Internal Degrees of Freedom and Quantum Tunneling of the Magnetization in Single-Molecule Magnets E NRIQUE DEL B ARCO Department of Physics – UCF Orlando.

Slides:



Advertisements
Similar presentations
Quasiparticle Scattering in 2-D Helical Liquid arXiv: X. Zhou, C. Fang, W.-F. Tsai, J. P. Hu.
Advertisements

Some New Geometric Phase Effects in Mn 12 Variants Jonathan Friedman Eduardo H. da Silva Neto Michael Foss-Feig Amherst College Funding: NSF, Research.
The Physical Methods in Inorganic Chemistry (Fall Term, 2004) (Fall Term, 2005) Department of Chemistry National Sun Yat-sen University 無機物理方法(核磁共振部分)
Relaxation Time Phenomenon & Application
Bob Sweet Bill Furey Considerations in Collection of Anomalous Data.
Second harmonic generation on multiferroics Optical spectroscopy seminar 2013 spring Orbán Ágnes, Szaller Dávid
II. Spontaneous symmetry breaking. II.1 Weinberg’s chair Hamiltonian rotational invariant Why do we see the chair shape? States of different IM are so.
YOU CAN locate and graph points on the coordinate plane.
Dynamics and thermodynamics of quantum spins at low temperature Andrea Morello Kamerlingh Onnes Laboratory Leiden University UBC Physics & Astronomy TRIUMF.
 From a single molecule to an ensemble of molecules at T ~0 : Both tunneling rate and decoherence increase  LZ probability: P LZ = 1 – exp[-  (  /ħ)
Stephen Hill, Saiti Datta and Sanhita Ghosh, NHMFL and Florida State University In collaboration with: Enrique del Barco, U. Central Florida; Fernando.
CHEM 515 Spectroscopy Vibrational Spectroscopy II.
19_01fig_PChem.jpg Spectroscopy. 18_12afig_PChem.jpg Rotational Motion Center of Mass Translational Motion r1r1 r2r2 Motion of Two Bodies Each type of.
Topics in Magnetism III. Hysteresis and Domains
PHYS Quantum Mechanics PHYS Quantum Mechanics Dr Jon Billowes Nuclear Physics Group (Schuster Building, room 4.10)
I.1 ii.2 iii.3 iv.4 1+1=. i.1 ii.2 iii.3 iv.4 1+1=
2002 London NIRT: Fe 8 EPR linewidth data M S dependence of Gaussian widths is due to D-strainM S dependence of Gaussian widths is due to D-strain Energies.
DNA PACKING: Distances Between DNA Molecules in Crystals Bryson W. Finklea St. John's College DIMACS REU.
Spin Tunneling and Inversion Symmetry E NRIQUE DEL B ARCO Department of Physics – UCF Orlando QCPS II Vancouver.
Coherent Manipulation and Decoherence of S=10 Fe8 Single- Molecule Magnets Susumu Takahashi Physics Department University of California Santa Barbara S.
I.1 ii.2 iii.3 iv.4 1+1=. i.1 ii.2 iii.3 iv.4 1+1=
Measuring quantum geometry From superconducting qubits to spin chains Michael Kolodrubetz, Physics Department, Boston University Theory collaborators:
Symmetry Issues E NRIQUE DEL B ARCO, C HRISTOPHER R AMSEY (UCF) S TEPHEN H ILL ( NHMFL and Physics Department, FSU – Tallahassee ) S ONALI J. S HAH, C.
Symmetries and conservation laws
Introduction to Single Molecular Magnet
Magnetic Material Engineering. Chapter 6: Applications in Medical and Biology Magnetic Material Engineering.
Berry Phase Effects on Bloch Electrons in Electromagnetic Fields
The Standard Model of Electroweak Physics Christopher T. Hill Head of Theoretical Physics Fermilab.
Slide 1/16 Where Are We Going…? Week 10: Orbitals and Terms  Russell-Saunders coupling of orbital and spin angular momenta  Free-ion terms for p 2 Week.
5. Exotic modes of nuclear rotation Tilted Axis Cranking -TAC.
Single-ion and exchange anisotropy effects in small single-molecule magnets* Richard A. Klemm University of Central Florida, Orlando, FL USA and Dmitri.
ENGLISH FOR DESIGN Principles of Design. Elements & Principles.
MOLECULAR SPECTROSCOPY  SPECTROSCOPY IS THAT BRANCH OF SCIENCE WHICH DEALS WITH THE STUDY OF INTERACTION OF ELECTROMAGNETIC RADIATION WITH MATTER.  ELECTROMAGNETIC.
Chirality of Nuclear Rotation S. Frauendorf Department of Physics University of Notre Dame, USA IKH, Forschungszentrum Rossendorf Dresden, Germany.
MOLECULAR SPECTROSCOPY  SPECTROSCOPY IS THAT BRANCH OF SCIENCE WHICH DEALS WITH THE STUDY OF INTERACTION OF ELECTROMAGNETIC RADIATION WITH MATTER.  ELECTROMAGNETIC.
Stephen Hill NHMFL and Florida State University, Physics Outline of talk: Idea behind the title of this talk Nice recent example: Radical Ferromagnet Mononuclear.
Neutron Scattering Studies of Tough Quantum Magnetism Problems
Spontaneous symmetry breaking and rotational bands S. Frauendorf Department of Physics University of Notre Dame.
Macroscopic quantum effects generated by the acoustic wave in molecular magnet 김 광 희 ( 세종대학교 ) Acknowledgements E. M. Chudnovksy (City Univ. of New York,
How do nuclei rotate? The nucleus rotates as a whole.
Single Molecular Magnets
Syntheses of high-spin and cluster molecules Hiroki OSHIO (University of Tsukuba) Syntheses and Magnetic measurements Dr. M. Nihei, A. Yoshida, K. Koizumi,
M. Ueda, T. Yamasaki, and S. Maegawa Kyoto University Magnetic resonance of Fe8 at low temperatures in the transverse field.
Symmetries of the Cranked Mean Field S. Frauendorf Department of Physics University of Notre Dame USA IKH, Forschungszentrum Rossendorf, Dresden Germany.
Unit 2 Vocabulary. Line of Reflection- A line that is equidistant to each point corresponding point on the pre- image and image Rigid Motion- A transformation.
Magnetic Interactions and Order-out-of-disorder in Insulating Oxides Ora Entin-Wohlman, A. Brooks Harris, Taner Yildirim Robert J. Birgeneau, Marc A. Kastner,
NMR study of a mixed-metal molecular magnet Yutaka FUJII (University of Fukui) Contents  Introduction (Magnetic properties)  Experimental results  1.
Spin-lattice relaxation of individual lanthanide ions via quantum tunneling Fernando LUIS Orlando December 20 th 2010 Quantum Coherent Properties of Spins-III.
Symmetries of the Cranked Mean Field S. Frauendorf Department of Physics University of Notre Dame USA IKH, Forschungszentrum Rossendorf, Dresden Germany.
Structure and dynamics of spin polarons induced by doping a Haldane spin-1 chain Collin Broholm * Johns Hopkins University and NIST Center for Neutron.
9.5 Symmetry Then: You drew reflections and rotations of figures. Now: 1. Identify line and rotational symmetries in two-dimensional figures. 2. Identify.
How do nuclei rotate? 4. Rotation about a tilted axis and reflection asymmetry.
Biot-Savart Law for a Single Charge Electric field of a point charge: Moving charge makes a curly magnetic field: B units: T (tesla) = kg s -2 A -1 The.
NMR Studies of nanoscale molecular magnets Y. Furukawa Y. Fujiyoshi S. Kawakami K. Kumagai F. Borsa P. Kogerler Hokkaido University (Japan) Pavia University.
Dynamics of novel molecular magnets V-ring and rare earth compounds Okayama Univ. H. Nojiri Introduction Magnetization step in V-rectangular ring Short.
Supported by: US National Science Foundation, Research Corporation, NHMFL, & University of Florida The effect of anisotropy on the Bose-Einstein condensation.
TC, U. Dorner, P. Zoller C. Williams, P. Julienne
Molecular Spectroscopy
and to what degree they may be forbidden depends on selection rules:
Constructions of Basic Transformations
T. Senthil Leon Balents Matthew Fisher Olexei Motrunich Kwon Park
Electronic polarization. Low frequency dynamic properties.
Nuclear Magnetic Resonance Spectroscopy
S. Hill, N. Anderson, A. Wilson, S. Takahashi, and J. Lawrence
Stephen Hill, Rachel Edwards Nuria Aliaga-Alcalde and George Christou
9.5 : Symmetry I can identify line and rotational symmetries in two‐dimensional figures. I can identify plane and axis symmetries in three‐dimensional.
Hiroyuki Nojiri, Department of Physics, Okayama University
Section 4.3 Rotations Student Learning Goal: Students will identify what a rotation is and then graph a rotation of 90, 180 or 270 degrees on a coordinate.
II. Spontaneous symmetry breaking
4. Rotation about a tilted axis and reflection asymmetry
Presentation transcript:

Internal Degrees of Freedom and Quantum Tunneling of the Magnetization in Single-Molecule Magnets E NRIQUE DEL B ARCO Department of Physics – UCF Orlando In collaboration with: Steve Hill (FSU & NHMFL) and David N. Hendrickson (UCSD) SPONSORED BY: 1

SMMs and Giant Spin Approximation GSA failure / multi-spin description / low-nuclearity SMMs A low nuclearity SMM: Mn 4 EPR and QTM Characterization Asymmetric Berry Phase Interference Symmetry Considerations Motion of Berry Phase Patterns Internal Degrees of Freedom OUTLINE 2

SMMs and the GSA MODEL 8  Mn III (S=2) =  Mn IV (S=3/2) = 6 ~ S = 10 3

SMMs and the GSA MODEL ~ S = 10 up down x y z 4

SMMs and the GSA MODEL ~ S = 10 up down x y z Magnetic field 5

SMMs and the GSA MODEL ~ S = 10 up down x y z on-resonance QT on (fast relaxation) QT off (non relaxation) off-resonance on-resonance 6

SMMs and the GSA MODEL 7

FAILURE of the GSA MODEL Anomalous term Barra et al. (1997) Low-lying excited states Mukhin et al. (2001) QTM btw. different spin lengths Ramsey et al. (2008) observed before in AF molecules Carreta et al. (2007) 8

MULTI-SPIN DESCRIPTION LOW NUCLEARITY SMMs Connection between D mol and d ion Higher-order molecular anisotropy Consequences of weak coupling and spin frustration Internal degrees of freedom and QTM: (Symmetry lowering effects) (Spin selection rules) S. Hill et al., Dalton Transactions (2010). Ni 4 (S = 4)Mn 6 (S = 4,12)Mn 3 (S = 2,6) 9

MULTI-SPIN DESCRIPTION THE CASE OF Mn 4 SMM [Mn 4 (Bet) 4 (mdea) 4 (Hmdea) 2 ] (BPh 4 ) 4 K. J. Heroux et al., unpublished. S = 9 (at low-T) Mn II (S = 5/2) Mn III (S = 2) 10

MULTI-SPIN DESCRIPTION THE CASE OF Mn 4 SMM 11

MULTI-SPIN DESCRIPTION THE CASE OF Mn 4 SMM ( ) 12 test: k=1?

MULTI-SPIN DESCRIPTION THE CASE OF Mn 4 SMM ( ) 13

MULTI-SPIN DESCRIPTION THE CASE OF Mn 4 SMM TIME REVERSAL INVARIANCE OF THE SPIN-ORBIT INTERACTION =ODD =EVEN 14

MULTI-SPIN DESCRIPTION THE CASE OF Mn 4 SMM Second order anisotropy (symmetries): a)3 mutually orthogonal two-fold rotation axes b)3 mutually orthogonal mirror planes c)Inversion center (b) Guarantees invariance w.r.t. reversal of H T IMPOSES SYMMETRIC BPI PATTERNS WHETHER H L =0 or H L  0 xy-mirror symmetry must be broken TO ALLOW ASYMMETRIC BPI PATTERNS W.R.T. H T REVERSAL TRI GUARANTEES THE TWO PATTERNS TO BE MIRROR IMAGES 15

MULTI-SPIN DESCRIPTION THE CASE OF Mn 4 SMM 16

MULTI-SPIN DESCRIPTION Euler angles: 17

MULTI-SPIN DESCRIPTION (z - easy axis) (x - hard axis) CENTRAL ION (2) EXTERNAL IONS (1,3) 18

SOME RELAXATION ISSUES 19

SOME RELAXATION ISSUES 20

SOME RELAXATION ISSUES 21

SOME RELAXATION ISSUES 22

23 ACKNOWLEDGEMENTS STUDENTS: Hajrah M. Quddusi and Simran Singh (UCF) Junjie Liu (FSU) Katie Heroux and Chris Beedle (UCSD)