2023
DOI: 10.1021/acsami.3c13668
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Low-Permittivity and Low-Temperature Cofired BaSO4–BaF2 Microwave Dielectric Ceramics for High-Reliability Packaged Electronics

Wei Wang,
Muhammad Shehbaz,
Xin Wang
et al.

Abstract: In developing low-temperature cofired ceramic (LTCC) technology for high-density packaging or advanced packaged electronics, matching the coefficient of thermal expansion (CTE) among the packaged components is a critical challenge to improve reliability. The CTEs of solders and organic laminates are usually larger than 16.0 ppm of °C1–, while most low-permittivity (εr) dielectric ceramics have CTEs of less than 10.0 ppm °C1–. Therefore, a good CTE match between organic laminates and dielectric ceramics is requ… Show more

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Cited by 11 publications
(3 citation statements)
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“…The analysis of the MT-CLTA sample infrared reflectance spectrum is performed by a classical three parameter resonator harmonic oscillator model using eq . .25ex2ex ε * ε ( ) = j = 1 n false( z j e false) 2 / m j V j ε 0 ω normalT j 2 ω 2 j γ j ω infix= ε ( ) + j = 1 n ω P j 2 ω normalT j 2 ω 2 j γ j ω where ε ∞ is the optical permittivity of ceramic, ω P j is the plasma frequency, ω o j is the transverse frequency, ω T j is the angular frequency of the transverse optical modes, and n is the number of transverse phonon modes, γ j represents defective phonon scattering of j th Lorentz oscillator, V j represents the unit volume of j th vibrational mode, m j denotes the converted mass of positive and negative ions, z j is charge number of j th mode, e represents the elementary charge, whereas normalΔ ε j = S j ω o j 2 , in which Δε j is j th oscillator contribution to permittivity and S j is j th oscillator strength, which can be approximated as contribution to static permittivity …”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…The analysis of the MT-CLTA sample infrared reflectance spectrum is performed by a classical three parameter resonator harmonic oscillator model using eq . .25ex2ex ε * ε ( ) = j = 1 n false( z j e false) 2 / m j V j ε 0 ω normalT j 2 ω 2 j γ j ω infix= ε ( ) + j = 1 n ω P j 2 ω normalT j 2 ω 2 j γ j ω where ε ∞ is the optical permittivity of ceramic, ω P j is the plasma frequency, ω o j is the transverse frequency, ω T j is the angular frequency of the transverse optical modes, and n is the number of transverse phonon modes, γ j represents defective phonon scattering of j th Lorentz oscillator, V j represents the unit volume of j th vibrational mode, m j denotes the converted mass of positive and negative ions, z j is charge number of j th mode, e represents the elementary charge, whereas normalΔ ε j = S j ω o j 2 , in which Δε j is j th oscillator contribution to permittivity and S j is j th oscillator strength, which can be approximated as contribution to static permittivity …”
Section: Resultsmentioning
confidence: 99%
“…in which Δε j is jth oscillator contribution to permittivity and S j is jth oscillator strength, which can be approximated as contribution to static permittivity. 38 Complex reflectance [R(ω)] gained by infrared spectra and complex permittivity [ε*(ω)] can be related by eq 3. 39 R( )…”
Section: Materials Characterizationmentioning
confidence: 99%
“…A lower dielectric constant (ε r ) reduces the signal coupling loss and improves the signal transmission speed at high frequencies. Hence, advancements in microwave dielectric ceramics are crucial for enhancing the application and user experience of 5G/6G technology in mobile communications, smart driving, healthcare, and other fields. …”
Section: Introductionmentioning
confidence: 99%