• Title/Summary/Keyword: LaserFIB

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The LaserFIB: new application opportunities combining a high-performance FIB-SEM with femtosecond laser processing in an integrated second chamber

  • Ben Tordoff;Cheryl Hartfield;Andrew J. Holwell;Stephan Hiller;Marcus Kaestner;Stephen Kelly;Jaehan Lee;Sascha Muller;Fabian Perez-Willard;Tobias Volkenandt;Robin White;Thomas Rodgers
    • Applied Microscopy
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    • v.50
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    • pp.24.1-24.11
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    • 2020
  • The development of the femtosecond laser (fs laser) with its ability to provide extremely rapid athermal ablation of materials has initiated a renaissance in materials science. Sample milling rates for the fs laser are orders of magnitude greater than that of traditional focused ion beam (FIB) sources currently used. In combination with minimal surface post-processing requirements, this technology is proving to be a game changer for materials research. The development of a femtosecond laser attached to a focused ion beam scanning electron microscope (LaserFIB) enables numerous new capabilities, including access to deeply buried structures as well as the production of extremely large trenches, cross sections, pillars and TEM H-bars, all while preserving microstructure and avoiding or reducing FIB polishing. Several high impact applications are now possible due to this technology in the fields of crystallography, electronics, mechanical engineering, battery research and materials sample preparation. This review article summarizes the current opportunities for this new technology focusing on the materials science megatrends of engineering materials, energy materials and electronics.

Nano Scale Compositional Analysis by Atom Probe Tomography: II. Applications on Electronic Devices and Nano Materials (Atom Probe Tomography를 이용한 나노 스케일의 조성분석: II. 전자소자 및 나노재료에서의 응용)

  • Jung, Woo-Young;Bang, Chan-Woo;Jang, Dong-Hyun;Gu, Gil-Ho;Park, Chan-Gyung
    • Applied Microscopy
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    • v.41 no.2
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    • pp.89-98
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    • 2011
  • Atom Probe Tomography (APT) can provide 3-dimensional information such as position and chemical composition with atomic resolution. Despite the ability of this technique, APT could not be applied for poor conductive materials such as semiconductor. Recently APT has dramatically developed by applying the laser pulsing and combining with Focused Ion Beam (FIB). The invention and combination of these techniques make possible site-specific sample preparation and permit the investigation of various materials including insulators. In this paper, we introduced the recently achieved state of the art applications of APT focusing on Si based FET devices, LED devices, low dimensional materials.

Microstructure and electrical properties of high power laser thermal annealing on inkjet printed Ag films

  • Yoon, Yo-Han;Yi, Seol-Min;Yim, Jung-Ryoul;Lee, Ji-Hoon;Joo, Young-Chang
    • Proceedings of the Materials Research Society of Korea Conference
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    • 2009.05a
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    • pp.36.2-36.2
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    • 2009
  • In this work, the high power CW Nd:YAG laser has been used for thermal treatment of inkjet printed Ag films-involving eliminating organic additives (dispersant, binder, and organic solvent) of Ag ink and annealing Ag nanoparticles. By optimizing laser parameters, such as laser power and defocusing value, the laser energy can totally be converted to heat energy, which is used to thermal treatment of inkjet printed Ag films. This results in controlling the microstructures and the resistivity of films. We investigated the thermal diffusion mechanisms during laser annealing and the resulting microstructures. The impact of high power laser annealing on microstructures and electrical characteristic of inkjet printed Ag films is compared to those of the films annealed by a conventional furnace annealing. Focused ion beam (FIB) channeling image shows that the laser annealed Ag films have large columnar grains and dense structure (void free), while furnace annealed films have tiny grains and exhibit void formation. Due to these microstructural characteristics of laser annealed films, it has better electrical property (low resistivity) compared to furnace annealed samples.

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Nature of Surface and Bulk Defects Induced by Epitaxial Growth in Epitaxial Layer Transfer Wafers

  • Kim, Suk-Goo;Park, Jea-Gun;Paik, Un-Gyu
    • Transactions on Electrical and Electronic Materials
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    • v.5 no.4
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    • pp.143-147
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    • 2004
  • Surface defects and bulk defects on SOI wafers are studied. Two new metrologies have been proposed to characterize surface and bulk defects in epitaxial layer transfer (ELTRAN) wafers. They included the following: i) laser scattering particle counter and coordinated atomic force microscopy (AFM) and Cu-decoration for defect isolation and ii) cross-sectional transmission electron microscope (TEM) foil preparation using focused ion beam (FIB) and TEM investigation for defect morphology observation. The size of defect is 7.29 urn by AFM analysis, the density of defect is 0.36 /cm$^2$ at as-direct surface oxide defect (DSOD), 2.52 /cm$^2$ at ox-DSOD. A hole was formed locally without either the silicon or the buried oxide layer (Square Defect) in surface defect. Most of surface defects in ELTRAN wafers originate from particle on the porous silicon.

An investigation on dicing 28-nm node Cu/low-k wafer with a Picosecond Pulse Laser

  • Hsu, Hsiang-Chen;Chu, Li-Ming;Liu, Baojun;Fu, Chih-Chiang
    • Journal of the Microelectronics and Packaging Society
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    • v.21 no.4
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    • pp.63-68
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    • 2014
  • For a nanoscale Cu/low-k wafer, inter-layer dielectric (ILD) and metal layers peelings, cracks, chipping, and delamination are the most common dicing defects by traditional diamond blade saw process. Sidewall void in sawing street is one of the key factors to bring about cracks and chipping. The aim of this research is to evaluate laser grooving & mechanical sawing parameters to eliminate sidewall void and avoid top-side chipping as well as peeling. An ultra-fast pico-second (ps) laser is applied to groove/singulate the 28-nanometer node wafer with Cu/low-k dielectric. A series of comprehensive parametric study on the recipes of input laser power, repetition rate, grooving speed, defocus amount and street index has been conducted to improve the quality of dicing process. The effects of the laser kerf geometry, grooving edge quality and defects are evaluated by using scanning electron microscopy (SEM) and focused ion beam (FIB). Experimental results have shown that the laser grooving technique is capable to improve the quality and yield issues on Cu/low-k wafer dicing process.

Secondary Electron Emission of ZnO Films

  • Choi, Jinsung;Lee, Sung Kwang;Choi, Joon Ho;Choi, Eun Ha;Jung, Ranju;Kim, Yunki
    • Applied Science and Convergence Technology
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    • v.24 no.6
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    • pp.273-277
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    • 2015
  • We investigated secondary electron emission characteristics of ZnO thin films prepared by pulsed laser deposition method with respect to the ambient oxygen pressure and the substrate temperature during the deposition. X-ray diffraction, UV-Vis spectrometry, atomic force microscopy, and ${\gamma}$-FIB were used to examine the structural, optical transmission, surface morphology, and secondary electron emission properties of the films, respectively. The secondary electron emission coefficient of the ZnO films increases as the O/Zn ratio of the films increases which was thought to result from either the ambient oxygen pressure increase or the substrate temperature decrease and as the grain size of the films decreases. It was confirmed that ZnO has better secondary electron emission characteristics than those of MgO, which is currently widely used as a material for PDP protecting layers.

Transmission Grating Formation in High Refractive-index Amorphous Thin Films Using Focused-Ion-Beam Lithography (접속이온빔 리소그라피를 이용한 고굴절 비정질 박막 투과 격자 형성)

  • Shin, Kyung;Kim, Jin-Woo;Park, Jeong-Il;Lee, Hyun-Yong;Lee, Young-Jong;Chung, Hong-Bay
    • The Transactions of the Korean Institute of Electrical Engineers C
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    • v.50 no.1
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    • pp.6-10
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    • 2001
  • In this study, we investigated the optical properties of sub-wavelength a-Si thin film transmission gratings, especially the polarization effect, the phase difference and the birefringence by using linearly polarized He-Ne laser beam (632.8nm). The a-Si transmission grating of the thickness $of < 0.1 \mum$ with four-type period($\Lambda = 0.4 \mum and 0.6 \mum$ for sub-wavelength and $\Lambda = 1.0 \mum and 1.4 \mum$ for above-wavelength) on quartz substrates have been fabricated using 50 KeV Ga+ Focused-Ion-Beam(FIB) Milling and $CF_4$Reactive-Ion-Etching(RIE) method. Finally, we obtained the trating array of a-Si thin film with a period $0.4 \mum, 0.6 \mum, 1.0 \mum, 1.4 \mum$ which have nearly equal finger spacing and width, sucessfully. Especially, for gratings with $\Lambda = 0.6 \mum(linewidth=0.25 \mum, linespace=0.35\mum), the \etamax at \theta_в=17.0^{\circ}$ is estimated to be 96%. As the results, we believe that the sub-wavelength grating arrayed a-Si thin film has the applicability as the optical device and components.

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Nano-size Patterning with a High Transmission C-shaped Aperture (고 투과 C 형 개구를 이용한 나노 크기 패턴 구현)

  • Park, Sin-Jeung;Kim, Yong-Woo;Lee, Eung-Man;Hahn, Jae-Won
    • Journal of the Korean Society for Precision Engineering
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    • v.24 no.11
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    • pp.108-115
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    • 2007
  • We have designed a high transmission C-shaped aperture using finite differential time domain (FDTD) technique. The C-shaped aperture was fabricated in the aluminum thin film on a glass substrate using a focused ion beam (FIB) milling. Nano-size patterning was demonstrated with a vacuum contact device to keep tight contact between the Al mask and the photoresist. Using 405 nm laser, we recorded a 50 nm-size dot pattern on the photoresist with the aperture and analyzed the spot size dependent on the dose illuminated on the aperture.

Fault Analysis of Semiconductor Device (반도체 장치의 결함해석)

  • Park, S.J.;Choi, S.B.;Oh, C.S.
    • Journal of Energy Engineering
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    • v.25 no.1
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    • pp.192-197
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    • 2016
  • We have surveyed on technical method of fault analysis of semiconductor device. Fault analysis of semiconductor should first be found the places of fault spots. For this process they are generally used the testers; EB(emission beam tester), EM(emission microscope), OBIRCH(optical beam induced resistance change method) and LVP(laser voltage probing) etc. Therefore we have described about physical interpretation and technical method in using scanning electron microscope, transmission electron microscope, focused ion beam tester and Nano prober.

Characteristics of Polarization and Birefringence for Submicron a-Ge Thin Film on Quartz Substrate Formed by Focused-Ion-Beam (석영 기판 위에 집속 이온빔 기술에 의해 형성된 비정질 게르마늄 박막 미세 패턴의 편광 및 복굴절 특성)

  • Shin, Kyung;Ki, Jin-Woo;Park, Chung-Il;Lee, Hyun-Yong;Chung, Hong-Bay
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 1999.05a
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    • pp.617-620
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    • 1999
  • In this study, the polarization e(fecal and the birefringence effect of amorphous germanium (a-Ge) thin films were investigated by using linearly polarized He-Ne laser beam. The a-7e thin films were deposited on the quarts substrate by plasma enhanced chemical vapor deposition (PECVD) and thermal vacuum evaporation In order to obtain the optimum grating arrays, inorganci resists such as Si$_3$N$_4$ and a-Se$_{75}$ Ge$_{25}$ , were prepared with the optimized thickness by Monte Carlo (MC) simulation. As the results of MC simulation, the thickness ofa-Se$_{75}$ Ge$_{25}$ resist was determined with Z$_{min}$ of 360$\AA$ . The resists were exposed to Ga$^{+}$-FIB with accelerating energies of 50 keV, developed by wet etching, and a-Ge thin film was etched by reactive ion-etching (RIE). Finally, we were obtained grating arrays which grating width and linewidth are 0.8${\mu}{\textrm}{m}$, respectively and we studied the polarization and birefringence effect in transmission grating array made of high refractive amorphous material, and the applicability as waveplates and polarizers in optical device.e.e.

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