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Modeling of Integrated RF Passive Devices Sharad Kapur and David E. Long www.integrandsoftware.com Custom Integrated Circuits Conference, 2010 Outline Introduction and motivation Three topics EM simulation using Integral methods


  1. Modeling of Integrated RF Passive Devices Sharad Kapur and David E. Long www.integrandsoftware.com Custom Integrated Circuits Conference, 2010

  2. Outline  Introduction and motivation  Three topics • EM simulation using Integral methods • Modeling layout dependent effects • Circuit models and component synthesis  Experiments  Conclusions 2

  3. Applications  Applications • Mobile • Wireless (WiFi, WiMax) • Wired (Ethernet) • Storage (Hard disks)  Passive components found these devices  A decade ago inductors, MIM capactors  Now a whole range of components and devices are being used 3

  4. Tech trends  Thick metals • 3um to 8um copper  High-resistivity substrates • 10  -cm to 1000  -cm  Fine feature sizes • 0.1  m width at 65nm  Many metal layers • High density MOM capacitors instead of MIM (2fF vs 4fF) 4

  5. IC processes  IC processes offer tight tolerances  Low variability  Chip real estate is expensive  Integration offers big cost savings • No extra packaging • Much tighter tolerances and better yield  When a device can be built with reasonable quality compared to an off-chip or an LTCC structure it will be integrated  Devices that used be considered exotic are now routinely used 5

  6. Passive components inductor ind + shield MOM cap Transformer 6

  7. Full circuits Full circuit 1 VCO 3 : inductors + interconnect+ capacitor bank 1. SiGe Semiconductor on IBM BiCMOS 2. STATS ChipPAC IPD technology Diplexer 2 3. Wipro on TSMC 90nm 7

  8. Modeling  Increased prevalence of passives has made fast and accurate modeling critical  Two aspects to modeling 1. Electromagnetic (EM) simulation to evaluate candidate designs (and possible refinement) 2. Converting EM simulation results that can be used in higher level simulators (like Spice). 8

  9. EM simulation  Two broad categories for solving Maxwell‟s equations 1. Differential formulations • Finite-difference, Finite element (FEM), FDTD 2. Integral Formulations • Method-of-Moments, Boundary element (BEM), Integral equation solvers 9

  10. Differential vs Integral Integral formulations Diff formulations  Planar dielectrics,  Flexible conductors  Imposes no constraint  Need to enforce on shape of metals, Maxwell‟s equations dielectric regions only on conductors  Need to enforce (Green‟s theorem) Maxwell‟s equations  Leads to smaller dense everywhere matrix to solve surrounding the object  Many techniques  Leads to large sparse developed recently matrix solve  For IC passives this approach is the best 10

  11. 3D Integral Formulation in EMX  EMX is a 3D EM simulator  3D volume integral formulation (time harmonic)  Unknowns (charge and currents) • Surface charges • Volume currents • 3D: Current vectors can be in x-y-z directions 11

  12. Matrix formulation (continuous form) Ax  B (A is a dense matrix)  Suppose that N elements in the mesh  Conventional approach O(N 3 ) time and O(N 2 ) memory • Cost is prohibitive • Double the size of the problem 8X time 12

  13. Innovations in numerical methods (GMRES) Ax  b  Iterative methods were developed in the numerical analysis community (GMRES, Yale, 1986)  Matrix vector products instead of matrix inversion n  2 n K { b , Ab , A b ,..., A b }  This reduced the time to O(N 2 ) 13

  14. Innovations in numerical methods (FMM) Ax  b  The Fast Multipole Method was developed in 1987  Developed N-body problem  Applied to capacitance byWhite at MIT for • FastCap, Fast Henry, (1990s).  Applied to 2.5D field solution • IES 3, Bell Labs, Kapur and Long, (1990s)  These sorts of problems can be solved in linear time (with a large constant)  All recent effort is decreasing this cost 14

  15. Exploiting regularity  Mesh generation was regarded as an orthogonal sub problem (typically unstructured Delauny triangulation)  Layout has a lot of structure  This structure can be imposed on the mesh  Identical interactions are repeated all over 15

  16. Adaptive frequency sweep  An adaptive frequency sweep  Reduced order model using Krylov subspace methods • Methods developed in the „00s (Bell Labs, MIT, CMU, Intel)  The reduced order model from a small set of EM solutions  Only few simulations need to be done 16

  17. Time and Memory scaling 1 inductor 64 inductors  Single frequency simulation (including iterative solve)  Compare speed and memory for 1, 2, 4, 8, …, 64 inductors 17

  18. Examples: Spiral Inductor 3D mesh Current Standard high Q spiral inductor used in lots of circuits. Thick copper and large size. Courtesy: TSMC. 65nm RFCMOS, 9LM thick metal technology. Published at RFIC 2009 “ Including Pattern-Dependent Effects in Electromagnetic Simulations of On- Chip Passive Components”, Integrand and TSMC 18

  19. Stacked Inductor 3D mesh Current Small stacked inductor. High inductance low Q (used in Chokes). Upto 20-30nH in small area Courtesy: TSMC. 65nm RFCMOS, 9LM thick metal technology. Published at RFIC 2009 “ Including Pattern-Dependent Effects in Electromagnetic Simulations of On- Chip Passive Components”, Integrand and TSMC 19

  20. MOM (finger)Capacitor 3D mesh of 0.6pF Cap High-density MOM caps (at 40nm can be 4fF/square micron). Important to parasitic inductance to get SRF. Courtesy: TSMC. 65nm RFCMOS, 9LM thick metal technology. Published at RFIC 2009 “ Including Pattern-Dependent Effects in Electromagnetic Simulations of On- Chip Passive Components”, Integrand and TSMC 20

  21. Transformer 3D mesh Current Used as a part of matching network. Can get reanonably high coupling “k” values of 0.8-0.9 in a standard thick metal CMOS process Courtesy: UMC. 90nm RFCMOS, 8LM thick metal technology. Published at CICC 2007 “ Synthesis of Optimal On- Chip Baluns”, Integrand and UMC 21

  22. Balun (with MiM caps) 3D mesh Current A balun is a passive component that transforms power from a BAL anced to an UN balanced port. FOM is usually insertion loss. 1dB insertion loss and is very competitive with off chip baluns. Courtesy: UMC. 90nm RFCMOS, 8LM thick metal technology. Published at CICC 2007 “ Synthesis of Optimal On- Chip Baluns”, Integrand and UMC 22

  23. BiCMOS Diplexer (with Thru Silicon Vias) 3D mesh Current Diplexer has a high-band and low band filter in the same circuit. Used in chips which operate in multiple bands. Fully passive circuit with inductors, resistors, capacitors, TSVs. Need to model all effects and coupling. Courtesy: SiGe Semiconductor. IBM BiCMOS 5PAE. 23

  24. IPD Diplexer 3D mesh Current Built on a “lossless” substrate so coupling is very strong between components. Methodology of design is to create inductors with EM simulation. Tune with caps. Resimulate and re design. Simulation time of about 1 hour for full circuit. Courtesy: STATSChipPAC, IPD technology (8um Cu on high resistivity Si substrate) 24

  25. CMOS VCO 3D mesh (inductor+ capacitor bank) High-frequency VCO. Inductor and 66 MiM capacitor bank. Inductor is small so coupling between inductor and interconnect must be considered. Block by block model fails to predict VCO behavior. Courtesy: Wipro, TSMC90nm, 1P5M 25

  26. Benchmark Summary  Multi-threaded EMX is 2-3X faster for small examples and 5-7X faster for larger examples on an 8 CPU machine.  The memory for the multi-threaded version goes up at a slower rate than the speedup. 26

  27. Layout dependent effects  In IC processes the width, thickness and resistance of wires vary depending on the width and spacing of the surrounding wires  These effects are called pattern dependent effects  Width and spacing dependence in the process description  EMX modifies the layout to mimic the fabrication process  Leads to improved simulation and modeling accuracy 27

  28. Pattern dependent effects  Fabricated metal width varies as a function of width and spacing of wires  Physical width vs drawn width as a function of width and spacing  Width can vary by 50% from drawn width 28

  29. Pattern dependent effects  Sheet resistance varies as a function of width and spacing of wires  Sheet resistance as a function of width and spacing  Sheet resistance can vary by 200% 29

  30. Mimic fabrication effects  EMX automatically modifies IC layout to mimic fabrication effects  When you have uniformly spaced wires “width” and “spacing” have intuitive meanings  Need to come up with a definition of width and spacing for general layout.  What happens when you have non-uniform layout? 30

  31. Modifying layout  Fabricated width is different from drawn width according to rules provided by foundry by a “bias” amount  Shaded regions represent original drawn geometry  Lines represents modified “grown” geometry based on local width and spacing 31

  32. EMX simulation of MOM capacitors The iRCX width-and-spacing dependence is more critical for structures that are not at minimum dimensions. The accuracy of EMX using iRCX is increased since the fabrication process is mimicked more closely.

  33. EMX simulation of Stacked inductors

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