solar cell operation

9
Mapping free carrier diffusion in GaAs with radiative and heat-generating recombination Tim Gfroerer and Ryan Crum Davidson College, Davidson, NC with Mark Wanlass National Renewable Energy Lab, Golden, CO ~ Supported by the American Chemical Society – Petroleum Research Fund ~

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Mapping free carrier diffusion in GaAs with radiative and heat-generating recombination Tim Gfroerer and Ryan Crum Davidson College, Davidson, NC with Mark Wanlass National Renewable Energy Lab, Golden, CO ~ Supported by the American Chemical Society – Petroleum Research Fund ~. -. -. -. - PowerPoint PPT Presentation

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Page 1: Solar Cell Operation

Mapping free carrier diffusion in GaAs with radiative and heat-

generating recombination 

Tim Gfroerer and Ryan CrumDavidson College, Davidson, NC

with Mark WanlassNational Renewable Energy Lab, Golden,

CO

~ Supported by the American Chemical Society – Petroleum Research Fund ~

Page 2: Solar Cell Operation

Solar Cell Operation

Conduction Band

Valence Band

PHOTONEN

ER

GY

ELECTRON

E-Field

E-Field

HOLE

E-Field

E-Field

+ +

++

---

-

-

CURRENTABSORPTION

When a photon is absorbed, an electron is excited into the conduction band, leaving a hole behind in the valence band.  Some heat is lost, reducing efficiency. Then an internal electric field sweeps the electrons and holes away, creating electricity.

HEAT

Page 3: Solar Cell Operation

Light- and Heat-Generating Recombination

Electrons can recombine with holes by releasing light or heat.This loss mechanism also reduces the efficiency of a solar cell.

Conduction Band

Valence Band

DefectLevel

-

+

HEAT

HEAT

Conduction Band

Valence Band

EN

ER

GY

Photon

-

+

Rate ≈ A x n (n = carrier density)Rate ≈ B x n 2 (n = carrier density)

Page 4: Solar Cell Operation

Experimental Setup

+-+-

+

+

+

+

-

+

-

+

-

-

+-

--

--

+

+

Laser spot ~4 mm diameter

GaAs sample (plan view)

ThermalCamera

LuminescenceCamera

Page 5: Solar Cell Operation

0 100 200 300 400

10-3

10-2

10-1

100

0-33 ms 33-67 ms 67-100 ms 100-133 ms

Tem

pera

ture

Diff

eren

ce (

K)

Distance (m)

Time Window:

Time evolution of thermal profile

Laser on!

Heat loss

Thermal diffusion

Page 6: Solar Cell Operation

Luminescence and Thermal Profiles

0 100 200 300 40010-5

10-4

10-3

10-2

10-1

100

Laser ExcitationLight EmissionT (Heat)

Nor

mal

ized

Lig

ht o

r H

eat

Sig

nal

Distance From Excitation Position (m)

Page 7: Solar Cell Operation

Square-root of the Luminescence

0 100 200 300 40010-5

10-4

10-3

10-2

10-1

100

Laser ExcitationLight Emission

(Light Emission)1/2

T (Heat)

Nor

mal

ized

Lig

ht o

r H

eat

Sig

nal

Distance From Excitation Position (m)

Rate ≈ B x n 2

Rate ≈ A x n

Page 8: Solar Cell Operation

Free-Carrier or Thermal Diffusion?!

0 100 200 300 40010-5

10-4

10-3

10-2

10-1

100

Laser ExcitationLight Emission

(Light Emission)1/2

T (Heat) Thermal Diffusion

Nor

mal

ized

Lig

ht o

r H

eat

Sig

nal

Distance From Excitation Position (m)

Page 9: Solar Cell Operation

Conclusions• We use optical and thermal imaging to

map the free-carrier density near a localized photo-excitation source.

• The density profiles agree when we account for the bimolecular nature of radiative recombination.

• BUT: a thermal diffusion calculation also mimics the temperature profile …

• So what have we measured?!We’ll figure it out!