameters! CO / ZGS (NGS) / SC Further questions: How does CO
behave under pressure? What is the relation between CO and the ZGS?
How about in other isostructural salts?
Slide 34
Development of CD above T MI CO of CD aboveT MI Because of
site-dependence? Precursor effect of CO? Pattern of CO C > B cf.
-ray Relation to the ZGS under pressure H S. Moroto 2003 Y. Takano
1999 C C
Slide 35
Measurements under pressure P = 0.1 ~ 1.1 GPa H 0 = 7 T (75
MHz) in the ab-plane Pressure cell by Prof. W. Kang, Ewha Womans
Univ., Seoul H0H0 -ET 2 I 3
Slide 36
T-dependence of Local Susceptibilities under pressure Local
susceptibility is the smallest on B molecule. B molecule is a
charge-poor site!
Slide 37
Title: Charge Ordering in $\alpha$-(BEDT-TTF)$_2$I$_3$ by
Synchrotron X-ray DiffractionAuthors: by Toru Kakiuchi, Yusuke
Wakabayashi, Hiroshi Sawa, Toshihiro Takahashi, Toshikazu
NakamuraPublished: October 25, 2007J. Phys. Soc. Jpn., Vol.76,
No.11, p.113702 Charge Ordering determined by Synchrotron X-ray
Diffraction CD in the metallic state at ambient pressure: B
molecule is charge- rich! ~ inconsistent to the NMR results?
Kakiuchi et al., JPSJ (2007)
Slide 38
Contact Point Dirac cone Theory explains this difficulty
Transfer energies evaluated from first principle calculation by
Kino A,A' = +0.54 B = +0.64 C = +0.29 Katayama et al., JPSJ (2008)
B molecule is charge-rich! Contact Point & Zero Gap State
(ZGS)
Slide 39
Theory explains this difficulty Katayama et al., Eur.Phys.
(2009) Local susceptibility is proportional to the density of state
around the contact point, and not to the local charge!
Slide 40
Theory explains this difficulty Local susceptibility is
determined by the density of states around the contact point.
U=0.4, V p =0.05, V c =0.17
Slide 41
ZG 1. Non-stripe CO develops at low temperatures and under
pressure. It does not break the lattice symmetry. 2. Charge-rich B
molecule has the smallest local susceptibility. It is consistent
with X-ray and theoretical analysis. 3. Non-stripe CO may be
relevant to the stabilization of the ZGS. Conclusions ZGS T
Slide 42
ZG Non-stripe CO should come from a band nature together with
Coulomb interaction. Characteristic time of charge dynamics, if
any, should be much shorter than the NMR time scale. The mechanism
of CD is quite different from the case of the - salt. ZGS T What is
the origin of CO in the metallic state of -I 3 salt?
Slide 43
Outline Introduction to NMR technique to probe charge degree of
freedom Charge fluctuation and charge ordering in -phase BEDT-TTF
salts Charge disproportionation in the zero-gap state of -BEDT-TTF
2 I 3 Coupling with the permanent electric dipolar moment of anion
in TMTSF 2 FSO 3 Charge disproportionation in type BETS salts
Summary
Slide 44
Bechgaard Salt with asymmetric anion, FSO 3 Crystal Structure
of (TMTSF) 2 FSO 3 a- axis FSO 3 - TMTSF molecule
Slide 45
(TMTSF) 2 FSO 3 under Pressure Y. J. Jo et al., 2003
Thermoelectric power Phase diagram Resistivity
Slide 46
77 Se-NMR Lineshape Coexistence of sharp & broad components
4 sharp peaks ~4 Se-sites in a unit cell Line broadening Sharp
component appears with short delay ~ 3 s with long delay ~ 600
s
Slide 47
77 Se-NMR T 1 -1 No anomaly at 90 K. Double comp. of T 1 -1
below 40 K. Broader line has shorter T 1 Sharper line has longer T
1
Slide 48
Angular dependence of 77 Se-NMR Lineshape
Slide 49
Inhomogeneous width assuming CD of 0.6~0.4 Angular dependence
of 77 Se-NMR Lineshape
Slide 50
Enhancement of 77 Se-NMR T 2 -1 Anomalous T 2 -1 enhancement
was not observed at ambient pressure. Double Peaks of T 2 - 1
around 90 K & 70 K. 90 K: the phase boundary (I). 70 K: inside
the intermediate phase. 0.65 GPa Possibility of slow Charge
fluctuations as in the q-ET salt.
Slide 51
0.4 GPa Anion dynamics seen by 19 F-NMR Coexistence of 3D-
rotated signal and Anion-ordered signal in the region between
boundary I & II. 3D-rotated signal Anion-ordered signal
Slide 52
0.4 GPa Anion dynamics seen by 19 F-NMR 3D-rotated signal
Anion-ordered signal
Slide 53
0.4 GPa T-dependence of 19 F-NMR T 1 -1 BBP relaxation
suggesting 3D-rotation Coupling with methyl-group rotation in AO
state?
Slide 54
Conclusions Metallic phase above I and Nonmagnetic Insulating
phase below II were confirmed. Large charge disproportionation was
found in the anomalous metallic phase with below I. Coexistence of
the metallic and insulating phase suggests the boundary II is of
first order. 19 F-NMR & X-ray analysis strongly suggest that;
Boundary I associates with the ordering of tetrahedrons; Boundary
II with the ordering of elec. dipoles. Metal Anomalous metal with
CD Nonmag. Insulator
Slide 55
CD was observed in the region where partial ordering of FSO 3
appears. Magnitude of CD is moderate compared with the other CD
systems. CD may be due to the intramolecular charge imbalance and
the first indication of the coupling between the electric dipoles
and the carriers. Metal Nonmag. Insulator What is the origin of CD
in FSO 3 salt? + - - +
Slide 56
Outline Introduction to NMR technique to probe charge degree of
freedom Charge fluctuations and charge ordering in - phase BEDT-TTF
salts Charge disproportionation in the zero-gap state of -BEDT-TTF
2 I 3 Coupling with the permanent electric dipolar moment of anion
in TMTSF 2 FSO 3 Charge disproportionation in -type BETS salts
Summary
Slide 57
-d interaction on -(BETS) 2 FeCl 4 : 77 Se NMR K. Hiraki 16, H.
Mayaffre 1, M. Horvatic 2, C. Berthier 12, H. Tanaka 3, A.
Kobayashi 4, H. Kobayashi 5 and T. Takahashi 6 1. Laboratoire de
Spectrometrie Physique, Universit Joseph Fourier 2. Grenoble High
Magnetic Field Laboratory 3. Nanotechnology Research Institute,
AIST 4. Department of Chemistry, University of Tokyo 5. Institute
for Molecular Science 6. Department of Physics, Gakushuin
University Acknowledgement We would like to thank prof. K. Takimiya
(Hiroshima University)
Slide 58
Structure and electronic properties H ext H. Kobayashi et al.,
J. A. C. S. 118, 368 (1996) H. Tanaka et al., J. A. C. S. 121, 760
(1999) H. Akutsu et al., PRB58, 9294 (1998) Brossard et al. EPJ B1,
439(1998) AFI Balicas et al. PRL87, 067002(2001) SC
Slide 59
Balicas et al. PRL87, 067002(2001) H ext Fe 5/2 spin Mechanism
of Field-Induced SC Orbital decoupling effect is suppressed by
applying external filed strictly parallel to the conducting 2D
layer (a*c plane). Jaccarino-Peter mechanism: Exchange field from
magnetic ions (Fe 2+ : S=5/2) compensates the external field; SC
appears when, H 0 + H exch H c2, where H exch = J /g B Our aims is
to confirm the exchange field seen by -electrons through 77 Se-NMR
AFI SC
Slide 60
H 0 dependence of NMR shift at 1.5K M10 magnet GHMFL
oct2005/apr2006 7/16 5 B J=322 T
Slide 61
Linewidth vs. magnetization Excess broadening below 30K is very
likely due to CD!
Slide 62
Angular dependence of linewidth in the Fe-salt Angular
dependence of spectral width is proportional to that of the central
shift, suggesting CD.
Slide 63
Angular dependence of linewidth in the Fe- and the Ga-salt Fe
ions are not relevant to CD! Organic BETS layers should be
responsible for CD!
Slide 64
Which mechanism gives the CD? Charge imbalance was already
suggested in the Fe-salt by; microwave/Matsui PRB 2003 1 H NMR/Endo
JPSJ 2002 X ray/Komiyama JPSJ 2004 I-V characteristics./ Toyota PRB
2002 15/16 Magnetic Fe ions are not relevant to the line
broadening. It should be attributed to the inhomogeneity of the
local susceptibility, , in the BETS layer, suggesting large CD,
while their dynamics have not yet been examined. Mechanism of CO is
not clarified yet.
Slide 65
Dielectric Anomaly H. Matsui, 2003
Slide 66
Outline Introduction to NMR technique to probe charge degree of
freedom Charge fluctuations and charge ordering in - phase BEDT-TTF
salt Charge disproportionation in the zero-gap state of -BEDT-TTF 2
I 3 Coupling with the permanent electric dipolar moment of anion in
TMTSF 2 FSO 3 Charge disproportionation in type BETS salts Summary
& Remarks
Slide 67
Summary-1 Anomalous NMR line broadening was observed in
metallic states of various molecular conductors; -(ET) 2 MZn(SCN)
4, (M=Rb, Cs) -(ET) 2 I 3 (TMTSF) 2 FSO 3 -(BEST) 2 MCl 4, (M=Fe,
Ga) Angular dependence of the width is proportional very well to
that of the central shift of the spectrum, which suggests the
appearance of CO/CD. Details of the nature of CO/CD are found quite
different among them.
Slide 68
Summary-2 -(ET) 2 MZn(SCN) 4, (M=Rb, Cs) Long-range CO in the
Rb-salt CD due to the competition of different COs -(ET) 2 I 3
Long-range CO; Non-stripe CO in the ZGS CD due to band formation,
enhanced by Coulomb correlation. (TMTSF) 2 FSO 3 CD in the metallic
state under pressure. Coupling with electric dipoles on FSO 3 anion
may be relevant. -(BEST) 2 MCl 4, (M=Fe, Ga) BETS layers are
responsible for CD in the metallic state. Mechanisms responsible
for CO/CD are full of variety!
Slide 69
Concluding remarks Increasing numbers of molecular conductors
are found to exhibit CO/CD. CO/CD are found to interplay with
various types of ground states. Even Superconductivity is found in
the vicinity of CO ed state. -(ET) 2 I 3 under uniaxial strain
(Tajima, 2003) -(DODHT) 2 PF 6 T c = 3.1 K at 16.5 kbar: Nishikawa,
2003) -(meso-DMBEDT-TTF) 2 PF 6 T c = 4.3 K at 4.0 kbar: Kimiura,
2004 CO/CD will open new possibility of molecular conductors and
other correlated systems!
Slide 70
Collabrators: Ko-ichi Hiraki, Yoshiki Takano, Ken-ichi Arai,
Shiro Harada, Hidetaka Satsukawa Dept. Physics, Gakushuin Univ. N.
Tajima, H.M. Yamamoto, R. Kato RIKEN, JST-CREST, and T. Naito,
Ehime Univ. !
Slide 71
Slide 72
Comparison with the other isostructural -phase I 3 salts BETS
BEDT-STF Single crystal 1 peace with double bond carbons enriched
with 13 C Ensemble of small single crystals with all Se sites
enriched with 77 Se isotope Large amount of small single crystals
containing natural 77 Se (7.5%) ET C C Se Single crystal 1 peace
with double bond carbons enriched with 13 C Small single crystal
containing natural 77 Se (7.5%) C C
Slide 73
-(BETS) 2 I 3 v.s. -(ET) 2 I 3 M. Inokuchi et al, BCSJ 68
(1995) 547 N. Tajima et al, EPL 80 (2007) 47002 -BETS 2 I 3 may
correspond to -ET 2 I 3 under pressure of ~1.1 GPa
Slide 74
Angular dependence of resonance shift for the 3 peaks
Sinusoidal dependences Relative phase Red-Green58 Black-Green78
Black-Red20 Amplitude ratio Green : Red : Black = 2.8 1 3.0 ~ 0.6
0.2 0.6