Plastic electronics is a concept that emerged forty years ago, with the discovery of electrically conductive polymers. Ten years later, the first electronic devices using organic solids in place of the ubiquitous inorganic semiconductors were realised. The best achievement of plastic electronics is constituted by Organic Light-Emitting Diodes (OLEDs) that equip the display of many smartphones, and even TV sets. The objective of this course is to provide a comprehensive overview of the physics of plastic electronic devices. After taking this course, the student should be able to demonstrate theoretical knowledge on the following subjects: Concept of organic semiconductors; Charge carrier transport in polymeric and organic semiconductors; Optical properties of organic semiconductors; Charge injection from metals to organic solids; Operating mode of the main plastic electronic devices: Organic light-emitting diodes (OLEDs), organic photovoltaic cells (OPVs) and organic field-effect transistors (OFETs).
Organic solar cell
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En provenance du cours de École Polytechnique
Plastic electronics
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À partir de la leçon
Plastic electronic devices
Rencontrer les enseignants
Gilles HorowitzEmeritus Research Fellow
Laboratoire de Physique des Interfaces et des Couches Minces (LPICM)
The device we described today is the organic solar cell or
organic photovoltaic cell or OPV.
The photovoltaic effect is the exact reverse of electroluminescence.
That is, it is when light energy Is converted into electrical energy.
The idea of using organic solids for conversion dates back to the 50s.
But for decades the efficiency of organic cells has remained desperately low.
It was only in 1986 that Ching Tang,
the very person that invented the two layer OLED one year later,
reported on a double-layer organic solar cell
that could convert light to electricity with an efficiency of 1%.
By that time,
the power conversion of silicon solar cells was already around 20%.
Then, came two major breakthroughs from the University of
California at Santa Barbara.
First, the elucidation of the mechanism
at the origin of the improved efficiency of the two layer structure,
namely, a fast electron transfer,
and then, the synthesis of a fullerene-based polymer by Fred Wudl,
that led to the bulk heterojunction solar cell.
Here we show the current-voltage characteristic of the
the cell by Chin Tang. The cell itself is a two layered diode
that associates an n type and a p type semiconductors.
As will be explained later,
the two layers now refer to as an electron acceptor and donor.
Here, the donor is copper phthalocyanine and the acceptor a perylene derivative.
Light come to the cell through a transparent tin oxide electrode.
In conventional solar cells, a photon of energy higher than the energy gap
promotes an electron from the top of the Valence bands to the conduction band.
This electron is next injected into an external circuit,
and then returns to the Valence band, meanwhile generating electrical energy.
All in all, light directly creates electrical charges.
However, in an organic solar cell, there is an additional step.
Light do not directly creates electrical charges. Instead it creates an exciton,
which in turn must be converted into an electron and a hole.
The issue with organics semiconductors that the excitons are tightly bound,
that is, the binding energy is around 1 electric volt,
so excitons are difficult to split into electrical charges.
The way towards high efficiency opened in the 1990s by two major breakthroughs.
First was the discovery of light induced electron transfer
between an electron donor D and an acceptor A.
The process can be decomposed into four steps.
First, the donor is promoted to its
excited state D star by the incident photon.
Then, the excitation is delocalized between the donor and the acceptor.
In the third step, electrical charge separation is initiated and
is finalized in the last step, leading to the formation of an electron-hole pair.
What is important now is that the lifetime of the delocalized exciton,
also called charge-transfer exciton, is much shorter than that of the exciton.
In the process described earlier, the acceptor was Fullerene,
a bulky molecule made of 60 carbon atoms arranged in a sphere.
However, fullerene is insoluble in most organic solvents, and
hence difficult to implement.
So the second important discovery
was the synthesis of a soluble fullerene derivative called PCBM.
The operation of the organic solar cell can now be visualized as follows.
A photon of energy higher than the optical gap hits the donor and
creates an exciton.
This exciton can migrate to the donor-acceptor interface through
thermal diffusion.
When the exciton reaches the interface, the electron drops in the LUMO
level of the acceptor, while the hole remains in the HOMO level of the donor.
This leads to the formation of the charge transfer exciton, with a reduced binding energy.
The next step is charge separation and extraction,
which occur under the effect of the built-in electric field in the diode,
due to the different work functions of the anode and the cathode.
The direction of the field makes both electrons and holes to be extracted
and collected at the electrodes.
The performance of the first two layer OPVs was limited
by the fact that the excitons that can reach the interface are those created
at a distance corresponding to their diffusion length.
The exciton diffusion length is typically around 10 nanometers;
that is, only one tenth of the typical thickness of the donor layer.
So, only less than 10% of the excitons could be retrieved.
The efficiency of the cells substantially increased
with the so-called bulk hetero-junction geometry,
when the donor and
the acceptor are blended through the thickness of the diode.
Here, the donor is in green and the acceptor in orange.
Because excitons are electrically neutral, they are insensitive to the electric field,
and can defuse in any direction.
Here we see that through a horizontal movement,
the exciton can easily reach the donor acceptor interface.
Besides, electrons and holes are electrically charged and
preferentially move along the electric field.
Moreover, the holes only move into the donor and electrons in the acceptor.
So in the bulk hetero-junction the movement of excitons and
electric charges are disconnected.
The electrical power provided by solar cell is estimated
from its current-voltage curve. A solar cell is basically a diode,
and its current-voltage curve in the dark follows the characteristics
of a diode, that is, no current under reverse bias and a current that rapidly increases under forward bias.
When the diode is illuminated,
a photo current adds to the dark current,
and the curve shifts along the y-axis.
At zero current, one has the open-circuit voltage, Voc,
and at zero voltage, the short-circuit current, I sc.
The electrical power supplied by the cell
is given by the product of the current times the voltage;
that is, the area of the orange rectangle in the figure.
More precisely, the output power is calculated
at the point where the area is at its maximum;
that is, at the potential V max and current I max.
Mathematically speaking, the maximum delivered
power is given by P max equals V max times I max,
or alternatively, the open circuit voltage times
the short circuit current multiplied by the fill factor, FF.
The power conversion efficiency is given by the ratio
between the maximum delivered electrical power to the incident light power.
To date, the best organic solar cells have a power conversion efficiency
of slightly above 10%.
This is twice lower than the efficiency of commercial silicon cells.
So currently, applications and envisioned in domains where
the compatibility of organic device is plastics is at work,
for instance, for the fabrication of light, flexible and easily portable cells.
Thank you for your attention.
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