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Measurement of Optical Bandgap Energies of Semiconductors

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A method for bandgap energy determination using diuse reection is presentedand compared to the traditional integrating sphere method. We have found thebandgap energies of ZnO, TiO 2 , Cu 2 O, Si, SnZrS 3 , SnZrSe 3 , Sn 2 S 3 , and BiCuOSepowders with both methods and found they agree within 0.03 eV. We havemeasured scattering from powder material in the infrared region of the spectrumwith a linear wavelength dependence. We have measured optical bowing of thebandgap energies of the SnZrS 3-x Se x system. We also describe in depth the OceanOptics spectrometer and its components.

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T/ (1 − R)

T/ (1 − R)Exact

T/ (1 − R)

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(F (R)ω )12

ω

(F (R)ω )12

ω

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T Sample (λ) = S Sample (λ)S Reference (λ)

RSample (λ) = S Sample (λ)S Reference (λ)

T Sample (λ) RSample (λ)

S Sample (λ)

S Reference (λ)

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T Sample (λ) = T Reference (λ) S Sample (λ) − S Background (λ)S Reference (λ) − S Background (λ)

RSample (λ) = RReference (λ) S Sample (λ) − S Background (λ)

S Reference (λ) − S Background (λ)

RReference (λ) T Reference (λ)

S Background (λ)

k

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θ = 0

E = E 0ei (kr − ωt )

ω k r

t

N i = n i + iκ i

N n

κ

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R01 = (n0 − n1)2 + κ1

2

(n0 + n1)2 + κ12

T 01 = 4n0n1

(n0 + n1)2 + κ12

d

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d

d d

R02 = r 01 + r12t01t10e− αd eiδ

1 − r10r 12e− αd eiδ

2

T 02 = n2

n0

t01t12e− αd2 ei δ

2

1 − r10r 12e− αd eiδ

2

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tmn = 2N mN m + N n

r mn = N m − N nN m + N n

δ = 4πn 1d

λ

R02 T 02

d

R02 = R01 + R12T 01T 10e− 2αd

1 − R10R12e− 2αd

T 02 = T 01T 12e− αd

1 − R10R12e− 2αd

T mn = nn

nm| tmn |2

Rmn = |r mn |2

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R03 = R02 + R23T 02T 021 − R02R23

T 03 = T 23T 02

1 − R20R23

R03 T 03

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dz

J (z ) I (z )

J (z ) z > d

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A = 1 − T − R

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α = 2ωκ

c =

4πκλ

c λ

κ λ

T 1 − R

− 1

= 1 − R02

T 23T 02−

R23

T 23R20

1 − R02

T 02+ T 20

R23

R02 + T 02 < 1

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T 1 − R

= T 23T 02

1 − R02

α n1 d

T 1 − R

= |t12 |2 | t23 |2

eαd − e− αd | r12 |2

R23

T 1 − R

= e− αd

T/ (1 − R) T / (1 − R)

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T/ (1 − R)

T/ (1 − R)Exact T / (1 − R)

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J (z ) I (z )

1s

dr (z )dz

= r (z )2 − 2(2a − 1)r (z ) + 1

r (z ) = J (z )I (z )

a = k + s

s

r (z )

a

a = (1 + R∞ )2

4R∞

f (R∞ ) = ks

= (1 − R∞ )2

4R∞

R∞ = r (∞ )

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k

ε

N

ε = N 2

κ = αλ4π

= εi

n

αω

= εi

n C

n κ λ εi

ω C

i = C 11

ω2 |P cv |D j

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D j

P cv

D j = 14π3 dS k

| k (E c − E v)

P cv = ψc | − e E ·r |ψv

S k E c − E v

i = C 21

(ω )2 (ω − E Bandgap ) p

αω = C (ω − E Bandgap ) p

ω E Bandgap p

C

p

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(αω )1

p ω

α = 0

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µ

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o

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± 10%

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± 5%

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0.01%

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(F (R)ω )12

ω

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(F (R)ω )12

ω

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(F (R)ω )12

ω

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x = 0 I (0)

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