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Journal of Minerals & Materials Characterization & Engineering, Vol. 10, No.4, pp.339-349, 2011
jmmce.org Printed in the USA. All rights reserved
Synthesis, Structural and Dielec tr ic Properties of Ferro el ec tr ic
Dichloridoglycine Zinc Dihydrate Single Crystals
S. Suresh1,*, A. Ramanand1, D. Jayaraman2, S.M. Priya3 and R. Vasanthakumari4
1Department of Physics, Loyola College, Chennai-600 034, India.
2Department of Physics, Loyola Institute of Technology, Chennai-602 103, India
3Department of Physics, Jeppiaar Engineering College, Chennai-600 119, India.
4Department of Polymer Technology, B.S.Abdur Rahman University, Vandalur,Chennai-
600 048, India.
*Corresponding Author: email@example.com
The strong electro mechanical coupling exhibited by the ferroelectric materials is the
remarkable feature of these materials. Therefore, they find applications in sensors, actuators for
producing ultrasonics and micro positioning. The material dichloridoglycine zinc dihydrate is a
centrosymmetric ferroelectric crystal. In the present study, this crystal has been grown from a
mixture of glycine and zinc chloride. The dielectric constant and the dielectric loss of the grown
crystal were studied as a function of frequency and temperature, and the corresponding
relaxation time (τ), relaxation frequency (Fr) and the activation energy have been calculated.
The ferroelectric property of the crystal has been confirmed by dielectric studies. The
ferroelectric characteristics of the crystal have been studied and reported.
Keywords: Ferroelectric single crystal, dichloridoglycine zinc dehydrate, sensors
Ferroelectric materials find wide applications in micro devices such as sensors and
actuators for use in ultrasonics, micro positioning and active damping due to their exceptional
electromechanical properties. The fundamental behavior utilized in these devices is the strong
electromechanical couplings exhibited by the ferroelectric material. The ferroelectric crystals
340 S. Suresh, A. Ramanand, D. Jayaraman, S.M. Priya and R. Vasanthakumari Vol.10, No.4
find important applications in optoelectronics such as capacitors, nonvolatile memory devices,
actuators, high-performance gate insulators, etc.
All ferroelectric materials are pyroelectric, however, not all pyroelectric materials are
ferroelectric. Below Curie temperature, ferroelectric and pyroelectric materials are polar and
possess a spontaneous polarization or electric dipole moment. However, this polarity can be
reoriented or reversed fully or partially through the application of an electric field with
ferroelectric materials. The nonpolar phase encountered above the Curie temperature is known as
the paraelectric phase. The direction of the spontaneous polarization confirms towards the crystal
symmetry of the material. The reorientation of the spontaneous polarization is a result of atomic
displacements. The magnitude of the spontaneous polarization is highest at temperatures well
below the Curie temperature and approaches zero as the Curie temperature is neared.
In recent times, the trend is to design organoelectronics for which the development of
organic ferroelectrics is mandatory [1–4]. In the present investigation dielectric constant and the
dielectric loss have been determined as a function of frequency and temperature for the
dichloridodiglycine zinc dihydrate crystal.
2. EXPERIMENTAL PROCEDURE
A supersaturated solution of glycine and zinc chloride was prepared in equimolar
proportion and stirred continuously using a magnetic stirrer for 3 days. The prepared solution
was filtered and kept undisturbed at room temperature. In the beginning some crystals of
irregular polymorphs were harvested and it was identified as dichloro-bis glycine-O- zinc
glycine, and after a few days seed crystals of dichloridodiglycine zinc dihydrate with an
excellent morphology was observed and it is found to be centrosymmetric.
2.1 Single Crystal XRD
X-ray diffracting data were collected using automatic diffractometer (MESSRS, ENRAF
NONIUS, Netherlands). The structure was solved by the direct method using SHELXL program.
From the analysis the cell parameters were found to be a = 14.4167 Å, b = 6.9068 Å, c = 12.9531
Å, β = 117.94 with space group C2/c and point group 2/m. ORTEP diagram and the packing
diagram of the grown crystal are shown in Figs.1 and 2, respectively.
Vol.10, No.4 Synthesis, Structural and Dielectric Properties 341
Fig.1. ORTEP representation of dichloridodiglycine zinc dihydrate crystals molecule with atom
Fig.2. Packing of molecules in dichloridodiglycine zinc dihydrate
crystals single crystal
342 S. Suresh, A. Ramanand, D. Jayaraman, S.M. Priya and R. Vasanthakumari Vol.10, No.4
2.2 Dielectric Properties
Good quality single crystals of dichloridodiglycine zinc dihydrate crystal were selected
for the dielectric measurements using HIOKI 3532-50 LCR HITESTER in the frequency range
of 50 Hz and 5 MHz at various temperatures. The selected sample was cut using a diamond saw
and polished using paraffin oil and fine grade alumina powder to obtain a good surface thickness
variation. Silver paint was applied on the opposite faces to make a capacitor with the crystal as a
dielectric medium. In the ferroelectric materials, the dielectric constant changes with temperature
according to the relation,
where B and C are constants independent of temperature. This relation is known as the Curie–
Weiss law. The parameters C and TC are called the Curie–Weiss constant and the Curie
temperature, respectively. The second term in Eq. (1) is usually much larger than the first one.
Therefore, one can ignore B and Eq. (2) can be rewritten as
From the Debye’s Equation, the frequency dependent dielectric constant is given by
is the dielectric constant at high frequency and equals to n2, where n is the optical index of
refraction. So, Eq. (3) can be re-written in another form by putting )(
For ferroelectric materials n2 is negligible with respect to )0(
From the Debye’s equation, the frequency dependent dielectric loss is given by
Vol.10, No.4 Synthesis, Structural and Dielectric Properties 343
By substituting Eq. (5) in Eq. (6), we obtain
and by substituting Eq. (2) in Eq. (7), we obtain
TT , then0
. Hence '
tends to maximum. Then Eq. (5) is rewritten as
This conclusion means that the dielectric peak at the phase transition temperature in ferroelectric
materials can be considered as)0(
. But '
is a function of the frequency, i.e.
max ncyhighfrequecylowfrequen rrr
Then Eq.(9) cannot be used for the calculation of the relaxation time, especially at the phase
transition temperature TC. Then the previous model which was described by Eq. (9) can be
modulated into another simplified model. Taking the relaxation time near the critical temperature
, Eq (5) is rewritten for lower frequency '
(L) and higher frequency '
From the above two equations one can find an equation to describe the value of C
344 S. Suresh, A. Ramanand, D. Jayaraman, S.M. Priya and R. Vasanthakumari Vol.10, No.4
Substituting the value of C
in Eq. (11), the value of )0(
can be obtained. By substituting
the value of )0(
in Eq. (5), one can obtain the value of
, the Debye’s Relaxation time, as a
function of temperature keeping frequency constant. Hence, the equation which gives the values
for all ranges of temperature, except at the phase transition temperature, can be rewritten as
The values of τ from the previous equation are corrected for the whole range of temperatures
both for ferroelectric phase and for paraelectric phase except atC
. From the Debye’s
relaxation time, the relaxation frequency (Fr) can be determined using the formula
The activation energy (Ea) can be calculated from the plot of Log )(1
versus 1000/T using the
3. RESULTS AND DISCUSSIONS
The plot of dielectric constant ('
) vs frequency for various temperatures is shown in
Fig.3. The dielectric constant is high in the lower frequency region and decreases with an
increase in frequency. The very high value of dielectric constant at low frequencies may be due
to the presence of all the four components namely, space charge, orientational, electronic and
ionic polarisations. At higher frequencies up to 200 kHz, the dielectric constant decreases
gradually. From 3 MHz to 5 MHz, there is an increase in the dielectric constant due to stray
capacitances [6–10]. The dielectric loss was also studied as a function of frequency for different
temperatures and is shown in Fig.4. The low dielectric loss at high frequencies for the given
Vol.10, No.4 Synthesis, Structural and Dielectric Properties 345
sample indicates very high purity of the crystal. These curves suggest that the dielectric loss is
strongly dependent on the frequency of the applied field. The temperature dependent dielectric
constant for various frequencies is shown in Fig.5. Dielectric measurements were carried out on
the polarizing plane in the temperature range of 328K-368K for various frequencies. From the
plot (Fig.5), it was clear that the dielectric constant increases at 368K called Curie temperature
(TC). This means that the crystal undergoes phase transition at 368K from paraelectric to
ferroelectric state. Thus, it is evident that the crystal possesses ferroelectric properties.
The temperature dependent dielectric constant ('
) for dichloridodiglycine zinc dihydrate
crystals shows that the dielectric constant ('
) initially increases up to 368 K then decreases
gradually. This indicates that the grown crystal begins to undergo phase transition from
paraelectric to ferroelectric at 368K, which is called as the Curie temperature (TC). Thus the peak
at 368 K indicates the ferroelectric phase transition for the dichloridodiglycine zinc dihydrate
crystals. The Debye’s relaxation time (
) for various frequencies ranging between 50 Hz and
900 Hz and the corresponding relaxation frequency were calculated for the dichloridodiglycine
zinc dihydrate crystals. The activation energy (Ea) at various frequencies ranging between 50 and
900 Hz was calculated from the slope of the graph between log )(1
vs. 1/T and is shown in
Fig.6. The value of activation energy was found to be 0.014 eV, 0.023 eV, 0.030 eV, 0.047 eV
and 0.060 eV for various frequencies of 50 Hz, 100 Hz, 200 Hz, 600 Hz and 900 Hz,
Fig. 3. Variation of dielectric constant ('
) with log f
346 S. Suresh, A. Ramanand, D. Jayaraman, S.M. Priya and R. Vasanthakumari Vol.10, No.4
Fig. 4. Variation of dielectric loss with log f
Fig. 5. Plot of Log )(1
Vol.10, No.4 Synthesis, Structural and Dielectric Properties 347
Fig. 6. Variation of dielectric constant ('
) vs. temperature
3.1 Ferroelectric Studies
The ferroelectric property of the crystal has been determined using Ferroelectric loop
tracer (Radiant Technologies). Fig. 7 shows polarization versus voltage behaviour of the grown
crystal with a voltage range from +200V to -200V. This figure shows that the material has good
ferroelectric nature with a remanant polarization (Pr) of approximately 30nC/cm2and the
coercivety (Vr) of about 177V which is quite high . The saturation of the loops at these low
frequencies indicates that the losses are minimal, suggesting that the crystal is highly resistive
with electrical resistivity ρ = 5.35×106 Ωcm2
348 S. Suresh, A. Ramanand, D. Jayaraman, S.M. Priya and R. Vasanthakumari Vol.10, No.4
Fig.7. P-V loop of dichloridodiglycine zinc dihydrate crystal
Single crystal of dichloridodiglycine zinc dihydrate has been grown by slow evaporation
method at a constant temperature of 40 0C. The grown crystal was characterized by single crystal
XRD analysis .The variation of dielectric constant and dielectric loss were studied as a function
of frequency and temperature. The Debye’s Relaxation time (τ), Relaxation frequency (Fr) and
the corresponding activation energy (Ea) have been calculated for the dichloridodiglycine zinc
dihydrate crystals. The ferroelectric behavior of the crystal was confirmed from the nature of
ferroelectric loop with remant polarization of 300 nc/cm2 and coercivety value of 177V.These
studies reveal that the dichloridodiglycine zinc dihydrate crystals are considered to be a
promising material for the fabrication of optoelectronic devices.
 K. Vinod Wadhawan, Introduction to Ferroic Materials, Gordon & Breach Publishers,
London (New York), 2000.
 O. Auciello, J.F. Scott, R. Ramesh, Phys. Today .51 (1998) 22.
 J. Dolinsek, D. Arcon, Hae Jin Kim, J. Seliger, V. Zagar, P. Vanek, J. Kroupa, Z. Zikmund,
J. Petzelt, Phys. Rev. B 57 (1998) R8063.
 Sachio Horiuchi, Reiji Kumai, Yoshinori Tokura, J. Am. Chem. Soc. 127 (2005) 5010
 Gergs MK, Egypt J Solids .29, (2006) 371–82.
Vol.10, No.4 Synthesis, Structural and Dielectric Properties 349
 Patil MG, Mahajan VC, Ghatage AK, Patil SA, Indian J Pure Appl Phys .34, (1996)166–
 Lal B, Khosa SK, Tickoo R, Bamzai KK, Kotru PN, Mater Chem Phys. 83, (2004) 158–68.
 Ramana Reddy AV, Ranga Mohan G, Ravinder D, Boyanov BS, J Mater Sci.34, (1999)
 Parkash C, Bajal JS, J Less-Common Met .107, (1985) 51–7.
 Ravinder D, Phys Status Solidi (a) .139, (1993) K69–72.
 C.Sakaki et al., JpnJ.Appl.Phys.40, (2001)6901
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