2021
DOI: 10.3390/ma14144017
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Sintering, Microstructure, and Dielectric Properties of Copper Borates for High Frequency LTCC Applications

Abstract: New ceramic materials based on two copper borates, CuB2O4 and Cu3B2O6, were prepared via solid state synthesis and sintering, and characterized as promising candidates for low dielectric permittivity substrates for very high frequency circuits. The sintering behavior, composition, microstructure, and dielectric properties of the ceramics were investigated using a heating microscope, X-ray diffractometry, scanning electron microscopy, energy dispersive spectroscopy, and terahertz time domain spectroscopy. The s… Show more

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Cited by 8 publications
(8 citation statements)
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“…34–36 The copper borates under investigation generally fulfil the theoretical conditions for attaining a low dielectric permittivity. 20 Consistent with the dumped harmonic oscillator model, 33 the transition from the microwaves region to submillimetre waves will entail a small change in the real part of the dielectric permittivity ( ε ′), but a quite marked increase in its imaginary part ( ε ′′), and consequently in the loss tangent (tan δ = ε ′′/ ε ′). 13,22,33,37 This effect was confirmed experimentally for the commercial Ferro A6M LTCC material ( and tan δ = 0.003 at 200 GHz and , tan δ = 0.012 at 1 THz) 33 and in our previous studies for the Zn 4 B 6 O 13 ceramics ( and tan δ = 0.005 at 90–140 GHz, and and tan δ = 0.007 at 1 THz) 13 and the doped Zn 2 SiO 4 ceramics ( and tan δ ≤ 0.005 at 90–140 GHz, and and tan δ = 0.008 at 1 THz).…”
Section: Resultsmentioning
confidence: 83%
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“…34–36 The copper borates under investigation generally fulfil the theoretical conditions for attaining a low dielectric permittivity. 20 Consistent with the dumped harmonic oscillator model, 33 the transition from the microwaves region to submillimetre waves will entail a small change in the real part of the dielectric permittivity ( ε ′), but a quite marked increase in its imaginary part ( ε ′′), and consequently in the loss tangent (tan δ = ε ′′/ ε ′). 13,22,33,37 This effect was confirmed experimentally for the commercial Ferro A6M LTCC material ( and tan δ = 0.003 at 200 GHz and , tan δ = 0.012 at 1 THz) 33 and in our previous studies for the Zn 4 B 6 O 13 ceramics ( and tan δ = 0.005 at 90–140 GHz, and and tan δ = 0.007 at 1 THz) 13 and the doped Zn 2 SiO 4 ceramics ( and tan δ ≤ 0.005 at 90–140 GHz, and and tan δ = 0.008 at 1 THz).…”
Section: Resultsmentioning
confidence: 83%
“…This effect was previously revealed for the undoped copper borate ceramics. 20 Fig. 5d illustrates good cooperation between the AgPd based internal conductor layer and the ceramic layer based on Li 2 WO 4 doped copper borate in a test LTCC structure.…”
Section: Resultsmentioning
confidence: 92%
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