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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 12 | Dec 2019 www.irjet.net p-ISSN: 2395-0072
ยฉ 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1571
Effect of Series Resistance and Layer Thickness on PCE and Fill Factor
in Organic Solar Cell with P3HT: PCBM Active Layer
Pooja Sinha1, Rahul Baghel2
1M.Tech scholar,Dept. of Electrical and Electronics Engineering, SSGI Durg-490001, Chhattisgarh, India
2Assistant Professor, Dept. of Electrical and Electronics Engineering, SSGI Durg-490001, Chhattisgarh, India
---------------------------------------------------------------------***----------------------------------------------------------------------
Abstract - This paper reports a study on the effect of series
and layer thickness on the performance of an organic
photovoltaic cell which is based on polymer/fullerene P3HT:
PCBM. Electrical simulation has been examined on ITO-
PEDOT: PSS-P3HT: PCBM-Al structure with GPVDM (General-
Purpose Photovoltaic Device Model) software. We used the
GPVDM software to investigate the effect of series resistance
and layer thickness on power conversion efficiency (PCE) and
fill factor (FF) in an organic solar cell which is based on P3HT:
PCBM as an absorbing layer. The changes were made by
applying the different series resistance and layer thickness
value. The results show that the power conversion efficiency
can be increased by changing the value of the seriesresistance
and layer thickness, in our case the power conversion
efficiency has been increased from 11.66% to 13.84% and fill
factor has been change from 66.29% to 70%.
Key Words: Organic photovoltaic cell, P3HT:PCBM,GPVDM,
series resistance, thickness effect.
1. INTRODUCTION
Organic photovoltaics (OPVs) have attracted considerable
interest over the past two decades due to their advantages
over inorganic solar cells. OPVs are lightweight, cheap and
non-toxic compared to inorganic solar cells. They are also
robust and versatile mechanically. Organic solar cells, as the
name implies, transform light from organic molecules into
electricity. For these solar cells, synthetic polymers and
small organic molecules are widely used. Their long chain
relocation via alternating double and single connections
helps to effectively transfer the electron in the cell. The
highest occupied molecular orbitals(HOMOs)andthelowest
unoccupied molecular orbitals (LUMOs) are these orbits. An
optical band gap in the half conductor area is the power
disparity between the low-energy HOMOs and the high-
energy LUMOs. Becauseoftheirversatilematerial properties
and low-cost processing, organic solar cellshavebeena very
remarkable area of research in recent years.
In the early 1950s, organic solar photovoltaic cells were
developed. Since 1965, organic chemistry has had a fast
growth and the first discovery of photoconductivity in
organic compounds was published in 1906. The product,
Solarmer, developed for the first time Organic Photovoltaic.
BHJ-based organic solar cells (Bulk Hetro-junction) are
composites of P3HT (Poly3-hexylthiophene) and PCBM
(phynyl-C-70buteric acid methyl ester) [1-2]. Gpvdm
(OPVDM's new name) is a free general-purpose device
simulation tool. Originallydesigned tosimulateorganicsolar
cells, it has now been expanded to simulate other system
categories, including OLEDs, OFETsandmanyotherforms of
solar cells of 1st, 2nd and 3rd generation. Thephysical model
solves drift-diffusion of electron and hole as well as
continuity equations of the carrier in position space to
describe the load movement within the device. The model
also solves the equation of Poisson to calculate the potential
of internal electrostatics. Recombination and carrier
trapping are described in the model using Shockley-Read-
Hall (SRH) formalism; it is feasible to arbitrarily define the
distribution of trap states. Both equations can be solved in a
steady state or in a time domain.
The model facilitates the study of the effect on system
performance of product parameters such as mobility,
energetic disorder, doping, and recombination cross-
sections. All internal device parameters such as current
density load frequency, position distribution of trapped
carriers and energy storage can be controlledthrough either
the graphical interface or directly from output data. The
system includes both an electrical and an optical solver,
allowing simulation of current / voltage characteristics and
the optical model profile within the device. The model is
available for Windows and Linux (x86 and ARM) and it is
easy to use graphical interface. Gpvdm is a tool used to
simulate and design solar cells to harvest the energy of the
sun.
Fig 1: GPVDM Home Window
2. ELECTRICAL SIMULATION
The significant parameters that influence its performance
should be explored in ordertoimprovethepowerconversion
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 12 | Dec 2019 www.irjet.net p-ISSN: 2395-0072
ยฉ 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1572
efficiency of organic solar cells. The GPVDM software
simulates the organic solar cell at various layer thicknesses.
This model consists of both electrical and optical properties
and is specifically designed to mimicorganicsolarcellsbased
on the P3HT and PCBM mixture of polymer material [7]. The
electrical simulation just reaches the device's active layer.
The current density-voltagecurve(j-v)plottedforVocandJsc
to be provided. The Voc is defined by the energygapbetween
the largest molecular orbital occupied (HOMO) representing
the donor level and the lowest unoccupied molecular orbital
(LUMO) describing the acceptor level [8]. The j-v curve
provides the fill factor specified as the ratio between the
maximum power point (Pmpp) and the device's theoretical
maximum power (Pmax) [8-11].
Here, Vmax and Pmax are the voltage and current density in
the maximum power point respectively. The power
conversion efficiency for a solar cell is defined by the
equation.
Where, Pin is the power density of the light and Pout is the
electric power generated by the bulk hetero junction solar
device at maximum power point. [12]
Architecture of organic solar cell is shown in figure 2.
Fig.2: Organic Solar Cell Model
Fig.2 demonstrates the PEDOT: PSS / P3HT: PCBM-based
organic solar cell design. In this example, the layer
configuration followed is ITO / PEDOT: PSS / P3HT: PCBM /
Al, where ETM (Electron Transfer Layer) is PEDOT: PSS and
HTM (Hole Transfer Layer) is P3HT: PCBM [5]. The Indium
Tin Oxide (ITO) film is used as a transparent electrode
because it has strong visible region transmittance and
conductive capacity [12]. Original parameters chosen from
OSC electrical parametersareshowninTable1.Theelectrical
and optical parameters oforganicsolarcellsarederivedfrom
the ITO layer and Al dependent gpvdm software database,
and the layer thickness values are taken as 1e-07 and 1e-07
respectively [13].
Our analysis is focused on the observation of different layer
thickness effects on the efficiency of power conversion [14].
Table 1 displays the reference value of the simulation
parameters.
S.No. Parameters PEDOT:PSS P3HT:PCBM
1 Layer
Thickness (m)
1e-07
(variable)
2.2e-
07(variable)
2 Relative
permittivity
3.8 3.8
3 Electron tail
slope (ev)
4.00E-002 4.00E-002
4 Hole tail slope
(ev)
6.00E-002 6.00E-002
5 Doner
Concentration
(m-3)
1.28E+027 1.28E+027
6 Acceptor
Concentration
(m-3)
2.86E-025 2.86E+025
Table.1: Simulation Parameters
Fig.3: J-V Characteristics for initial layer values
The j-v curve is shown in Fig 3, in which PCE (Power
conversion efficiency) is 11.66%, fill factor is 66.29%, short
circuit density of current is -224A/mandopencircuitvoltage
Voc is 0.78V [15].
3. RESULTS AND DISCUSSIONS
In our simulation, optimization method is used to fix all
parameters and modify the values one by one until we have
the parameters that give maximum Power Conversion
Efficiency. Figure 4 represents the curveeffectofPEDOT:PSS
layer thickness on PCE in organic solar cell.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 12 | Dec 2019 www.irjet.net p-ISSN: 2395-0072
ยฉ 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1573
Fig 4. Effect of PEDOT: PSS layer thickness on PCE
In Fig 4, it is shown that a PEDOT:PSS layer thickness of
1.25ร—10-8 m givesthemaximalvalueofPCEwhichis12.86%,
with a fill factor of 65.29%, an open circuit voltage of 0.78V
and a short-circuit density of current of -251.27 A/m 2. Now
we fix the value of PEDOT: PSS layer thickness at 1.25ร—10-8
m and change the value of P3HT: PCBM layer thickness to
obtain curve in Figure 5.
Fig 5. Effect of P3HT: PCBM layer thickness on PCE
In Figure 5, it is shown that P3HT:PCBM layer thickness of
2.2ร—10-7 m gives the maximal value of PCE which is 12.86%,
where fill factor is 65.29%, open-circuit voltage is 0.78 V and
short-circuit density of current is -251.27 A/m. Fig 4 and Fig
5 presents different layer thickness effect on PCE for a
PEDOT:PSS and P3HT:PCBM based planar organic solar cell
where we see that the efficiency increased from 11.66 % in
initial default parameters to 12.86 % with optimized
parameters.
Fig 6. J-V characteristics for optimized layer values
In Fig 6, J-V characteristic of the organic solar cell is shown
with optimized parameters.
In addition of this research work, the illumination J-V
characteristics are simulated at different resistances 1ฮฉ, 3ฮฉ,
5ฮฉ, and 7ฮฉ. The J-V characteristic curves are shown in the fig
7. It is clear from the J-V characteristics curves that the short
circuitcurrent decrease withincreaseintheseriesresistance
continuously,at 1ฮฉ the shortcircuitcurrent ismaximumand
minimum at 7ฮฉ. As series resistance increases, the voltage
drop between the junction voltage and the terminal voltage
becomes greater for the same current. The result is that the
current-controlled portion of the I-V curve begins to sag
toward the origin, producing a significant decrease in the
terminal voltage and a slight reduction in ISC, the short
circuit current. Very high values of RS will also produce a
significant reduction in ISC; in these regimes, series
resistance dominates and the behavior of the solar cell
resembles that of a resistor. These effects are shown for
crystalline silicon solar cells in the j-v curves [16].
Fig 7. J-V characteristics at different series resistance 1ฮฉ,
3ฮฉ, 5ฮฉ, 7ฮฉ
4. CONCLUSION
Organic solar cellโ€™spowerconversionefficiencywasanalyzed
using the GPVDM solar cell software simulation. Results
indicate that a good choice of series resistance and layer
thickness of different materials used in the solar cell
considerably increased the PCE ratio. From the simulation
results it is found that an improvement of 2.18% is made by
setting layer thickness of PEDOT: PSS to 1.25ร—10-8 m and
layer thickness of P3HT: PCBM to 2.2ร—10-7 m, and setting
series resistance to 1 ฮฉ .Further PCE enhancements can be
done by changing layer structure and materials.
REFERENCES
[1] M.Erray, M.Hanine, E-M.Boufounas, and A.El Amrani,
Effects of carriers charge mobility and work functionon
the performance of PEDOT: PSS and P3HT: PSS based
organic photovoltaic cell, Journal of IEEE conference,
2018.
[2] G. Li, V.Shrotriya, Y. Yao, eT Y. Yang, Investigation of
annealing effects and film thickness dependence of
polymer solar cells based on poly (3-hexylthiophene), J.
Appl. Phys, 2005.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 12 | Dec 2019 www.irjet.net p-ISSN: 2395-0072
ยฉ 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1574
[3] Electrical Simulation of Organic Solar Cell at Different
Charge Carrier Mobility, IOSR Journal ofAppliedPhysics
(IOSR-JAP), Mar-Apr, 2017.
[4] S.R. Cowan, N.Banerji, W.L.Leong, A.J.Heeger, Charge
formation, recombination, and sweep-out dynamics in
organic solar cells, Adv.Funct, 2012.
[5] C.-T. Lee et C.-H. Lee, ยซ Conversion efficiency
improvement mechanisms of polymer solar cells by
balance electronโ€“hole mobility using blended P3HT:
PCBM active layer.
[6] Roderick C. I. MacKenzie, Thomas Kirchartz,GeorgeF.A.
Dibb, and Jenny Nelson, Modeling No geminate
Recombination in P3HT: PCBM Solar Cells, J. Phys.
Chem.2011.
[7] B.M.Omer, Understanding photo-degradation
mechanism in P3HT: PCBM bulk heterojunction solar
cells AMPS-1D simulation study: Photo-degradation
mechanism in P3HT: PCBM bulk heterojunction solar
cells, Phys. sept. 2016.
[8] A.B.walker, A. Kambili, et S.J.Martin, Electrical transport
modeling in organic electroluminescent devices, 2002.
[9] R. Hanfland, M.A. Fischer, W.Brรผtting, U.Wรผrfel,
R.C.I.MacKenzie, The physical meaning of charge
extraction by linearly increasingvoltagetransientsfrom
organic solar cells, Appl. Phys.,2013.
[10] F. Deschler, D. Riedel, B. Ecker, E. von Hauff, E. Da Como,
R.C.I. MacKenzie, Increasing organic solar cell efficiency
with polymer interlayers, Phys. Chem. Chem. Phys.,
2012.
[11] R.C.I. MacKenzie, C.G. Shuttle, M.L. Chabinyc, J. Nelson,
Extracting microscopic device parameters from
transient photocurrent measurements of P3HT: PCBM
solar cells, Adv. Energy Mater,2012.
[12] Nikhil Rastogi, Narendra Singh, Sandeep Saxena,
Analysis Of Photovoltaic Dsevice at Different Series
Resistances,Universal Journal ofMaterialsScience,2017.
[13] Gpvdm manual Roderick C. I. MacKenzie April 6, 2018.
[14] Ball, J.M., et al., Optical properties and
limitingphotocurrent of thin-film perovskite solar cells,
Energy& Environmental Science,2014.
[15] A.Hima,A.Khechekhouche ,GPVDM simulation of layer
thickness effect on power conversion efficiency of
CH3NH3PbI3 based planar heterojunction solar cell,
IJECA-ISSN, June 2018.
[16] J.Yan, Handbook of Clean Energy Systems,
https://books.google.co.in/books, 1118388585. Vol. 6
(2015).

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IRJET- Effect of Series Resistance and Layer Thickness on PCE and Fill Factor in Organic Solar Cell with P3HT: PCBM Active Layer

  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 12 | Dec 2019 www.irjet.net p-ISSN: 2395-0072 ยฉ 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1571 Effect of Series Resistance and Layer Thickness on PCE and Fill Factor in Organic Solar Cell with P3HT: PCBM Active Layer Pooja Sinha1, Rahul Baghel2 1M.Tech scholar,Dept. of Electrical and Electronics Engineering, SSGI Durg-490001, Chhattisgarh, India 2Assistant Professor, Dept. of Electrical and Electronics Engineering, SSGI Durg-490001, Chhattisgarh, India ---------------------------------------------------------------------***---------------------------------------------------------------------- Abstract - This paper reports a study on the effect of series and layer thickness on the performance of an organic photovoltaic cell which is based on polymer/fullerene P3HT: PCBM. Electrical simulation has been examined on ITO- PEDOT: PSS-P3HT: PCBM-Al structure with GPVDM (General- Purpose Photovoltaic Device Model) software. We used the GPVDM software to investigate the effect of series resistance and layer thickness on power conversion efficiency (PCE) and fill factor (FF) in an organic solar cell which is based on P3HT: PCBM as an absorbing layer. The changes were made by applying the different series resistance and layer thickness value. The results show that the power conversion efficiency can be increased by changing the value of the seriesresistance and layer thickness, in our case the power conversion efficiency has been increased from 11.66% to 13.84% and fill factor has been change from 66.29% to 70%. Key Words: Organic photovoltaic cell, P3HT:PCBM,GPVDM, series resistance, thickness effect. 1. INTRODUCTION Organic photovoltaics (OPVs) have attracted considerable interest over the past two decades due to their advantages over inorganic solar cells. OPVs are lightweight, cheap and non-toxic compared to inorganic solar cells. They are also robust and versatile mechanically. Organic solar cells, as the name implies, transform light from organic molecules into electricity. For these solar cells, synthetic polymers and small organic molecules are widely used. Their long chain relocation via alternating double and single connections helps to effectively transfer the electron in the cell. The highest occupied molecular orbitals(HOMOs)andthelowest unoccupied molecular orbitals (LUMOs) are these orbits. An optical band gap in the half conductor area is the power disparity between the low-energy HOMOs and the high- energy LUMOs. Becauseoftheirversatilematerial properties and low-cost processing, organic solar cellshavebeena very remarkable area of research in recent years. In the early 1950s, organic solar photovoltaic cells were developed. Since 1965, organic chemistry has had a fast growth and the first discovery of photoconductivity in organic compounds was published in 1906. The product, Solarmer, developed for the first time Organic Photovoltaic. BHJ-based organic solar cells (Bulk Hetro-junction) are composites of P3HT (Poly3-hexylthiophene) and PCBM (phynyl-C-70buteric acid methyl ester) [1-2]. Gpvdm (OPVDM's new name) is a free general-purpose device simulation tool. Originallydesigned tosimulateorganicsolar cells, it has now been expanded to simulate other system categories, including OLEDs, OFETsandmanyotherforms of solar cells of 1st, 2nd and 3rd generation. Thephysical model solves drift-diffusion of electron and hole as well as continuity equations of the carrier in position space to describe the load movement within the device. The model also solves the equation of Poisson to calculate the potential of internal electrostatics. Recombination and carrier trapping are described in the model using Shockley-Read- Hall (SRH) formalism; it is feasible to arbitrarily define the distribution of trap states. Both equations can be solved in a steady state or in a time domain. The model facilitates the study of the effect on system performance of product parameters such as mobility, energetic disorder, doping, and recombination cross- sections. All internal device parameters such as current density load frequency, position distribution of trapped carriers and energy storage can be controlledthrough either the graphical interface or directly from output data. The system includes both an electrical and an optical solver, allowing simulation of current / voltage characteristics and the optical model profile within the device. The model is available for Windows and Linux (x86 and ARM) and it is easy to use graphical interface. Gpvdm is a tool used to simulate and design solar cells to harvest the energy of the sun. Fig 1: GPVDM Home Window 2. ELECTRICAL SIMULATION The significant parameters that influence its performance should be explored in ordertoimprovethepowerconversion
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 12 | Dec 2019 www.irjet.net p-ISSN: 2395-0072 ยฉ 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1572 efficiency of organic solar cells. The GPVDM software simulates the organic solar cell at various layer thicknesses. This model consists of both electrical and optical properties and is specifically designed to mimicorganicsolarcellsbased on the P3HT and PCBM mixture of polymer material [7]. The electrical simulation just reaches the device's active layer. The current density-voltagecurve(j-v)plottedforVocandJsc to be provided. The Voc is defined by the energygapbetween the largest molecular orbital occupied (HOMO) representing the donor level and the lowest unoccupied molecular orbital (LUMO) describing the acceptor level [8]. The j-v curve provides the fill factor specified as the ratio between the maximum power point (Pmpp) and the device's theoretical maximum power (Pmax) [8-11]. Here, Vmax and Pmax are the voltage and current density in the maximum power point respectively. The power conversion efficiency for a solar cell is defined by the equation. Where, Pin is the power density of the light and Pout is the electric power generated by the bulk hetero junction solar device at maximum power point. [12] Architecture of organic solar cell is shown in figure 2. Fig.2: Organic Solar Cell Model Fig.2 demonstrates the PEDOT: PSS / P3HT: PCBM-based organic solar cell design. In this example, the layer configuration followed is ITO / PEDOT: PSS / P3HT: PCBM / Al, where ETM (Electron Transfer Layer) is PEDOT: PSS and HTM (Hole Transfer Layer) is P3HT: PCBM [5]. The Indium Tin Oxide (ITO) film is used as a transparent electrode because it has strong visible region transmittance and conductive capacity [12]. Original parameters chosen from OSC electrical parametersareshowninTable1.Theelectrical and optical parameters oforganicsolarcellsarederivedfrom the ITO layer and Al dependent gpvdm software database, and the layer thickness values are taken as 1e-07 and 1e-07 respectively [13]. Our analysis is focused on the observation of different layer thickness effects on the efficiency of power conversion [14]. Table 1 displays the reference value of the simulation parameters. S.No. Parameters PEDOT:PSS P3HT:PCBM 1 Layer Thickness (m) 1e-07 (variable) 2.2e- 07(variable) 2 Relative permittivity 3.8 3.8 3 Electron tail slope (ev) 4.00E-002 4.00E-002 4 Hole tail slope (ev) 6.00E-002 6.00E-002 5 Doner Concentration (m-3) 1.28E+027 1.28E+027 6 Acceptor Concentration (m-3) 2.86E-025 2.86E+025 Table.1: Simulation Parameters Fig.3: J-V Characteristics for initial layer values The j-v curve is shown in Fig 3, in which PCE (Power conversion efficiency) is 11.66%, fill factor is 66.29%, short circuit density of current is -224A/mandopencircuitvoltage Voc is 0.78V [15]. 3. RESULTS AND DISCUSSIONS In our simulation, optimization method is used to fix all parameters and modify the values one by one until we have the parameters that give maximum Power Conversion Efficiency. Figure 4 represents the curveeffectofPEDOT:PSS layer thickness on PCE in organic solar cell.
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 12 | Dec 2019 www.irjet.net p-ISSN: 2395-0072 ยฉ 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1573 Fig 4. Effect of PEDOT: PSS layer thickness on PCE In Fig 4, it is shown that a PEDOT:PSS layer thickness of 1.25ร—10-8 m givesthemaximalvalueofPCEwhichis12.86%, with a fill factor of 65.29%, an open circuit voltage of 0.78V and a short-circuit density of current of -251.27 A/m 2. Now we fix the value of PEDOT: PSS layer thickness at 1.25ร—10-8 m and change the value of P3HT: PCBM layer thickness to obtain curve in Figure 5. Fig 5. Effect of P3HT: PCBM layer thickness on PCE In Figure 5, it is shown that P3HT:PCBM layer thickness of 2.2ร—10-7 m gives the maximal value of PCE which is 12.86%, where fill factor is 65.29%, open-circuit voltage is 0.78 V and short-circuit density of current is -251.27 A/m. Fig 4 and Fig 5 presents different layer thickness effect on PCE for a PEDOT:PSS and P3HT:PCBM based planar organic solar cell where we see that the efficiency increased from 11.66 % in initial default parameters to 12.86 % with optimized parameters. Fig 6. J-V characteristics for optimized layer values In Fig 6, J-V characteristic of the organic solar cell is shown with optimized parameters. In addition of this research work, the illumination J-V characteristics are simulated at different resistances 1ฮฉ, 3ฮฉ, 5ฮฉ, and 7ฮฉ. The J-V characteristic curves are shown in the fig 7. It is clear from the J-V characteristics curves that the short circuitcurrent decrease withincreaseintheseriesresistance continuously,at 1ฮฉ the shortcircuitcurrent ismaximumand minimum at 7ฮฉ. As series resistance increases, the voltage drop between the junction voltage and the terminal voltage becomes greater for the same current. The result is that the current-controlled portion of the I-V curve begins to sag toward the origin, producing a significant decrease in the terminal voltage and a slight reduction in ISC, the short circuit current. Very high values of RS will also produce a significant reduction in ISC; in these regimes, series resistance dominates and the behavior of the solar cell resembles that of a resistor. These effects are shown for crystalline silicon solar cells in the j-v curves [16]. Fig 7. J-V characteristics at different series resistance 1ฮฉ, 3ฮฉ, 5ฮฉ, 7ฮฉ 4. CONCLUSION Organic solar cellโ€™spowerconversionefficiencywasanalyzed using the GPVDM solar cell software simulation. Results indicate that a good choice of series resistance and layer thickness of different materials used in the solar cell considerably increased the PCE ratio. From the simulation results it is found that an improvement of 2.18% is made by setting layer thickness of PEDOT: PSS to 1.25ร—10-8 m and layer thickness of P3HT: PCBM to 2.2ร—10-7 m, and setting series resistance to 1 ฮฉ .Further PCE enhancements can be done by changing layer structure and materials. REFERENCES [1] M.Erray, M.Hanine, E-M.Boufounas, and A.El Amrani, Effects of carriers charge mobility and work functionon the performance of PEDOT: PSS and P3HT: PSS based organic photovoltaic cell, Journal of IEEE conference, 2018. [2] G. Li, V.Shrotriya, Y. Yao, eT Y. Yang, Investigation of annealing effects and film thickness dependence of polymer solar cells based on poly (3-hexylthiophene), J. Appl. Phys, 2005.
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 12 | Dec 2019 www.irjet.net p-ISSN: 2395-0072 ยฉ 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 1574 [3] Electrical Simulation of Organic Solar Cell at Different Charge Carrier Mobility, IOSR Journal ofAppliedPhysics (IOSR-JAP), Mar-Apr, 2017. [4] S.R. Cowan, N.Banerji, W.L.Leong, A.J.Heeger, Charge formation, recombination, and sweep-out dynamics in organic solar cells, Adv.Funct, 2012. [5] C.-T. Lee et C.-H. Lee, ยซ Conversion efficiency improvement mechanisms of polymer solar cells by balance electronโ€“hole mobility using blended P3HT: PCBM active layer. [6] Roderick C. I. MacKenzie, Thomas Kirchartz,GeorgeF.A. Dibb, and Jenny Nelson, Modeling No geminate Recombination in P3HT: PCBM Solar Cells, J. Phys. Chem.2011. [7] B.M.Omer, Understanding photo-degradation mechanism in P3HT: PCBM bulk heterojunction solar cells AMPS-1D simulation study: Photo-degradation mechanism in P3HT: PCBM bulk heterojunction solar cells, Phys. sept. 2016. [8] A.B.walker, A. Kambili, et S.J.Martin, Electrical transport modeling in organic electroluminescent devices, 2002. [9] R. Hanfland, M.A. Fischer, W.Brรผtting, U.Wรผrfel, R.C.I.MacKenzie, The physical meaning of charge extraction by linearly increasingvoltagetransientsfrom organic solar cells, Appl. Phys.,2013. [10] F. Deschler, D. Riedel, B. Ecker, E. von Hauff, E. Da Como, R.C.I. MacKenzie, Increasing organic solar cell efficiency with polymer interlayers, Phys. Chem. Chem. Phys., 2012. [11] R.C.I. MacKenzie, C.G. Shuttle, M.L. Chabinyc, J. Nelson, Extracting microscopic device parameters from transient photocurrent measurements of P3HT: PCBM solar cells, Adv. Energy Mater,2012. [12] Nikhil Rastogi, Narendra Singh, Sandeep Saxena, Analysis Of Photovoltaic Dsevice at Different Series Resistances,Universal Journal ofMaterialsScience,2017. [13] Gpvdm manual Roderick C. I. MacKenzie April 6, 2018. [14] Ball, J.M., et al., Optical properties and limitingphotocurrent of thin-film perovskite solar cells, Energy& Environmental Science,2014. [15] A.Hima,A.Khechekhouche ,GPVDM simulation of layer thickness effect on power conversion efficiency of CH3NH3PbI3 based planar heterojunction solar cell, IJECA-ISSN, June 2018. [16] J.Yan, Handbook of Clean Energy Systems, https://books.google.co.in/books, 1118388585. Vol. 6 (2015).