Magnetism and LightMagnetism and Light...Magnetism and LightMagnetism and Light Theo RasingTheo...

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Magnetism and Light Magnetism and Light Theo Rasing Theo Rasing Radboud Universeit Nijmegen

Transcript of Magnetism and LightMagnetism and Light...Magnetism and LightMagnetism and Light Theo RasingTheo...

Magnetism and LightMagnetism and Light

Theo RasingTheo RasingRadboud Universeit

Nijmegen

Magnetism on the timescaleMagnetism on the timescalef th h i t tif th h i t ti

Challenges and Opportunitiesof the exchange interactionof the exchange interaction

Theo RasingRadboud University Nijmegen

JFe-Fe=1.4x10-19 J ~ 40 fs

Magnetism and LightMagnetism and Light

40f40fs

Magnetism and LightMagnetism and Light

TiTi l i til i tiTimeTime--scales in magnetismscales in magnetism

1 ns

100 psSpin

excitation

Spin-orbit (LS)1 ps

100 ps

10 ps L S~ 1 ps - 1 ns

~ 0 01 ps – 0 1 psExchange

interaction1 ps

100 fs~ 0.1 ps-1 ps

0.01 ps 0.1 psinteraction

1 fs

10 fs

1010--100 100 femtosecondfemtosecond!!

L thL th l i til i tiLengthLength--scales in magnetismscales in magnetisml= ~nml nm

Tb+THzTb THz

+f !nm+fs!

JFe-Fe=1.4x10-19 J ~ 40 fsNew Mechanisms? New Mechanisms?

1-2eV,10-100fs

1996 Beaurepaire et al:

60fs60fs

Magnetization is changed within a picosecond!!!g g p

Ultrafast excitation of spins in DyFeO3via the Inverse Faraday effect

Referee A:+

n (d

eg)

0.2“But, unfortunately, the observed signal

Referee A:

day

rota

tio H

0.1H

the observed signal is so small that it

seemsimpractical to utilize

DyFeOT = 95 K

3Fara

d

0 15 30 45 60

0.0impractical to utilize the inverse Faraday

effect for the 0 15 30 45 60

Time delay (ps)

A Kimel et al Nature 435 655 (2005)

purposeof ultrafast control of magnetization in A. Kimel et al, Nature 435 655 (2005). gmetallic materials.”

Ultrafast all optical recording

Femtosecond Magnetic

Ultrafast all optical recording

gRecording in GdFeCo!

C.D. Stanciu et al., patent #P77323PC00,PRL 99, 047601 (2007)

GdFeCo: multi-sublattice ferrimagnet!

Femtosecond Magnetic

GdFeCo: multi sublattice ferrimagnet!

gRecording in GdFeCo!

Ult f t l i d d lUltrafast laser induced reversalin multi-sublattice magnetsg

Gd Fe

40 fs

Fe Gd

12

Gd FGd Fe

Fe GdFe Gd

Angular momentum transfer?Angular momentum transfer?Role of temperature?Role of temperature?Role ofRole of sublatticessublattices??Role of Role of sublatticessublattices??

….. …..

Beyond Landau-Lifshitz dynamics

T i l l b t fi ld 1T

=0.28 Ghz/T

Typical laboratory fields  1T Reversal time  1 ns!

Magnetism on the timescale of exchange: g g

LONGITUDINAL spin dynamics ?

Onsager’s relations for spin dynamicsBaryakhtar, JETP 1984y ,

Generalized force

Magnetic free energy

Generalized positionangular momentum

Symmetry of kinetic coefficients

Anti‐symmetricprecession

Symmetriclongitudinal

More general: multiple sublatticesRate of change free energy

Longitudinal dynamics to lowest order

exchangerelativistic

J.H. Mentink et al., Phys. Rev. Lett. (2012)

More general: multiple sublattices

formation sublattice mutual alignmentspin moment sublattices

Temperature dominated: T>>T t 100fsTemperature dominated: T>>TC , t100fs

Temperature dominated regimep gRelativistic relaxation dominates

Gdelectrons

Gd

Fe Fe

Bloch relaxationDistinct dynamics Gd and Fe

Brown Phys. Rev. 1963Kubo et al. Prog. Theor. Phys. Suppl. 1970

Exchange dominated: T<TC , t1psConservation total angular momentum

S1What if S2=0?

S22

Nonequilibrium

Ground state AFM transient FM!Equilibrium value

Nonequilibrium

Ground state AFM, transient FM!

Exchange dominated regimeExchange dominated regime

MGd M’GdM M

MFe M’Fe

conserve total magnetization M

Gd Gd

spin-spin interactions

Fe Fe

Transfer of magnetization between sublattices!Transfer of magnetization between sublattices!Baryakhtar Fiz. Nizk. Temp. 1985

Laser-induced spin dynamicsUltrafast heating of electrons

10‐100 fslaser pulse

Jex 25 meV 40 fslaser pulse 40 fs

A b h d h d i d i !Access to both temperature and exchange dominated regime!

Element specific view Element specific view ?

BESSY

X rays

BESSYLaser pump – X-ray probe

X-rays400-1400 eV

10-50 ps (FWHM)

50 fs laser pulses1.5 eV, 5-50 mJ/cm2

3 kHz rep. rate

TR-XMCD @BESSYG

1.8 mJ/cm2 @ 190 K

» Fe and Gd sub-lattices switch simultaneously within 50 ps

Gd29Fe62.1Co8.9

Can’t we look faster?

FEMTO SLICING!FEMTO-SLICING!

X-rays400-1400 eV400-1400 eV

100 fs (FWHM)

Element-specific magnetization reversal: 100 fs time resolution

Fe: 100±23 fs

Gd: 427±102 fs

• Different magnetization switching dynamics at Fe and Gd sites !!!

Mentink:

Switching via a novel non-equilibrium state

H

•Transient FERROMAGNETICFERROMAGNETIC

ALIGNMENT for ~1.2 ps

• The system evolves against the exchange interaction !!!

JFe-Gd=4.77x10-20 J ~ 140 fs

Ultrafast magnetism in multi sublatticeUltrafast magnetism in multi-sublatticemagnets

Gd Fe

40 fsFe Gd

Bloch relaxation

Exchange relaxation

What about multi-sublattice ferromagnets?g

Prediction: ultrafast demagnetizationFM coupling

– Coupling makes one sublattice faster, other slower

positive/negative

Coupling makes one sublattice faster, other slower

AFM couplingp g

always positive

– Both sublattices faster than in uncoupled case!

J.H. Mentink et al., Phys. Rev. Lett. (2012)

JFe-Ni=1.4x10-19 J ~ 40 fsFeNiFeNi

1-2eV,10-100fs

simulations experimentsimulations experiment

F l h NiFe slower than Ni

Nanolocalization of all-optical switchingSmallest switching obtained:

~200 nm200 nm

PerspectivesPerspectives

t hemergent phenomena

PerspectivesPerspectives

Sk i ?Skyrmions?

PerspectivesPerspectives

THz

PerspectivesPerspectives

J= J(t) H(t)

Xrays+XMCD+nm+fs!

To conclude:

Coherent optical control of magnetism !With light

Coherent optical control of magnetism !

All-optical ultrafast magnetic recording

Novel (linear) ultrafast reversal path!

Novel transient ferromagnetic state

Future challengesFemto magnetism!

Combine chemical, magnetic

spatial and time resolution: X(Z)FEL!

with many thanks to:IMM

A.V. KimelA.Kirilyuk

Ioffe InstituteProf. R.V. PisarevP. UsachevA.Kirilyuk

F. HansteenD.StanciuA.v.Etteger

Nihon UniversityProf. A. ItohA. Tsukamoto

K.VahaplarA. KalashnikovaJ. Mentink

University of KonstanzDenise HinzkeUlrich NowakBessyUniversity of York

R. ChantrellT.A. OstlerJ B k

BessyI. RaduC. StammT KachelJ.Barker

R.EvansT.KachelN.PontiusHerman Durr (Stanford)

STW, NWO, EU,NanoNed, UltraMagnetron, FANTOMAS

Spectroscopy of Solids and Interfaces

Several PhD / postdoc positions available!

2011