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Credit seminar
Size dependent optical properties of Zn
doped Cr2O3 nanoparticles
Submitted by:
Name: Gaurav Kumar Yogesh
Program: M.Sc. Physics (Nanophysics)
Reg. No. CUPB/M.Sc./PMS/SBAS/2013-14/01
Supervisor: Dr. Kamlesh Yadav
Centre for Physical and Mathematical Sciences
5/22/2015 1
 Introduction
 Historic background
 Method to prepare nanoparticles
 Properties of nanoparticles
 Material and methods
 Experimental analysis
 Results and discussion
 Conclusions
 Review of literature
 References
5/22/2015 2
 Technologies ,which incorporate the materials, to manipulate
measures or features with atleast one of its critical dimensions
between 1 nm to 100nm.
 Nanomaterials can be of two types; engineered or non-engineered
 Engineered nanoparticles are intentionally created to meet the
specific applications e.g. CNT, Fullerene etc.
 Non-engineered nanoparticles are unintentionally created by
nature such as volcanic ash, DNA and protein.
5/22/2015 3
www.essentialchemicalindustry.org
5/22/2015 4
 Gold colloids were used for
aesthetic (decoration) and
curative purposes
 the Lycurgus Cup (4th Century
B.C) is ruby red in transmitted
light and green in reflected
light, due to the presence of
gold colloids
 1857: Faraday reported
formation of deep-red
solutions of colloidal Au
LS-FCM University di Bologna
5/22/2015 5
 Fasters
 Lighters
 Can get into small spaces
 Cheaper
 More energy efficient
 Less waste product
 Use less materials to produce
 Different properties
http://snf.stanford.edu/Education/Nanotechnologynt scales
5/22/2015 6
 Top-Down approach
 These approach use larger (macroscopic) initial structure, which
can be eternally controlled in the process of nanostructure.
 Typical examples are etching through the mask and ball milling
and applications of several plastic deformation.
 Bottom-Up approach
 These approaches include the miniaturization of materials
components (up to atomic level) with further self assembly process
leading to the formation of nanostructure
 Typical examples are quantum dot formation during epitaxial
growth and formation of nanoparticles from colloidal dispersion.
5/22/2015 7
 Two of the reasons:
1. Ratio of surface area-to-volume of structure increases
most atoms are at or near the surface, which make them
more weakly bonded and more reactive.
2. Quantum mechanical effects are important, size of
structure is on same scale as the wavelengths of
electrons, and quantum confinement occurs resulting in
changes in electronic and optical properties
5/22/2015 8
 Supercomputer in your palm,
 Very tiny motors, pumps, micro sensor,
and accelerometers;
 Energy storage (batteries) and
conversion (solar cells)
using nanowires and nanotubes
 Stain and wrinkle resistant clothes, transparent zinc oxide sunscreen,
fast-absorbing drugs and nutrients.
5/22/2015 9
 To synthesise the nanoparticles by using the novel solvent and cost
effective
 To study the doping effect on its optical and structural properties.
 To compare the various results on its process of synthesising the
nanoparticles and doping effects
5/22/2015 10
 All the reagents were of AR/GR quality and were purchased from
the Sigma-Aldrich, Loba- Chemi Pt. Ltd., and were used without
further purification.
 Infrared (IR) spectra of nanoparticles were recorded with KBr on a
Bruker FT-IR spectrometer.
 Surface morphology and size of the particles has been recorded with
gold coating on the samples
 UV-visible spectroscopy was used to record the optical band of the
nanoparticles.
5/22/2015 11
For the characterisation of the samples we do the following analysis
1. Morphological and structural analysis:
 FESEM had been used to study the morphological and structure of
prepared samples.
2. Optical analysis:
 The optical band gap of the material had been calculated by the
(Shimazdu 02206) UV-visible spectrometer
3. Spectroscopical analysis:
 The various functional groups and the characteristics peaks due to
the various compounds can be observed by (Brucker Ltd) FTIR
spectrometer
 All the experimental analysis has been performed at the lab of
(Centre for Physical and Mathematical sciences) central university
of Punjab, Bathinda
5/22/2015 12
http://www.iitk.ac.in/meesa/SEM/tutorial/SEM_MS
5/22/2015 13
 FESEM image of the prepared samples of respective particle sizes are 55,
41, 26, 22 nm.
Fig. FESEM image of Zn doped Cr2O3 nanoparticles
5/22/2015 14
 FTIR stands for Fourier Transform Infrared Spectroscopy.
 Works on the principle of the Michelson's Interferometer.
 FTIR spectrometer acquires broadband NIR and FIR spectra.
 FTIR is method of obtaining the infrared spectra by collecting an inferogram
of a sample signal, using the interferometer and then a Fourier transform on
the inferogram to obtain the spectrum
 FTIR spectrometer collects and digitised the interferogram, perform the FT
function and display the spectrum
 Every bond or the functional groups requires the different frequency for
absorption, hence characteristic peaks is observed for the every functional
groups or the part of the molecules.
 According to principle
Applied Infrared frequency = Natural frequency of vibration
5/22/2015 15
 Fig. FTIR characteristics peaks of the Zn doped Cr2O3 nanoparticles
5/22/2015 16
Fig. FTIR set-up of central university of Punjab, Bathinda
5/22/2015 17
 Optical band gap of the following samples are calculated by Tauc
relation, by extrapolating the slope of the peaks gives the optical
band of the nanomaterials.
Fig. Optical band of the samples are obtained by the FTIR data5/22/2015 18
Name of the
samples
Method of
preparation of
the samples
Average
particles
size(nm)
Optical
band gap
(eV)
Characteristic peaks
observed in FTIR
(Cr-O Vibration)
cm-1
Sample-1 Sol-gel 55 1.50 619
Sample-2 Sol-gel 26 3.50 484
Sample-3 Hydrothermal 22 3.70 760
Sample-4 Sol gel 41 2.09 803
5/22/2015 19
 Decrease in the size of nanoparticles results in the increase in the
optical band gap of the nanomaterials.
 It arises due the quantum confinement .
 Surface Plasmon resonance: The resonance condition is established
when the frequency of incident photons matches the natural
frequency of surface electrons oscillating against the restoring force
of positive nuclei. SPR in subwavelength scale nanostructures can
be polaritonic or plasmonic in nature.
5/22/2015 20
Fig. Variation of the particle size with
Band gap of nanoparticles
Fig. Variation of the refractive of the
Nanoparticles with Band gap
5/22/2015 21
 Size dependent optical properties of nanomaterials.
 Refractive index of the nanomaterials is decreases with the increases
in the band gap.
 Confirmation of the quantum size effect.
 Cr2O3 nanoparticles can be used in creating the highly efficient solar
cells and optoelectronic devices.
 Because of large band gap(≈ 3 eV) used in the insulating materials.
 The band gap of the nanoparticles can altered by changing the
environmental conditions or the preparing technique.
 It can used in manufacturing the Transparent conducting Oxide (TCO)
materials which have both simultaneous property of conducting and
transparent.
5/22/2015 22
 Abdullah, M., Rajab, F. M., & Al-Abbas, S. M. (2014). Structural and optical
characterization of Cr2O3 nanostructures: Evaluation of its dielectric properties. AIP
Advances, 4(2), 027121.
 Athar, M., & Das, A. J. (2014). Therapeutic Nanoparticles: State-of-the-art of
nanomedicine. Advanced Materials Review, 1(1), 25-37.
 Bañobre-López, M., Vázquez-Vázquez, C., Rivas, J., & López-Quintela, M. A. (2003).
Magnetic properties of chromium (III) oxide nanoparticles. Nanotechnology, 14(2), 318.
 Cao, H., Qiu, X., Liang, Y., Zhao, M., & Zhu, Q. (2006). Sol-gel synthesis and
photoluminescence of p-type semiconductor Cr 2 O 3 nanowires. Applied physics
letters, 88(24), 241112-241112-241113.
 Esparza, I., Paredes, M., Martinez, R., Gaona-Couto, A., Sanchez-Loredo, G., Flores-
Velez, L. M., & Dominguez, O. (2011). Solid State reactions in Cr 2 O 3-ZnO
nanoparticles synthesized by triethanolamine chemical precipitation. Materials Sciences
and Applications, 2(11), 1584.
 Farzaneh, F. (2011). Synthesis and Characterization of Cr2O3 Nanoparticles with
Triethanolamine in Water under Microwave Irradiation. Journal of Sciences, Islamic
Republic of Iran, 22(4), 329-333.
 Fernandez-Garcia, M., Martinez-Arias, A., Hanson, J., & Rodriguez, J. (2004).
Nanostructured oxides in chemistry: characterization and properties. Chemical Reviews,
104(9), 4063-4104.5/22/2015 23
 Jaswal, V. S., Arora, A. K., Singh, J., Kinger, M., & Gupta, V. D. (2014). Synthesis
and Characterization of Chromium Oxide Nanoparticles. Oriental Journal of
Chemistry, 30(2), 559-566.
 Jin, H., Huang, Y., & Jian, J. (2015). Plate-like Cr 2 O 3 for highly selective sensing
of nitric oxide. Sensors and Actuators B: Chemical, 206, 107-110.
 Kawabata, A., Yoshinaka, M., Hirota, K., & Yamaguchi, O. (1995). Hot Isostatic
Pressing and Characterization of Sol‐Gel‐Derived Chromium (III) Oxide. Journal of
the American Ceramic Society, 78(8), 2271-2273.
 Lei, S., Peng, X., Liang, Z., Li, X., Wang, C., Cheng, B., . . . Zhou, L. (2012). Self-
template formation and properties study of Cr 2 O 3 nanoparticle tubes. Journal of
Materials Chemistry, 22(4), 1643-1651.
 Li, D., Han, Z., Zheng, J., Wang, X., Geng, D., Li, J., & Zhang, Z. (2009). Spin
canting and spin-flop transition in antiferromagnetic Cr 2 O 3 nanocrystals. Journal
of Applied Physics, 106(5), 053913-053913-053915.
 Li, L., Yan, Z. F., Lu, G. Q., & Zhu, Z. H. (2006). Synthesis and structure
characterization of chromium oxide prepared by solid thermal decomposition
reaction. The Journal of Physical Chemistry B, 110(1), 178-183.
 Lota, G., Frackowiak, E., Mittal, J., & Monthioux, M. (2007). High performance
supercapacitor from chromium oxide-nanotubes based electrodes. Chemical physics
letters, 434(1), 73-77.5/22/2015 24
 Meenambika, R., Ramalingom, S., & Chithambara Thanu, T. (2013). Effect of
calcinations temperature on the structure of Cr 2 O 3 nanoparticles prepared by novel
solvent free synthesis. Paper presented at the Advanced Nanomaterials and Emerging
Engineering Technologies (ICANMEET), 2013 International Conference on.
 Mohanapandian, K., & Krishnan, A. (2014). Effect of Concentration of Ni 2 on the
Physio Chemical Properties of Cr2o3 Nano Particles.
 Pei, Z., Xu, H., & Zhang, Y. (2009). Preparation of Cr 2 O 3 nanoparticles via C 2 H 5
OH hydrothermal reduction. Journal of Alloys and Compounds, 468(1), L5-L8.
 Rao, T. M., Yang, Y., & Sayari, A. (2009). Ethane dehydrogenation over pore-expanded
mesoporous silica supported chromium oxide: 1. Catalysts preparation and
characterization. Journal of Molecular Catalysis A: Chemical, 301(1), 152-158.
 Robertson, J. (2004). High dielectric constant oxides. The European physical journal
applied physics, 28(03), 265-291.
 Vayssieres, L., & Manthiram, A. (2003). 2-D mesoparticulate arrays of α-Cr2O3. The
Journal of Physical Chemistry B, 107(12), 2623-2625.
 Vigil, O., Cruz, F., Morales-Acevedo, A., Contreras-Puente, G., Vaillant, L., & Santana,
G. (2001). Structural and optical properties of annealed CdO thin films prepared by
spray pyrolysis. Materials Chemistry and Physics, 68(1), 249-252
5/22/2015 25
5/22/2015 26

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synthesis of doped chromium oxide nanoparticles

  • 1. Credit seminar Size dependent optical properties of Zn doped Cr2O3 nanoparticles Submitted by: Name: Gaurav Kumar Yogesh Program: M.Sc. Physics (Nanophysics) Reg. No. CUPB/M.Sc./PMS/SBAS/2013-14/01 Supervisor: Dr. Kamlesh Yadav Centre for Physical and Mathematical Sciences 5/22/2015 1
  • 2.  Introduction  Historic background  Method to prepare nanoparticles  Properties of nanoparticles  Material and methods  Experimental analysis  Results and discussion  Conclusions  Review of literature  References 5/22/2015 2
  • 3.  Technologies ,which incorporate the materials, to manipulate measures or features with atleast one of its critical dimensions between 1 nm to 100nm.  Nanomaterials can be of two types; engineered or non-engineered  Engineered nanoparticles are intentionally created to meet the specific applications e.g. CNT, Fullerene etc.  Non-engineered nanoparticles are unintentionally created by nature such as volcanic ash, DNA and protein. 5/22/2015 3
  • 5.  Gold colloids were used for aesthetic (decoration) and curative purposes  the Lycurgus Cup (4th Century B.C) is ruby red in transmitted light and green in reflected light, due to the presence of gold colloids  1857: Faraday reported formation of deep-red solutions of colloidal Au LS-FCM University di Bologna 5/22/2015 5
  • 6.  Fasters  Lighters  Can get into small spaces  Cheaper  More energy efficient  Less waste product  Use less materials to produce  Different properties http://snf.stanford.edu/Education/Nanotechnologynt scales 5/22/2015 6
  • 7.  Top-Down approach  These approach use larger (macroscopic) initial structure, which can be eternally controlled in the process of nanostructure.  Typical examples are etching through the mask and ball milling and applications of several plastic deformation.  Bottom-Up approach  These approaches include the miniaturization of materials components (up to atomic level) with further self assembly process leading to the formation of nanostructure  Typical examples are quantum dot formation during epitaxial growth and formation of nanoparticles from colloidal dispersion. 5/22/2015 7
  • 8.  Two of the reasons: 1. Ratio of surface area-to-volume of structure increases most atoms are at or near the surface, which make them more weakly bonded and more reactive. 2. Quantum mechanical effects are important, size of structure is on same scale as the wavelengths of electrons, and quantum confinement occurs resulting in changes in electronic and optical properties 5/22/2015 8
  • 9.  Supercomputer in your palm,  Very tiny motors, pumps, micro sensor, and accelerometers;  Energy storage (batteries) and conversion (solar cells) using nanowires and nanotubes  Stain and wrinkle resistant clothes, transparent zinc oxide sunscreen, fast-absorbing drugs and nutrients. 5/22/2015 9
  • 10.  To synthesise the nanoparticles by using the novel solvent and cost effective  To study the doping effect on its optical and structural properties.  To compare the various results on its process of synthesising the nanoparticles and doping effects 5/22/2015 10
  • 11.  All the reagents were of AR/GR quality and were purchased from the Sigma-Aldrich, Loba- Chemi Pt. Ltd., and were used without further purification.  Infrared (IR) spectra of nanoparticles were recorded with KBr on a Bruker FT-IR spectrometer.  Surface morphology and size of the particles has been recorded with gold coating on the samples  UV-visible spectroscopy was used to record the optical band of the nanoparticles. 5/22/2015 11
  • 12. For the characterisation of the samples we do the following analysis 1. Morphological and structural analysis:  FESEM had been used to study the morphological and structure of prepared samples. 2. Optical analysis:  The optical band gap of the material had been calculated by the (Shimazdu 02206) UV-visible spectrometer 3. Spectroscopical analysis:  The various functional groups and the characteristics peaks due to the various compounds can be observed by (Brucker Ltd) FTIR spectrometer  All the experimental analysis has been performed at the lab of (Centre for Physical and Mathematical sciences) central university of Punjab, Bathinda 5/22/2015 12
  • 14.  FESEM image of the prepared samples of respective particle sizes are 55, 41, 26, 22 nm. Fig. FESEM image of Zn doped Cr2O3 nanoparticles 5/22/2015 14
  • 15.  FTIR stands for Fourier Transform Infrared Spectroscopy.  Works on the principle of the Michelson's Interferometer.  FTIR spectrometer acquires broadband NIR and FIR spectra.  FTIR is method of obtaining the infrared spectra by collecting an inferogram of a sample signal, using the interferometer and then a Fourier transform on the inferogram to obtain the spectrum  FTIR spectrometer collects and digitised the interferogram, perform the FT function and display the spectrum  Every bond or the functional groups requires the different frequency for absorption, hence characteristic peaks is observed for the every functional groups or the part of the molecules.  According to principle Applied Infrared frequency = Natural frequency of vibration 5/22/2015 15
  • 16.  Fig. FTIR characteristics peaks of the Zn doped Cr2O3 nanoparticles 5/22/2015 16
  • 17. Fig. FTIR set-up of central university of Punjab, Bathinda 5/22/2015 17
  • 18.  Optical band gap of the following samples are calculated by Tauc relation, by extrapolating the slope of the peaks gives the optical band of the nanomaterials. Fig. Optical band of the samples are obtained by the FTIR data5/22/2015 18
  • 19. Name of the samples Method of preparation of the samples Average particles size(nm) Optical band gap (eV) Characteristic peaks observed in FTIR (Cr-O Vibration) cm-1 Sample-1 Sol-gel 55 1.50 619 Sample-2 Sol-gel 26 3.50 484 Sample-3 Hydrothermal 22 3.70 760 Sample-4 Sol gel 41 2.09 803 5/22/2015 19
  • 20.  Decrease in the size of nanoparticles results in the increase in the optical band gap of the nanomaterials.  It arises due the quantum confinement .  Surface Plasmon resonance: The resonance condition is established when the frequency of incident photons matches the natural frequency of surface electrons oscillating against the restoring force of positive nuclei. SPR in subwavelength scale nanostructures can be polaritonic or plasmonic in nature. 5/22/2015 20
  • 21. Fig. Variation of the particle size with Band gap of nanoparticles Fig. Variation of the refractive of the Nanoparticles with Band gap 5/22/2015 21
  • 22.  Size dependent optical properties of nanomaterials.  Refractive index of the nanomaterials is decreases with the increases in the band gap.  Confirmation of the quantum size effect.  Cr2O3 nanoparticles can be used in creating the highly efficient solar cells and optoelectronic devices.  Because of large band gap(≈ 3 eV) used in the insulating materials.  The band gap of the nanoparticles can altered by changing the environmental conditions or the preparing technique.  It can used in manufacturing the Transparent conducting Oxide (TCO) materials which have both simultaneous property of conducting and transparent. 5/22/2015 22
  • 23.  Abdullah, M., Rajab, F. M., & Al-Abbas, S. M. (2014). Structural and optical characterization of Cr2O3 nanostructures: Evaluation of its dielectric properties. AIP Advances, 4(2), 027121.  Athar, M., & Das, A. J. (2014). Therapeutic Nanoparticles: State-of-the-art of nanomedicine. Advanced Materials Review, 1(1), 25-37.  Bañobre-López, M., Vázquez-Vázquez, C., Rivas, J., & López-Quintela, M. A. (2003). Magnetic properties of chromium (III) oxide nanoparticles. Nanotechnology, 14(2), 318.  Cao, H., Qiu, X., Liang, Y., Zhao, M., & Zhu, Q. (2006). Sol-gel synthesis and photoluminescence of p-type semiconductor Cr 2 O 3 nanowires. Applied physics letters, 88(24), 241112-241112-241113.  Esparza, I., Paredes, M., Martinez, R., Gaona-Couto, A., Sanchez-Loredo, G., Flores- Velez, L. M., & Dominguez, O. (2011). Solid State reactions in Cr 2 O 3-ZnO nanoparticles synthesized by triethanolamine chemical precipitation. Materials Sciences and Applications, 2(11), 1584.  Farzaneh, F. (2011). Synthesis and Characterization of Cr2O3 Nanoparticles with Triethanolamine in Water under Microwave Irradiation. Journal of Sciences, Islamic Republic of Iran, 22(4), 329-333.  Fernandez-Garcia, M., Martinez-Arias, A., Hanson, J., & Rodriguez, J. (2004). Nanostructured oxides in chemistry: characterization and properties. Chemical Reviews, 104(9), 4063-4104.5/22/2015 23
  • 24.  Jaswal, V. S., Arora, A. K., Singh, J., Kinger, M., & Gupta, V. D. (2014). Synthesis and Characterization of Chromium Oxide Nanoparticles. Oriental Journal of Chemistry, 30(2), 559-566.  Jin, H., Huang, Y., & Jian, J. (2015). Plate-like Cr 2 O 3 for highly selective sensing of nitric oxide. Sensors and Actuators B: Chemical, 206, 107-110.  Kawabata, A., Yoshinaka, M., Hirota, K., & Yamaguchi, O. (1995). Hot Isostatic Pressing and Characterization of Sol‐Gel‐Derived Chromium (III) Oxide. Journal of the American Ceramic Society, 78(8), 2271-2273.  Lei, S., Peng, X., Liang, Z., Li, X., Wang, C., Cheng, B., . . . Zhou, L. (2012). Self- template formation and properties study of Cr 2 O 3 nanoparticle tubes. Journal of Materials Chemistry, 22(4), 1643-1651.  Li, D., Han, Z., Zheng, J., Wang, X., Geng, D., Li, J., & Zhang, Z. (2009). Spin canting and spin-flop transition in antiferromagnetic Cr 2 O 3 nanocrystals. Journal of Applied Physics, 106(5), 053913-053913-053915.  Li, L., Yan, Z. F., Lu, G. Q., & Zhu, Z. H. (2006). Synthesis and structure characterization of chromium oxide prepared by solid thermal decomposition reaction. The Journal of Physical Chemistry B, 110(1), 178-183.  Lota, G., Frackowiak, E., Mittal, J., & Monthioux, M. (2007). High performance supercapacitor from chromium oxide-nanotubes based electrodes. Chemical physics letters, 434(1), 73-77.5/22/2015 24
  • 25.  Meenambika, R., Ramalingom, S., & Chithambara Thanu, T. (2013). Effect of calcinations temperature on the structure of Cr 2 O 3 nanoparticles prepared by novel solvent free synthesis. Paper presented at the Advanced Nanomaterials and Emerging Engineering Technologies (ICANMEET), 2013 International Conference on.  Mohanapandian, K., & Krishnan, A. (2014). Effect of Concentration of Ni 2 on the Physio Chemical Properties of Cr2o3 Nano Particles.  Pei, Z., Xu, H., & Zhang, Y. (2009). Preparation of Cr 2 O 3 nanoparticles via C 2 H 5 OH hydrothermal reduction. Journal of Alloys and Compounds, 468(1), L5-L8.  Rao, T. M., Yang, Y., & Sayari, A. (2009). Ethane dehydrogenation over pore-expanded mesoporous silica supported chromium oxide: 1. Catalysts preparation and characterization. Journal of Molecular Catalysis A: Chemical, 301(1), 152-158.  Robertson, J. (2004). High dielectric constant oxides. The European physical journal applied physics, 28(03), 265-291.  Vayssieres, L., & Manthiram, A. (2003). 2-D mesoparticulate arrays of α-Cr2O3. The Journal of Physical Chemistry B, 107(12), 2623-2625.  Vigil, O., Cruz, F., Morales-Acevedo, A., Contreras-Puente, G., Vaillant, L., & Santana, G. (2001). Structural and optical properties of annealed CdO thin films prepared by spray pyrolysis. Materials Chemistry and Physics, 68(1), 249-252 5/22/2015 25