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Dynamics of clusters and molecules in strong electromagnetic fields: A TDDFT-MD approach Ionization...

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Dynamics of clusters and molecules in strong electromagnetic fields: A TDDFT-MD approach Ionization Environment Time-resolved dynamics Laser Projectile Fondamental studies of mechanisms of irradiation and response of clusters coupled with environment
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Page 1: Dynamics of clusters and molecules in strong electromagnetic fields: A TDDFT-MD approach Ionization Environment Time-resolved dynamics Laser Projectile.

Dynamics of clusters and moleculesin strong electromagnetic fields:

A TDDFT-MD approach

Ionization

Environment

Time-resolved dynamics

Laser

Projectile

Fondamental studies of mechanisms of irradiationand response of clusters coupled with environment

Page 2: Dynamics of clusters and molecules in strong electromagnetic fields: A TDDFT-MD approach Ionization Environment Time-resolved dynamics Laser Projectile.

model-potential electrons

TDDFT-MD

Gen. QM/MMDyn. polar. TDCI

Sta

tics

Dyn

am

ics

ElectronsEnvironment

Methods on the market

Car-Parinello, BO/MDCar-Parinello, BO QM/MM

model-potential electrons

Today: CNOH molecules

+ H2O "environment"

Nan@Ar,Ne,Kr@ MgO

Page 3: Dynamics of clusters and molecules in strong electromagnetic fields: A TDDFT-MD approach Ionization Environment Time-resolved dynamics Laser Projectile.

Nan

n valence e-

n ions (Na+)

TDLDA + ADSIC MD-TDDFT(LDA)non-adiab. dynamics

(≠BO)• explicit• pseudopotentials

TDDFT-MD

laserprojectile

Today, ions are: C4+, O6+, N7+, H+

Page 4: Dynamics of clusters and molecules in strong electromagnetic fields: A TDDFT-MD approach Ionization Environment Time-resolved dynamics Laser Projectile.

Numerical details

represented on 3D grid: 483, 643, 723, 963, …

Goedecker-like (non-local)

dt = 0.5 as

50 fs for H2O

643 54 h 70h

962 x 72 138 h 234 h

fixed ions moving ions

propagation: time-splitting

Verlet algorithm

box size

Home-made codes

Page 5: Dynamics of clusters and molecules in strong electromagnetic fields: A TDDFT-MD approach Ionization Environment Time-resolved dynamics Laser Projectile.

(Time-resolved) observables

from electrons: optical responsecloud deformation, shape, localizationionization

> number of emitted e-

> kinetic E spectrum of emitted e-

> angular distribution of emitted e-

> level depletion

from ions: potential and kinetic (temperature) Eglobal deformation and shapebond lengths, energies

Today: • projectile + H2O• laser + (H2O) H3O+

• laser/proj. + C2H4

Page 6: Dynamics of clusters and molecules in strong electromagnetic fields: A TDDFT-MD approach Ionization Environment Time-resolved dynamics Laser Projectile.

water = electronic insulator gap 10 eV

0.1 au

threshold

Why TDLDA-MD ?

projectile + H2O

charg

e

velocity0

adiab.

sudden

cf. J. Kohanoff

Page 7: Dynamics of clusters and molecules in strong electromagnetic fields: A TDDFT-MD approach Ionization Environment Time-resolved dynamics Laser Projectile.

adiab.

Why TDLDA-MD ?ch

arg

e

velocity0

"fixed e-" +

ionic MD

suddene- TDDFT

+fixed ions

??

Which theory for:dynamical description of

irradiation and response of

electrons and ions ?

?

?

H+ + H2O

C + H2O

Page 8: Dynamics of clusters and molecules in strong electromagnetic fields: A TDDFT-MD approach Ionization Environment Time-resolved dynamics Laser Projectile.

H+ + H2O, low v

Page 9: Dynamics of clusters and molecules in strong electromagnetic fields: A TDDFT-MD approach Ionization Environment Time-resolved dynamics Laser Projectile.

C + H2O, high v

Page 10: Dynamics of clusters and molecules in strong electromagnetic fields: A TDDFT-MD approach Ionization Environment Time-resolved dynamics Laser Projectile.

Laser irradiation of (H2O)H3O+

Epol

I0=1013W/cm2

FWHM=20 fsfrequency scan

IP=-20.6 eV

off-resonant but...

off-resonant

vibrations

2

Page 11: Dynamics of clusters and molecules in strong electromagnetic fields: A TDDFT-MD approach Ionization Environment Time-resolved dynamics Laser Projectile.

C2H4 : optical response

IP: -11.7 eV

6.8 eV

Yabana, Bertsch (2001)

Fourier Transform

8.16 eV 136 eV

Page 12: Dynamics of clusters and molecules in strong electromagnetic fields: A TDDFT-MD approach Ionization Environment Time-resolved dynamics Laser Projectile.

Laser pol.I = 1013 Wcm-2

FWHM = 20 fs

C2H4 : laser irradiation

below resonances on resonance well above resonance

Page 13: Dynamics of clusters and molecules in strong electromagnetic fields: A TDDFT-MD approach Ionization Environment Time-resolved dynamics Laser Projectile.

Ionization (level depletion) from a given electronic levelCompare cases with similar (small) net ionization

C2H4 : ionization mechanisms

Page 14: Dynamics of clusters and molecules in strong electromagnetic fields: A TDDFT-MD approach Ionization Environment Time-resolved dynamics Laser Projectile.

Ionization

Environment

Time resolved dynamics

Laser

Projectile

Dynamical description of irradiationand response of electrons and ions with coupling to environment

Irradiation

of

clusters

and

molecules

by intense

electro-

magnetic

fields

Environment- Hierarchical model Dynamical QM/MM- Na@Ar, Kr, Ne - Na @ MgO - Na@H2O in the oven- C, N, O @ H2O in near future- C, N, O @ H2O @Ar in future

Dynamics of ionization- Self Interaction problem (SIC)- Benchmark TDSIC calculations - Simple approximations in the oven- Dynamical correlations in the future (electronic transport)

Time resolved dynamicsKey importance of non adiabaticelectron-ion dynamics for understanding mechanisms

Thanks toE. Suraud, P.-G. Reinhard,Z.P. Wang,U. Ndongmouo, J. MessudS. Vidal, andyou for your attention !


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