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r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 1R. Kulke, W. Simon, A. Lauer, M. Rittweger, P. Waldow,S. Stringfellow, R. Powell, M. Harrison, J.-P. Bertinet
onon
presented by presented by Dietmar KötherDietmar Köther
r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 2
October 98 - September 01
Rapid Manufacture of Microwave and Power ModulesEuropean Brite Euram III Project (BE-97-4883)
Partner Country• Marconi-CL GB• SOREP-ERULEC F• IMST GER• HYWEL NL• TNO NL• NMRC IE
Partner Country• Marconi-CL GB• SOREP-ERULEC F• IMST GER• HYWEL NL• TNO NL• NMRC IE
RAMPRAMPRAMP
r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 3LTCC Test Tiles
Ferro A6M, Au FX30-025
Ferro A6M, Ag FX33-229
DuPont 951 AX, Ag 6145
DuPont 951 AX, Au 5743 post fire
r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 4Geometry Parameters1. Ferro A6M, Au FX30-025:
t = 10 – 12 µmh = 184 –190 µmw = 238 µµµµmRa = 0.4 µm
2. Ferro A6M, Ag FX33-229:t = 14 – 16 µmh = 184 –190 µmw = 237 µµµµmRa = 0.4 µm
3. DuPont 951 AX, Ag 6145: t = 22 – 24 µmh = 190 –195 µmw = 195 µµµµmRa = 0.4 µm
4. DuPont 951 AX, Au 5743 post fire:t = 10 – 12 µmh = 175 –180 µmw = 180 µµµµmRa = 0.4 µm
MS Line
GND Mesh
th
w
LTCC Cross Section
r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 5Measured Parameters + Results
DC-ConductivityS-Parameter or Spectrum up to 40 GHz (On-Wafer)
Substrate ThicknessMicrostrip Line Width and ThicknessVia Diameter and PositionConductor Diffusion into Substrate SurfaceCircuit Geometry (ring, gap, line length …)
Quality Factor Q Effective Permittivity εeff
of Microstrip Line Total Line Losses α
GeometryGeometry DC + RF ParametersDC + RF Parameters
Evaluation ResultsEvaluation Results
r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 6Formulas
Insertion Loss: S21
Attenuation: a21(f) = −20 log|S21(f)|
3dB-Bandwidth: 2∆fn = fn(l)– fn(u)
Loaded Quality: QL(fn) = fn / (2∆fn)
Unloaded Quality: Q(fn) = QL(fn) / [1-|S21(fn)|]
Effective Permittivity: εeff = (c0 n)2 / (πd fn)2
Total Line Losses: α = (27.288 fn √εeff) / (c0 Q) [dB/m]
n: resonance frequencyd: ring diameter
r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 7Measurement of |S21||S21| [dB]
-80
-70
-60
-50
-40
-30
-20
-10
0 5 10 15 20 25 30 35 40Frequency / GHz
f1
f2
f3f4
f5f6
f8f7
f10f9f12f11
f13
measured on Ferro Ag: gap = 50µm
r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 8QualityUnloaded Q
20
40
60
80
100
120
140
160
180
0 5 10 15 20 25 30 35 40Frequency / GHz
Q: Ferro AuQ: DuPont AgQ: DuPont AuQ: Ferro Ag
DuPont 951, Au: εr=7.8, h=180µm, w=180µm, t=10µm, ρ== 8 mΩ/square, RGH=0.4µm, tanδ=4.7x10-3; (post-fire)DuPont 951, Ag: εr=7.8, h=180µm, w=195µm, t=10µm, ρ== 3 mΩ/square, RGH=0.4µm, tanδ=4.7x10-3
Ferro A6-M, Au, εr=5.9, h=190µm, w=240µm, t=12µm, ρ==7 mΩ/square, RGH=0.4µm, tanδ=1.2x10-3
Ferro A6-M, Ag, εr=5.9, h=190µm, w=250µm, t=12µm, ρ== 5 mΩ/square, RGH=0.4µm, tanδ=1.2x10-3
r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 9Measured Line LossesLosses [dB/cm]
00.10.20.30.40.50.60.70.80.9
11.1
0 5 10 15 20 25 30 35 40Frequency / GHz
DuPont, AuDuPont, AgFerro, AuFerro, Ag
DuPont 951, Au: εr=7.8, h=180µm, w=180µm, t=10µm, ρ== 8 mΩ/square, RGH=0.4µm, tanδ=4.7x10-3; (post-fire)DuPont 951, Ag: εr=7.8, h=180µm, w=195µm, t=10µm, ρ== 3 mΩ/square, RGH=0.4µm, tanδ=4.7x10-3
Ferro A6-M, Au, εr=5.9, h=190µm, w=240µm, t=12µm, ρ==7 mΩ/square, RGH=0.4µm, tanδ=1.2x10-3
Ferro A6-M, Ag, εr=5.9, h=190µm, w=250µm, t=12µm, ρ== 5 mΩ/square, RGH=0.4µm, tanδ=1.2x10-3
r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 10Ferro A6M: LossesLosses [dB/cm]
0
0.1
0.2
0.3
0.4
0.5
0 5 10 15 20 25 30 35 40Frequency / GHz
Ferro, AuFerro, AgRho+RGH+Tan(delta)Rho+RGHRho
Simulation with LineCalc: w=238µµµµm, t=12µµµµm, ρρρρ/ρρρρAu=1.6, RGH=0.4µµµµm, tanδδδδ=1.2x10-3
Ferro A6Mεεεεr = 5.9h = 190µµµµmRGH = 0.4µµµµmtanδδδδ = 1.2x10-3
Agw = 237µµµµmt = 12µµµµmρρρρ===== 5 mΩΩΩΩ/sq.
Auw = 238µµµµmt = 12µµµµmρρρρ===== 7 mΩΩΩΩ/sq.
RhoRho
RghRgh
tantanδδδδδδδδ
r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 11DuPont 951: LossesLosses [dB/cm]
00.10.20.30.40.50.60.70.80.9
11.1
0 5 10 15 20 25 30 35 40Frequency / GHz
DuPont 951, AgDuPont 951, AuRho+RGH+Tan(delta)Rho+RGHRho
DuPont 951εεεεr = 7.8h = 180µµµµmt = 10µµµµmRGH=0.4µµµµmtanδδδδ=4.7x10-3
Simulation with LineCalc: w=180µµµµm, t=10µµµµm, ρρρρ/ρρρρAu=1.6, RGH=0.5µµµµm, tanδδδδ=5x10-3
Agw = 195µµµµmt = 10µµµµmρρρρ===== 3 mΩΩΩΩ/sq.
Au (post-fire)w = 180µµµµmt = 10µµµµmρρρρ===== 8 mΩΩΩΩ/sq.
RhoRho
RghRgh
tantanδδδδδδδδ
r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 12Effective Permittivity
1. Unexpected Measured Results2. Geometry Inspection: Diffused Top Conductor3. Full Wave Analysis (FDTD)
E-Field Distribution Influence on εeff and ZL
4. Libra Circuit Simulation without correction with correction
5. Comparison of Measured and Simulated Data
Correction approach of diffused or recessed top conductor
r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 13Conductor Cross-View
Dupont 951 / Ag 6145 Ferro A6M / Ag Fx33-229
Dupont 951 / Au 5743 Ferro A6M / Au Fx30-025
Silver Conductor
Gold Conductor
post
-fire
co-fi
re
co-fi
reco
-fire
r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 14FDTD-Simulations
E-Field Concentration
MS-Line Recessed MS-Line
r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 15FDTD-Simulations II
effective Permittivity
4
4.2
4.4
4.6
4.8
0 10 20 30 40 50Frequency / GHz
recessed
50% recessed
on topmeas. on Ferro Au
Line Impedance / ΩΩΩΩ
50
52
54
56
58
60
0 10 20 30 40 50Frequency / GHz
recessed
50% recessed
on top
0%
100%
50%
0%
100%
50%
r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 16Circuit Simulation with Libra
r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 17Ferro AG Ring-Resonator
0 10 20 30 40freq / GHz
0
-20
-40
-60
-80
-100
-120
|S12| / dB
MEAS: S12_G50SIM: S12_G50
with correction:εr = 6.25h = 167 µmw = 245 µmt = 15 µm
ZL = 48.3 ΩΩΩΩεεεεeff = 4.3
0 10 20 30 40freq / GHz
0
-20
-40
-60
-80
-100
-120
|S12| / dB
MEAS: S12_G50SIM: S12_G50
no correction:εr = 5.9h = 185 µmw = 245 µmt = 15 µm
ZL = 52.4 ΩΩΩΩεεεεeff = 4.1
r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 18εεεεeff: Measurement + Simulation
effective Permittivity
4.1
4.3
4.5
4.7
4.9
5.1
5.3
5.5
5.7
0 5 10 15 20 25 30 35 40Frequency / GHz
DuPont: measuredDuPont: sim. with correctionDuPont: simulationFerro: measuredFerro: sim. with correctionFerro: simulation
DuPont: εr = 7.8, Silvermeasured + simulated
simulated (no correction)
Ferro: εr = 5.9, Goldmeasured + simulated
simulated (no correction)
r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 19Outlook: LTCC RF-Benchmark
Conductors Vias Cavities
microstrip line
ground
stripline
ground
h = 130µm
h = 200µm
h = 200µm
h = 200µm
h = 130µm
h = 130µm
DuPont 951:εr = 7.8
r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 20TestlayoutX = 66 mmY = 66 mm
StriplineRing-
Resonators
Coupled Striplines
StriplineCalibration
Kid
Microstrip to Stripline
Transitions
X = 0Y = 0
Resolution Test Lines
MicrostripCalibration
Lines
MicostripRing-
Resonators
Conductivity Measurement
r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 21Conclusion
Test Procedure for LTCC RF-Evaluation;Resulting Parameters:• Quality Factor Q• Effective Permittivity εεεεeff
• Line Losses ααααCorrection Approach for Diffused Top ConductorsBenchmarking Activity has started
r.kulke, dokumente/DuPont/ring_resonators.ppt May-01
LTCC 22LTCCLTCC @@@@@@@@ IMST
Multilayer Library for LTCC-Elements (ADS)
Consulting: Material, Foundry, RF + Antennas
LTCC-Prototyping Capability
Evaluation and Characterization• Modules, Circuits and Antennas (GHz-Frequencies)
Introduction to Production