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35th Winter Colloquium on The Physics of Quantum Electronics Snowbird, Utah -- January 2-6, 2005

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Creating and Manipulating Electronic Coherences in Functionalized Semiconductor Nanostructures

Sabas Abuabara, Luis G.C. Rego and Victor S. Batista

Department of Chemistry, Yale University, New Haven, CT 06520-8107

TiO2-anatase semiconductor nanostructure functionalized with catecholadsorbates

- Interfacial Electron Transfer Dynamics
- Relevant timescales and mechanisms
- Dependence of electronic dynamics on the crystal symmetry and dynamics

- Effect of nuclear dynamics
- Whether nuclear motion affects transfer mechanism or timescale
- Implications for quantum coherences

- Hole Relaxation Dynamics
- Decoherence timescale
- Possibility of coherent control

L.G.C. Rego, S.T. Abuabara and V.S. Batista, J. Chem. Phys., submitted (2004)

L.G.C. Rego, S.T. Abuabara and V.S. Batista Quant. Inform. Comput., submitted (2004)

S. Flores and V.S. Batista J. Phys. Chem. B 108 ,6745 (2004)

L.G.C. Rego and V.S. Batista, J. Am. Chem. Soc.125, 7989 (2003)

V.S. Batista and P. Brumer, Phys. Rev. Lett.89, 5889 (2003), ibid. 89, 28089 (2003)

VASP/VAMP simulation packageHartree and Exchange Correlation Interactions: Perdew-Wang functional Ion-Ion interactions: ultrasoft Vanderbilt pseudopotentials

TiO2-anatase nanostructure functionalized by adsorbed catechol

124 atoms:

32 [TiO2] units = 96

catechol [C6H6-202] unit = 12

16 capping H atoms = 16

O-H stretch, 3700 cm-1

(H capping atoms)

C-H stretch

3100 cm-1

C-C,C=C stretch

1000 cm-1,1200 cm-1

TiO2 normal modes

262-876 cm-1

- Accurate description of charge delocalization requires simulations in extended model systems.
- Simulations in small clusters (e.g., 1.2 nm nanostructures) are affected by surface states that speed up the electron injection process
- Periodic boundary conditions alone often introduce artificial recurrencies (back-electron transfer events).

[-101]

Three unit cells extending the system in

[-101] direction

[010]

..

- H is the Extended Huckel Hamiltonian in the basis of Slater type atomic orbitals (AOâ€™s) including
- 4s, 3p and 3d AOâ€™s of Ti 4+ ions
- 2s and 2p AOâ€™s of O 2- ions
- 2s and 2p AOâ€™s of C atoms
- 1s AOâ€™s of H atoms
- 596 basis functions per unit cell
- S is the overlap matrix in the AOâ€™s basis set.

How good is this tight binding Hamiltonian?

photoexcitation

LUMO,LUMO+1

HOMO

HOMO

Band gap =3.7 eV

Conduction Band

Valence Band

ZINDO1 Band gap =3.7 eV

Exp. (2.4 nm) = 3.4 eV

Exp. (Bulk-anatase) = 3.2 eV

, where

and with

are the instantaneous MOâ€™s

obtained by solving the extended-HÃ¼ckel generalized eigenvalue equation:

Which in t0 limit we approximate as

Derive propagator for midpoint scheme:

Hamiltonian changes linearly during time step /

Forward and Backwards propagation equal

TiO2 system extended in [-101] direction with PBC in [010] direction

Grey â€˜Balloonsâ€™ are isosurface of electronic density

Allow visualization of mechanism

Propagation Schemecontâ€™d

- With this scheme, we can calculate for all t>0 :
- electronic wavefunction
- electronic density
- Define the Survival Probability for electron(hole) to be found on specific adsorbate molecule

PMOL(t)

Compute Hole Population on each adsorbate

t=15 ps

Super-exchange hole transfer

After photoinduced electron-hole pair separation due to

electron injection

Hole is left behind, off resonant w.r.t. conduction and valence bands

Dynamics on Adsorbate Monolayer

PMOL(t)

PMOL(t)

(3)

(1)

(2)

We investigate the feasibility of manipulating the underlying hole relaxation dynamics by merely affecting the relative phases of the state components (e.g., by using femtosecond laser pulses)

L

C

LUMO

CB

superexchange

hole

HOMO

w12

2p pulses

HOMO-1

VB

TiO2 semiconductor

Adsorbate molecules (C, L,â€¦)

- Proposals for the Inhibition of Decay by Using Pulses:
- G.S. Agarwal, M.O. Scully and H. Walther
- (a) Phys. Rev. Lett.86, 4271 (2001);
- (b) Phys. Rev. A63, 44101 (2001)
- L. Viola and S. Lloyd Phys. Rev. A58, 2733 (1998),
- L. Viola, E. Knill and S. Lloyd Phys. Rev. Lett.82, 2417 (1999)
- D. Vitali and P. Tombesi Phys. Rev. A59, 4178 (1999)
- W.M. Itano, D.J. Heinzen, J.J. Bollinger and D.J. Wineland
- Phys. Rev. A41, 2295 (1990)

t = 200 fs, w12

t= k*t

Apply pulsed radiation tuned to frequency w21

2-p pulses (200 fs spacing)

2-p pulses (200 fs spacing)

14 fs

60 fs

2-p pulses (200 fs spacing)

2 fs

42 fs

Investigation of Coherent-Control contâ€™d

- We have investigated interfacial electron transfer and hole tunneling relaxation dynamics according to a mixed quantum-classical approach that combines ab-initio DFT molecular dynamics simulations of nuclear motion with coherent quantum dynamics simulations of electronic relaxation.
- We have investigated the feasibility of creating entangled hole-states localized deep in the semiconductor band gap. These states are generated by electron-hole pair separation after photo-excitation of molecular surface complexes under cryogenic and vacuum conditions.
- We have shown that it should be possible to coherently control superexchange hole-tunneling dynamics under cryogenic and vacuum conditions simply by applying a sequence of ultrashort 2p-pulses with a frequency that is resonant to an auxiliary transition in the initially populated adsorbate molecule.
- We conclude that large scale simulations of quantum dynamics in complex molecular systems can provide valuable insight into the behavior of the quantum coherences in exisiting materials which might be essential to bridge the gap between the quantum information and quantum control communities.

- NSF Nanoscale Exploratory Research (NER) Award ECS#0404191
- NSF Career Award CHE#0345984
- ACS PRF#37789-G6
- Research Corporation, Innovation Award
- Hellman Family Fellowship
- Anderson Fellowship
- Yale University, Start-Up Package
- NERSC Allocation of Supercomputer Time
- PQE XXXV Organizers:Â Â Â Â M. Scully, G. R. Welch, M. S. Zubairy, P. Brumer
- Thank you !