Perovskite Solar Cells a short general overview presentation hadi maghsoudi device structure crystal structure preparation synthesis method review papers

1. Short Overview of
Perovskite Solar Cells
New Promising Materials for Next Generation Solar Cells
Hadi Maghsoudi
27 February 2015
Slides at: http://www.slideshare.net/hadimaghsoudi/perovskite-solar-cells

2. Basic Structure of a Photovoltaic Solar Cell
• A photovoltaic solar cell is made of three main part:
• Light Absorber; converting incident photons to electron and holes
• Carrier Collector/s; capturing the carriers (electron and holes)
• Metal Contacts: transferring the carriers to the circuit
• The heart of a solar cell is the absorber layer
2Basic schematic of a photovoltaic solar cell

3. Three Generations of Solar Cells
• Wafer based:
• Monocrystalline silicon 25%
• Polycrystalline silicon 20%
• Multi-junction cell (different band-gap materials) 40%
• Thin Films:
• Amorphous thin film silicon 13%
• CdTe (Cadmium Telluride) 17%
• CIGS (Copper Indium Gallium Selenium) 20%
• Low Cost and high Efficient:
• DSSC (Dye-sensitized solar cells)
• QDSSC (Quantum Dot-sensitized solar cells)
• OPV (Organic photovoltics)
• QDs-Polymer Hybrid solar cells
• Perovskite Solar Cells
3
Highest efficiency

4. Emergence of Perovskite Solar Cells
• Efficiency jump in photovoltaics research
• From 3.8 % in 2009 to 15.9 % in 2014
4Science 18 October 2013: Vol. 342 no. 6156 pp. 317-318
15% perovskite solar cell made in University of Oxford

5. Superiorities of Perovskite Solar Cells
1. High efficiency; with an efficiency of 15.9% after only several
years work.
2. Facile low temperature solution-based fabrication method;
3. High absorption coefficient.
4. Higher stability in air.
5. High diffusion length, high charge-carrier mobilities.
• it means that the light-generated electrons and holes can move large
enough distances to be extracted as current, instead of losing their energy
as heat within the cell
6. very high values of open-circuit voltages (VOC) typically
obtained.
5

6. Perovskite Crystal Structure
• Usually have stoichiometry of AMX3
• X is an oxide or halide anion such as Cl, Br and I.
• M refers to a metal cation with a coordination number of 6.
• The MX6 octahedra share corners and A is usually a large cation
that fills the cuboctahedral holes with coordination number of
12.
• A can be Ca, K, Na, Pb, Sr, other rare metals.
6CrystEngComm, 2010, 12, 2646-2662

7. Organic–inorganic Hybrid Perovskites
• First three-dimensional organic–inorganic hybrid perovskite,
discovered by replacing caesium in CsPbX3 (X = Cl, Br or I)
with methylammonium cations (MA = CH3NH3
+) by Dieter
Weber, in 1978.
• CH3NH3PbI3 is most common used materials for making high
efficiency perovskite solar cells.
• CH3NH3PbI3 is a semiconducting pigment with a direct bandgap
of 1.55 eV with absorption coefficient as high as 104–105 cm−1
7JACS, 136, 622, 2014
Methylammonium (MA)

8. Organic–inorganic Hybrid Perovskites cont.
• The unit cell parameter 𝑎 increases from 5.68 to 5.92 and to
6.27 Å as the size of halide increases from X = Cl to Br and to I,
respectively.
• The large size and aspherical shape of MA cause distortion in
network and drives several phase transitions by decreasing T.
• For T <160 K orthorhombic, 162.2 K<T< 327.4 K tetragonal
and T > 327.4 K cubic.
8
Phys. Rev. B 90, 045207

9. Band Gap Tuning
• Bandgap tuning is required to extend the absorption to longer
wavelengths without sacrificing the absorption coefficient.
• Changing in any of A, M and X in AMX3 changes the bandgap
• The bandgap also can be tuned in between 1.55 eV and 1.17 eV
by varying the ratio of lead to tin
9
Small
Volume 11, Issue 1, pages 10-25, 30 OCT 2014 DOI: 10.1002/smll.201402767
http://onlinelibrary.wiley.com/doi/10.1002/smll.201402767/full#smll201402767-fig-0002
FA: formamidinium HC(NH2)2
+

10. Device structure
• The device structure, related materials, and interfacial
modification are key factors in performance of solar cells.
• Two typical structures can be constructed: a) mesoscopic
nanostructure and b) planar structure.
• Mesoporous TiO2 layer usually is used to collect the electrons
• Organic Hole transporting material (HTM) collects the holes
• Planar structure has simpler structure and higher efficiency
10
Small
Volume 11, Issue 1, pages 10-25, 30 OCT 2014 DOI: 10.1002/smll.201402767
http://onlinelibrary.wiley.com/doi/10.1002/smll.201402767/full#smll201402767-fig-0004

11. Preparation Method
• There are two common methods:
1) one step coating: spin-coating a mixed CH3NH3I and PbI2solution
2) two-step coating: spin-coating CH3NH3I after coating with PbI2
11
Small
Volume 11, Issue 1, pages 10-25, 30 OCT 2014 DOI: 10.1002/smll.201402767
http://onlinelibrary.wiley.com/doi/10.1002/smll.201402767/full#smll201402767-fig-0005

12. Preparation Method cont.
• All deposition process happens at a low temperature (below 150
°C), which is suitable for the fabrication of flexible solar cells
based on PET substrates.
• The concentration of the CH3NH3I solution affects the crystal
size from about 90 nm to about 700 nm.
• Photovoltaic performance was strongly influenced by the
CH3NH3I concentration, i.e., the crystal size of CH3NH3PbI3
• CH3NH3PbI3 degrades in humid conditions and forms PbI2 at
higher temperatures due to the loss of CH3NH3I
• Lead (Pb) compounds are very toxic and harmful to the
environment.
• Video instruction of fabricating perovskite soalr cells:
• https://www.youtube.com/watch?v=RqW9HrasNPA
12

13. Future Challenges of Perovskite Solar Cells
• Improving efficiency to exceed thin film CdTe solar cells
• By understanding their material properties and optimal cell designs
• Increasing air and temperature stability
• Replacing toxic Pb with a greener element
• Is AMX3 (perovskite structure) the best stoichiometry? Have we
tried other structures?
13

14. References
1. Small, Volume 11, Issue 1, pages 10-25, 30 OCT 2014 DOI:
10.1002/smll.201402767
2. Nature Materials 13, 838–842 (2014) doi:10.1038/nmat4065
3. Science 18 October 2013: Vol. 342 no. 6156 pp. 317-318
4. CrystEngComm, 2010, 12, 2646-2662 10.1039/C001929A
5. PHYSICAL REVIEW B 90, 045207 (2014)
6. Nature Photonics 8, 506–514 (2014)
doi:10.1038/nphoton.2014.134
7. Angewandte Chemie International Edition Volume 53, Issue
11, pages 2812–2824, March 10, 2014
8. Phys. Rev. B 90, 045207 – Published 24 July 2014
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