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International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 –
6480(Print), ISSN 0976 – 6499(Online), Volume 6, Issue 3, March (2015), pp. 01-06 © IAEME
1
GAMMA RADIATION-INDUCED TRANSFORMATIONAL
CHANGE IN IR SPECTRUM OF EBHA NEMATIC LIQUID
CRYSTAL
Sudhaker Dixit1
, Rajiv Manohar2
1
University Institute of Engineering & Technology, Babasaheb Bhimrao Ambedkar University,
A Central University, Lucknow-226001
2
Liquid Crystal Research Lab, Physics Department, University of Lucknow, Lucknow- 226007
ABSTRACT
Gamma ray irradiation technique is the powerful technique to modify the dielectric and
electro-optical properties of liquid crystals. It prefers than any other modification technique because
no catalysts or additives are required to initiate the reaction. The present paper reports a comparative
study of IR spectrum for both irradiated and unirradiated EBHA NLC. The dielectric spectrum and
ionic conductivity is also evaluated and well explained in this paper. In addition to this, we have also
suggested the concept of the peak data information graph for better understanding of IR spectrum.
Keywords: Nano Materials, Condensed Matter Physics, Gamma Radiation, Dielectric, IR Spectrum
1. INTRODUCTION
Radiation materials science describes the interaction of radiation with matter. A broad subject
covering many forms of irradiation and of matter.The consequences of radiation to core components
includes changes in shape and volume by tens of percent, increases in hardness by factors of five or
more, severe reduction in ductility and increased embrittlement, and susceptibility to
environmentally induced cracking. For these structures to fulfill their purpose, a firm understanding
of the effect of radiation on materials is required in order to account for irradiation effects in design,
to mitigate its effect by changing operating conditions, or to serve as a guide for creating new, more
radiation-tolerant materials that can better serve their purpose [1].
The phenomenon of gamma radiation induced conductivity in solid insulators has been
studied by several investigators. Most attention has been given to studies of organic insulators [2-4],
and some have been made of inorganic insulators [5-7]. Up to now, only few reports were dedicated
to radiation effects on physicochemical properties and on the conductivity of the liquid crystals
INTERNATIONAL JOURNAL OF ADVANCED RESEARCH IN ENGINEERING
AND TECHNOLOGY (IJARET)
ISSN 0976 - 6480 (Print)
ISSN 0976 - 6499 (Online)
Volume 6, Issue 3, March (2015), pp. 01-06
© IAEME: www.iaeme.com/ IJARET.asp
Journal Impact Factor (2015): 8.5041 (Calculated by GISI)
www.jifactor.com
IJARET
© I A E M E
International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 –
6480(Print), ISSN 0976 – 6499(Online), Volume 6, Issue 3, March (2015), pp. 01-06 © IAEME
2
materials [8]. Data regarding radiation effects on liquid crystal and organo-photonic material is
almost non-existent [9].
Preliminary studies on some liquid crystals suggest that their physical and chemical
properties are highly affected by radiation. Most of these suggest that the transition temperatures and
the stability of various liquid crystalline mesophases are strongly affected by radiation [10]. Some of
the electrical properties such as electrical conductivity and charge carrier mobility subjected by
ionizing radiation have been studied very first in 1988 by Kovalchuk et al. [11]. Talor et al. first
reported on the degradation of light transmission characteristics of a smectic C liquid crystal [12].
Graham et al. also reported on the effect of space radiation dose on the nematic liquid crystal
variable retarders (LCVR) [13]. Such other radiation effects on the liquid crystal materials namely
electron beam radiation, UV radiation, ion beam radiation has also been reported [14].
Absorption of gamma rays by liquid crystal may cause physical conformational changes due
to thermal and thermo-mechanical effects. These physical changes may cause scattering of light,
changes in transmission and reflection properties of filters and coatings. Early liquid crystal phase
retarders were screened at Raytheon for radiation sensitivity circa 1989 under the AFRL Beam
agility technique program (F33615-87-1507). Phase retarders were used as surrogates for optical
phased arrays and subjected to increasing gamma ray dose from a cobalt-60 source, upto a total dose
of 9.5 Mrad. It was the first known radiation testing of liquid crystal [15].
In the present paper we have reported the variation in IR spectra of a nematic liquid crystal
caused by gamma radiation.In addition to this we have also evaluated the dielectric spectrum for
both gamma irradiated and unirradiated EBHA NLC.
2. EXPERIMENTAL DETAILS
2.1 Material Used
The liquid crystal sample under investigation is a rod shaped nematic liquid crystal molecule.
The structure and its phase transition behavior are given in the Figure 1.
Figure 1.Chemical structure with transition scheme for EBHA nematic liquid crystal.
2.2 Preparation of cell
Two similar cells having active areas 25 mm2
, (sheet resistance and the visible light
transmission is 10 /mm2
and more than 90% respectively) were prepared by using transparent and
highly conducting ITO (Indium Tin Oxide) (Diamonds Coating UK) coated optically flat glass
substrates used as electrodes. These electrodes give a base to the LC sample to align. Planar
alignment is obtained by treating both adhesion promoter and polymer (Nylon 6/6) and then rubbed
unidirectional with a velvet cloth. Although the homeotropic cell has been prepared by applying
lecithin on the ITO coated surface.The thickness of the cell was maintained at 5 µm by means of
Mylar spacer. The complete preparation of cell has been given in our earlier papers [16]. The correct
and proper alignment of the LC molecules is extremely important, for precise measurement of
International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 –
6480(Print), ISSN 0976 – 6499(Online), Volume 6, Issue 3, March (2015), pp. 01-06 © IAEME
3
electrical properties and which in turn influences dielectric parameters and thus plays an extremely
important role in molecular geometry.
2.3 Gamma Ray treatment
We have irradiated the EBHA NLC. The irradiation used a 60
Co source, at the dose rate of
2.9 kGy/h, up to a total dose for 34.5 h is 100 kGy.
2.4 Dielectric study
The dielectric behavior of the material has been studied by using a computer controlled
impedance/ gain phase analyzer Hewlett Packard (HP 4194 A). The dielectric parameters have been
measured as a function of temperature and frequency. In order to vary the temperature of the
sample holder a microprocessor based heating device Instec hot plate (HCS-302) with an accuracy of
± 0.010
C has been used. Before taking measurements the sample was left for 15 minutes at a
particular temperature.
The Threshold voltage measurement has also been done by using the same computer
controlled impedance/ gain phase analyzer Hewlett Packard (HP 4194 A). The dielectric permittivity
has been measured as a function of voltage.
2.5 FT-IR Study
FTIR measurements are carried out using IRAffinity-1 (Shimadzu) Fourier Transform
Infrared Spectrophotometer. The measurements have been done in the wave number range 500- 4000
cm-1
, keeping air as reference.
3. RESULT AND DISCUSSION
Due to the wealth of information that FT-IR spectroscopy provides on molecular state,
orientation, and dynamics, it has often been used to characterize liquid crystals and liquid crystal
systems. Moreover, it has been observed that the IR spectrum of a liquid crystal system depends on
its phase (isotropic or mesogenic). Thus, in addition to the dependence on concentration, the IR
spectra of liquid crystalline system have a significant dependence on their director alignment and
molecular phase, which is controlled by temperature for thermotropic liquid crystals.
In this way the radiated and unirradiated samples are analyzed by FT-IR spectroscopy. The
FT-IR spectrum for the unirradiated and gamma irradiated EBHA nematic liquid crystal is shown in
figure 2.
Figure 2. Variation in transmittance with respect to wavelengthfor EBHA NLC
International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 –
6480(Print), ISSN 0976 – 6499(Online), Volume 6, Issue 3, March (2015), pp. 01-06 © IAEME
4
For better understanding of the IR spectra, assignments of the major peaks of the liquid
crystal material are shown in peak data information (PDI) graphs. The PDI graphs for the
unirradiated and gamma irradiated liquid crystalline materials have been shown in figure 3. Using
PDI graphs FT-IR study suggests that up to given dose of gamma radiation, the liquid crystal system
causes chemical change which is responsible for shifting of absorption peaks. Which is responsible
for variation in transmittance as shown in figure.Figures also suggest the gamma irradiated EBHA
NLC exhibit a high transmittance as compared with unirradiated EBHA NLC.
Figure 3. PDI graph for EBHA NLC
When the frequency of a specific vibration is equal to the frequency of the IR radiation
directed to the molecule, the molecule absorbs the radiation. The total number of observed bands is
generally different from the total number of fundamental vibrations. It is reduced because some
modes are not IR active and a single frequency can cause more than one mode of motion to occur.
Conversely additional bands are generated by the appearance of overtones, combination of
fundamental frequencies, coupling interactions of two fundamental absorption frequencies. Thus we
can say that the shifting of absorption peaks is due to the gamma induced physic-chemical change in
liquid crystal molecule. In this way the dielectric response of the sample with frequency has been
taken (figure 4).
Figure 4. Complex dielectric permittivity with variation in frequency
International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 –
6480(Print), ISSN 0976 – 6499(Online), Volume 6, Issue 3, March (2015), pp. 01-06 © IAEME
5
The observed value of complex dielectric permittivity for both irradiated and unirradiated
EBHA NLC, nature of variation with frequency is same, but the values have increased for gamma
irradiated EBHA NLC sample.Actually irradiation causes a chemical change in liquid crystalline
materials, it may include cross linking, chain scission, formation of alkyl groups, depletion of hetero
atoms. Effect of gamma irradiation or such other ionizing radiation is primarily chain
scission.Therefore many physical and chemical properties can show modification with gamma
irradiation.Radiation mainly affects in two basic ways, both resulting with excitation or ionization of
atoms.In this fashion ionic conductivity of liquid crystal material has also been investigated and
shown in figure 5.The ionic conductivity for irradiated EBHA NLC sample is comparatively higher
than that of unirradiated EBHA NLC sample.
Figure 5. Variation in ionic conductivity of EBHA NLC caused by gamma radiation
4. CONCLUSION
We observe that the nature of variation of dielectric permittivity with frequency and
temperature remains same for both the gamma irradiated and the unirradiated EBHA samples, but
the value of dielectric permittivity for the gamma irradiated sample is higher as compared to the
unirradiated EBHA sample. This increment in the gamma irradiated sample can be explained on the
basis of physicochemical change inthe EBHA molecules due to irradiation.Also the effect of gamma
irradiation on EBHA NLC sample has been evaluated using FT-IR. New concept of PDI graph has
been shown for better understanding of IR spectra.
REFERENCES
1. Gary S. Was, “Fundamentals of Radiation Materials Science,” Springer, Berlin, Heidelberg,
New York, 2007.
2. J.F.Fowler, Proc. Roy. Soc., 1956, 464-470.
3. S.E. Harrison, IEEE Conference Paper, 1962, 62-1251.
4. F.N. Coppage, A.W.Snyder, ibid, 1963, 63-118.
5. G.C. Huth, General Electric Company Aircraft Nuclear Propulsion Department, Paper, 1958,
58- 331.
6. V.E. Culler, H.E.Rexford, Proc. IEEE, 1965, 112, 11024-11039.
7. H.J.Wintle, Internat. J. Appl. Radiation and Isotopes, 1960, 8, 132-148.
8. H. Ohoka, M. Ozaki, L.M. Blinov, M.I. Barnik, N.M. Shtykov, K.Yoshino, Mol. Cryst. Liq.
Cryst., 2001, 366, 283-293.
International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 –
6480(Print), ISSN 0976 – 6499(Online), Volume 6, Issue 3, March (2015), pp. 01-06 © IAEME
6
9. R.B. Meyer,P.S.Pershan, Sol. State. Comms, 1973, 13, 989-992.
10. A.Derzhanski, A.Petrov, M.Mitov, J. Phys. (Paris), 1978, 39, 273-285.
11. A.V.Kovalchuk,O.D. Lavrentovich,V.A. Linev, Sov. Tech. Phys. Lett., 1988, 14, 381-382.
12. R.C. Webb, L.C. Cohn, E.W. Taylor, R.A. Greenwell, Proc. SPIE, 1995, 2482, 3–15.
13. A. Graham, G. Kopp, C. Vargas-Aburto, Uribe, R. Proc. SPIE 1996, 2811, 46–50.
14. M.C.Rath, S.K.Sarkar, V.K.Wadhawan, R.Verma, I.M.L. Das, R.Dabrowski,M.Tykarska,
R.Dhar, Opto.-Electron. Rev., 2008, 16, 399–403.
15. J. Stockley, S.Serati, D.Dauwe, T. Deaton, J.Nonnast, SPIE Proc., 2006, 6308, 6630805-17.
16. S.P. Yadav, K.K. Pandey, A.K. Misra, S. Dixit, R. Manohar, Can. J. Phys.,2011, 89, 661-665.
17. Bhagyajyothi, Immanuel J., P. Bhaskar, L.S. Sudheer and Parvathi C. S., “Advanced Lock-In
Amplifier For Detection of Phase Transitions In Liquid Crystals” International Journal of
Advanced Research in Engineering & Technology (IJARET), Volume 4, Issue 2, 2013, pp.
17 - 26, ISSN Print: 0976-6480, ISSN Online: 0976-6499.
18. C. Basavaraju and Dr. Chandrakanth.H.G, “FFT Based Spectrum Analysis Model for An
Efficient Spectrum Sensing” International Journal of Advanced Research in Engineering &
Technology (IJARET), Volume 5, Issue 12, 2014, pp. 87 - 96, ISSN Print: 0976-6480, ISSN
Online: 0976-6499.

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Gamma radiation induced transformational change in ir spectrum of ebha nematic liquid crystal

  • 1. International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 – 6480(Print), ISSN 0976 – 6499(Online), Volume 6, Issue 3, March (2015), pp. 01-06 © IAEME 1 GAMMA RADIATION-INDUCED TRANSFORMATIONAL CHANGE IN IR SPECTRUM OF EBHA NEMATIC LIQUID CRYSTAL Sudhaker Dixit1 , Rajiv Manohar2 1 University Institute of Engineering & Technology, Babasaheb Bhimrao Ambedkar University, A Central University, Lucknow-226001 2 Liquid Crystal Research Lab, Physics Department, University of Lucknow, Lucknow- 226007 ABSTRACT Gamma ray irradiation technique is the powerful technique to modify the dielectric and electro-optical properties of liquid crystals. It prefers than any other modification technique because no catalysts or additives are required to initiate the reaction. The present paper reports a comparative study of IR spectrum for both irradiated and unirradiated EBHA NLC. The dielectric spectrum and ionic conductivity is also evaluated and well explained in this paper. In addition to this, we have also suggested the concept of the peak data information graph for better understanding of IR spectrum. Keywords: Nano Materials, Condensed Matter Physics, Gamma Radiation, Dielectric, IR Spectrum 1. INTRODUCTION Radiation materials science describes the interaction of radiation with matter. A broad subject covering many forms of irradiation and of matter.The consequences of radiation to core components includes changes in shape and volume by tens of percent, increases in hardness by factors of five or more, severe reduction in ductility and increased embrittlement, and susceptibility to environmentally induced cracking. For these structures to fulfill their purpose, a firm understanding of the effect of radiation on materials is required in order to account for irradiation effects in design, to mitigate its effect by changing operating conditions, or to serve as a guide for creating new, more radiation-tolerant materials that can better serve their purpose [1]. The phenomenon of gamma radiation induced conductivity in solid insulators has been studied by several investigators. Most attention has been given to studies of organic insulators [2-4], and some have been made of inorganic insulators [5-7]. Up to now, only few reports were dedicated to radiation effects on physicochemical properties and on the conductivity of the liquid crystals INTERNATIONAL JOURNAL OF ADVANCED RESEARCH IN ENGINEERING AND TECHNOLOGY (IJARET) ISSN 0976 - 6480 (Print) ISSN 0976 - 6499 (Online) Volume 6, Issue 3, March (2015), pp. 01-06 © IAEME: www.iaeme.com/ IJARET.asp Journal Impact Factor (2015): 8.5041 (Calculated by GISI) www.jifactor.com IJARET © I A E M E
  • 2. International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 – 6480(Print), ISSN 0976 – 6499(Online), Volume 6, Issue 3, March (2015), pp. 01-06 © IAEME 2 materials [8]. Data regarding radiation effects on liquid crystal and organo-photonic material is almost non-existent [9]. Preliminary studies on some liquid crystals suggest that their physical and chemical properties are highly affected by radiation. Most of these suggest that the transition temperatures and the stability of various liquid crystalline mesophases are strongly affected by radiation [10]. Some of the electrical properties such as electrical conductivity and charge carrier mobility subjected by ionizing radiation have been studied very first in 1988 by Kovalchuk et al. [11]. Talor et al. first reported on the degradation of light transmission characteristics of a smectic C liquid crystal [12]. Graham et al. also reported on the effect of space radiation dose on the nematic liquid crystal variable retarders (LCVR) [13]. Such other radiation effects on the liquid crystal materials namely electron beam radiation, UV radiation, ion beam radiation has also been reported [14]. Absorption of gamma rays by liquid crystal may cause physical conformational changes due to thermal and thermo-mechanical effects. These physical changes may cause scattering of light, changes in transmission and reflection properties of filters and coatings. Early liquid crystal phase retarders were screened at Raytheon for radiation sensitivity circa 1989 under the AFRL Beam agility technique program (F33615-87-1507). Phase retarders were used as surrogates for optical phased arrays and subjected to increasing gamma ray dose from a cobalt-60 source, upto a total dose of 9.5 Mrad. It was the first known radiation testing of liquid crystal [15]. In the present paper we have reported the variation in IR spectra of a nematic liquid crystal caused by gamma radiation.In addition to this we have also evaluated the dielectric spectrum for both gamma irradiated and unirradiated EBHA NLC. 2. EXPERIMENTAL DETAILS 2.1 Material Used The liquid crystal sample under investigation is a rod shaped nematic liquid crystal molecule. The structure and its phase transition behavior are given in the Figure 1. Figure 1.Chemical structure with transition scheme for EBHA nematic liquid crystal. 2.2 Preparation of cell Two similar cells having active areas 25 mm2 , (sheet resistance and the visible light transmission is 10 /mm2 and more than 90% respectively) were prepared by using transparent and highly conducting ITO (Indium Tin Oxide) (Diamonds Coating UK) coated optically flat glass substrates used as electrodes. These electrodes give a base to the LC sample to align. Planar alignment is obtained by treating both adhesion promoter and polymer (Nylon 6/6) and then rubbed unidirectional with a velvet cloth. Although the homeotropic cell has been prepared by applying lecithin on the ITO coated surface.The thickness of the cell was maintained at 5 µm by means of Mylar spacer. The complete preparation of cell has been given in our earlier papers [16]. The correct and proper alignment of the LC molecules is extremely important, for precise measurement of
  • 3. International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 – 6480(Print), ISSN 0976 – 6499(Online), Volume 6, Issue 3, March (2015), pp. 01-06 © IAEME 3 electrical properties and which in turn influences dielectric parameters and thus plays an extremely important role in molecular geometry. 2.3 Gamma Ray treatment We have irradiated the EBHA NLC. The irradiation used a 60 Co source, at the dose rate of 2.9 kGy/h, up to a total dose for 34.5 h is 100 kGy. 2.4 Dielectric study The dielectric behavior of the material has been studied by using a computer controlled impedance/ gain phase analyzer Hewlett Packard (HP 4194 A). The dielectric parameters have been measured as a function of temperature and frequency. In order to vary the temperature of the sample holder a microprocessor based heating device Instec hot plate (HCS-302) with an accuracy of ± 0.010 C has been used. Before taking measurements the sample was left for 15 minutes at a particular temperature. The Threshold voltage measurement has also been done by using the same computer controlled impedance/ gain phase analyzer Hewlett Packard (HP 4194 A). The dielectric permittivity has been measured as a function of voltage. 2.5 FT-IR Study FTIR measurements are carried out using IRAffinity-1 (Shimadzu) Fourier Transform Infrared Spectrophotometer. The measurements have been done in the wave number range 500- 4000 cm-1 , keeping air as reference. 3. RESULT AND DISCUSSION Due to the wealth of information that FT-IR spectroscopy provides on molecular state, orientation, and dynamics, it has often been used to characterize liquid crystals and liquid crystal systems. Moreover, it has been observed that the IR spectrum of a liquid crystal system depends on its phase (isotropic or mesogenic). Thus, in addition to the dependence on concentration, the IR spectra of liquid crystalline system have a significant dependence on their director alignment and molecular phase, which is controlled by temperature for thermotropic liquid crystals. In this way the radiated and unirradiated samples are analyzed by FT-IR spectroscopy. The FT-IR spectrum for the unirradiated and gamma irradiated EBHA nematic liquid crystal is shown in figure 2. Figure 2. Variation in transmittance with respect to wavelengthfor EBHA NLC
  • 4. International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 – 6480(Print), ISSN 0976 – 6499(Online), Volume 6, Issue 3, March (2015), pp. 01-06 © IAEME 4 For better understanding of the IR spectra, assignments of the major peaks of the liquid crystal material are shown in peak data information (PDI) graphs. The PDI graphs for the unirradiated and gamma irradiated liquid crystalline materials have been shown in figure 3. Using PDI graphs FT-IR study suggests that up to given dose of gamma radiation, the liquid crystal system causes chemical change which is responsible for shifting of absorption peaks. Which is responsible for variation in transmittance as shown in figure.Figures also suggest the gamma irradiated EBHA NLC exhibit a high transmittance as compared with unirradiated EBHA NLC. Figure 3. PDI graph for EBHA NLC When the frequency of a specific vibration is equal to the frequency of the IR radiation directed to the molecule, the molecule absorbs the radiation. The total number of observed bands is generally different from the total number of fundamental vibrations. It is reduced because some modes are not IR active and a single frequency can cause more than one mode of motion to occur. Conversely additional bands are generated by the appearance of overtones, combination of fundamental frequencies, coupling interactions of two fundamental absorption frequencies. Thus we can say that the shifting of absorption peaks is due to the gamma induced physic-chemical change in liquid crystal molecule. In this way the dielectric response of the sample with frequency has been taken (figure 4). Figure 4. Complex dielectric permittivity with variation in frequency
  • 5. International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 – 6480(Print), ISSN 0976 – 6499(Online), Volume 6, Issue 3, March (2015), pp. 01-06 © IAEME 5 The observed value of complex dielectric permittivity for both irradiated and unirradiated EBHA NLC, nature of variation with frequency is same, but the values have increased for gamma irradiated EBHA NLC sample.Actually irradiation causes a chemical change in liquid crystalline materials, it may include cross linking, chain scission, formation of alkyl groups, depletion of hetero atoms. Effect of gamma irradiation or such other ionizing radiation is primarily chain scission.Therefore many physical and chemical properties can show modification with gamma irradiation.Radiation mainly affects in two basic ways, both resulting with excitation or ionization of atoms.In this fashion ionic conductivity of liquid crystal material has also been investigated and shown in figure 5.The ionic conductivity for irradiated EBHA NLC sample is comparatively higher than that of unirradiated EBHA NLC sample. Figure 5. Variation in ionic conductivity of EBHA NLC caused by gamma radiation 4. CONCLUSION We observe that the nature of variation of dielectric permittivity with frequency and temperature remains same for both the gamma irradiated and the unirradiated EBHA samples, but the value of dielectric permittivity for the gamma irradiated sample is higher as compared to the unirradiated EBHA sample. This increment in the gamma irradiated sample can be explained on the basis of physicochemical change inthe EBHA molecules due to irradiation.Also the effect of gamma irradiation on EBHA NLC sample has been evaluated using FT-IR. New concept of PDI graph has been shown for better understanding of IR spectra. REFERENCES 1. Gary S. Was, “Fundamentals of Radiation Materials Science,” Springer, Berlin, Heidelberg, New York, 2007. 2. J.F.Fowler, Proc. Roy. Soc., 1956, 464-470. 3. S.E. Harrison, IEEE Conference Paper, 1962, 62-1251. 4. F.N. Coppage, A.W.Snyder, ibid, 1963, 63-118. 5. G.C. Huth, General Electric Company Aircraft Nuclear Propulsion Department, Paper, 1958, 58- 331. 6. V.E. Culler, H.E.Rexford, Proc. IEEE, 1965, 112, 11024-11039. 7. H.J.Wintle, Internat. J. Appl. Radiation and Isotopes, 1960, 8, 132-148. 8. H. Ohoka, M. Ozaki, L.M. Blinov, M.I. Barnik, N.M. Shtykov, K.Yoshino, Mol. Cryst. Liq. Cryst., 2001, 366, 283-293.
  • 6. International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 – 6480(Print), ISSN 0976 – 6499(Online), Volume 6, Issue 3, March (2015), pp. 01-06 © IAEME 6 9. R.B. Meyer,P.S.Pershan, Sol. State. Comms, 1973, 13, 989-992. 10. A.Derzhanski, A.Petrov, M.Mitov, J. Phys. (Paris), 1978, 39, 273-285. 11. A.V.Kovalchuk,O.D. Lavrentovich,V.A. Linev, Sov. Tech. Phys. Lett., 1988, 14, 381-382. 12. R.C. Webb, L.C. Cohn, E.W. Taylor, R.A. Greenwell, Proc. SPIE, 1995, 2482, 3–15. 13. A. Graham, G. Kopp, C. Vargas-Aburto, Uribe, R. Proc. SPIE 1996, 2811, 46–50. 14. M.C.Rath, S.K.Sarkar, V.K.Wadhawan, R.Verma, I.M.L. Das, R.Dabrowski,M.Tykarska, R.Dhar, Opto.-Electron. Rev., 2008, 16, 399–403. 15. J. Stockley, S.Serati, D.Dauwe, T. Deaton, J.Nonnast, SPIE Proc., 2006, 6308, 6630805-17. 16. S.P. Yadav, K.K. Pandey, A.K. Misra, S. Dixit, R. Manohar, Can. J. Phys.,2011, 89, 661-665. 17. Bhagyajyothi, Immanuel J., P. Bhaskar, L.S. Sudheer and Parvathi C. S., “Advanced Lock-In Amplifier For Detection of Phase Transitions In Liquid Crystals” International Journal of Advanced Research in Engineering & Technology (IJARET), Volume 4, Issue 2, 2013, pp. 17 - 26, ISSN Print: 0976-6480, ISSN Online: 0976-6499. 18. C. Basavaraju and Dr. Chandrakanth.H.G, “FFT Based Spectrum Analysis Model for An Efficient Spectrum Sensing” International Journal of Advanced Research in Engineering & Technology (IJARET), Volume 5, Issue 12, 2014, pp. 87 - 96, ISSN Print: 0976-6480, ISSN Online: 0976-6499.