Closed-form formulae for frequency-dependent 3-D interconnect inductance

Zhu, Zhengming; Xiao, Xia; Streiter, R.; Ruan, Gang; Otto, Thomas; Wolf, H.; Geßner, Thomas

doi:10.1016/s0167-9317(01)00574-3

Cited by 15 publications

(14 citation statements)

References 13 publications

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“…(1), the field dependence of R can be obtained. As far the skin depth δ is concerned, the self‐inductance L s of one segment of ribbon has the following semiexperimental formula 19: where t is the thickness of ribbon. The total self‐inductance of the patterned ribbon is the sum of L s for each segment.…”

Section: Theory Modelmentioning

confidence: 99%

Enhancement of magnetoimpedance effect in Co‐based amorphous ribbon with a meander structure

Chen¹,

Zhou²,

Lei³

et al. 2010

Physica Status Solidi (a)

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A model for the enhanced giant magnetoimpedance (GMI) effect in field‐annealed Co‐based ribbon with a meander structure is developed. Three different kinds of ribbon are fabricated by a MEMS method and the field dependence of the GMI effect is measured at 10 MHz. Good agreement between theory and experiment shows the validity of this model. A larger change of inductance L in the meander structure results in the increasing of impedance Z and the enhanced GMI effect.

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Section: Theory Modelmentioning

confidence: 99%

Enhancement of magnetoimpedance effect in Co‐based amorphous ribbon with a meander structure

Chen¹,

Zhou²,

Lei³

et al. 2010

Physica Status Solidi (a)

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“…The efficiency of the method for the mutual coupling was verified against data from literature [15], simulation data [14] and the Grover's formula [8]. The comparative results shown in Fig.…”

Section: B Mutual Coupling Of An Interconnect Pairmentioning

confidence: 92%

A wideband and SPICE-compatible model for interconnect coupling prediction in nanoscale VLSI circuits up to 60 GHz

Pharmayeni¹,

Akmeliawati

Legowo³

2011

2011 6th International Conference on Design &Amp; Technology of Integrated Systems in Nanoscale Era (DTIS)

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“…The zeroth-order resonant frequency (m-O) is at 2.45 GHz, with a total of 10MHz of bandwidth, as can be seen in simulated return loss shown in the Fig.3. For calculation of inductance and capacitance were taken into account the self inductance and mutual inductance formula for two parallel wires of equal length, the self inductance of single-tum loop, the capacitance between the wires and of the gap of the loop [7], [8], [9] and [10]. The values calculated for the capacitances were; C R == C L == O.86pF , and for the inductances were; L R == L; == 4.9nH.…”

Section: Ill Simulationof Thezorwmentioning

confidence: 99%

Metamaterial isotropic sensor

Pires¹,

Fontgalland²,

Melo³

et al. 2009

2009 SBMO/IEEE MTT-S International Microwave and Optoelectronics Conference (IMOC)

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In this paper is presented a resonant type wire antenna of the compact size, it was implemented using a compo site right/left-handed transmission line. The array of three antennas can be used as isotropic sensor. It was built with the junction of three cells that presented resonant frequency in the mode zeroth-order (infinite wavelength). Keywords-Metamaterials; composite right/left-handed (CRLH); Compact antenna; resonant antenna; Isotropic sensor. I. INTROD UCTION With the discovery and development of composite right/left-handed transmission line (CRLH TL) theory many researchers have been guided to develop novel types of microwave devices using this property [1]-[6] and [12]. A number of RF/microwav e practical component, antenna and system applications, based on the concept of CRLH metamaterials have already been demonstrated to exhibit unprecedented perform ances and functionaliti es [2]. The effect of the metamaterial transmission line (TL) is an extraordinary consequence of the permittivity and permeability. The CRLH TL has the unique property of an infinite-wavelength wave at specific non-zero frequency because of the zero permittivity and perme ability [1], [2] and [3]. The CRLH concept takes into account and exploits the dual nature of real Left-Handed (LH)structures, which also include natural Right-Handed (RH) contributions. At low frequencies the RH effects are weak and propagation is essenti ally LH, leading to backward wave propagation, whereas they become dominant at higher frequencies, leading to forward wave propagation [4]. The LH metamaterial and the CRLH metamaterials were proposed and applied for enhan cing antenna designs; they are basically the dual of traditional transmission lines. The recognition of this dual nature of metamaterials and the developm ent of advanced analysis has paved the way for a novel generation of microwave components including antennas. Metamaterials have increasingly attracted researchers' attention because of its unique electromagnetic properti es. It has been proven that metamaterials can be applied to antenna application where the size of the antenna is substantially reduced [5].In this paper, we employ the metamaterials effects and characteristics to create a resonant type wire antenna of the compact size where the resonant frequency in the mode zerothorder (infinite wavelength) is independent of the physical length, so that the resonator can be arbitrarily of smalI length [6].CAPES and CNPq , Brazilian government agenc ies 978-1-4244-5357-3/09/$26.00©2009IEEE

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Closed-form formulae for frequency-dependent 3-D interconnect inductance

Cited by 15 publications

References 13 publications

Enhancement of magnetoimpedance effect in Co‐based amorphous ribbon with a meander structure

Enhancement of magnetoimpedance effect in Co‐based amorphous ribbon with a meander structure

A wideband and SPICE-compatible model for interconnect coupling prediction in nanoscale VLSI circuits up to 60 GHz

Metamaterial isotropic sensor

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