ISSN 1054660X, Laser Physics, 2011, Vol. 21, No. 9, pp. 1539–1544.
© Pleiades Publishing, Ltd., 2011.
Original Text © Astro, Ltd., 2011.
1539
1
1. INTRODUCTION
Ultrashort picosecond’s pulse laser is a powerful
tool in the fields of micromachining, remote sensing,
raging, chemical processing, coherent telecommuni
cations, etc. This kind of laser is usually obtained by
means of the passive Qswitching and modelocking
techniques due to the advantages of simplicity, com
pactness and low cost. However if the single saturable
absorber, such as Cr
4+
:YAG, is used [1–5], the singly
passively QML lasers have the poor shottoshot sta
bility and reproducibility as well as a low controllabil
ity for the pulse repetition rate. So the doubly QML
lasers can be employed to generate stable QML pulses
with higher peak power and the optional repetition
rate [6–9].
So far, some neodymiumdoped crystals have been
employed for QML lasers. Among them, Nd:YVO
4
has
been investigated in detail and has become the most
common medium for lasers operating at low pump
power levels [2, 8, 10, 11]. Meanwhile as an isomor
phism of Nd:YVO
4
, Nd:LuVO
4
crystals have been
proved to be excellent laser materials for diode
pumped QML lasers [4, 12–16]. Based on the
Nd:YVO
4
and Nd:LuVO
4
, a new class of mixed vana
date crystals Nd:Lu
x
Y
1–
x
VO
4
is developed. In com
parison to Nd:YVO
4
and Nd:LuVO
4
, the
Nd:Lu
0.15
Y
0.85
VO
4
crystal has longer fluorescence life
time (106
μ
s) and smaller emission crosssections
(6.4
×
10
–19
cm
2
) [17], which makes it more suitable
for application in pulsed laser systems, because
1
The article is published in the original.
smaller emission cross section of vanadate crystals
enhances its energy storage capacities, leading to
higher pulse energy and peak power. Moreover in a
Nd:Lu
0.15
Y
0.85
VO
4
crystal, the lattice sites formerly
occupied by Y ions in Nd:YVO
4
crystal are now occu
pied at random by Lu and Y ions. This modification of
the local crystal field neighboring the Nd ions will lead
to the inhomogeneous broadening of the fluorescence
line widths, which is much broader than those of the
vanadate single crystals (~1–2 nm) [17, 18] and even
mixed crystals (~2–4 nm) [19–22]. The inhomoge
neous broadening of the fluorescence line also leads to
the pulse energy enhancement.
For this kind of mixed crystal, the passively CW
modelocked laser has been reported [17, 23, 24], in
which shorter pulses and higher peak power can be
generated. Moreover, the passively Qswitching per
formance with Nd:Lu
0.2
Y
0.8
VO
4
crystal demonstrates
that it is a promising laser host material [25–28].
However, it is still lack of reports on simultaneously
QML Nd:Lu
x
Y
1–
x
VO
4
laser, which is also expected to
generate stable pulses.
In this paper, a diodepumped duallossmodu
lated QML Nd:Lu
0.15
Y
0.85
VO
4
laser with acoustooptic
(AO) modulator and Cr
4+
:YAG saturable absorber is
presented for the first time as far as we know. The pulse
width, singlepulse energy and so on have been mea
sured for different smallsignal transmissions (
T
0
) of
Cr
4+
:YAG, different reflectivity (
R
) of output coupler
(OC) and modulation frequencies (
f
p
) of the AO mod
ulator. The experimental results further confirm the
SOLID STATE
AND LIQUID LASERS
Characteristics of DiodePumped DualLossModulated
QSwitched and ModeLocked Nd:Lu
0.15
Y
0.85
VO
4
Laser
1
G. Zhang
a
, S. Z. Zhao
a
,
*, D. C. Li
a
, K. J. Yang
a
, G. Q. Li
a
,
K. Cheng
a
, Y. Zhang
a
, and B. Zhao
b
a
School of Information Science and Engineering, Shandong University, Jinan 250100, China
b
College of Chemistry and Chemical Engineering, Fuzhou University, Fuzhou 350108, China
*email: shengzhi_zhao@sdu.edu.cn
Received February 26, 2011; in final form, March 5, 2011; published online July 4, 2011
Abstract
—A diodepumped duallossmodulated Qswitched and modelocked (QML) Nd:Lu
0.15
Y
0.85
VO
4
laser with acoustooptic (AO) modulator and Cr
4+
:YAG saturable absorber is presented. The stable QML
laser pulse with high peak power and complete modulation depth has been obtained. The QML laser charac
teristics such as the pulse width, singlepulse energy etc. have been measured for different smallsignal trans
missions (
T
0
) of Cr
4+
:YAG, different reflectivity (
R
) of output coupler and modulation frequencies of the AO
modulator (
f
p
). The results show that the pulse energy increases with decreasing
f
p
and increasing
T
0
, while
the pulse width decreases with decreasing
f
p
and increasing
T
0
. At
f
p
= 10 kHz,
R
= 90%, and
T
0
= 91%, the
highest pulse energy and peak power of modelocked pulses is obtained.
DOI:
10.1134/S1054660X11150357