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monochromator, (Cornerstone 260, Newport, Irvine, CA, USA). The light that exits
the monochromator (λexc = 430 nm) is focused on to the colloidal solution. The
second one is an IR laser module of 780 nm. Both down- and up-conversion are
detected using a second monochromator (Cornerstone 260, Newport, Irvine, CA,
USA), positioned at a 90˝ angle to the first monochromator. The monochromator is
scanned over the visible wavelength region and the fluorescence signal is detected
bythephotomultiplier tube(PMT77340,Newport, Irvine,CA,USA), locatedat the
exit port of the second monochromator. Then, the visible fluorescent emission is
monitoredusingapowermeter (2935C,Newport, Irvine,CA,USA).
Transmission electron microscope (TEM) (JEOL 1400, Peabody, MA, USA),
is used to image the synthesized REDC NPs. The mean diameter of the
nanoparticles is calculated using ImageJ software through Gaussian distribution
of many size measurements. The operating parameters of the XRD (PANalytical
X’Pert PRO, Amestrdam, The Netherlands), are 45 KV, 40 A and Cu Kα radiation
(λ=0.15406nm). The conductivity of the solution of the synthesized nanoparticles
ismeasuredbyA500Orionmeter (Thermoscientific,TechPark,Singapore).
7
The optical absorption is measured using a dual‐beam UV‐Vis‐NIR spectrometer (UV‐3101PC
Shimadzu, Tokyo, Japan). After the annealing procedure, a solution of nanoparticles is prepared
with a concentration of 0.02 mg of nanoparticles in 10 mL of DI water. The colloidal solution is
illuminated with both near‐UV and near infra‐red (NIR) excitations in an experimental apparatus
that was designed to measure the down‐ and up‐conversion process, as described in Figure 8. The
fluorescence spectroscopy system consists of two excitation sources. The first one, the near UV
excitation, is a Xenon lamp coupled to a monochro ator, (Cornerstone 260, Newport, Irvine, CA,
USA). The light that exits the monochromator (λexc = 430 nm) is focused on to the colloidal solution.
The second one is an IR laser module of 780 nm. Both down‐ and up‐conversion are detected using
a second monochromator (Cornerstone 260, Newport, Irvine, CA, USA), positioned at a 90° angle to
the first monochromator. The monochromator is scanned over the visible wavelength region and
the fluorescence signal is detected by the photomultiplier tube (PMT 77340, Newport, Irvine, CA,
USA), located at the exit port of the second monochromator. Then, the visible fluorescent emission
is monitored
using
a power meter (2935C, Newport, Irvine, CA,
USA).
Transmission electron microscope (TEM) (JEOL
1400,
Peabody,
MA, USA),
is
used to image the
synthesized REDC NPs. The mean diameter of the nanoparticles is calculated using ImageJ
software through Gaussian distribution of many size measurements. The operating parameters of
the XRD (PANalytical X’Pert PRO, Amestrdam, The Netherlands), are 45 KV, 40 A and
Cu Kα radiation (λ = 0.15406 nm). The conductivity of the solution of the synthesized nanoparticles
is measured
by A500 Orion meter (Thermo scientific,
Tech Park, Singapore).
Figure 8. Up‐ and down‐conversion fluorescence setup.
3.3. Coating Procedure
The synthesized nanoparticles are coated on the back sides of polycrystalline solar cells
(2 inches × 2 inches) ordered from Solar Winds Inc., Austin, TX, USA. Coating has been operated
Figure8. Up-anddown-conversionfluorescencesetup.
3.3. CoatingProcedure
The synthesized nanoparticles are c ated on the back sides of pol crystalline
solar cells (2 inchesˆ 2 inches) ordered from Solar Winds Inc., Austin, TX, USA.
Coating has been operated using spin coater at 1500 rpm for a minute. Before
coating, the electrodes on the backside of the cell have been covered through a
scotch and released after the coating. That could avoid the direct contact between
the nanoparticles and the metallic electrodes. The surface profile is detected
using 3D optical surface profiler ZeGage (Zygo, Middlefield, CT, USA), with
concentrating on the edge between coated cell and non-coated electrode to detect
the thickness.
183
Photovoltaic Materials and Electronic Devices
- Title
- Photovoltaic Materials and Electronic Devices
- Author
- Joshua M. Pearce
- Editor
- MDPI
- Location
- Basel
- Date
- 2016
- Language
- English
- License
- CC BY-NC-ND 4.0
- ISBN
- 978-3-03842-217-4
- Size
- 17.0 x 24.4 cm
- Pages
- 216
- Keywords
- Perovskite, Plasmonics, Nanostructured Materials, Anti-Reflection Coatings, Transparent Conductive Oxides, Amorphous Silicon, Dye-sensitized Solar Cells (DSSCs) Materials, Organic Photovoltaic Materials, Solar Energy Materials
- Categories
- Naturwissenschaften Physik
- Technik