Femtosecond transient grating effect and stoichiometry of
TeO
2
–Nb
2
O
5
–TiO
2
glass
Zhenyu Zhao
a,
⁎
, Aimin Yan
a
, Zhijuan Hu
a
,WangzhouShi
a,
⁎⁎
, Zhenrong Sun
b
,JianLin
c
a
Key laboratory of Optoelectronic Materials and Devices, Department of Physics, Shanghai Normal University, Shanghai 200234, China
b
State Key Laboratory of Precision Spectroscopy, East China Normal University, Shanghai 200062, China
c
School of Material Science and Engineering, Tongji University, Shanghai 200092, China
abstractarticle info
Article history:
Received 24 June 2013
Received in revised form 9 October 2013
Available online xxxx
Keywords:
Optical materials;
Optical properties;
Nonlinear optics
We observed efficient transient optical grating effect from the TiO
2
–Nb
2
O
5
–TeO
2
glasses excited by femtosecond
laser pulses. The glass samples were prepared via melt-quenching technique. The optical nonlinearities were
calibrated by forward degenerate four wave mixing (DFWM) experiment with 50 fs laser pulse at 800 nm. The
magnitude of the third order nonlinear susceptibility χ
(3)
was about 7–9×10
− 13
esu, and its temporal response
is up to the resolution limit of the laser 50fs pulse-width. It has been found that χ
(3)
is critically dependent on the
stoichiometry of between TiO
2
and TeO
2
. The results of Raman experiment have indicated that TiO
2
dopant
induces transformation from the [TeO
4
] unit into [TeO
3
] via [TeO
3+1
], and it results in reinforcement in the
rigidity of the glass network so that the χ
(3)
was suppressed.
© 2013 Elsevier B.V. All rights reserved.
1. Introduction
The rapid development of optical telecommunication requires a high-
speed all-optical switching m aterial and hig h-gain broad ba ndwidth
Raman medium [1]. Tellurite oxide glasses are recognized as one of the
most prospective candidate materials due to their excellent performance,
such as high infra red transm ittance, hig h refracti vity, ultrafas t optical
response, chemical durability, t hermal stabili ty and compatibility wi th
current fiber technology [2–6]. Compared to other oxide glasses, tellurite
oxide glasses possess the largest Kerr nonlinearity χ
(3)
at femtosecond
regime [7–9]. Especially, niobic tellurite oxide glasses have become a
successful material for optical switching by inducing nanocrystals [10],
rare earth elemen t [11], or transition metal oxide [12].Furthermore,
inducing titanium dioxide (TiO
2
) are able to improve the optical
performance of niobic tellurite glasses [13,14]. For both titanium and
tellurium possess d-orbital electron, however, there is insufficie nt
investigation on the competition between TiO
2
and TeO
2
to the ultrafast
nonlinearity of glasses.
In this paper, we report the femtosecond transient grating effect from
a ternary tellurite oxide glasses in compositions xTiO
2
–20Nb
2
O
5
–(80− x)
TeO
2
(x=2, 5, 10). The glasses in the present investigation were prepared
by replacing a portion of TeO
2
by TiO
2
in a base 80TeO
2
–20Nb
2
O
5
(wt.%)
glasses. The transient grating effect of glasses were measured by forward
degenerate four wave mixing (F-DFWM) setup, where the χ
(3)
as a
function of time is calibrated. The construction of glass networks is
investigated by Raman spectroscopy and differential thermal analysis
(DTA). Finally, the origins of ultrafast transient grating effect in glass
samples are discussed.
2. Experiments
Glass samples were prepared by melting the powder of optical grade
TeO
2
,Nb
2
O
5
and TiO
2
at the proportion: xTiO
2
–20Nb
2
O
5
–(80 − x)TeO
2
(x=2,5,10) in a platinum crucible at 850°C for 25minutes and annealed
at 380 °C for 4 hours. The as-received samples were polished to a mean
thickness of 2 mm. A schematic diagram of the laser induced transient
grating is shown in Fig. 1, which is named forward DFWM as well. A
Ti:Sapphire amplified laser system (Spectra-Physics Spitfire) is used as
excitation source to generate 50-femtosecond pulses with a central
wavelength of 800 nm at a repetition rate of 1 KHz. A low repetition
ratio can prohibit thermal lensing effects on nonlinear refractive
index. The maximum pulse energy was 6 μJ with a shot-to-shot
fluctuation less than 1% rms. The pulse-duration was kept constant
throughout the experiments. The laser output was split into two
beams at comparable intensity of 3 μJ. The two beams were combined
at the glasses samples by a lens of 10 cm focal length in the forward
incident geometry. Each incident beam was approximately crossed at
an angle of 12° resulting in a grating period of 5 μm, calculated from
[15]:
Λ ¼
λ
2sin θ=2ðÞ
; ð1Þ
Here, Λ is the grating period, λ is the optical wavelength, θ is the
crossing angle between the 2 incident beams. One of the incident
beams was controlled by a computer-driven time-delay line. The other
Journal of Non-Crystalline Solids 382 (2013) 70–73
⁎ Corresponding author. Tel./fax: +86 21 6432 2078.
⁎⁎ Corresponding author. Tel./fax: +86 21 6432 8895.
E-mail addresses: zyzhao@shnu.edu.cn (Z. Zhao), wzshi@shnu.edu.cn (W. Shi).
0022-3093/$ – see front matter © 2013 Elsevier B.V. All rights reserved.
http://dx.doi.org/10.1016/j.jnoncrysol.2013.10.014
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