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Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

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Page 1: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

Applied Physics Department

Seminar 791Solar cells Fabrication

ByEnas Hamasha

SupervisorDr. Adnan Shariah

Page 2: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

introduction

In 1953 developed the first silicon cellThis cells uses in application spacecraft (standard technology)

Development to supply cells for communication satellites

And other space craft.

In 1973,start applying solar cell in renewable energy resources, with some change in standard technology.

Page 3: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

The standard technology stages for making cells

1. Reduction of sand to metallurgical-grade silicon.

2. Purification of MG-Si to semiconductor grade silicon.

3. Conversion of semiconductor grad silicon to single crystal silicon wafers.

4. Processing of single-crystal silicon wafer into solar cells.

5. Solar cell to solar module

Page 4: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah
Page 5: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

1-sand to metallurgical-grad silicon

Silicon is the second most a abundant element in the earths crust.

The source material for the extraction of silicon is silicon dioxide the major constituent of sand.

We will extract the Si by reduced crystalline form of silicon dioxide in large arc furnace.

Page 6: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah
Page 7: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah
Page 8: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

Produce MG-Si in this furnace by carbon (in the form of mixture of wood chips, coke, and coal) according this reaction

SiO2(s)+C(s)-----------Si(l)+CO2 (g)

Solidification

MG-Si (metallurgical grade silicon)

Page 9: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

Then silicon is periodically poured from the furnace and blown with O/chlorine mixture to further purify it.

Next poured into shallow troughs, where it solidifies and is subsequently broken into chunks

Page 10: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

Characteristic 1 million metric tons of this MG-si are produce globally each year (large production).

Use MG-Si in the steel and aluminum industries.

The total processing energy requirement are acceptable.

The result the MG-Si is inexpensive.

99% pure with the major impurities being iron and aluminum

Page 11: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah
Page 12: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

2-MG-silicon to semiconductor-grade silicon

For use in solar cells as well as other semiconductor devices, silicon must be much purer than MG-Si.

The standard process to purifying its known siemens process

Page 13: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

Siemens process

The MG-Si is converted to a volatile compound that is condensed and refined by fractional distillation

Ultra pure silicon is then extracted from this refined product.

Abed of fine MG-Si particle is fluidized with HCl in the presence of a Cu catalyst.

Page 14: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

MG-Si(s) +3HCl(l) --SiHCl3(g) +H2(g)

Con

dens

er a

nd

mul

tiple

fr

actio

nal

dist

illat

ions

SeG-SiHCl3 (l)

Semiconductor-grade purity

trichlorosilane

Page 15: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

The gases emitted are passed through a condenser and the resulting liquid subjected to multiple fractional distillation to produce SeG-SiHCl3 (trichlorosilane), the source material for the silicon industry.Then extract SeG-Si, the SeG-SiCHl3 is reduced by hydrogen when mixture of the gases are heated. Silicon is deposited in fine-grained polycrystalline from onto an electrically heated silicon rod.

Page 16: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

SeG-SiHCl3(g) +H2SeG-Si(s) + 3HCl

Polycrystalline

Semiconductor-Grade Silicon

Page 17: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

Characteristics

Requirement a lot of energy.

Low yield ~37%

The high cost of this stage.

Reach to purity 99.9999%

Page 18: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

3-semiconductor –grade poly crystalline to single-crystal wafers

Silicon must very pure and be in a single-crystal form with essentially zero defect in the crystal structure.

The major method used to produce such material commercially is the

Czochralski process

Page 19: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

Czochralski process

The SeG polycrystalline silicon is melted in crucible with trace levels of one of the dopants required in the completed device added ,

Page 20: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

For solar cells ,boron , a p-type dopant ,is normally used, using a seed crystal and with very close temperature control, it is possible to pull from the melt.

Page 21: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

a large cylindrical single crystal of silicon, of diameter in excess of 12.5 cm and

1-2m in length are routinely grown in this manner.

Page 22: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

Then the large single crystal is sliced up into wafers which are as thin as possible

(Silicon solar cells need only be 300μm or so thick to absorb most of the appropriate wavelength in sunlight)

Page 23: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

characteristic

The present wafering technology its difficult to cut wafers from the large crystals which are any thinner than 300μm and still retain reasonable yields.

More than half the silicon is wasted as kerfs or cutting loss in the process

The low overall yields of single-crystal

Page 24: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

4-single-crystal wafers to solar cells

After etching the silicon wafers and cleaning them, additional impurities are introduced into the cell in controlled manner by a high-temperature impurities diffusion process.

To make solar cell, n-type impurities must be introduced to give a p-n junction ,phosphorus is the impurity generally used

Page 25: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

Process to doped n-type

A carrier gas is bubbled through phosphorus oxychloride (POCl3),mixed with a small a mount of oxygen, and passed down a heated furnace tube in which the wafers are stacked ,this grows an oxide layer on the surface of the wafers containing phosphorus, at the temp involved (800—1100)°Cthe phosphorus diffuses from the oxide into the silicon After about 20min the p impurities override the B impurities in the region near the surface of the wafers to give a thin, heavily doped n-type region

Page 26: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah
Page 27: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

In subsequent processing the oxide layer is removed as are the junction at the side and back of

the cell to give the structure in figure

Page 28: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

Vacuum evaporation The standard technology to metal contact are then attached to both the n-type and the p-type region ,the metal to be deposited is heated in a vacuum to a high enough temp to cause it to melt and vaporize, it will then condense on any cooler parts of the vacuum system in direct line of sight, including the solar cells, the back contact is normally deposited over the entire back surface, while the top contact is required in the form of a grid.

Page 29: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

Techniques for defining top grid

1. Use a metal shadow mask 2. The metal can be deposited over the

entire front surface of the cell and subsequently etched a way from unwanted region using a photographic technique known

photolithography

Page 30: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah
Page 31: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

The contact made up three separate layer

1. Thin layer of titanium is used as the bottom layer.

2. Layer of silver in the top.

3. The sandwiches layer is palladium.

Page 32: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

After deposition the contacts are sintered at 500-600 °C to give good adherence and low contact resistance, Finally a thin antireflection (AR) coating is deposited on the top of the cell by the same vacuum evaporation process.

Page 33: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

To minimize reflection from the flat surface solar cell wafers are textured, this means a creating a roughened surface, so that incident light will have a larger probability of being absorbed into the solar cell. This is performed by etching in a week alkaline solution such as Hf.

Texturing surface

Page 34: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah
Page 35: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

Characteristics

Yield of about 90% from starting wafers to completed terrestrial cells can be obtained.

This make the processing very labor-intensive.

The vacuum evaporation equipment is expensive compared to its throughput.

the material expensive such Ag.

Page 36: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

5 .solar cell to solar module

After interconnecting between cells solar cells require encapsulation by glass to:

1. Mechanical protection 2. Electrical isolation 3. Chemical protection4. Mechanical rigidity to support the prattle cells

and their flexible interconnection

Page 37: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

we will connect many cells to make module and connect more than two modules to make panel and the many panel to make array show below:

Page 38: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah
Page 39: Applied Physics Department Seminar 791 Solar cells Fabrication By Enas Hamasha Supervisor Dr. Adnan Shariah

THANK YOU

Questions ?