Femtosecond lasers and their applications for optical memory - examples of research are presented below.
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Trestles femtosecond Ti:Sapphire laser
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pump laser
Teahupoo Rider femtosecond amplified
Ti:Sapphire laser
Mavericks femtosecond
Cr:Forsterite laser
Tamarack femtosecond fiber laser (Er-doped
fiber)
Buccaneer femtosecond OA fiber laser (Er-doped
fiber) and SHG
Cannon Ultra-broadband light source
Tourmaline femtosecond Yt-doped fiber laser
Femtosecond pulse measurement instrumentation -
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Reef scanning and single shot
femtosecond autocorrelators
Avoca SPIDER -
Spectral phase interferometry for direct electric-field reconstruction (SPIDER)
Rincon third order femtosecond
cross-correlator (third order autocorrelator TOAC) also referred to as
contrastmeter
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Beacon femtosecond fluorescence
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Femtosecond Systems and Accessories -
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Femtosecond Micromachining
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Pismo pulse picker (ultrafast
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Wavelength conversion:
second and third harmonics generators for femtosecond lasers
Kirra Optical Faraday Rotators and
Isolators
Lasers, misc.
DPSS green laser
Compact pulsed Nd:YAG lasers
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Deep Sea excimer lasers
Precision Optical Components, Crystals and Wafers
We offer variety of materials that can be used for optical data
storage.
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Optics from A to Z - just few examples of our
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Femtosecond Laser Structuring of As2S3 Glass for Erasable
and Permanent Optical Memory
Saulius Juodkazis, Andrei V. Rode, Toshiaki Kondo, Hiroaki Misawa, Marek Samoc,
Barry Luther-Davies
The nonlinear absorption coefficient of As2S3 glass has been measured to be 2.0
cm/GW for femtosecond pulses at 800 nm. Femtosecond laser structuring via two
photon absorption in bulk As2S3 glass by erasable and permanent photo-darkening
is demonstrated using both holographic and direct multi-beam laser writing.
Three-dimensional optical memory using a human fingernail
Akihiro Takita, Hirotsugu Yamamoto, Yoshio Hayasaki, Nobuo Nishida,
and Hiroaki Misawa
Optics Express, Vol. 13, Issue 12, pp. 4560-4567
Keywords (OCIS):
(140.7090) Lasers and laser optics : Ultrafast lasers
(210.4680) Optical data storage : Optical memories
(300.6280) Spectroscopy : Spectroscopy, fluorescence and luminescence
Abstract
We realized optical data storage in a human fingernail. A structural change is
recorded by irradiating a focused femtosecond laser pulse and is read out with
fluorescent observation by making use of an increased fluorescence intensity.
The shape of the structural changes drastically depends on the irradiated pulse
energy. The fluorescence spectrum of the structure coincided with the
auto-fluorescence spectra of a fingernail and a heated fingernail. It is
suggested that the increased fluorescence is most likely caused by a local
denaturation of the keratin protein by the femtosecond laser pulse irradiation.
We demonstrate that the increased fluorescence effect is useful for reading out
three-dimensionally recorded data.
Femtosecond laser induced PL change in Sm-doped sodium
borate glass and 3D optical memory
Seungphil Lee a, b, Myeongkyu Leea, and Kisoo Limb
a Department of Materials Science and Engineering, Yonsei University, 134
Shinchon-dong, Seodaemun-ku, Seoul 120-749, Korea
bDepartment of Physics, Chungbuk National University, 48 Gaesin-dong, Cheongju,
Chungbuk 361-763, Korea
Abstract
We report on a femtosecond laser-induced photoluminescence (PL) change in Sm-doped
sodium-borate glass and its potential application to three-dimensional optical
memory. Irradiation with a femtosecond pulsed laser (800 nm, 1 kHz, 100 fs)
induced a new PL peak near 682 nm, resulting from the photoreduction of Sm ions
from Sm3+ to Sm2+. This makes it possible to readout the stored data by
detecting the new PL peak as a signal. Multilayer patterns of various dot sizes
and interlayer spacings were fabricated by femtosecond pulsed laser. These
patterns were read out by a fluorescent confocal microscope which detected the
emission at 682 nm as a signal. Here we discuss the feasibility of 3D optical
memory by use of PL change in Sm-doped sodium borate glass.
Keywords: 3D optical memory; Femtosecond laser; Photoluminescence change
Application of femtosecond-laser induced nanostructures in
optical memory.
Shimotsuma Y, Sakakura M, Miura K, Qiu J, Kazansky PG, Fujita K,
Hirao K.
Fukui Institute for Fundamental Chemistry, Kyoto University, Nishihiraki-cho
34-4, Takano, Sakyo-ku, Kyoto 606-8103, Japan.
The femtosecond laser induced micro- and nanostructures for the application to
the three-dimensional optical data storage are investigated. We have observed
the increase of refractive index due to local densification and atomic defect
generation, and demonstrated the real time observation of photothermal effect
after the femtosecond laser irradiation inside a glass by the transient lens (TrL)
method. The TrL signal showed a damped oscillation with about an 800 ps period.
The essential feature of the oscillation can be reproduced by the pressure wave
creation and propagation to the outward direction from the irradiated region.
The simulation based on elastodynamics has shown that a large thermoelastic
stress is relaxed by the generation of the pressure wave. In the case of
soda-lime glass, the velocity of the pressure wave is almost same as the
longitudinal sound velocity at room temperature (5.8 microm/ns). We have also
observed the localized photo-reduction of Sm3+ to Sm2+ inside a transparent and
colorless Sm(3+)-doped borate glass. Photoluminescence spectra showed that some
the Sm3+ ions in the focal spot within the glass sample were reduced to Sm2+
ions after femtosecond laser irradiation. A photo-reduction bit of 200 nm in
three-dimensions can be recorded with a femtosecond laser and readout clearly by
detecting the fluorescence excited by Ar+ laser (lambda = 488 nm). A
photo-reduction bit can be also erased by photo-oxidation with a cw Ar+ laser
(lambda = 514.5 nm). Since photo-reduction bits can be spaced 150 nm apart in a
layer within glass, a memory capacity of as high as 1 Tbit can be achieved in a
glass piece with dimensions of 10 mm x 10 mm x 1 mm. We have also demonstrated
the first observation of the polarization-dependent periodic nanostructure
formation by the interference between femtosecond laser light and electron
acoustic waves. The observed nanostructures are the smallest embedded structures
ever created by light. The period of self-organized nanostructures can be
controlled from approximately 140 to 320 nm by the pulse energy and the number
of irradiated pulses. Furthermore, we have also observed the self-assembled
sub-wavelength periodic structures created in silica glass by femtosecond pulses
on the plane of the propagation of light.
Bulk photochromism in a tungstate-phosphate glass: A new
optical memory material?
J. Chem. Phys. 125, 161101 (2006); DOI:10.1063/1.2364476
Published 30 October 2006
Gaël Poirier
Departamento de Ciências Exatas, Universidade Federal de Alfenas, UNIFAL CEP
37130–000, Alfenas-MG, Brazil
Marcelo Nalin and Lucila Cescato
Laboratory of Optics, Department of Physics of Condensed Matter, Instituto de
Física Gleb Wataglin, UNICAMP, PoBox 6165, CEP 13083-970, Campinas SP, Brazil
Younes Messaddeq and Sidney J. L. Ribeiro
Laboratory of Photonic Materials, Instituto de Química, UNESP, PoBox 355, CEP
14800-900, Araraquara SP, Brazil
In this work, we present a new photochromic tungstate based glass which have
both absorption coefficient and refractive index modified under laser exposure.
The photosensitive effect is superficial under ultraviolet (UV) irradiation but
occurs in the entire volume of the glass under visible irradiation. The effect
can be obtained in any specific point inside the volume using an infrared
femtosecond laser. In addition, the photosensitive phenomenon can be erased by
specific heat treatment. This glass can be useful to substitute actual data
storage supports and is a promising material for 3-dimensional (3D) and
holographic optical storage.
Femtosecond Photonics: Microfabrication and Optical Data Storage