Resonance enhancement of twophoton crosssection for optical storage in the presence of hot band abso - PowerPoint PPT Presentation

1 / 13
About This Presentation
Title:

Resonance enhancement of twophoton crosssection for optical storage in the presence of hot band abso

Description:

This shows that addition of oxygen atoms increases -conjugation. ... derivatives: Effective symmetry of -conjugation pathway', J. Porphyrines and ... – PowerPoint PPT presentation

Number of Views:70
Avg rating:3.0/5.0
Slides: 14
Provided by: msu142
Category:

less

Transcript and Presenter's Notes

Title: Resonance enhancement of twophoton crosssection for optical storage in the presence of hot band abso


1
Resonance enhancement of two-photon cross-section
for optical storage in the presence of hot band
absorption
N. Makarov, A. Rebane, M. Drobizhev, D.
Peone (Department of Physics, Montana State
University, Bozeman, MT 59717, USA) H. Wolleb, H.
Spahni (Ciba Specialty Chemicals Inc, P.O. Box
Ch-4002 Basle, Switzerland) E. Makarova, E.
Lukyanets (Organic Intermediates and Dyes
Institute, Moscow, Russia)
2
Outline
  • Principles of 3D 2PA optical memory
  • 2PA-sensitive photochromes
  • Resonance enhancement
  • 2PA vs. 1PA
  • 2PA in phthalocyanines
  • Summary

3
Principles of 3D 2PA optical memory
4
Need for 2PA-sensitive photochromes
Access with 1 pulse 100fs, 100MHz gt 1TB
read/write in 24 hrs Each bit have to be written
and read by only 1 femtosecond pulse!
5
2PA resonance enhancement
  • A fundamental trade-off between 2PA and 1PA
  • tune laser frequency as close as possible to the
    resonance
  • tune as far as possible to decrease 1PA
    background

6
2PA vs. 1PA
Absorption spectra at different temperatures as
calculated from fluorescence spectrum
Power dependence of the fluorescence signal
7
2PA-sensitive phtalocyanines
8
2PA-sensitive phtalocyanines
  • The change of substituents from butyl groups at
    ?-positions to alkoxy groups at ?-positions
    (molecule 1 vs. 2) increases 2PA cross-sections
    by a factor of nearly 2. This also results in the
    red shift of entire 1PA spectrum by 30 nm (500
    cm-1). The 2PA spectrum also experiences the red
    shift. This shows that addition of oxygen atoms
    increases ?-conjugation.
  • Addition of extra CHO group (molecule 1 vs. 6)
    results in a slight decrease of 2PA cross-section
    as compared to better purified compound 1 and in
    slight increase of the cross-sections compared to
    1a and 1b. The 1PA spectrum practically does not
    change.
  • Substituting an external benzene ring with
    another alkoxy group (molecule 4 vs. 6) produces
    a nearly symmetrical molecule. This shifts both
    Qx and Qy peaks closer to each other so that they
    overlap. A similar shift appears in 2PA spectrum.
    The value of 2PA cross-section reduces by a
    factor of nearly 2, which is probably because of
    reduce of the difference in dipole moments in
    more symmetrical molecule.
  • Addition of extra hydrogen atoms (molecule 3 vs.
    4) reduces degree of symmetry. This slightly
    increases the 2PA cross-section for molecule 3.
    However, its cross-section is smaller than for
    molecules 1 and 6. The reason is more symmetry
    and thus less difference in dipole moments in the
    molecule 3
  • Change of substituent from molecule 3 to 5 makes
    the molecule less symmetrical, and thus increase
    2PA cross-section. However, molecule 6, and
    especially 1 have the highest 2PA cross-sections
    among all studied samples.

9
2PA-sensitive phtalocyanines comparison for 3D
memory
For molecules 3 and 5 absorption spectra of
tautomer forms T1 and T2 significantly overlaps
that makes them not practical as photochromes for
3D optical memory
10
SNR-SBR comparison
11
Summary
  • Because of the requirement of fast speed writing
    and readout, the storage materials need to have
    high molecular 2PA cross section, ?2gt103-104 GM
  • It is evident that the crucial points in this
    approach are the two-photon sensitivity of a
    molecule and the possibility of its photochemical
    transformation from one form to another
  • Careful choice of excitation frequency, along
    with suitable combination of 1PA and 2PA
    properties allow minimizing the negative impact
    of underlying near resonance hot band absorption
  • A brief analysis of changes in 2PA spectra and
    cross-sections due to different substituent
    groups is provided and allow to deduce
    structure-to-properties relations
  • We conclude that from the set of studied
    molecules compound 1 is the most promising for
    rewritable 3D optical memory.

12
References
  • D.A. Parthenopoulos, P.M. Rentzepis,
    Three-Dimensional Optical Storage Memory,
    Science, 245, 843-845 (1989).
  • M. Drobizhev, A. Karotki, M. Kruk, A. Rebane,
    Resonance enhancement of two-photon absorption
    in porphyrins, Chem. Phys. Lett., 355, 175-182,
    (2002).
  • M. Drobizhev, Y. Stepanenko, Y. Dzenis, A.
    Karotki, A. Rebane, P.N. Taylor, H.L. Anderson,
    Understanding Strong Two-Photon Absorption in
    -Conjugated Porphyrin Dimers via Double-Resonance
    Enhancement in a Three-Level Model, J. Am. Chem.
    Soc., 126, 15352-15353 (2004).
  • M. Drobizhev, F. Meng, A. Rebane, Y. Stepanenko,
    E. Nickel, C.W. Spangler, Strong two-photon
    absorption in new asymmetrically substituted
    porphyrins interference between charge-transfer
    and intermediate-resonance pathways, J. Phys.
    Chem. B, 110, 9802-9814 (2006).
  • M. Drobizhev, Y. Stepanenko, Y. Dzenis, A.
    Karotki, A. Rebane, P.N. Taylor, H.L. Anderson,
    Extremely strong near-IR two-photon absorption
    in conjugated porphyrin dimmers quantitative
    description with three-essential-states model,
    J. Phys. Chem. B, 109, 7223-7236 (2005).
  • M. Drobizhev, A. Karotki, M. Kruk, N. Zh.
    Mamardashvili, A. Rebane, Drastic enhancement of
    two-photon absorption in porphyrins associated
    with symmetrical electron-accepting
    substitution, Chem. Phys. Lett., 361, 504-512
    (2002).
  • I. Renge, H. Wolleb, H. Spahni, U.P. Wild,
    Phthalonaphthalocyanines New Far-Red Dyes for
    Spectral Hole Burning, J. Phys. Chem. A 101,
    6202-6213, (1997).
  • A.A. Gorokhovskii, R.K. Kaarli, L.A. Rebane,
    Hole Burning in Contour of a Pure Electronic
    Line in a Shpolskii System, JETP Lett., 20,
    216-218, (1974).
  • M. Drobizhev, A. Karotki, A. Rebane, Persistent
    Spectral Hole Burning by Simultaneous Two-Photon
    Absorption, Chem. Phys. Lett., 334, 76-82,
    (2001).
  • A. Rebane, M. Drobizhev, A. Karotki, Y. Dzenis,
    C.W. Spangler, A. Gong, F. Meng, New two-photon
    materials for fast volumetric rewritable optical
    storage, in Proc. SPIE, Advanced Optical and
    Quantum Memories and Computing, Eds. H.J. Coufal,
    Z.U. Hasan, (SPIE, Belligham, WA, 2004), 5362,
    pp. 10-19.
  • M. Drobizhev, A. Karotki, M. Kruk, A.
    Krivokapic, H.L. Anderson, A. Rebane, Photon
    energy upconversion in porphyrins one-photon
    hot-band absorption versus two-photon
    absorption, Chem. Phys. Lett., 370, 690-699
    (2003).
  • A. Karotki, M. Drobizhev, Y. Dzenis, P.N.
    Taylor, H.L. Anderson, A. Rebane, Dramatic
    enhancement of intrinsic two-photon absorption in
    a conjugated porphyrin dimer, Phys. Chem. Chem.
    Phys., 6, 7-10 (2004).
  • M. Drobizhev, A. Karotkii, A. Rebane, Dendrimer
    molecules with record large two-photon absorption
    cross section, Opt. Lett., 26, 1081-1083 (2001).
  • M. Drobizhev, N.S. Makarov, A. Rebane, E.A.
    Makarova, E.A. Lukyanets, Two-photon absorption
    in tetraazachlorin and its benzo-and
    2,3-naphtho-fused derivatives Effective symmetry
    of ?-conjugation pathway, J. Porphyrines and
    Phtalocyanines, Proc. Of the International
    Conference on Porphyrines and Phtalocyanines,
    ICPP-4, Rome, Italy, 2-7 July, 2006 (to be
    published).

13
M.E. Marhic, Storage limit of two-photon-based
three-dimensional memories with parallel access,
Opt. Lett., 16, 1272-1273 (1991).
For systems that use parallel access by
simultaneous writing or reading of bits located
in an entire common plane, diffraction sets a
limit to the storage density that is far smaller
than that for sequential operation. Comparable
densities can be achieved by using a
three-dimensional waveguiding structure.
Write a Comment
User Comments (0)
About PowerShow.com