Loading...

Messages

Proposals

Stuck in your homework and missing deadline?

Get Urgent Help In Your Essays, Assignments, Homeworks, Dissertation, Thesis Or Coursework Writing

100% Plagiarism Free Writing - Free Turnitin Report - Professional And Experienced Writers - 24/7 Online Support

Complete Thesis on High Efficiency Organic Solar Cell

Category: Chemistry Paper Type: Dissertation & Thesis Writing Reference: APA Words: 7700

The demand of the energy is likely to increase in the previous few decades for example the need of the sources of energy like the coal, uranium and gas there has augmented investigate of the sources of energy that can be renewable. The overall Oil prices disaster probable to add to to meet augmented command for energy. These days, the main present which is measured as basis of power is said to be the fossil fuel, that is also major issue of the global warming on the earth and it is also important to augmented warmth and hoist in the level of sea [1]. This is also likely to guide us to make an effectual answer to features this difficulty and it is also pending up with cheap energy source, and the energy renewable sources. For cause there is also said to be a investigate on intend of additional money-making basis of energy has complete.

Because it is recognized, sun and the wind are careful the major foundation for the energy that is renewable which is also said to be the low cost. There is also said to be very different educational and manufacturing seats research exposed that the quantity of the rays of the sun that is also likely to hit the earth is equal to the quantity that the whole planet use in a year [2]. On the other hand, the there is a big gap flanked by the expenses of power shaped from remnant fuel in contrast with the renewable energy is disadvantage for this type of expertise. As a result, this quandary turns out to be the fascination of the researchers through the wide-reaching. In this case there is also one of the customs that can change the sun’s energy into electrical energy is from side to side the devices of the photovoltaic.

1.1 Introductions of High Efficiency Organic Solar Cell

It is stated in the abstract that the Charles Fritts in 1883 is likely to residential the first instrument of the photovoltaic. It was a continuance of labour of the development of the Edmund in the case of the effect of the photovoltaic. In spite of the increase in competence of all of the devices, they motionless need a lot of capital for their growth, and therefore, are more expensive. consequently, there has in the previous few years important investigate conduct in expression of getting better the competence for cells and to decrease manufacture cost that can be offer material of the inorganic semiconductors [5]. It was with competence speed at concerning 1percent. He used covered semiconductor selenium by a skinny movie of gold appearance a association.

The primary photovoltaic cell was in the year 1954, which was also said to be cell residential of the silicon solar with Chapin with a authority competence of 6 percent that improved later to an competence of 44.7 percent in the year 2013 [4]. After that, the photovoltaic cell was established by the hypothesis of contacts metal-semiconductor [3].This is also said to be the type of the material used in it has show to be extremely winning as in the untreated light produce the diodes. From side to side there is also different research, and the organic materials show talented description for request in photovoltaic cells. For instance polymers conjugated and dendrites [9]. As of the low down developed price and high competence for material of the organic semiconductors, there is motionless a room for development of by this knowledge to arise with main sources of power generation scheme [6].

1.2 Solar Cell Development History of High Efficiency Organic Solar Cell

From about 170 years till the year 1839 the time when it is observes by the Alexandre Edmond Becquerel by means of the electrode in conductive answer uncovered the light at the very primary effect of the photovoltaic [11]. These are said to be the years that can be alienated into six periods of time preliminary with the detection of the years from the year 1839 to the 1904. Table1 is likely to provide the mainly noteworthy events throughout this primary period. In additions the Adams and Day examine in the year 1877, the photovoltaic effect in solidified selenium and also in the year 1904, a solar cell of the semiconductor-junction with the help of the copper & copper oxide complete by the Hallwachs. On the other hand, this era was with no any real sympathetic of the notion at the back the procedure of the entire plan.

In instant stage of the past of the photovoltaic in the era from the case of the year from the 1905 to 1950, there is also said to be the possible growth and the theoretical base for photovoltaic the mechanism procedure and were devise for the reason that in the Table2. In this era, the theory of the Einstein’s photon was also solitary of key proceedings [13], the description of Czochralski crystal enlargement means for the silicon and germanium single crystal enlargement [14] and in the epoch there was growth of the band hypothesis for the high wholesomeness semiconductors of the solitary crystal [15]. Eventually, the main manager for the 6th era that is too probable to complete form about 2000 awaiting the year 2013 was also supposed to be the global payment in operation of the photovoltaic cell with the United States in concert first and foremost position. The major control country in that occasion was the China, Japan, and Germany. The mainly extraordinary proceedings in this era are obtainable in the table 6.

1.3 The photovoltaic effect of High Efficiency Organic Solar Cell

                                                               

Figure 1: Semiconductor photoelectric effect

The photovoltaic effect is said to b the a procedure in which the whole electrons or previous free transporter can be shaped in reply to occurrence light onto a get in touch with junction (metal-semiconductor).at what time a fabric soak up light, and if the occurrence photons are of superior work purpose as compare with the metal, this guide electrons to be physically cast out. these are the Two types of silicon are created from side to side squeezing of other rudiments into the silicon structure: n-type, that is likely to has spare electrons, and in the case of the p-type, which is missing also a electrons in the case.

Organic semiconductors of High Efficiency Organic Solar Cell

Some of the Organic materials are talented equipment for manufacture of low cost solar cell of the devices.  In this case the Organic materials for electronic request are paying attention in 6th in the light emit diode, transistors and solar cells) and this underway when the behaviour polymers naked in 1980s [21]. Because of their chemical arrangement, the materials of the organic semiconductor measured to be high-quality conductive materials as compare with the other semiconductor materials.

                                                                               

Figure 2: Orbital shapes for s orbital, p orbitals and their combination.

                                                                              

Figure 3: Hybridization between (2s and 2p(x,y)) orbitals.

there are about Two sorts of bonds are framed due to the hybridisation the primary is σ bonds that is also said to be the single bonds between carbon-carbon and carbon-hydrogen particles and the second one is π bonds have delocalised electrons. From Fig 3, three carbon electrons frame σ bonds where these electrons are restricted. This setup leaves the forward (not hybridized) electron to give the π bond as appeared in Fig. 4. Electrons in these bonds are in charge of the electrical conductivity of natural semiconductors [22] while atomic orbitals which shape σ and π bonds speak to the vitality levels for natural semiconductor materials.

Figure 4: Schematic diagram of bond and orbitals for two ap2 hybridised carbon atoms

The LUMO (Lowest Unoccupied Molecular Orbital) along with HOMO (High Occupied Molecular Orbital) is the after-effect of joining the (conduction band) hostile to holding π* sub-atomic orbital’s with the (valance band) π holding sub-atomic orbital’s. The hole amid them is the vitality hole which speaks to the conductivity that natural cell relies upon. It is obvious from Fig.4 that σ bonds are greatly filled through electrons where π bonds are unfilled. Then again, when the band hole's vitality progresses toward becoming as little as conceivable the resistance of electrons to move to Lowest Unoccupied Molecular Orbital increments. The properties of natural semiconductor polymers (electrical conductivity, optoelectronic, shading (assimilation as well as emanation) along with photograph prompted charge exchange) lead them to be a basic player in numerous applications within both electronic as well as optical field, for example, natural field-impact transistors, natural photovoltaic cells, as well as sensors [23]. The fundamental favourable position in this sort of materials is the capacity to tune the band hole by changing the blend materials as well as it can be utilized to cover huge surfaces. Conjugated polymer materials consolidate amid mechanical properties of polymers as well as electronic properties of metals as well as semiconductors. Be that as it may, the little sub-atomic materials (oligomers, dendrimers, colors, colors, fluid gem, along with organo-mineral crossover materials) additionally in light of π conjugated electron [24, 25].

Electron transport materials of High Efficiency Organic Solar Cell

An perfect acceptor are likely to have quite a few possessions that is also said to be the good harvesting light, constancy under dispensation and functioning conditions, far above the ground electron mobility, and low down cost of mixture) that are also mutual to make an well-organized constituent. so it is also a Indene-C70 has also been synthesize at a senior LUMO level of the 3.72 eV (0.19 eV superior than that of PCBM). IC70BA likely to possesses high-quality solubility in ordinary organic solvents and more able to be seen amalgamation [27].

Hole transport materials of High Efficiency Organic Solar Cell

The most encouraging materials of the p-type (opening transport) for request in the gadgets of the OPV can be conjugated sponsor polymers and this is on explanation of they can perhaps join their immense movies framing properties (reasonable levels of the HOMO and LUMO, escalated light assimilation and elevated gap motilities) to complete improved electronic quality make them significantly more successful [28].

Transparent conducting electrode of High Efficiency Organic Solar Cell

The movies of the Transparent conducting which have thin leading movies can accomplish an extensive estimation of conductivity and keep up a transmission [29]. The Indium tin oxide (ITO) is watchful as the primary current oxide materials of the straightforward directing [30]. It is a semi-director - type straightforward which has a wide group electrons of roughly 4 eV [31].

1.4.4 Top electrode of High Efficiency Organic Solar Cell

The Cathode materials are hypothetical to be a metal of low function of the work to take out electrons through a physically powerful electric meadow. The mainly ordinary metals have near to the ground work purpose used as cathode in the case of the devices of the OPV is magnesium calcium, and aluminium. [32].

1.4.5 Buffer layers of High Efficiency Organic Solar Cell

The major difficulty faces in the case of the organic solar cells is two electrodes touch both the contributor polymer and molecule of the acceptor and guide to the arrangement of acceptor electrons at a boundary that is also likely to situate very shut to the anode. Consequently, and owing the decrease of the operational electrical energy device, if some of the electrons transfer to the anode, they will recombine with no trouble [33].

1.5 Basic operation principles of Organic solar cells of High Efficiency Organic Solar Cell

In the case of the semiconductors that are said to be inorganic, the photons are rehabilitated in a straight line into carrier of straight charge and the transporter composed at the suitable electrodes. As in the devices of the organic photovoltaic, a couple of hole and electron that is also likely to form side to side the excitation of particle through photon [35]. The length of the diffusion of the entire electron is concerning 5-15 nm and then decomposes.

Figure 6: diagram illustrate the power generation in an organic solar cell.

1.5.1 Light absorption of High Efficiency Organic Solar Cell

The amalgamation usually happen when a photon that encompass energy equivalent to or better than band gap in the case of the material absorbed semiconductor, which has aptitude to free an electron from the leaving behind the HOMO to the LUMO a space in previous height. It can form attraction of the coulombic together with the electron which [36]. Figure 7 shows electron binding energy.

Figure 7: Excition binding energy

1.5.2 Exciton migration and dissociation of High Efficiency Organic Solar Cell

The possibility of the dissociating of an exciton is in general made obtainable by the formation of a heterojunction flanked by two semiconductors that are said to be organic whereby the moment semiconductor that can be particular which the electron result from the exciton can be able to drop in it. This let go the dissimilarity of the energy flanked by the LUMO and the HOMO therefore, violation of the bound states.

1.5.3 Charges transport and collection of High Efficiency Organic Solar Cell

After the age of free charges have been at the interface, it is required that they land at the outside circuit in gadget of the OPV, while the electrons can be overjoyed however the material that goes about as the electron acceptor and the gaps can be transported through the material that goes about as the electron contributor. Utilizing ultra-thin inward layers, for example, metal oxides like ZnOx and LiF to give an ideal match to the vitality stature of natural semiconductors [38].

1.6 Electrical Characterization of organic solar cells

1.6.1 Equivalent circuit diagram of solar cells organic

It demonstrated through a diode parallel with present foundation in a perfect case however for all intents and purposes an arrangement and a shunt obstruction should be incorporated into the model in a way that; the arrangement resistor Rs thinks about free relocation or development of bearers of the charge in the vehicle medium and the shunt resistor Rsh is benefited to recombination of charge transporters around the separation territory as appeared in Figure 8[39].

Figure 8: Equivalent circuit diagram of organic solar cells.

1.6.2 Current-voltage characterisation of High Efficiency Organic Solar Cell

The attributes of the voltage (J-V) current-density is after the exponential reaction of a diode with low current in turn around predisposition and high current in forward inclination when done in a dull place. At the point when light is coordinated on a gadget other than the diode trademark and the superposition of the dim trademark and the photocurrent are fundamentally the J-V trademark under lighting a photocurrent in the cell develops. The J-V attributes of the gadget and the photocurrent term, Jph is depicted by equation of Shockley:

J= J0 [exp (eV/ nkT) -1]-Jph

Where J is said to be the current density, and on the other side the  J0 is the overturn diffusion present compactness of diode, e the basic accuse, V is also said to be voltage that is applied, n is the idealist issue, k is the constant Boltzmann and T in this case is temperature.

 

(9)                                                                                          (9A)

Figure 9: shows the plot of J-V for typical solar cell under illumination.

Figure 9A: series Effect confrontation RS on the figure of an curve I-V

Figure 9 B: shunt resistance Effect RSH on the figure of I-V curve

1.6.2.1 Voltage of Open-circuit of High Efficiency Organic Solar Cell

the VOC is said to be the voltage of open circuit crosswise over cell by then like a similar gadget open-circuited exactly when J= 0. For this situation, no power is produced at the voltage cause control = current*voltage and J = 0. In any case, the voltage limits inside which power can be created are characterized by the VOC. The point at the procedures of generation of photocurrent and dull current remunerate each other is the open-circuit voltage [41]

1.6.2.2  Current of Short-circuit of High Efficiency Organic Solar Cell

Whenever V=0, the density of the current is short out present JSC density, similar to VOC, which in comparative conditions as the cathodes of the two cell's being short-circuited. For this situation in addition, no power is produced yet the beginning of intensity age is set apart by the JSC. The photocurrent thickness will be equivalent to the JSC in viable gadgets. JSC is in fact negative with the traditions signs utilized here.

1.6.2.3  Fill-factor of High Efficiency Organic Solar Cell

At the Vmax voltage and Jmax current density, the eventual authority density produce (Pmax) come about where the ensuing creation of the J and V is highest or smallest amount in complete worth.

𝐽𝑚𝑎𝑥𝑋𝑉𝑚𝑎𝑥

𝐽𝑆𝐶𝑋𝑉𝑂𝐶

FF=

 


             

Far above the ground FF is desired as it is connected to higher utmost power; yet, the characteristic diode-like of solar cells consequence in FF forever being below one.

1.6.2.4 Efficiency Power conversion of High Efficiency Organic Solar Cell

The mainly talk about parameter of the performance of solar cell is quantity of conversion competence of the power distinct because η which is distorted into production authority (Plight). It is designed as relation flanked by the produce utmost power that is produce through a solar cell and the authority of occurrence light, the method of PCE is written as subsequent:

 

1.7.1 Materials of High Efficiency Organic Solar Cell

From the "Sigma-Aldrich the “Poly (3-hexylthiophene-2,5-diyl) (P3HT)” was purchased. However, the Titanium oxide (TiOx) and Poly (amidoamine) (PAMAM) dendritic wedges were combined in the School of Chemistry, Bangor University. Poly (3,4-ethylenedioxythiophene)- poly(styrenesulfonate) (PEDOT: PSS) arrangements (CLEVIOS AL 4083) and pH500 were obtained from Heraeus. IC70BA was acquired from Solaris Chem Inc.

1.7.1.1 (P3HT) Poly (3-hexylthiophene-2,5-diyl) of High Efficiency Organic Solar Cell

TheRegio-standard is known as the infers that every 3-hexylthiophene unit in the chain in this polymer is situated such that the C6H13 deposit gathered; in order to make a beeline for tail or straight on. Regio-consistent poly (3-hexylthiophene) (P3HT) is utilized as an electron giver/gap transporter and light safeguard.

Because of these properties the polymer has the characteristics of better requesting and self-association amid statement, there are also the implementation of the gadget portability toexpand generously.

Thus, the synthetic structure of the material is appeared in the Fig. 3.1 

Figure 3.1: The chemical structure of Poly (3-hexylthiophene-2,5-diyl)

The optical and electrical properties that are considered in the P3HT have been utilized to assess that the level of the HOMO level; which is at 5.1 eV as well as at LUMO level 3.2 bandgap 1.9 eV and the eV.

P3HT can be utilized as an opening transporting polymer to mix theOPV cells and enhancing PCE.

There is focus on the mixture of the OPV cell that focused or created by Gang Li et al. (2005) that utilizing fullerene subordinate; “phenyl-C61-butyric corrosive methyl ester (PCBM)” as well as theP3HT solvent C60 subsidiary. An all-around blended mix film was then shaped by PCBM and P3HT amid dissolvable tempering, as P3HT framed a crystalline fibril-like morphology installed with PCBM totals. Afterward or considering the PCBM mix arrangements were threw on PEDOT: PSS/ITO, vanishing rates were shifted to control the morphology of the mix film.

The ingestion proficiency of the conjugated polymer is additionally enhanced as the p3HT totals and structures fibril-like crystalline morphology. The mobility of the hole focus on the mix PCBM-P3HT conjugated polymer is accounted for to build due to the mixed layers' stage isolated morphology.

Consequently, it is analyzed that P3HT that there is the thin film that focus on the serving of the electron donoramid photoexcitation and has a high opening portability. Thus, around 2 × 10-1 cm2 V-1 s-1 in very much solidified movies and10-3 cm2 V-1 s-1 in thin ineffectively composed movies. There is an expansive ingestion range of 400 to 650 P3HT and it has a 550 nm wavelength optical retention crest and nm, in the rich locale vitality with respect to the solar based range at 1.5 AM.

1.7.1.2  Indene-C70 bisadduct (IC70BA)

With the comprising of 60 carbon particles (C60); the buckminsterfullerenes are steady, sweet-smelling, cluster or round formed groups found in 1985.

However,buckminsterfullerenes hasthe electroactive properties, they have increased huge consideration. Up to the six electrons when in arrangement; the C60 is promptly accessible and goes about as electron acceptor that has high electron versatility and acknowledges.

The solar powered cells that have high efficiencies of up to 3.6% with a copper phtalocyanine benefactor and it is broadly connected in bilayer heterojunction (BHJ). They arebasically accomplished through vacuum affidavit. They are restricted solvency and along these lines with the testimony.

In the year 1995, Hummelen and colleagues had announced that the methano-fullerene subordinate and the C60 adaptation and Phenyl-C61-butyric corrosive methyl ester (PC61BM)are the soluble version.

With the separation in BHJ solar oriented cells; the effective charge; there is the coming about due to ultrafast photoinduced electron exchange to PCBM; there are also the support of p-type polymer that were likewise given that year.

With these two disclosures there are pushed of the natural solar powered cell advancement further. Generally utilized acceptor in OPV; the PCBM is the most consistent. Semiconductorsin the circular shape offers it advantage over other planar 3D electron transport is conceivable in it. Focusing on the end goal to address this, a C70 simple of it, in OPV gadgets as it had a more grounded assimilation; called the PC71BM was created to have a higher photocurrent in the solar powered range's blue area. Consequently, the principle downside is the feeble retention of visible light.

With the solar oriented cells the conjunction with appropriate low-band hole polymersare concerned as exceedingly upgrade for those of the fusing the C60 and C70 analogs achieve over 8% PCE. 

Materials with bring down LUMO have been executed for realizing further enhancements. To empower the tuning of their LUMO and HOMO levels; solubilizing bunches are additionally being connected to the fullerene center to reach the end goal to and furthermore to permit the natural electronic gadgets (OED's) arrangement handling. Furthermore to accomplish higher open circuit voltage (VOC); the different mono, bis and tris adducts have additionally been produced to exploit the progressions in LUMO levels and. For example,in order toprevalent photovoltaic execution at 0.84 V VOC and 6.48% PCE there is the focus to utilized P3HT-based OSCs as acceptorIndene-C60 bisadduct (IC60BA) that has a LUMO level at 3.74 eV (0.17 eV up-moved than that of PCBM) demonstrates.

In the Figure 3.4 there is the demonstration of the substance structure for various C60-based fullerene subsidiaries.After utilizing pre-warm strengthening for 10 minutes at 1500C; the P3HT/IC70BA PSCs with methyl-thiophene added substances have been appeared to have higher PCEs of up to 6.69% with a 0.86 V VOC. With the higher LUMO level of 3.72 eV (0.19 eV higher than that of PCBM); the indene-C70 bisadduct (IC70BA) has additionally been orchestrated.

1.7.1.3  Poly (styrenesulfonate) and poly (3,4-ethylenedioxythiophene) (PEDOT: PSS)

Poly (styrenesulfonate) and poly (3, 4-ethylenedioxythiophene) (PEDOT: PSS) due to its hole conducting properties is utilized; it is known as a part of organic electronics. Cushions or cathode material between dielectric material and the door terminal; it was before utilized as dynamic in the gate electrode.

It has been utilized as a part of OSCs as an anode cushion layer on account of these properties.It has various points of interest, for example, the high straightforwardness, thermal stability, high transparency and mechanical adaptability.

While its electron fondness is 2.2 eV ; it is extraordinary compared to other opening directing supports and there are enough low to block electrons; as it has a high ionization potential that is relatively equivalent to ITO work.

With the blend PEDOT: PSS is utilized for enhancing the ITO-anode contact. It is a solitary part polymer with two ionomers. Conveying positive charge while the other part (PSS) the primary segment (PEDOT) is a polythiophene polymer and sodium polystyrene sulfonate polymer conveying negative charge.

Figure 3.5 focus to demonstrates the chemical structure of PEDOT-PSS

1.7.1.4 Copper(II) chloride (CuCl2 ) of High Efficiency Organic Solar Cell

Copper chloride is a substance compound has thegreat hydration characteristicand made up of the crystals of brown powder. However, it can be decomposes to CuCl and Cl2 at 1000 °C:

1.7.1.4.1 Characteristics of High Efficiency Organic Solar Cell

Consequently, the copper chloride is exceptionally very much broke down in water, and in addition in methanol and ethanol, the copper chloride compound loses the twofold hydrate by warming it over 70 ° C crystalline water. Aqueous arrangements of biodegradable copper chloride, pH of 0.2 mW arrangement of 3.6yet its debasement in CH3)2CO and diethyl ether is powerless. These arrangements have darker shading when focused and end up green until the point that they are done in blue.

1.7.1.5 Uses

1.7.1.5.1 Organic engineered applications of High Efficiency Organic Solar Cell

Copper (II) chloride has response is performed in a polar dissolvableand there are the applications in the amalgamation of natural compounds. However, there are chlorinate the alpha position of carbonyl compounds:for example, (DMF), that frequently manages the sight of lithium chloride, which quickens the response.

Copper (II) chloride get dried when has the advances the hydrolysis of acetonesCuCl2, within the sight of oxygen, can likewise oxidize phenols.

 

1.7.1.6 Lithium chloride of High Efficiency Organic Solar Cell

Lithium chloride is known as the salt is a run of the mill concoction and has the compound with the recipe LiCl; it is a ionic compound.

 

Lithium chloride was utilized quickly in the 1940s as well as the Lithium salts for the most part affect the focal sensory system. There are the contrasting option to nourishment salt, as there are destructive impacts of the compound on the body then it was prohibited.

1.7.1.6.1 Characteristics of High Efficiency Organic Solar Cell

As it disintegrates well in ethanol and pyridine; the lithium chloride complex is all around broke down in water, the compound is as various hydrates. For example, high dissolvability in polar solvents and its high nitrate, which isn't so in other soluble base metal chlorides, thus, the little size of the lithium particle + Li brings about properties.

1.7.1.6.2 Chemical properties of High Efficiency Organic Solar Cell

From the response of lithium hydroxideor lithium chloride is brought from carbonate with hydrochloric corrosive:

LiOH+HCI →LiCI+ H + 2O

Li2 CO3+2HCI →2LiCI+ H2 O+CO2↑

The arrangements of lithium chloride can fill in as a wellspring of chloride particle; moreover, LiCl likewise assimilates up to four counterparts of smelling salts/mol. There are some other ionic chloride; hasten upon treatment with silver nitrate, example can be given of the shaping:

LiCl + AgNO3 → AgCl + LiNO3

1.8 Experimental methods

The experimental methods included the spin covering as well as the thermal dissipation; the initial step of the procedure of this strategy focuses on the vacuum throw amid the procedure as we explain both the methods in below:

1.8.1 Spin coating:

The fundamental reason for the usage of turn covering strategy is for testimony of thin films [45], the initial step of the procedure of this system starts when a little measure of arrangement (covering materials) is connected into the focal point of the level substrate, which is held by a vacuum hurl amid the procedure. From that point forward, the substrate begins pivoting at a settled.

1.8.2 Thermal evaporation:

Metal vapor as well as the deposition of a buffer layer by thermal evaporating is carried out using a Kurt. J. Lesker mini-spectros framework as describe in Fig.10.

1.9 Experimental points of interest

1.9.1 Substrate arrangement

First there was cutting ITO glass substrates into little pieces with measurements of 2.5 cm x 2 cm, then it was cleaned with cleanser, warm water and deionised water, for the dissolvable and any outstanding photoresists there was thesubstrates to be in ultrasonic shower for 10 minutes.

Figure 10: mini-spectros  system  diagram Kurt  Lesker 

1.9.2    Deposition film

1.9.2.1 Spin coating of the hole transport layer of High Efficiency Organic Solar Cell

4000 the EMS spin coater model was used, in this process as well as for conducting poly the  spin-cast    (3,  4-ethylenedioxylenethiophene)  (PEDOT:PSS)  was  (4000  rpm)  after  passing from  aqueous  solution with  approximate  thickness  of  ~40 nm for 40 second a 0.45 μm filter. In air at 140 the substrate was derived for 10 minutes as well as for active layer in the glove box this similar process is carried out (P3HT:IC70BA)(1/0.8  w/w). Approximately the thickness is 100nm.

1.9.2.2 Top Electrodes Evaporation:

Lithium fluoride (LiF) as well as Aluminum (Al) electrodes On the top of the electron transport layer as well as were deposited through shadow mask. Respectively, the thickness was between 0.7 to 100nm


Figure 11:
preparation process of device:  a)  with  PEDOT:  PSS  deposited  ITO  glass  b)  on  top  of  the  PEDOT:  PSS  active  layer  deposited  c)  Lithium fluoride (LiF)  along with  d)  through  shadow mask on top of the LiF Aluminum (Al) deposited. 

1.9.3 Thin film characterization of High Efficiency Organic Solar Cell

Atomic Force Microscopy (AFM) of High Efficiency Organic Solar Cell

AFM or else (Atomic force microscopy) microscopic probe technique is scanning which helps scientist to study exterior morphology of thin films because of its high-resolution.

1.9.4 Electrical characterisation 

1.9.4.1 Setup of Vacuum system of High Efficiency Organic Solar Cell

With a low vacuum system used this designed a vaccum system that contained to a rotary pump steel Chamber connected.  on  the device the intensity (measured  using  a  light  intensity  meter)  of  the  incident  light  as well as depending on the separation among the light source alongside the test could be differed from ~1 to 200 mW/cm. A light power proportional to AM1.5 radiation from the incandescent light was set utilizing an AM1.5 adjusted Si photodiode (Thorlabs SM1PD2A). Figure 12 demonstrates the schematic plan of the estimation setup as well as a photo of the framework.

Figure 12: Diagram of a framwork

1.9.4.2 DC measurements of High Efficiency Organic Solar Cell

The estimations of the present thickness voltage were taken under both dull as well as light through applying voltage to the Aluminum (Al) terminal even as the ITO electrode associated with PC driven LCR meter HP 4284A controlled during a uniquely designed examination by MATLAB program that can quantify J-V bends as well as different parameters, for example, FF, VOC, JSC along with PCE.

1.9.4.3 Ultra-violet/visible Spectroscopy of High Efficiency Organic Solar Cell:

UV-visible absorption spectra the device is used to obtain several material Hitachi Model U-2000 Double Beam Ultra-Violet/Visible (UV/VIS) spectrophotometer.

1.9.5 Cells structure of Organic solar 

1.9.5.2 Organic solar cells Bulk Heterojunction (BHJ):

The fundamental thought remains behind a heterojunction is utilizing two unique materials have diverse electron affinities as well as distinctive ionization possibilities. At the interface along with due to the solid came about possibilities, exciton separation might be adjusted: material with the bigger electron partiality will acknowledge electron as well as the material with bring down ionization potential will acknowledge gap, as it is known, the distinctions within potential vitality are bigger than the exciton restricting vitality [46].In a private way, the tolerant materials as well as the giving are blended to shape an interpenetrating system that is three dimensional. Typically the BHJ gadgets contain a few segments; one of them in any event is a polymer semiconductor (for the most part is a conjugated polymer). In view of the bicontinous arrange is composed taking placing a nanometer, this prompts an extensive territory of interface which implies each excitation made has capacity to achieve the interface. With higher JSC the likelihood of recombination is diminished. In the polymer an excitation stage is fit to exchange an electron from the polymer to the acceptor as well as this brings about the arrangement of an interfacial charge exchange state which at that point unwinds thermally with an electron gap division separate (thermalization length). The likelihood of the coveted separation for the most part relies upon the proportion of the partition remove (an) along with the coulomb catch sweep (rc) [47]. The size along with massiveness of the solubilizing parts of the polymer spine influence specifically on the obstruction that exists among the charges division which can raise the vitality level of charge exchange. A high interface region must be available as well as adequate permeation pathways must be made to keep away from any type of bimolecular recombination misfortunes, the morphology affects the execution of the gadgets [48].in expansion to this, the natural materials as well as the terminals interfaces are definitive also. The principle point of support layer is to maintain a strategic distance from circumstances where the charge transporters achieve the contrary cathodes as well as to augment the VOC too [49]. Correlation with BHJ cells, bilayer arrangement prepared require symmetrical dissolvable frameworks to keep away from break down the fundamental layer which influence restriction of materials could be utilized. In the BHJ gadgets, it is conceivable to store the dynamic layer as of one arrangement utilizing diverse strategies.

  Figure 14: (A) solar cell of  an  organic  BHJ (bulk  heterojunction) device structure ;  (B)  bulk  heterojunction cell energy  band  diagram.

References of High Efficiency Organic Solar Cell

A. Alias, Z. Zabidi, A. Ali, and M. Harun, “Optical characterization and properties of polymeric materials for optoelectronic and photonic applications”, International journal of applied science and technology, Vol. 3, pp. 11-38, 2013.

A. Cheknane, H. Hilal, F. Djeffal, B. Benyoucef, and J. Charles, “An equivalent circuit approach to organic solar cell modelling", Microelectronics Journal, Vol. 39, pp. 1173–1180, 2008.

A. Hains, Z. Liang, M. Woodhouse, and B. Gregg, “Molecular Semiconductors in Organic Photovoltaic Cells", Chemical reviews, Vol. 110(11), pp.6689–6735, 2010.

Alferov, Zh. I., V. M. Andreev, M. B. Kagan, I. I. Protasov, and V. G. Trofim, 1970, ‘‘Solar-energy converters based on p-n AlxGa12xAs-GaAs heterojunctions,’’ Fiz.Tekh. Poluprovodn. 4, 2378 (Sov. Phys. Semicond. 4, 2047 (1971))

Alshahrani, T. M. (2016). Advanced Materials for Organic Solar Cells: Influence of Generation and pH on PAMAM-Based Devices By, (February).

B. Klajnert, M. Bryszewska. “Dendrimers: properties and applications”.ActaBiochimicaPolonica. Vol.48 (1), pp.199-208, 2001.

B. Qiab and J. Wang, “Fill factor in organic solar cells", Physical Chemistry Chemical Physics, Vol. 15, pp. 8972-8982, 2013.

Bloch, F, Z. Phys. (1928), 52, 555.

D. Hecht, L. Hu, and G. Irvin, “Emerging transparent electrodes based on thin films of carbon nanotubes, graphene, and metallic nanostructures”, Advanced materials, Vol. 23, pp. 1482-1513, 2011.

D. M. Chapin, C. S. Fuller, and G. L. Pearson (May 1954). "A New Silicon p-n Junction Photocell for Converting Solar Radiation into Electrical Power". Journal of Applied Physics 25 (5): 676–677. doi:10.1063/1.1721711

Dai, B. L., Winkler, B., Dong, L., Tong, L., & Mau, A. W. H. (2001). Conjugated Polymers for Light-Emitting Applications **, (12), 915–925.

David C. Brock (Spring 2006). "Useless No More: Gordon K. Teal,Germanium, and Single-Crystal Transistors". Chemical HeritageNewsmagazine (Chemical Heritage Foundation) 24 (1). Retrieved 2008-01-21.

Dou, Y. Liu, Z. Hong, G. Li, and Y. Yan, “Low-bandgap near-IR conjugated polymers/molecules for organic electronics”, Chemical reviews, Vol. 115(23), pp. 12633–12665, 2015.

E. Becquerel (1839). "Mémoire sur les effetsélectriquesproduits sous l'influence des rayonssolaires". ComptesRendus9: 561–567. Issue date: May 7, 1935.

Einstein, A, “On the Quantum Theory of Radiation” PhyikalischeZeitschrift 18(1917).

Eliseeva, S. V., &Bünzli, J.-C. G. (2011). Rare earths: jewels for functional materials of the future. New Journal of Chemistry, 35(6), 1165.https://doi.org/10.1039/c0nj00969e

Fraunhofer ISE. (2013). World record solar cell with 44.7% efficiency. Press Release. Retrieved from https://www.ise.fraunhofer.de/en/press-and-media/press-releases/presseinformationen-2013/world-record-solar-cell-with-44.7-efficiency

G. Rupprecht. “Investigations of the electrical and non-electrical conductivity of thin indium oxide layers”, Journal of Physics, Vol. 139(5), pp. 504-517, 1954.

G. Yu, J. Gao, J. Hummelen, F. Wudi, A. Heeger. “Polymer Photovoltaic Cells: Enhanced Efficiencies via a Network of Internal Donor-Acceptor Heterojunctions”, Science, Vol. 270 (5243), pp. 1789-1791, 1995.

Gerald L. Pearson, Daryl M. Chapin, and Calvin S. Fuller (AT&T) receivepatent US2780765, "Solar Energy Converting Apparatus."(1957)

H. J. Hovel and J. M. Woodall, “High Efficiency AlGaAs-GaAs Solar Cells”,Appl. Phys. Lett. 21, 379-381 (1972).

Hasegawa, T., & Takeya, J. (2009). Organic field-effect transistors using single crystals. Science and Technology of Advanced Materials, 10(2), 24314. https://doi.org/10.1088/1468-6996/10/2/024314

http://en.wikipedia.org/wiki/German_Renewable_Energy_Act

I. Hancox, K. V. Chauhan, P. Sullivan, R. A. Hatton, A. Moshar, C. P. A. Mulcahy and T. S. Jones. “Increased efficiency of small molecule photovoltaic cells by insertion of a MoO3 hole-extracting layer", Energy & Environmental Science, Vol.3, pp. 107-110, 2010.

J. Anthony, A. Facchetti, M. Heeney, S. Marder and X. Zhan. “n-Type Organic Semiconductors in Organic Electronics”, Advanced Materials, Vol.22 (34), pp. 3876–3892, 2010.

J. Blakesley and D. Neher, “Relationship between energetic disorder and open-circuit voltage in bulk heterojunction organic solar cells", Physical review B, Vol. 84, pp. 075210-12, 2011.

J. Zhang, S. Lee, and B. Sun, “Effect of Series and Shunt Resistance on Organic-Inorganic Hybrid Solar Cells Performance", ElectrochimicaActa, Vol. 146, pp. 845-849, 2014.

L. Chen, Z. Xu, Z. Honga and Y. Yang, “Interface investigation and engineering – achieving high performance polymer photovoltaic devices”, Journal of Materials Chemistry, Vol. 20, pp. 2575–2598, 2010.

M. Harun, E. Saion, A. Kassim, N. Yahya and E. Mahmud. “Conjugated Conducting Polymers: A Brief Overview”. Journal for the advancement of science and art. Vol.2, pp. 63-68, 2007.

Mihailetchi, V. (2005). Device physics of organic bulk heterojunction solar cells. PhD, Holland. Retrieved from http://dissertations.ub.rug.nl/faculties/science/2005/v.d.mihailetchi/?pLanguage=en&pFullItemRecord=ON

N. Nehaoua, Y. Chergui, and D. Mekki, “Determination of organic solar cell parameters based on single or multiple pin structures", Vacuum, Vol. 84(2), pp. 326-329, 2009.

N. Sahu, B. Parija and S. Panigrahi. ‘Fundamental understanding and modeling of spin coating process: A review’, Indian Journal of Physics, Vol. 83(4), pp. 493-502, 2009. 

Nelson, J. (2003). The Physics of Solar Cells, Imperial College Press, London, p. 363.

P. Edwards, A. Porch, M. Jones, D. Morgan and R. M. Perks. “Basic materials physics of transparent conducting oxides”, Dalton Transactions, Vol. 2004(19), pp. 2995-3002, 2004.

P. Sullivan, G. Collis, L. Rochford, J. Arantes, P. Kemppinen, T. Jones and K. Winzenberg, “An N-ethylated barbituric acid end-capped bithiophene as an electron-acceptor material infullerene-free organic photovoltaics", Chemical Communications, Vol. 51, pp. 6222—6225, 2015.

Pudasaini, P. R., &Ayon, a. (2013). Low-cost, high-efficiency organic/inorganic hetero-junction hybrid solar cells for next generation photovoltaic device. Journal of Physics: Conference Series, 476, 12140. https://doi.org/10.1088/1742-6596/476/1/012140

R. Po, C. Carbonera, A. Bernardi and N. Camaioni. “The role of buffer layers in polymer solar cells”, Energy & Environmental Science, Vol. 4. pp. 285-310, 2010.

Radosavljevi, J., &Amelija, Đ. (2001). Defining of the Intensity of Solar Radiation on Horizontal and Oblique Surfaces on Earth, 2, 77–86.

T.Clarke, J. Durrant. “Charge Photogeneration in Organic Solar Cells”, Chemical Reviews, Vol. 110(2665), pp. 6736-6767, 2010.

U. Würfel, D. Neher, A. Spie and S. Albrecht, “Impact of charge transport on current–voltage characteristics and power-conversion efficiency of organic solar cells", Nature communications, Vol. 6, pp. 1-9, 2014.

V. Murugesan, K. Sun and J. Ouyang, “Highly efficient inverted polymer solar cells with a solution-processable dendrimer as the electron-collection interlayer”, Applied Physics Letters, Vol. 102, pp. 083302-4, 2013.

W. Beek, M. Wienk and R. Janssen, Efficient hybrid solar cells from zinc oxide nanoparticles and a conjugated polymer, Advanced Materials, Vol. 16(12), pp. 1009- 1013, 2004.

W. Cai, X. Gong and Y. Cao. “Polymer solar cells: recent development and possible routes for improvement in the performance”, Solar Energy Materials and Solar Cells, Vol. 94(2), pp. 114-127, 2010.

W. Ma, C. Yang, X. Gong, K. Lee and A. Heeger. “Thermally Stable, Efficient Polymer Solar Cells with Nanoscale Control of the Interpenetrating Network Morphology”, Vol. 15(10), pp. 1617–1622, 2005.

W.G. Adams and R.E. Day (1877) “The action of light on selenium” in Proceedings of the Royal Society, A25, 113.

Wang, J. L., Zhong, C., Tang, Z. M., Wu, H., Ma, Y., Cao, Y., & Pei, J. (2010). Solution-processed bulk heterojunction photovoltaic cells from gradient ??-conjugated thienylenevinylene dendrimers. Chemistry - An Asian Journal, 5(1), 105–113. https://doi.org/10.1002/asia.200900245

Wilson, A. H., Proc. Roy. Soc. A (1931), 133, 458; 134, 277.

Xu, T., & Yu, L. (2014). How to design low bandgap polymers for highly efficient organic solar cells. Materials Today, 17(1), 11–15. https://doi.org/10.1016/j.mattod.2013.12.005

Y, Yuan, J. Huang and G. Li. “Intermediate layers in tandem organic solar cells: review”, Green, Vol. 1, pp. 65–80, 2011.

R.  Po,  C.  Carbonera,  A.  Bernardi  and  N.  Camaioni.“The  role  of  buffer  layers  in  polymer  solar  cells Energy  &  Environmental  Science,  Vol.  4.  pp.  285-310, 2010. 

 Y,  Yuan,  J.  Huang  and  G.  Li.“Intermediate  layers  in  tandem  organic  solar  cells:  review,  Green,  Vol.  1,  pp.  6580,  2011.

 N.  Sahu,  B.  Parija  and  S.  Panigrahi.  Fundamental  understanding  and  modeling  of  spin  coating  process:  A  review,Indian  Journal  of  PhysicsVol.  83(4),  pp.  493-502,  2009.   

A.  Hains,  Z.  Liang,  M.  Woodhouse,  and  B.  Gregg,  “Molecular  Semiconductors  in  Organic  Photovoltaic  Cells",  Chemical  reviews,  Vol.  110(11),  pp.6689–6735,  2010.

P.  Sullivan,  G.  Collis,  L.  Rochford,  J.  Arantes,  P.  Kemppinen,  T.  Jones  and  K.  Winzenberg, “An  N-ethylated  barbituric  acid  end-capped  bithiophene  as  an  electron-acceptor  material  infullerene-free  organic  photovoltaics", Chemical  Communications, Vol.  51,  pp.  6222—6225,  2015.

I.  Hancox,  K.  V.  Chauhan,  P.  Sullivan,  R.  A.  Hatton,  A.  Moshar,  C.  P.  A.  Mulcahy  and T.  S.  Jones.  “Increased  efficiency  of  small  molecule  photovoltaic  cells  by  insertion  of  a MoO3  hole-extracting  layer",  Energy  &  Environmental  Science,  Vol.3,  pp.  107-110,  2010.

A.  Cheknane,  H.  Hilal,  F.  Djeffal,  B.  Benyoucef,  and  J.  Charles,  “An  equivalent  circuit  approach  to  organic  solar  cell  modelling", Microelectronics  Journal,  Vol.  39,  pp.  1173–1180,  2008.

J.  Zhang,  S.  Lee,  and  B.  Sun,  “Effect  of  Series  and  Shunt  Resistance  on  Organic-Inorganic  Hybrid  Solar  Cells  Performance",  Electrochimica  Acta,  Vol.  146,  pp.  845-849,  2014.

J.  Blakesley  and  D.  Neher, “Relationship  between  energetic  disorder  and  open-circuit voltage  in  bulk  heterojunction  organic  solar  cells", Physical  review  B,  Vol.  84,  pp.  075210-12,  2011.

J.  Blakesley  and  D.  Neher, “Relationship  between  energetic  disorder  and  open-circuit voltage  in  bulk  heterojunction  organic  solar  cells",  Physical  review  B,  Vol.  84,  pp. 075210-12,  2011.

N.  Nehaoua,  Y.  Chergui,  and  D.  Mekki,  “Determination  of  organic  solar  cell  parameters  based  on  single  or  multiple  pin  structures", Vacuum, Vol.  84(2),  pp.  326-329,  2009.

B.  Qiab  and  J.  Wang, “Fill  factor  in  organic  solar  cells",  Physical  Chemistry  Chemical  Physics,  Vol.  15,  pp.  8972-8982,  2013.

  U.  Würfel,  D.  Neher,  A.  Spie  and  S.  Albrecht, “Impact  of  charge  transport  on  current–voltage  characteristics  and  power-conversion  efficiency  of  organic  solar  cells",  Nature  communications,  Vol.  6,  pp.  1-9,  2014.

W.  Beek,  M.  Wienk  and  R.  Janssen,  Efficient  hybrid  solar  cells  from  zinc  oxide  nanoparticles  and  a  conjugated  polymer,  Advanced  Materials,  Vol.  16(12),  pp.  1009-  1013,  2004.

Mihailetchi,  V.  (2005).  Device  physics  of  organic  bulk  heterojunction  solar  cells.  PhD,  Holland.  Retrieved  from  http://dissertations.ub.rug.nl/faculties/science/2005/v.d.mihailetchi/?pLanguage=en&pFullItemRecord=ON

T.Clarke,  J.  Durrant.  “Charge  Photogeneration  in  Organic  Solar  Cells”,  Chemical  Reviews,  Vol.  110(2665),  pp.  6736-6767,  2010.48-  W.  Ma,  C.  Yang,  X.  Gong,  K.  Lee  and  A.  Heeger.  “Thermally  Stable,  Efficient  Polymer  Solar  Cells  with  Nanoscale  Control  of  the  Interpenetrating  Network  Morphology”,  Vol.  15(10),  pp.  1617–1622,  2005.

W.  Cai,  X.  Gong  and  Y.  Cao.  “Polymer  solar  cells:  recent  development  and  possible  routes  for  improvement  in  the  performance”,  Solar  Energy  Materials  and  Solar  Cells,  Vol.  94(2),  pp.  114-127,  2010.

L.  J.  Stone,  M.  luton,  lu3.  J.  Gilroy.  (1949).  "Lithium  Chloride  as  a  Substitute  for  Sodium  Chloride  in  the  Diet".  Journal  of  the  American  Medical  Association.  139  (11):  688–692

Talbott  J.  H.  (1950).  "Use  of  lithium  salts  as  a  substitute  for  sodium  chloride".  Arch  Med  Interna.  85  (1):  1–10.  PMID  15398859.

"Case  of  trie  Substitute  Salt".  Time.  28  February  1949.

Ulrich  Wietelmann,  Richard  J.  Bauer  "Lithium  and  Lithium  Compounds"  in  Ullmann's  Encyclopedia  of  Industrial  Chemistry  2005,  Wiley-VCH:  Weinheim.

hönnerscheid  Andreas;  Nuss  Jürgen;  Mühle  Claus;  Jansen  Martin  (2003).  "Die  Kristallstrukturen  der  Monohydrate  von  Lithiumchlorid  und  Lithiumbromid".  Zeitschrift  für  anorganische  und  allgemeine  Chemie.  629:  312–316.  doi:10.1002/zaac.200390049.

Kamali  A.R.;  Fray  D.J.;  Swandt  C.  (2011).  "Thermokinetic  characteristics  of  lithium  chloride".  J  Therm  Anal  Calorim.  104:  619–626.  doi:10.1007/s10973-010-1045-9.

Holleman,  A.  F.;  Wiberg,  E.  Inorganic  Chemistry  Academic  Press:  San  Diego,  2001.  ISBN  0-12-352651-5.

Hönnerscheid  Andreas;  Nuss  Jürgen;  Mühle  Claus;  Jansen  Martin  (2003).  "Die  Kristallstrukturen  der  Monohydrate  von  Lithiumchlorid  und  Lithiumbromid".  Zeitschrift  für  anorganische  und  allgemeine  Chemie.  629:  312–316.  doi:10.1002/zaac.200390049.

      Kamali  A.R.;  Fray  D.J.;  Swandt  C.  (2011).  "Thermokinetic  characteristics  of  lithium  chloride".  J  Therm  Anal  Calorim.  104:  619–626.  doi:10.1007/s10973-010-1045-9.

Krishna,  Palakodety  Radha;  G.  Dayaker  (2007).  "A  stereoselective  total  synthesis  of  (−)-andrachcinidine  via  an  olefin  cross-metathesis  protocol".  Tetrahedron  Letters.  Elsevier.  48  (41):  7279–7282. doi:10.1016/j.tetlet.2007.08.053.

Chandrasekhar,  M.;  Kusum  L.  Chandra;  Vinod  K.  Singh  (2003).  "Total  Synthesis  of  (+)-Boronolide,  (+)-Deacetylboronolide,  and  (+)-Dideacetylboronolide".  Journal  of  Organic  Chemistry.  68  (10):  4039–4045.  doi:10.1021/jo0269058.  PMID  12737588.

J.  Brussee;  J.  L.  G.  Groenendijk;  J.  M.  Koppele;  A.  C.  A.  Jansen  (1985).  "On  the  mechanism  of  the  formation  of  s(−)-(1,  1'-binaphthalene)-2,2'-diol  via  copper(II)amine  complexes".  Tetrahedron.  41  (16):  3313.  doi:10.1016/S0040-4020(01)96682-7.

C.  E.  Castro;  E.  J.  Gaughan;  D.  C.  Owsley  (1965).  "Cupric  Halide  Halogenations".  Journal  of  Organic  Chemistry.  30  (2):  587.  doi:10.1021/jo01013a069.

S.  H.  Bertz,  E.  H.  Fairchild,  in  Handbook  of  Reagents  for  Organic  Synthesis,  Volume  1:  Reagents,  Auxiliaries  and  Catalysts  for  C-C  Bond  Formation,  (R.  M.  Coates,  S.  E.  Denmark,  eds.),  pp.  220-3,  Wiley,  New  York,  1738.

Wells,  A.F.  (1984)  Structural  Inorganic  Chemistry,  Oxford:  Clarendon  Press.  ISBN  0-19-855370-6.  Peter  Baláž  (2008).

Mechanochemistry  in  Nanoscience  and  Minerals  Engineering.  Springer.  p.  167.  ISBN  3-540-74854-7.  Marina  Brustolon  (2009).

Electron  paramagnetic  resonance:  a  practitioner's  toolkit.  John  Wiley  and  Sons.  p.  3.  ISBN  0-470-25882-9.

Our Top Online Essay Writers.

Discuss your homework for free! Start chat

Top Rated Expert

ONLINE

Top Rated Expert

1869 Orders Completed

ECFX Market

ONLINE

Ecfx Market

63 Orders Completed

Assignments Hut

ONLINE

Assignments Hut

1428 Orders Completed