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Dive into the research topics where Shom Ponoth is active.

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Featured researches published by Shom Ponoth.


Journal of Applied Physics | 2002

Processing dependent thermal conductivity of nanoporous silica xerogel films

Anurag Jain; Svetlana Rogojevic; Shom Ponoth; William N. Gill; Joel L. Plawsky; Eva E. Simonyi; Shyng-Tsong Chen; Paul S. Ho

Sintered xerogel films (porous SiO2) show a much higher thermal conductivity than other low dielectric constant (low-K) materials available for the same value of K. The thermal conductivity of xerogels which we have processed using different methods is compared with that of other low-K materials such as silica hybrid (silsesquioxanes) and polymeric low-K materials. The methods used were: (1) single solvent (ethanol) method, (2) binary solvent (mixture of ethanol and ethylene glycol) method, (3) sintering. For the xerogel films, we show that process history is as important as the chemistry of the solid matrix or the porosity in determining the thermal conductivity. The thermal conductivity, measured by the 3-ω method or the photothermal deflection method, is affected by phonon scattering, which in turn is effected by the size and distribution of pores and particles and the presence of imperfections such as interfaces, substituted chemical species, impurities, microcracks, and microporosity. The thermal con...


Journal of Vacuum Science and Technology | 2002

Optimized oxygen plasma etching of polyimide films for low loss optical waveguides

N. Agarwal; Shom Ponoth; Joel L. Plawsky; P. D. Persans

Sidewall roughness in waveguides is one of the consequences of a reactive ion etch (RIE) step. Sidewall roughness increases scattering losses and can impediment the scaling of waveguide dimensions to on-chip levels. This article presents results from our experiments on the study of optimal RIE conditions to minimize roughness on waveguide sidewalls. Roughness in planar polyimide films was studied for different plasma etch conditions to obtain an understanding of how roughness evolves. Pressure was found to be the dominant factor affecting interface roughness. RIE done at lower pressures was found to increase the roughness on the film surface. We propose that the roughness produced depends on the angle of incidence of the etchant species with respect to the surface the more obliquely the etchant species were incident on the surface, the lower was the roughness produced. Roughness produced on waveguide sidewalls was studied by measuring their propagation loss. For sidewalls, lower pressure RIE resulted in s...


Applied Physics Letters | 2001

Roughness evolution in polyimide films during plasma etching

N. Agarwal; Shom Ponoth; Joel L. Plawsky; P. D. Persans

We report an experimental study on the evolution of etch front roughness in fluorinated polyimide films in oxygen based plasmas. For standard low-pressure (40 mT) etching conditions, the root-mean-square roughness, w, of the polymer surface increases with the amount of material etched, d, as w=0.0265(d−116)β with β=1, independent of etch rate, rf power, and gas composition. The etched surfaces can be described by the statistics of self-affine surfaces with scaling exponent, α=0.6±0.1 and lateral correlation length, ξ, of ∼0.3 μm. A dramatic reduction in roughness is observed under higher pressure etching conditions of 1000–2000 mT.


Journal of Vacuum Science & Technology B | 2003

Fabrication of controlled sidewall angles in thin films using isotropic etches

Shom Ponoth; N. Agarwal; P. D. Persans; Joel L. Plawsky

Angular structures in thin films have applications in microelectronics and optoelectronics. In this study we analyze isotropic etching of a two-layer system for the fabrication of angular sidewalls. Such a process is attractive because of its bulk processing capability. The isotropic etch process is demonstrated to provide good control of the sidewall angle. Theoretical analysis along with numerical simulation of the slope etching process is used to understand profile evolution. The numerical simulations showed that to obtain a flat angular sidewall face, reaction controlled etching is needed. Angular sidewalls are fabricated in plasma enhanced chemical vapor deposition (PECVD) silicon oxide with PECVD silicon nitride as the sacrificial layer using an isotropic, buffered hydrofluoric acid based, wet chemical etch. PECVD silicon nitride is shown to be a good material for use as the sacrificial layer because of its etch rate controllability through deposition conditions. Controlled angles ranging from 5° to...


Applications of Photonic Technology 6 | 2003

Siloxane-based polymer epoxies for optical waveguides

Shom Ponoth; P. D. Persans; Ram Ghoshal; N. Agarwal; Joel L. Plawsky; A. I. Filin; Q. Z. Fang

We introduce a new class of siloxane-based epoxy polymers for thin film optical waveguide applications. The thickness of spun-on films can be controlled by varying either spin speed or viscosity using solvents. Cured films exhibit excellent adhesion to silicon oxide and Al and excellent thermal and chemical stability. Waveguides of ~2 micron thickness on silicon oxide exhibit <0.2dB/cm loss at 830 nm. We demonstrate the formation of a 45° vertical mirror using reactive ion etching slope transfer from photoresist to epoxy polymer film.


international interconnect technology conference | 2002

Optical waveguides with embedded air-gap cladding integrated within a sea-of-leads (SoL) wafer-level package

Anthony V. Mule; Muhannad S. Bakir; Joseph Paul Jayachandran; Ricardo A. Villalaz; Hollie A. Reed; N. Agrawal; Shom Ponoth; Joel L. Plawsky; P. D. Persans; Paul A. Kohl; Kevin P. Martin; Elias N. Glytsis; Thomas K. Gaylord; James D. Meindl

Optical waveguides are integrated into a Sea-of-Leads (SoL) wafer-level package. A photosensitive polycarbonate composite is incorporated to provide a buried air-gap cladding that allows a refractive index contrast, /spl Delta/n, between waveguide core and cladding regions of /spl Delta/n = 0.52. The final package contains 1000 electrical input/output (I/O) interconnects and 32 large-area optical waveguides for electrical chip-to-chip and optical intra-chip clock or data interconnection, respectively. Monolithic fabrication of passive optical interconnect components is described.


MRS Proceedings | 1999

Optical Properties of a Polyimide for Waveguide Applications in On-Chip Interconnects

N. Agarwal; X. Huang; P. D. Persans; Joel L. Plawsky; Shom Ponoth; Xiang Zhang; S. P. Murarka

In this work. we report on characterization methods and the optical properties of a polyimide (Ultradel 9020D). The prism coupling technique was used to couple light into polyimide thin films. The scattered light from the surface was imaged to determine the optical loss at different wavelengths. The coupling angle was used to find the refractive index of the films. The stability of the polymer in terms of refractive index and absorption losses was studied by heat treatment under nitrogen at elevated temperatures. No significant change was observed in the properties of the film at annealing temperatures below 200°C. The bulk and surface losses were separated and it was found that the waveguide losses were dominated by bulk losses. Temperature stability of the polymer was evaluated by annealing the polymer at 125°C for up to 30 hours. No significant changes were seen in the optical losses for these times.


Journal of Vacuum Science & Technology B | 2004

Plasma silicon oxide–silica xerogel based planar optical waveguides

Shom Ponoth; N. Agarwal; P. D. Persans; Joel L. Plawsky

In this study, silica xerogels are used as the cladding for high-refractive-index-contrast waveguide systems. Silicon oxide, due to its relatively low refractive index, is an extensively used cladding material. The lower-refractive-index silica xerogel films enable us, to report losses for planar-slab waveguide systems with silicon oxide as the core. A spin-on sol-gel process was used for the silica xerogel deposition. The silicon oxide core was deposited using plasma enhanced chemical vapor deposition (PECVD), with silane and nitrous oxide as the reactive gases. Slab waveguides systems with core thickness of 1 μm and refractive-index contrast (Δn) as high as 0.35 were fabricated. With regard to the PECVD process, a deposition temperature of 150 °C enabled a stable structure, however, unacceptably high optical losses of 7±1.01 dB/cm at a wavelength of 650 nm and 5.59±0.69 dB/cm at 830 nm were measured using a prism-coupler based setup. On increasing the deposition temperature of the silicon–oxide film to ...


Interlayer Dielectrics for Semiconductor Technologies | 2003

Dielectric materials in optical waveguide aplications

P.D. Persans; F. Huang; N. Agarwal; Shom Ponoth; Joel L. Plawsky

Publisher Summary This chapter summarizes optical waveguide applications of dielectric materials. It discusses the general considerations, including a review of various waveguide applications and desirable specifications of optical waveguide devices. The general characteristics of inorganic and organic dielectric materials are also reviewed. The chapter also reviews the literature on specific organic and inorganic materials, including the information on both fundamental limitations and demonstrated applications.


MRS Proceedings | 2002

Silicon CMOS BEOL Compatible Optical Waveguide Micro-mirrors

Shom Ponoth; N. Agarwal; P. D. Persans; Joel L. Plawsky

Optical waveguides are being explored for on-chip purposes to overcome the speed limitations of electrical interconnects. Passive optical components like waveguides and vertical outcouplers are important components in such schemes. In this study we fabricate planar waveguides with integrated vertical micro-mirrors using standard Back End of the Line silicon (BEOL) CMOS based processes. Around 1.6 μm of a hybrid alkoxy siloxane polymer with a refractive index of ∼ 1.50 at the intended wavelength of 830 nm is used as the core and plasma deposited silicon oxide with a refractive index of ∼ 1.46 is used as the cladding. The angular face in the polymer waveguide that would function as the mirror surface was fabricated by a pattern transfer method which involves transferring the angle in a template to the waveguide using anisotropic reactive ion etching. The sidewall angle realized in a positive resist on patterning was used as the angle template. Exposure and development conditions were adjusted for Shipley® S1813 photoresist to generate a sidewall angle of ∼ 65°. The anisotropic Reactive Ion Etching (RIE) was done using a CF4/O2 plasma chemistry. A gas composition of 50/50 CF4/O2 was chosen in order to minimize the etch related roughness of the polymer and the photoresist. The metallization of the mirror faces was done using a self-aligned maskless technique which ensures metal deposition only on the angular face and also eliminates a lithography step.

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Joel L. Plawsky

Rensselaer Polytechnic Institute

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P. D. Persans

Rensselaer Polytechnic Institute

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N. Agarwal

Rensselaer Polytechnic Institute

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Svetlana Rogojevic

Rensselaer Polytechnic Institute

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William N. Gill

Rensselaer Polytechnic Institute

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X. Huang

Rensselaer Polytechnic Institute

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A. I. Filin

Rensselaer Polytechnic Institute

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Anthony V. Mule

Georgia Institute of Technology

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Anurag Jain

Rensselaer Polytechnic Institute

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