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Semiconductor device characterization using
XPS and UPSCentre of Excellence in Nanoelectronics
Indian Institute of Technology, Bombay
04/18/2023 IIT Bombay 2
Introduction Data Processing List according to each Analysis Ultraviolet Photoelectron Spectroscopy XPS Applications in Semiconductor Devices
• MIS Contacts• MOSCAP structures
• MoS2 and MoS2-TiO2 structures
OUTLINE
04/18/2023 IIT Bombay 3
Introduction
X-ray Photoelectron Spectroscopy (XPS) is a surface-sensitive spectroscopic technique that is used to measure : elemental composition empirical formula chemical state and electronic state of the elements that
exist within a material
The Versa Probe is PHI’s second generation XPS based Multi-technique system. The unique strength of the system is its ability to image and analyze features as small as 10μm in diameter.
Model: PHI 5000 Versa Probe-II
04/18/2023 IIT Bombay 4
Data Processing List according to each Analysis
04/18/2023 IIT Bombay 5
Introduction Data Processing List according to each Analysis Ultraviolet Photoelectron Spectroscopy XPS Applications in Semiconductor Devices
• MIS Contacts• MOSCAP structures
• MoS2 and MoS2-TiO2 structures
OUTLINE
04/18/2023 IIT Bombay 6
Ultraviolet Photoelectron Spectroscopy (UPS)
If ultraviolet photons (rather than X-rays) are used, the technique is called Ultraviolet Photoelectron Spectroscopy (UPS).
Other than the photon source, instrumentation is identical to that of XPS.
The optional Ultraviolet photon source provides low energy photons for Valence Band and Fermi edge measurements.
Helium gas can be used to generate single and doubly ionized UV photon sources.
04/18/2023 IIT Bombay 7
Introduction Data Processing List according to each Analysis Ultraviolet Photoelectron Spectroscopy XPS Applications in Semiconductor Devices
• MIS Contacts• MOSCAP structures
• MoS2 and MoS2-TiO2 structures
• Al2O3 thin film• Nickel Silicide
OUTLINE
04/18/2023 IIT Bombay 8
XPS Applications in Semiconductor Devices
XPS was used for the study of Metal Insulator Semiconductor (MIS) contacts fabricated on low-doped bulk n-Ge substrates
n-Ge
YbTiO2
Au
• Depth Profile of the structure gives a plot of Atomic Concentration vs. Sputter Time• Presence of TiO2 is detected from the plot
TiO2
Ti2p scan after 35, 37, 39 min sputter times
After 35 min sputter (energy interval on x axis is 0.25 eV)
After 37 min sputter (energy interval on x axis is 0.1 eV)
After 35 min sputter (energy interval on x axis is 0.1 eV)
• Similar spectra seen at 3 different points in the depth profile• Spectral deconvolution shown on next slide
4504554604654704753000
3200
3400
3600
3800
4000
4200
Spectrum Ti(II)2p3/2 (454.41 eV)
Ti(IV) 2p3/2 Ti(II)2p1/2
Ti(III) 2p 1/2 Ti(IV) 2p1/2 (463.13)
Ti(III) 2p3/2 (458.27 eV)
Energy (eV)
Counts
• Different oxidation states of Ti • Presence of Ti(II), Ti(III) and Ti(IV) from this it is
concluded that it has oxygen deficient phase• The intensity of O1s peak at 532eV increases
suggests oxygen vacancies thus, oxygen deficient TiO2 has been formed at the interface.
5285305325345365380
0.2
0.4
0.6
0.8
1
1.2
Binding Energy (eV)
O1s bare TiO2
5285295305315325335345355365375380
0.2
0.4
0.6
0.8
1
1.2
Binding Energy (eV)
O1s interface TiO2
4504524544564584604624644664684700
0.2
0.4
0.6
0.8
1
1.2
Binding Energy (eV)
Ti2p bare TiO2
04/18/2023 IIT Bombay 11
Introduction Basic Theory of XPS XPS as a Surface Analysis Technique Data Processing List according to each Analysis Ultraviolet Photoelectron Spectroscopy XPS Applications in Semiconductor Devices
• MIS Contacts• MOSCAP structures
• MoS2 and MoS2-TiO2 structures
OUTLINE
04/18/2023 IIT Bombay 12
Inte
nsi
ty (a.u
.) O1s Al2O
3
526 528 530 532 534 536
O1s HfO2
Binding Energy (eV)
Inte
nsity (
a.u
.)
Inte
nsi
ty (a.u
.)
O1s HfAlO(Al=11.6%)
0
5
10
15
20
25
30
35
HfAlO(Al:Hf=1:2)
HfAlO(Al:Hf=2:1)
HfAlO(Al:Hf=3:3)
% A
l
HfO2
Recipe Used
529.8
530.0
530.2
530.4
530.6
530.8
531.0
HfO2
HfAlO(Al:Hf=1:2)
HfAlO(Al:Hf=3:3)
O1s
pea
k po
sitio
n(eV
) Al2O
3
HfAlO(Al:Hf=2:1)
Figure shows O1s peak position as function of Al%
Al% determination using XPS
XPS Applications in Semiconductor Devices (contd.)
XPS was used for the study of MOSCAP structures fabricated on Ge substrates
HfO2/HfAlO/Al2O3
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Shift in Hf4f peak after PDA of HfO2/GeO2/Ge indicating
formation of GeOHf
Effect of Post Deposition Anneal (PDA) on HfO2
0 5 10 15 200.0
0.2
0.4
0.6
0.8
1.0
Inte
nsity
(A.U
.)
Time (min)
Hf4f without PDA Hf4f with PDA O1s without PDA O1s with PDA Ge3d without PDA Ge3d with PDA
HfO2 Ge
substrate
13 14 15 16 17 18 19 20 21 22 23
0.31eVInte
nsi
ty (a.
u.)
Binding Energy (eV)
Hf4f withPDA Hf4f without PDA
Depth profile of HfO2/GeO2/Ge indicating GeO2 growth and formation of GeOHf,
XPS Applications in Semiconductor Devices (contd.)
04/18/2023 IIT Bombay 14
Introduction Basic Theory of XPS XPS as a Surface Analysis Technique Data Processing List according to each Analysis Ultraviolet Photoelectron Spectroscopy XPS Applications in Semiconductor Devices
• MIS Contacts• MOSCAP structures
• MoS2 and MoS2-TiO2 structures
OUTLINE
Mo-3d and S-2p core level shifts to higher binding energy from MoS2 to TiO2–MoS2 confirms charge transfer at the interface.
XPS Applications in Semiconductor Devices (contd.)
XPS was used to study MoS2 and TiO2-MoS2 structures
10 5 0 -50
2M
4M
6M
8M
Coun
ts (a
.u.)
Binding Energy(eV)
MoS2
TiO2-MoS
2
12.0 11.6 11.2 10.8
11.9
MoS2
TiO2-MoS
2
11.6
He I-UPS measurements of TiO2–MoS2 and MoS2 show a reduction in work-function (0.3 eV) using TiO2 as an interlayer
XPS Applications in Semiconductor Devices (contd.)
UPS was used to study MoS2 and TiO2-MoS2 structures
-2 0 2 4 6 8 10121416182022
0
20
40
60
80
100
Ato
mic
concentr
ation (%
)
Sputter time (min)
Al2p si2p c1s N1s O1s
-2 0 2 4 6 8 10 12 14 16
0
20
40
60
80
100
Ato
mic
perc
enta
ge (%
)
Sputter time (min)
Al2p si2p c1s N1s O1s
Figure 1(a) and 1(b) shows atomic concentration of spray coated Al2O3
film after furnace annealing of 400 o C and 850o C respectiely in O2 ambient
Depth profile of Al2O3 thin film by XPS
XPS Analysis of Al2O3 thin film
Chemical and interface properties of Al2O3 film is studied with the help of X-
ray photoelectron spectroscopy (XPS) depth profile analysis and the results are shown in the figure .
XPS analysis shows presence of SiOx interfacial layer after furnace annealing and the thickness of SiOx interfacial layer increases as the annealing temperature increases. Si and O are interdiffused which indicates presences of SiOx. The Length of inter diffused region is more for high temp anneal.
The carbon and nitrogen content is almost zero throughout the sample. The carbon signal at the surface is attributed to unavoidable inclusion of
carbon from XPS instrument.
The Atomic percentage of chemical components present in the film indicates that the Al2O3 film is almost stoichiometric in nature
NiSi on Si
• NiSi is formed by deposition of Ni on Si and by thermal annealing at the temperature of 500 0C, for 60 sec.
• The formation of NiSi can be realised by the metal diffusion through semiconductor at that elevated temperature
Ni
Si
Nickel silicide
Si
The depth profile of the nickel silicide(NiSi) is shown in the figure.
The sputter rate was used to be 2.5 nm/ cycle
The inset shows the Ni/Si ratio of the thin film. Which indicates that Ni/Si ~ 1 till 27 nm. This observation indicates that the NiSi film is uniform till 27 nm.
The thickness was confirmed by cross-sectional SEM.
Ref:S. Roy, K. Midya, S. P. Duttagupta, and D. Ramakrishnan; Nano-scale NiSi and n-type silicon based Schottky Barrier diode as a near infra-red detector for room temperature operation; J. Appl. Phys. 116, 124507 (2014).
Depth Profile of NiSi/n-Si
Si and O are interdiffused which indicates presences of SiOx. the Length of inter diffused region is more for high temp anneal.
Reduction of Langmuir-Blodgett Graphene Oxide monolayer sheets
• Thickness of as-transferred GO monolayer sheets obtained by AFM height profile was found to be ~1 nm
In the de-convoluted C-1s core level spectra
C-1s core level
Peaks at 284.5 eV and 285.4 eV are, respectively, assigned to sp2-C (graphitic) and the damaged alternant hydrocarbon structure/sp3-C, while the component at 289.7 eV is attributed to the π–π* shake up satellite of the 284.5 eV peak.
The peaks at 286.3 eV, 287.2 eV, and 288.4 eV are, respectively, attributed to oxygen functionalities, namely, C–O, C=O, and COOH
Gulbagh Singh, V. D. Botcha, D. S. Sutar, S.S. Talwar, R.S. Srinivasa and S.S. Major, “Highly reduced graphene oxide monolayer sheets” (Under Review Under Review in Carbon).
04/18/2023 IIT Bombay 22
Conclusion
Survey Spectra of XPS helps us to detect the element present on the surface of a material The composition of the detected element can be calculated from the Narrow Spectra Sputtering is used to analyze the composition of Depth Profiles Angle Resolved XPS enables us to analyze the depth profiles at various angles Scanning X-ray Imaging (SXI) for secondary electron, images all conducting and insulating samples UPS can be used for work-function, valence band and Fermi edge measurements
Si and O are interdiffused which indicates presences of SiOx. the Length of inter diffused region is more for high temp anneal.
04/18/2023 IIT Bombay 23
Thank You !