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EECS 170C Lecture Week 1 Spring 2014 EECS 170C
Prof. M. Green / U.C. Irvine
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Lowpass Filter Example
ideal op-amp From standard circuit analysis: Is this design? Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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Lowpass Filter Design 2 equations with 3 unknowns
ideal op-amp Specifications: In a design, solution is not necessarily unique. How do we choose among solutions? 2 equations with 3 unknowns not a unique solution! Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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Additional constraint #1:
Capacitors should be no larger than 1 pF: Set C2 = 1 pF R2 = 318 R1 = 159 Additional constraint #2: For f > f3dB, magnitude should exhibit -40 dB/decade rolloff: f f3dB -20 dB/decade The given circuit topology cannot satisfy this constraint. Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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2nd-order filter topology (2 capacitors) needed:
Since all critical frequencies are determined by RC time constants, R & C each randomly varying by 5% results in frequencies varying by 10%! Additional constraint #3: Under the condition that R’s and C’s vary randomly within ±10%, f3B should vary no more than ±5% This constraint is impossible to meet for any RC filter! Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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VG Vin Vout Vin Vout Possible solution #1: Possible solution #2:
Replace resistors with triode-biased MOSFETs with gates controlled by dc voltage VG, realizing electrically controllable resistors. Critical frequencies can be controlled by VG. Vin Vout Possible solution #2: Replace resistors with configuration consisting of capacitor and switches, with switches controlled by clock signal with period Tc. Critical frequencies are determined by Tc and capacitor ratios. Critical frequencies can be controlled by Tc. Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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Aspects of Design (Synthesis)
Desired behavior & specifications are given; component values & circuit topology are not. Solution is usually found iteratively: An initial circuit is proposed and analyzed. If specifications are not met, the circuit is modified and re-analyzed. There is usually not a unique solution that satisfies the specifications. However, each solution exhibits its own set of tradeoffs (e.g., size, cost, robustness) that must be considered. It may not be possible to meet all of the specifications simultaneously using a given technique or technology. Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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Analog vs. Digital Signal Representation
Precision in specifying and measuring voltage signal is determined by random noise generated by circuit components. Dynamic Range is determined by ratio of maximum amplitude (usually determined by supply voltage) and noise level. Analog representation: Digital representation: Dynamic Range in specifying and measuring digital signal is determined by number of bits used in representing the signal. 16 possible digits Dynamic Range = 16 Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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Continuous vs. Discrete Methods of Timing
Voltage signal is defined at any arbitrary instant of time. There is no limit on the highest frequency that can be generated or measured. Continuous-time signaling: Voltage signal is defined only at discrete values of time kT, where k is an integer. The highest frequency that can be observed is 1/2T – the Nyquist frequency. Discrete-time signaling: Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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Passive Components Power dissipation in a resistor:
Components that always dissipate power are said to be passive. Power supplied by VS: Power dissipated in RL: This is the reason we need transistors! Power gain: Power amplification is impossible if only passive components are present. Prof. M. Green / U.C. Irvine Spring 2014 EECS 170C
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Active Components A component that is not passive is said to be active. (assuming rin >> RS , rout << RL) Power amplification is possible with active devices -- that’s why we need transistors. Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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Discrete Circuit Realized on a Printed Circuit Board (PCB)
Simple discrete design on a PCB. Orders of magnitude difference in capacitor values, but packaging takes roughly same volume. Also includes resistors, supply connections, sockets for ICs. Dimensions cm’s on a side. Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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Integrated Circuit on a Monolithic Substrate
IC layout mm on a side. Point out pads, inductors, interconnect, other circuitry. Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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Circuit Realization: Discrete vs. Monolithic
Each component takes roughly the same area on the board independent of its value. Passive components can be chosen to a desired accuracy, subject to cost. Most circuit nodes can be observed for testing and verification. Dimensions on order of cm. The area of a component is directly related to its value. Individual component values exhibit large variances; however, like components with identical geometries in close proximity exhibit very close matching (<1%). Access to the circuit is only through pre-determined nodes that are connected to pads which then bonded out to the package. Dimensions on order of mm, encapsulated in a package. Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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Example of Matching Design an amplifier with an accurate gain of +10:
Assume Av can take values between 10,000 and 50,000. Very small depends only on resistor ratio Let R1 = 9k , R2 = 1k: Av = 10,000 Vout /Vin = 9.990 independent of individual resistor values Av = 50,000 Vout /Vin = 9.998 Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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Manufacturability of ICs
1. Die Size X This slide shows the effect of die size on yield. Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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Active air-cooling heat sink
2. Power Dissipation Power dissipated in the IC is converted to heat, raising the temperature of the die & package. Elevated die temperature can degrade circuit performance or even permanently damage the silicon. To accelerate heat removal, a heat sink may need to be used, requiring more space. Passive heat sinks Active air-cooling heat sink Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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IC must operate properly in the presence of variations in:
3. Robust Design IC must operate properly in the presence of variations in: Processing in fabrication technology Individual component values can vary ±15% or more Voltage supply Supply voltages can vary ±10% Temperature Circuit should operate to spec at 0--70° C ambient temperature “PVT” Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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Univ. of California, Irvine
Use of Approximation KCL at Vout: KCL at VX: Spring 2014 EECS 170C Prof. M. Green Univ. of California, Irvine Prof. M. Green / U.C. Irvine 19
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My Research 1. High-speed frequency divider:
The operation of “real” high-speed clock dividers is more complex … Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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Clock divider based on CML D flip-flop:
Divider sensitivity curve: Vmin = minimum input clock amplitude required for correct operation. (function of input frequency) fso = self-oscillation frequency Vmax = maximum dc differential voltage that can be applied to the input clock for which the circuit self-oscillates. Vmax Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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Divider test chip measurements
Divider chip photograph Measured sensitivity curves: Conventional (DFF) divider Modified regenerative divider Ring oscillator divider Designed at Broadcom using 0.13 µm CMOS process; shunt-peaking was used. Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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2. Equalization of broadband receivers:
Normally the equalizer and CDR are designed and implemented as separate blocks. Common elements in each of the two blocks can be identified and combined... Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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Circuit Details Shunt-peaking CML summer.
2-stage shunt-peaking CML slicer. Differentially-tuned LC VCO. Retimer generates low-ISI retimed data. Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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Measurement Setup Test setup Test board
Die photo. Implemented in Jazz Semiconductor 0.18µm BiCMOS Process (only CMOS transistors used). Test setup Test board Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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Equalizer + CDR Operation (2)
2.4 m cable Cable output eye diagram. Recovered clock RJ = 1.83 ps rms Retimer output eye diagram Jitter = 4.14 ps rms 3.6 m cable Cable output eye diagram. Recovered clock RJ = 2.15 ps rms Retimer output eye diagram Jitter = 4.96 ps rms Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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÷2 ÷2 2. Equalization of broadband receivers:
4:1 Multiplexer Tree Structure: Din0 D Q D-FF A Din1 B Select D Q D Q D Q A Dout D-FF Latch D-FF retimer B Select 10 GHz Din2 D Q D Q 40 GHz D Q 20 GHz D-FF Latch D-FF A B Select Din3 D Q D Q 20 GHz D-FF Latch 10 GHz 10 GHz 20 GHz 40 GHz PLL ÷2 ÷2 10 GHz Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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40GHz Differential Push-Push VCO
Resonates at 40 GHz Virtual ground node Resonates at 20 GHz Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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Chip Board and Die Micrograph
40 Gb/s output 20 GHz clock 40 Gb/s output 20 GHz clock output 40Gb/s Distributed buffer Push-push differential VCO 625 MHz Reference clock PLL Clock buffers 40Gb/s MUX and retimer 20Gb/s inputs 20 Gb/s inputs Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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Measured 40 Gb/s Output 40Gb/s MUX output (Differential) with 450 mV differential peak-to-peak vertical eye opening and 1.14 ps rms jitter Spring 2014 EECS 170C Prof. M. Green / U.C. Irvine
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