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Using a three head Laytec detector system on a 6x2 Thomas Swan ...

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<str<strong>on</strong>g>Using</str<strong>on</strong>g> a <str<strong>on</strong>g>three</str<strong>on</strong>g> <str<strong>on</strong>g>head</str<strong>on</strong>g> <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> <str<strong>on</strong>g>detector</str<strong>on</strong>g> <str<strong>on</strong>g>system</str<strong>on</strong>g> <strong>on</strong><br />

a <strong>6x2</strong> <strong>Thomas</strong> <strong>Swan</strong> MOCVD reactor<br />

A.J.SpringThorpe and W. Beny<strong>on</strong><br />

Nati<strong>on</strong>al Research Council of Canada<br />

Institute for Microstructural Sciences<br />

Canadian Phot<strong>on</strong>ics Fabricati<strong>on</strong> Centre<br />

1200 M<strong>on</strong>treal Rd., Ottawa.Ontario<br />

Canada [K1A 0R6]


CPFC<br />

<strong>6x2</strong> [7x2] T/S MOCVD reactor<br />

�Mainly 3x3 and 1x4 c<strong>on</strong>figurati<strong>on</strong><br />

�For InP and GaAs based alloys<br />

�Quartz diffuser plate<br />

�Exhaust pipe-line “Widget”<br />

�<str<strong>on</strong>g>Laytec</str<strong>on</strong>g> ‘in-situ’ m<strong>on</strong>itoring<br />

�Pyrometry @ 950nm<br />

�reflectance @ 633nm [GaAs] and 950nm [InP]<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

2


InP-based materials<br />

�1.3 and 1.55μm lasers<br />

� FP, DFB and BH<br />

�InGaAsP, InGaAs and InAlGaAs<br />

�P-i-N <str<strong>on</strong>g>detector</str<strong>on</strong>g>s - InGaAs<br />

�APD’s, QWIP’s<br />

�HBT’s<br />

�Quantum Dots<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

3


GaAs, GaInAs, GaInP and AlGaAs<br />

�980nm lasers<br />

�Waveguides<br />

�Bragg reflectors<br />

�Multi-juncti<strong>on</strong> Solar Cells<br />

�QWIP’s - QCL’s<br />

�Quantum Dots<br />

�2DEG’s<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

4


Single <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> reflectance <str<strong>on</strong>g>head</str<strong>on</strong>g><br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

5


<str<strong>on</strong>g>Laytec</str<strong>on</strong>g> optical m<strong>on</strong>itoring <str<strong>on</strong>g>head</str<strong>on</strong>g> placement <strong>on</strong> the MOCVD reactor<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

6


<str<strong>on</strong>g>Laytec</str<strong>on</strong>g> <str<strong>on</strong>g>detector</str<strong>on</strong>g> <str<strong>on</strong>g>head</str<strong>on</strong>g> layout<br />

DTT 1: 633 nm<br />

950 ± 70 nm DTT 2: 633 nm<br />

950 ± 70 nm<br />

950 ± 10 nm<br />

DTT 3: 950 ±<br />

70 nm<br />

A<br />

B<br />

C<br />

D<br />

D Ξ<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

B<br />

C sees the susceptor<br />

7


GaAs and AlAs calibrati<strong>on</strong><br />

Mirror<br />

White light<br />

AsH 3<br />

Detectors<br />

@633nm<br />

@950nm<br />

GaAs substrate<br />

TMG<br />

TMA<br />

TMA-1 TMG-1 TMA-2 TMG-2<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

8


InP growth rate calibrati<strong>on</strong> @ ~650 o C<br />

4.758Å/s<br />

4.625Å/s<br />

4.758Å/s<br />

+2.9%<br />

-1.8%<br />

Relative reflectance<br />

0.380<br />

0.360<br />

0.340<br />

0.320<br />

0.300<br />

0.280<br />

Relative reflectance @ 950nm<br />

Detector 1<br />

Detector 2<br />

Detector 3<br />

0.260<br />

1500 2000 2500 3000 3500 4000 4500<br />

time/s<br />

Special 3x3 susceptor to use all <str<strong>on</strong>g>three</str<strong>on</strong>g> <str<strong>on</strong>g>detector</str<strong>on</strong>g>s<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

9


Reflectance at 950nm during n-InP epitaxy<br />

Substrate<br />

1.3E18 S-InP<br />

5E18 Si-InP<br />

5E17 Si-InP<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

10


MOCVD Quantum dots<br />

�InAs<br />

�50%InGaAs<br />

�Need ‘in-situ’ m<strong>on</strong>itoring<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

11


Formati<strong>on</strong> of InAs QDs – RHEED signature<br />

T=0s,<br />

0ML InAs<br />

GaAs c(4x4)<br />

T=1s,<br />

0.08ML InAs<br />

T=QD-0.5s,<br />

T=QD 0.5s,<br />

1.86ML InAs<br />

T=QD+0.5s,<br />

1.94ML InAs<br />

T=QD+2.0s,<br />

2.06ML InAs<br />

T=QD+4s,<br />

2.21ML InAs<br />

With thanks to Dr.Z. Wasilewski of NRC/IMS Epitaxy<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

12


A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

13


TMI bubbler c<strong>on</strong>figurati<strong>on</strong><br />

Carrier<br />

gas in<br />

0-1000 sccm<br />

Pusher<br />

Massflow c<strong>on</strong>trollers<br />

Flow in<br />

0-1000 sccm<br />

Minimum flow ~50 sccm<br />

Ξ ~0.1mL/s<br />

x<br />

x x<br />

To exhaust<br />

Pressure<br />

c<strong>on</strong>troller<br />

C<strong>on</strong>trol<br />

valves<br />

Organometallic<br />

Bubbler<br />

To<br />

reactor<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

14


Minimum InAs growth rate calibrati<strong>on</strong><br />

RADS:-<br />

5x 15sec TMI @ ~50sccm<br />

200sec TEG @ 190sccm<br />

T g ~ 500 o C<br />

GaAs – 353.9 Å – 1.77Å/s<br />

InAs – 3.81Å - ~0.254Å/s - ~0.083mL/s<br />

22sec ~ 1.84mL<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

15


Estimati<strong>on</strong> of InAs critical depositi<strong>on</strong> thickness<br />

Relative reflectance<br />

1.014<br />

1.012<br />

1.010<br />

1.008<br />

1.006<br />

1.004<br />

1.002<br />

1.000<br />

SI-GaAs - 0deg<br />

SI-GaAs - 2deg<br />

Critical<br />

depositi<strong>on</strong><br />

thickness<br />

~2+-0.22mL<br />

0 50 100 150 200 250 300<br />

Growth time [sec<strong>on</strong>ds]<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

16


Estimati<strong>on</strong> of 50%InGaAs critical depositi<strong>on</strong> thickness<br />

5.0 5.2 5.4 5.6 5.8 6.0 6.2 6.4 6.6 6.8 7.0 mL<br />

Relaxati<strong>on</strong> starts after ~5.8mL<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

17


Comparis<strong>on</strong> between 633nm and 950nm reflectance<br />

633nm 950nm<br />

5.0 5.2 5.4 5.6 5.8 6.0 6.2 6.4 6.6 6.8 7.0 mL 5.0 5.2 5.4 5.6 5.8 6.0 6.2 6.4 6.6 6.8 7.0 mL<br />

δR~1.2% δR~0.8%<br />

Reflectance changes are ~50% larger at 633nm as compared to 950nm<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

18


Surface dot growth test –<br />

Structure<br />

22 sec InAs<br />

Reflectance at 633nm<br />

Cooldown<br />

AFM scan<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

19


Buried dot growth test –<br />

Structure<br />

Photoluminesce<br />

532nm – 11mW<br />

22 sec InAs<br />

Reflectance at 633nm<br />

GaAs<br />

Surfscan<br />

10μm defects<br />

Plan View TEM<br />

500nm<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

20


Structure<br />

Indium-Flush to improve surface morphology - 2<br />

25 sec InAs ~2mL<br />

10nm GaAs<br />

Ramp to 620C<br />

25nm GaAs<br />

60 sec anneal<br />

Surfscan<br />

Reflectance at 633nm<br />

10nm GaAs<br />

25nm GaAs<br />

Plan View TEM<br />

500nm<br />

~1.5E9 dots/cm 2<br />

~22nm in size<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

21


Reflectance @ 633nm<br />

1.025<br />

1.020<br />

1.015<br />

1.010<br />

1.005<br />

1.000<br />

0.995<br />

0.990<br />

M1163 Reflectance @ 633nm<br />

Temperature (C)<br />

Reflectance @ 633nm<br />

640<br />

620<br />

600<br />

580<br />

560<br />

540<br />

0.985<br />

520<br />

0 50 100 150 200 250 300<br />

Time (sec<strong>on</strong>ds)<br />

500nm<br />

2.5mL InAs<br />

Increased InAs depositi<strong>on</strong><br />

Temperature ( o C)<br />

InAs ~2.5 and 3.0mL<br />

10nm GaAs<br />

Ramp to 620C<br />

25nm GaAs<br />

60 sec anneal<br />

1.025<br />

1.020<br />

1.015<br />

1.010<br />

1.005<br />

1.000<br />

0.995<br />

0.990<br />

~1.8E10/cm 2 ~3.2E10/cm 2<br />

Reflectance @ 633nm<br />

3.0mL InAs<br />

M1162 Reflectance @ 633nm<br />

Reflectance @ 633nm<br />

0.985<br />

520<br />

0 50 100 150 200 250 300<br />

Time (sec<strong>on</strong>ds)<br />

Temperature(oC)<br />

500nm<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

640<br />

620<br />

600<br />

580<br />

560<br />

540<br />

22<br />

Temperature ( o C)


50% InGaAs surface QD’s <strong>on</strong> vicinal substrates – AFM 1μm square<br />

0-deg - 6.6E10/cm2 2-deg – 8.4E10/cm2 5-deg – 9.6E10/cm2 10-deg – 1E11/cm2<br />

1075<br />

0.00 2.00 4.00 6.00 8.00 10.00<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

PL wavelength [nm]<br />

1275<br />

1250<br />

1225<br />

1200<br />

1175<br />

1150<br />

1125<br />

1100<br />

10 deg<br />

Arsine [sccm]<br />

0 Deg<br />

2 Deg<br />

5 Deg<br />

23


C<strong>on</strong>clusi<strong>on</strong>s:-<br />

�The <str<strong>on</strong>g>three</str<strong>on</strong>g> <str<strong>on</strong>g>head</str<strong>on</strong>g> reflectance unit enables precise growth rate<br />

and temperature uniformity measurements<br />

�Simple reflectance measurements can be used to<br />

m<strong>on</strong>itor the <strong>on</strong>set of relaxati<strong>on</strong> in quantum dot depositi<strong>on</strong><br />

�Shorter wavelengths are better – ~1.3% δR @ 633nm<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

24


Acknowledgements:-<br />

�For TEM analysis<br />

Dr. Xiaohua Wu – NRC/IMS*<br />

Mr.Guy Parent – NRC/IMS<br />

�For AFM analysis<br />

Ms.Sim<strong>on</strong>a Moisa – NRC/IMS<br />

�For financial support<br />

Canadian Phot<strong>on</strong>ics Fabricati<strong>on</strong> Centre<br />

CMC Micro<str<strong>on</strong>g>system</str<strong>on</strong>g>s<br />

*Nati<strong>on</strong>al Research Council of Canada/Institute for Microstructural Sciences<br />

A.J.SpringThorpe – <str<strong>on</strong>g>Laytec</str<strong>on</strong>g> seminar - Metz – June 2008<br />

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