Laser Physics, Nonlinear
Optics
Baku State
University, Azerbaijan, Baku, rkasumova@azdata.net
Second harmonic generation
of laser radiation in AgGa(Se1-xSx)2 crystal
In addition to the short-wave region of
spectrum, for IR-region of the spectrum, where as is known, there are two
atmospheric windows (which is very important in application) coherent
radiation, tunable according to frequency, has a wide range of application. For
instance, on the basis of parametric frequency converters, LIDARs, which are
used to investigate the Earth and atmosphere are constructed. Despite the
importance of applications, nonlinear crystals, which
provide for smooth tuning of laser radiation in an entire optical diapason has
not been elaborated yet. For frequency conversion of laser radiation in
IR-region of spectrum CGA crystals are more often used, which is distinguished
among other transparent crystals in this region of spectrum, for its extremely
high quadratic nonlinearity in 236 pm/V. Recently the increased interest in CGA
crystals is because of their achievements in its technological elaboration,
which is related to get the same media with improved optical qualities, at
bigger dimensions and resistant to higher radiations [1-9].
Search of
the prospect materials for the tasks of modern nonlinear optics goes on.
Nonlinear crystals of the IR-range of spectrum take a particular place [1-7].
Recent years the nonlinear crystals of mixed type have turned to be the subject
of the researches. It is connected with that realization of the efficient
tuning of radiation in a broad range of spectrum needs in the nonlinear
crystals for which the condition of uncritical phase matching is kept in the
chosen range of spectrum. In compounds of mixed type on the account of
increasing the content of one element and decrease of the other’s content, the
possibility of elaboration of crystals with uncritical phase matching on the
chosen radiation wavelength is experimentally shown [10-12]. Among the crystals
of mixed type we can cite Zn1−xMgx Se [10], AgGaxIn1−xSe2 [11] and AgGa(Se1−xSx)2 [12].
For the analysis of nonlinear process the
use of the direct numerical account of reduced equations is possible. However,
the development of the analytical method will allow one to obtain the concrete
analytical expressions and determine the optimum parameters of the task with
the aim of obtaining maximum conversion efficiency. The simultaneous account
for changes of phases and losses of interacting waves works well in the
constant –intensity approximation [13] taking into regard the reverse reaction
of excited wave to pump wave.
In the present work the results of
investigation of pump intensity impact on conversion efficiency in AgGa(Se1-xSx)2 crystal in conditions of existing experiment have
been considered. Comparison has been made of the received results on conversion
efficiency with the analogous results obtained in the experiment. The applied
analytical method permits to calculate the optimum parameters of both crystal
–converter and a source of radiation. For example, optimal crystal length at
the given losses and pump intensity what makes possible an estimation of
expected efficiency of conversion.
In
the experiment for real frequency converters, it is impossible to ensure a
condition of phase matching (Δ
= 0).
An error that is followed from the condition of phase matching determines its
width. Phase mismatching is affected by spectral width of pump radiation line,
deviation from phase matching angle which is caused by divergence of laser
radiation and instability of temperature for a crystal converter. Then the
information that we have, particularly on angular width of phase matching will
make possible to calculate the maximum divergence of light beam for pumping.
Let’s determine deviation angle from
the direction of the phase matching for mixed type AgGaxIn1-xSe2
(for x=0.6 reflecting indium content in crystal) in which second harmonic
generation of CO2 laser radiation occurs on pump wavelength of 9.64
mcm (scalar phase matching of the first type for îî®å interaction).
For this crystal, the calculation was carried out using coefficients in the
relation of Sellmeier for the main values of refractive indices cited in [4,
10].
The result of calculation for angular
dispersion coefficient of the second order is equal to 19.4 10-6 cm-1ang.min.-2.
It is shown that with increasing the
concentration of indium in the mixed crystal from 1 to 0.6, the dependence becomes more flat. It testifies the
transition to the regime of uncritical character of crystal towards following
condition of phase matching.
Thus, the results of studying nonlinear
interaction of waves with regard for changes of interacting waves phases in the
process of second harmonic generation in AgGa(Se1-xSx)2 crystals permit to
state the following. By a choice of the optimum values of nonlinear medium
length, pump intensity, phase match and with the account for the influence of
linear losses in a medium it is possible to increase efficiency of conversion
to second harmonic in these crystals of mixed type and to select conditions for
fulfilling or increasing a degree of uncritical angular phase matching.
References
1.
A.S. Borshecvskii, N.A. Goryunova, F.P.
Kesamanly, D.N. Nasledov, Semiconducting AIIBIVC2v
compounds, Phys.
Stat. Sol. 21 (1967) 9-55.
2.
R.L. Byer, H. Kildal, CdGeAs2 – a new nonlinear
crystal phasematchable at 10.6 mm, Appl.
Phys. Lett. 19 (1971) 237-240.
3.
G.D. Boyd, E. Buehler, F.G. Storz, Linear and nonlinear
optical properties of ZnGeP2 and CdSe, Appl. Phys. Lett. 18 (1971) 301-304.
4.
P.G. Schunemann, T.M. Pollak, Single crystal growth of
large, crack-free CdGeAs2 J.
Cryst. Growth 174 (1997) 272-277.
5.
K.L. Vodopyanov, G.M. H. Knippels, A.F.G. van der Meer, J.P.
Maffetone, I. Zwieback, Optical parametric generation in CGA crystal, Opt.
Commun. 202 (2002) 205-208.
6.
S. Das, Generation of tunable mid-IR radiation
by second harmonic in a CdGeAs2 crystal, Quantum Electronics 42 (2012) 228-230.
7.
Yu.M. Andreev, V.V. Badikov, V.G. Voevodin, L.G. Geiko, P.P.
Geiko, M.V. Ivashenko, A.I. Karapuzikov, I.V. Sherstov, Radiation resistance of nonlinear crystals at a wavelength
of 9.55 μm, Quantum Electronics, 31
(2001) 1075-1078.)
8. P.P. Geiko, Phase matching and group-velocity
matching conditions in nonlinear mixed AgGa(Se1-xSx )
crystals, Atmospheric and Oceanic Optics 16
(2003) 828-834.
9. G.C. Bhar, S. Das, U. Chatterjee, and K.L. Vodopyanov,
Temperature-tunable second-harmonic generation in zing germanium diphosphide,
Appl. Phys. Lett. 54 (1989) 313-314.
10. N.V. Kovalenko, Zn1−xMgxSe: A promising
material for non-linear optics, J. of Nonlinear Optical Physics and Materials 20 (2011) 123-127.
11. Yu.M. Andreev, I.S. Baturin, P.P. Geiko, and A.I. Gusamov, Frequency
doubling of CO2 -laser radiation in new nonlinear crystal AgGaxIn1−xSe2, Quantum Electronics 29 (1999) 66-70.
12. P.P. Geiko, Phase matching and group-velocity matching conditions in
nonlinear mixed AgGa(Se1−xSx)2 crystals, Atmospheric and Oceanic
Optics 16 (2003) 828-834.
13. Z.H. Tagiev, R.J. Kasumova, R.A. Salmanova, and N.V. Kerimova,
Constant-intensity approximation in a nonlinear wave theory, J. Opt. B: Quantum
Semiclas. Opt. 3 (2001) 84-87.