Silicon Surface Characterization · L'H, Y., Mireles, L. K. X-ray photoelectron spectroscopy (XPS)...
Transcript of Silicon Surface Characterization · L'H, Y., Mireles, L. K. X-ray photoelectron spectroscopy (XPS)...
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Allen Puente-Urbina and Lukas Schlemper
06.11.2018 1
Silicon Surface Characterization
Allen Puente-Urbina and Lukas Schlemper
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Outline
Introductory remarks
▪ General aspects of:
▪ Integrated circuits (IC) and packaging
▪ 3D stacking using through silicon vias (vertical interconnect access) (TSV)
Characterization of silicon wafers
▪ Composition, physical and mechanical properties:
▪ Composition of different parts
▪ Topology
▪ Mechanical strain
Conclusions
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Integrated circuits (IC)
Electronic circuit formed on a small piece of semiconducting material
Performs the same function as a larger circuit made from discrete
components
Trend:
▪ Increase integration to improve capabilities
▪ Increase performance (e.g. electrical and thermal)
▪ Decrease size
▪ Decrease costs
▪ …
Knickerbocker, J. U., Andry, P. S., Dang, B., Horton, R. R., Interrante, M. J., Patel, C. S., Polastre, R. J.,
Sakuma, K., Sirdeshmukh, R., Sprogis, E. J. Sri-Jayantha, S. M. IBM J. Res. Dev., 2008, 52, 553-569.
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3D stacking using through silicon vias (TSV)
Vias: vertical interconnect access
TSV
TSV
Wolverton, M. Stressing out copper TSVs with temperature, Phys.org, 2014.
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TSV fabrication
Zhang, Y., Ding, G., Wang, H., Cheng, P., Liu, R. J. Micromech. Microeng., 2015, 25, 045009.
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Characterization of 3D devices
Composition
Surface
Anti-diffusion layer
TSV additives
Physical and mechanical
Surface topology
Wafer-to-wafer interconnects
Stress
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Surface analysis
Inkson, B. J. Scanning electron microscopy (SEM) and transmission electron microscopy (TEM) for
materials characterization. In Materials characterization using nondestructive evaluation (NDE) methods,
Elsevier, 2016.
L'H, Y., Mireles, L. K. X-ray photoelectron spectroscopy (XPS) and time-of-flight secondary ion mass
spectrometry (ToF SIMS). In Characterization of Polymeric Biomaterials, Elsevier, 2017.
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Surface analysis
06.11.2018Allen Puente-Urbina and Lukas Schlemper 8
Inkson, B. J. Scanning electron microscopy (SEM) and transmission electron microscopy (TEM) for
materials characterization. In Materials characterization using nondestructive evaluation (NDE) methods,
Elsevier, 2016.
Secondary electrons
▪ Topography
Back-scattered eletrons
▪ Contrast for different elements
X-rays
▪ Elemental analysis
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Localized analyses
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To reach specific locations:
▪ Chemical etching
▪ Gas etching
▪ Plasma etching
▪ Ion etching
Quirk, M., Serda, J. Semiconductor manufacturing technology (Vol. 1), Prentice Hall, 2001.
Rigort, A., Plitzko, J. M. Arch. Biochem. Biophys., 2015, 581, 122-130.
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Localized analyses
06.11.2018Allen Puente-Urbina and Lukas Schlemper 10Okoro, C., Levine, L. E., Xu, R., Hummler, K., Obeng, Y. J. Appl. Phys., 2014, 115, 243509.
Anti-diffusion
layer
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Elemental analysis
06.11.2018Allen Puente-Urbina and Lukas Schlemper 11
Inkson, B. J. Scanning electron microscopy (SEM) and transmission electron microscopy (TEM) for
materials characterization. In Materials characterization using nondestructive evaluation (NDE) methods,
Elsevier, 2016.
Two types of detection:
▪ Energy dispersive X-ray spectroscopy
(EDS)
▪ Wave dispersive X-ray spectroscopy
(WDS)
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Elemental analysis: EDS and WDS
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Williams, D. B., Carter, C. B. Transmission electron microscopy: A textbook for materials science, Springer,
2009.
Henry, D., Goodge, J. Wavelength-dispersive X-ray spectroscopy (WDS). Science Education Resource
Center at Carleton College, serc.carleton.edu, 2018.
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Elemental analysis: XPS
06.11.2018Allen Puente-Urbina and Lukas Schlemper 13Vickerman, J. C., Gilmore, I. S., Surface analysis – The principal techniques, 2nd Edition, Wiley, 2009.
EB = hν – Ekin – ϕ
▪ EB: binding energy
▪ hν : X-rays energy
▪ Ekin: kinetic energy
▪ ϕ: work function (depends on both
the spectrometer and the material)
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Surface profile
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Lee, D. H., Cho, N. G. Meas. Sci. Technol., 2012, 23, 105601.
Cross, S. E., Kreth, J., Wali, R. P., Sullivan, R., Shi, W., Gimzewski, J. K. Dent. Mater., 2009, 25, 1517-
1526.
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▪ Real-time CTE analysis
▪ k: stress vs temperature slope
▪ α: CTE of the compounds
▪ Mf: biaxial modulus
▪ Elemental Analysis
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Annealing process
Kiene, M., Morgen, M., Zhao, J.-H., Hu, C., Cho, T., Ho, P. S. Characterization of low-dielectric constant
materials. In Handbook of silicon semiconductor metrology, CRC Press, 2001.
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Elemental Analysis
Stable Isotope Laboratory. Elemental analysis principles. Earth and Planetary Sciences, University of
California Santa Cruz, websites.pmc.ucsc.edu, 2018.
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▪ Two practical methods
▪ Raman-spectroscopy
▪ X-Ray diffraction
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Strain measurements
Bianco, F., Fedus, K., Enrichi, F., Pierobon, R., Cazzanelli, M., Ghulinyan, M., Pucker, G. and Pavesi,
L. Semicond. Sci. Tech., 2012, 27, p.085009.
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Raman measurement
▪ Basics:
▪ Si: 514-520 nm
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Bianco, F., Fedus, K., Enrichi, F., Pierobon, R., Cazzanelli, M., Ghulinyan, M., Pucker, G. and Pavesi,
L. Semicond. Sci. Tech., 2012, 27, p.085009.
Spolenak, R., Wyss, A., Wermelinger, T., Süess, M. Raman spectroscopy for stress analysis. Raman
Workshop 2018, ETH Zurich.
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Raman measurement: Temperature
▪ Ratio Stokes : Anti-Stokes
▪ 𝐼𝐴𝑛𝑡𝑖 − 𝑆𝑡𝑜𝑘𝑒𝑠 = 𝐼𝑆𝑡𝑜𝑘𝑒𝑠 exp(−ħ𝜔
𝑘𝑇)
▪ Thermal expansion:
▪ Shift to lower wavenumbers
▪ Allows for temperature measurement
Bianco, F., Fedus, K., Enrichi, F., Pierobon, R., Cazzanelli, M., Ghulinyan, M., Pucker, G. and Pavesi,
L. Semicond. Sci. Tech., 2012, 27, p.085009.
Spolenak, R., Wyss, A., Wermelinger, T., Süess, M. Raman spectroscopy for stress analysis. Raman
Workshop 2018, ETH Zurich.
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▪ Signal intensity:
▪ 𝑒𝑠 : electrical field of scattered light
▪ ∆𝜇: Raman tensor
▪ 𝑒𝑖 : electrical field of incident light
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Raman measurement: Stress I
Bianco, F., Fedus, K., Enrichi, F., Pierobon, R., Cazzanelli, M., Ghulinyan, M., Pucker, G. and Pavesi,
L. Semicond. Sci. Tech., 2012, 27, p.085009.
Spolenak, R., Wyss, A., Wermelinger, T., Süess, M. Raman spectroscopy for stress analysis. Raman
Workshop 2018, ETH Zurich.
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▪ Allows measurement of uniaxial stress along the z’-axis:
▪ Combination of the measurements:
▪ p, q, r: phonon deformation potentials (PDP)
▪ εij: strain tensor components
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Raman measurement: Stress II
Bianco, F., Fedus, K., Enrichi, F., Pierobon, R., Cazzanelli, M., Ghulinyan, M., Pucker, G. and Pavesi,
L. Semicond. Sci. Tech., 2012, 27, p.085009.
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▪ Only 𝜔3 can be calculated:
▪ εij = sii σii
▪ Additional polarization can be used to measure the other axis
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Raman measurement: Stress III
Bianco, F., Fedus, K., Enrichi, F., Pierobon, R., Cazzanelli, M., Ghulinyan, M., Pucker, G. and Pavesi,
L. Semicond. Sci. Tech., 2012, 27, p.085009.
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▪ Local stress measurement:
▪ Focal point of the exciting laser
▪ Depth information
▪ Resolution: ca. 0.5 μm
▪ Min. detectable stress: 25 MPa
▪ Penetration depth: ca. 770 nm
▪ Use repeatedly to map
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Raman measurement: Stress IV
Spolenak, R., Wyss, A., Wermelinger, T., Süess, M. Raman spectroscopy for stress analysis. Raman
Workshop 2018, ETH Zurich.
Bianco, F., Fedus, K., Enrichi, F., Pierobon, R., Cazzanelli, M., Ghulinyan, M., Pucker, G. and Pavesi,
L. Semicond. Sci. Tech., 2012, 27, p.085009.
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X-Ray diffraction
▪ Similar to Raman measurements:
▪ Change in lattice parameters
▪ Fit on new peaks
▪ Gaussian: stress
▪ Lorentzian: grain size
▪ Resolution is not sufficient
▪ Relaxation
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Lippert, T. Characterisation of thin films. Functional Inorganics Course 2018, ETH Zurich.
Bowen, D. K., Tanner, B. K. X-ray metrology in semiconductor manufacturing, CRC Press, 2006.
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Measuring the joints
▪ Small-angle X-ray Scattering
▪ SAXS
▪ Depth analysis
▪ Penetration depth
▪ Scattering is element dependant atomic scattering factor
▪ Problem:
▪ Separate the weak, scattered beam
▪ Use collimation:
▪ Point-collimation: 2D restriction
▪ Line-collimation: 1D restriction
▪ Not quite suitable
Roessle, M. Basics of X-ray scattering. EMBO Course 2012, Luebeck University of Applied Science.
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Measuring the joints
▪ Second X-ray approach
▪ Sources: Ir-192, Co-60, Cs-137
▪ Shine through
▪ Scattering according to atoms
Hogan, H., Aviation Aftermarket Defense, 2015, 35.
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Conclusions
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▪ A comprehensive analysis of three-dimensional chips requires different
techniques with specific capabilities
▪ It is important to consider techniques with characteristics that allow the
determination of the parameters of interest
▪ The level of development and availability of an analytical technique influence its
application
Thank you!