Time-periodic stiffness modulation in elastic metamaterials for selective wave filtering: Theory and experiment
… (b)–(d) Normalized 2D-FT magnitude j ^Wðκ;ωÞj associated with the wave field wðx; tÞ
shows narrow-band frequency reflection of the reflected waves in the κ < 0 half plane at fm=2, …
shows narrow-band frequency reflection of the reflected waves in the κ < 0 half plane at fm=2, …
Experimental and numerical investigation of the SBS-threshold increase in an optical fiber by applying strain distributions
JMC Boggio, JD Marconi… - Journal of lightwave …, 2005 - ieeexplore.ieee.org
We study, experimentally and numerically, the increase of the stimulated Brillouin scattering
(SBS) threshold in dispersion-shifted fibers (DSFs) by applying three different tensile-strain …
(SBS) threshold in dispersion-shifted fibers (DSFs) by applying three different tensile-strain …
Experimental observation of nonreciprocal band gaps in a space-time-modulated beam using a shunted piezoelectric array
In this work, we experimentally achieve 1-kHz-wide directional band gaps for elastic waves
spanning a frequency range from approximately 8 to 11 kHz. One-way propagation is …
spanning a frequency range from approximately 8 to 11 kHz. One-way propagation is …
Dynamic mechanical analysis of particulate‐filled epoxy resin
…, PG König, JD Marconi - Journal of applied polymer …, 2003 - Wiley Online Library
The dynamic mechanical properties of epoxy composites filled with different amounts of
quartz powder were investigated. The storage modulus and loss tangent were measured at …
quartz powder were investigated. The storage modulus and loss tangent were measured at …
Near-IR emission in Pr3+ single doped and tunable near-IR emission in Pr3+/Yb3+ codoped tellurite tungstate glasses for broadband optical amplifiers
MP Belançon, JD Marconi, MF Ando, LC Barbosa - Optical materials, 2014 - Elsevier
A study of the broadband near-infrared emission in Pr 3+ single doped and Pr 3+ /Yb 3+
codoped tellurite–tungstate glasses for optical amplification is presented. In the Pr 3+ single …
codoped tellurite–tungstate glasses for optical amplification is presented. In the Pr 3+ single …
[HTML][HTML] A framework for cooperative intrusion detection
…, D Tobin, J McConnell, J Marconi… - Proc. 21st NIST …, 1998 - books.google.com
The trend towards a strong interdependence among networks has serious security implications.
Not only does the compromise of one network adversely affect resources needed by …
Not only does the compromise of one network adversely affect resources needed by …
[BOOK][B] Cause marketing: Build your image and bottom line through socially responsible partnerships, programs, and events
J Marconi - 2002 - dl.acm.org
… Marconi outlines what a commitment to socially responsible business and marketing can
mean in terms of a company's image, reputation, market share, and profitability …
mean in terms of a company's image, reputation, market share, and profitability …
Generalized plane wave expansion method for non-reciprocal discretely modulated waveguides
… m κ m x − n ω m t d x d t ρ ˆ m , n = 1 T m 1 λ m ∫ − λ m 2 λ m 2 ∫ − T m 2 T m 2 ρ x , t e j m
… j p κ m x − q ω m t e j κ x − ω t w x , t = ∑ p = − P P ∑ q = − Q Q Ŵ p , q e j p κ m x − q ω m t e j …
… j p κ m x − q ω m t e j κ x − ω t w x , t = ∑ p = − P P ∑ q = − Q Q Ŵ p , q e j p κ m x − q ω m t e j …
Spectroscopic properties of tellurite glasses co-doped with Er3+ and Yb3+
… Ψ J to an excited state Ψ ′ J ′ is given by:(2) f c a l = 8 π 2 m e c 3 h ν ( 2 J + 1 ) ( n 2 + 2 ) 2
9 n ∑ λ = 2 , 4 , 6 Ω λ < Ψ J | | U λ | | Ψ ′ J ′ > 2 … index of the medium, J is the total angular …
9 n ∑ λ = 2 , 4 , 6 Ω λ < Ψ J | | U λ | | Ψ ′ J ′ > 2 … index of the medium, J is the total angular …
Optical characterization, infrared emission and visible up-conversion in Er3+ doped tellurite glasses
M Seshadri, EF Chillcce, JD Marconi, FA Sigoli… - Journal of non …, 2014 - Elsevier
… According to J–O … ′J′), depends on the three J–O intensity parameters, Ω λ (λ = 2, 4 and
6) as(2) f cal = 8 π 2 mc ⋅ n 2 + 2 2 3 h 2 J + 1 λ ⋅ 9 n × ∑ λ = 2 , 4 , 6 Ω λ SL J U λ S ′ L ′ J …
6) as(2) f cal = 8 π 2 mc ⋅ n 2 + 2 2 3 h 2 J + 1 λ ⋅ 9 n × ∑ λ = 2 , 4 , 6 Ω λ SL J U λ S ′ L ′ J …