Title: Low EMI oscillators Product: HM series MERCURY www.mercury-crystal.com TN No.: TN-020 Date: March 3, 2004 Revision: 2 Page 1 of 1 Title: Low EMI Spread Spectrum Clock Oscillators Background Traditional ways of dealing with EMI (Electronic Magnetic Interference) problems include using EMI filters, ferrite beads, chokes, adding power layer and ground plane to the board, more metal shielding and special coating and RF gaskets. However, the principle sources of EMI problem come from the system clocks including frequency timing generators, crystal oscillators, VCOs and PLLs. It is obvious that the most efficient and economic way to reduce EMI for the whole system is to use low EMI spread spectrum clock (SSC) oscillators. The advantages of using low EMI oscillators are easy passage of regulatory testing, short time-to-market and cost reduction. Spread Spectrum Technology (SST) Maximum allowable EMI radiation is normally referred to the peak EMI emissions not the averaged emissions. A good approach is to spread out the concentrated mode energy on one particular frequency to a broader bandwidth and controlled frequency range (for example: center frequency ±1%) with a controlled modulation rate. The total mode energy remains the same but the peak energy got spread out to near-by frequencies. This frequency modulation technique is known as Spread Spectrum Technology (SST). In stead of patching the EMI problems with filtering and shielding, SST provides efficient and low cost solutions to the expensive EMI problems. Spread Spectrum Clock Oscillator (SSC) takes advantage of the SST to provide low EMI frequency sources. In most of the cases, system designers face the EMI problem at the time their products fail the EMI/EMC regulations at the test labs. Mercury HM series low EMI crystal oscillators provide drop-in replacement solution for situation like these. The big plus is no board re-spinning. As shown in the following spectrum comparison graphs, a conventional clock (un-modulated) has narrow band width and peak radiation energy. By the SST, a 10 dB or more of the EMI reduction can be expected. The modulation carrier frequency is usually in the range of 6 to 55 KHz (Mercury model and frequency dependent) which makes the modulation process transparent to the oscillator frequency. Consequently, electronic devices have lower EMI emissions but not affected by the resultant instantaneous frequencies. Center Spread vs. Down Spread The controlled modulation process can be on all of one side of the nominal frequency (down spread) or 50% up and 50% down (center spread). Pick 100 MHz SSC as an example, its center frequency is modulated between 99.500 MHz and 100.500 MHz with center spread of 0.5%; the frequency range is between 99.500 MHz and 100.0 MHz if down spread at 0.5%. By moving the center frequency, a down spread 0.5% modulation can be considered a process equivalent to a center spread of 0.25%. In another word, modulation between 99.500 MHz and 100.0 MHz (down 0.5%) is equivalent to center spread 0.25% with center frequency at 99.750 MHz. A. 100 MHz at center spread 0.5% B. 100 MHz at down spread 0.5% “B” is equivalent to 99.750 MHz at center spread of 0.25% Instantaneous Frequencies (min.) 99.500 99.500 99.500 Center Frequency 100.000 99.750 Instantaneous Frequencies (max.) 100.500 100.000 100.000 The down spread is preferred if a system can not tolerate operating frequency higher than the nominal frequency (over-clocking problem). In the above 100 MHz center spread 0.5% example, there is a period of time that the system running between 100.000 MHz and 100.500 MHz, these instantaneous frequencies are higher than the system clock and may erode system timing margin. Using down spread can avoid this problem with the sacrifice of a slightly slower clock rate. Down-center spread (also called asymmetric spread), a compromised way of the two, is another choice and available in some Mercury HM series Title: Low EMI oscillators MERCURY www.mercury-crystal.com Product: HM series TN No.: TN-020 Date: March 3, 2004 Revision: 2 Page 2 of 2 Conventional Clock Conventional Clock dB dB EMI reduction fo - (fo*1%) Spread spectrum clock EMI reduction fc fo - (fo*0.5%) fc fo=fc fo + (fo*0.5%) F F fo + (fo*0.5%) fo T fo fo - (fo*0.5%) T fo - (fo*1%) Modulation Carrier frequency Modulation Carrier frequency Figure 1: Spectrum comparisons. 1% down spread and ±0.5% center spread as examples Modulation Carrier Frequency: The modulation carrier frequency (sweep rate) is typically around KHz range which is relatively slower compared with the MHz range of the clock frequency. As shown in figure 1, the output frequency is slowly swept within the pseudo triangle shape wave envelope from the f(max). to fo(nominal) then to f(min) then to fo(nominal)., back and forth. The resultant instantaneous frequencies are always between f(max) and f(min). The modulation percentage determines the bandwidth of the span while the modulation carrier frequency determines the spacing of the spectral. EMI Reduction at Harmonics: As seen in figure 2 and figure 3, higher order harmonic frequencies do get stronger EMI reduction. They also show that the greater modulation percentage reduces EMI emissions more. It needs to be pointed out that the fundamental frequency as well as every harmonics all gets EMI reduction by the SST. Date: March 3, 2004 Title: Low EMI oscillators MERCURY www.mercury-crystal.com Product: HM series Revision: 2 TN No.: TN-020 Page 3 of 3 EMI Reduction (dB) Group: P SST Fout = 125 MHz 28 25 22 19 16 13 10 7 1 3 5 7 9 11 13 15 17 HARMONICS 0.50% 1% 1.50% 2% 3% 3.5% Figure 2: EMI reduction at harmonics for Mercury HM series group P Group: W SST Fout = 16.384 MHz EMI Reduction (dB) 18 16 14 12 10 8 6 4 2 0 1 3 5 7 9 11 13 15 17 HARMONICS 1.25% 3.75% Figure 3: EMI reduction at harmonics for Mercury HM series group W 19 19 Date: March 3, 2004 Title: Low EMI oscillators MERCURY www.mercury-crystal.com Product: HM series Revision: 2 TN No.: TN-020 Page 4 of 4 Measurement Data: EMI reduction data shown below are actual measurement data taken from Mercury 3HM57 series group “R”. SSC 100 MHz at various spread percentages and harmonics at each percentage are shown. TS305B Spectrum analyzer Waveform @SSC=OFF TS305B Spectrum analyzer Waveform @SSC=+/-0.25% 0 0 -3.33dBm -10 -20 -20 -30 -30 -40 -40 [dBm] [dBm] -10 -50 -50 -60 -60 -70 -70 -80 -80 -90 -90 -100 -100 96 97 98 99 100 101 102 103 -11.19dBm 96 104 97 98 99 TS305B Spectrum analyzer Waveform @SSC=+/-0.5% 102 103 104 103 104 0 -10 -12.98dBm -20 -20 -30 -30 -40 -40 [dBm] [dBm] 101 TS305B Spectrum analyzer Waveform @SSC=+/-1.5% 0 -10 -50 -60 -60 -70 -80 -80 -90 -90 -100 -100 97 98 99 100 101 102 103 -18.54dBm -50 -70 96 104 96 97 98 99 Frequency[MHz] -3.21 -10 100 101 102 Frequency[MHz] TS305B Spectrum Analyzer Waveform @SSC=OFF 0 TS305B Spectrum Analyzer Waveform @SSC=+/-0.25% 0 -10.04 -20.15 -20 -24.25 -30 -10 -25.40 -40 -30 -50 -40 -60 -11.21 -20.19 -20 -35.04 [dBm] [dBm] 100 Frequency[MHz] Frequency[MHz] -33.37 -37.72 -38.87 -48.97 -50 -70 -60 -80 -70 -90 -80 -90 -100 0 100 200 300 400 500 600 700 800 -100 900 1000 1100 1200 0 Frequency[MHz] 100 200 300 400 500 600 700 800 900 1000 1100 1200 Frequency[MHz] TS305B Spectrum Analyzer Waveform @SSC=+/-0.5% TS305B Spectrum Analyzer Waveform @SSC=+/-1.5% 0 0 -10 -10 -12.80 -20 -29.09 -30 -36.75 -40 -41.23 -42.47 -51.40 -50 -60 [dBm] [dBm] -19.46 -20 -24.45 -30 -80 -80 -90 -90 -100 -100 200 300 400 500 600 700 Frequency[MHz] 800 900 1000 1100 1200 -48.47 -58.77 -60 -70 100 -46.35 -50 -70 0 -41.22 -40 0 100 200 300 400 500 600 700 Frequency[MHz] 800 900 1000 1100 1200 Date: March 3, 2004 Title: Low EMI oscillators MERCURY www.mercury-crystal.com Product: HM series Revision: 2 TN No.: TN-020 Page 5 of 5 -24 -22 -18 -16 50 MHz 32.768 MHz 25 MHz -14 -12 25 MHz -10.1 dB -15.5 dB -17.6 dB -22.9 dB 32.768 MHz -9.9 dB -15.6 dB -17.8 dB -23.0 dB 50 MHz -10.1 dB -16.3 dB -18.2 dB -23.3 dB 25 MHz, 32.768 MHz and 50.0 MHz at center spread ±0.25%, ±0.5% and ±1.5%. -10 -8 off 0.25 0.5 1.0 0.75 1.5. SSC % 1.25 TS302B(Down Spread) Spectrum Analyzer Waveform@SSC=OFF TS304B(Center Spread) Spectrum Analyzer Waveform @SSC=OFF 0 0 -3.78dBm -20 -20 -30 -30 -40 -40 -50 -60 -50 -60 -70 -70 -80 -80 -90 -90 -100 -100 22 23 24 25 26 -3.76dBm -10 [dBm] [dBm] -10 27 28 22 23 24 Frequency[MHz] 0 0 -10 -17.11dBm -40 -50 -60 -40 -50 -60 -70 -70 -80 -80 -90 -90 -100 -100 24 25 Frequency[MHz] 28 26 27 TS3024 SSC :OFF - (+/-1.5%) Reduction = 13.06dBm -30 [dBm] -30 23 27 -16.82dBm -20 TS302B SSC :OFF - (-3.0%) Reduction = 13.33dBm 22 26 TS304B(Center Spread) Spectrum Analyzer Waveform @SSC=+/-1.5% -10 -20 25 Frequency[MHz] TS302B(Down Spread) Spectrum Analyzer Waveform @SSC=-3.0% [dBm] Gain (dB) SSC is off SSC=±0.25% SSC=±0.5% SSC=±1.5% -20 28 22 23 24 25 Frequency[MHz] 25 MHz at down spread -3% and center spread ±1.5%. The EMI reduction is about the same. 26 27 28 Date: March 3, 2004 Title: Low EMI oscillators MERCURY www.mercury-crystal.com Product: HM series Revision: 2 TN No.: TN-020 Page 6 of 6 Start-up Current Tr Tf Time Consumption Rise Time Fall Time (u. sec.) (mA) (n. sec.) (n. sec.) Duty Cycle (%) Logic “1” Logic “0” 200 SSC=OFF 290 200 780 Center 780 Spread ±0.25% 880 3.1 3.0 3.0 8.4 8.1 1.9 2.1 1.9 2.2 2.8 2.0 2.3 2.5 2.5 2.3 48.4 48.5 48.6 49.1 50.0 3.40 3.31 3.39 3.31 3.23 0.14 0.25 0.16 0.14 0.18 8.3 2.3 2.1 48.9 3.30 0.15 880 780 880 780 880 8.4 8.5 8.5 8.9 8.7 2.4 2.6 2.7 1.4 1.7 1.5 2.3 2.1 1.0 1.0 49.4 49.5 49.2 48.6 49.1 3.16 3.32 3.36 3.19 3.16 0.25 0.06 0.11 0.14 0.14 980 8.5 2.1 0.5 49.1 3.40 0.14 Center Spread ±0.5% Center Spread ±1.5% +3.3V, 25.000 MHz, group “R” oscillator parameter comparisons, Ta=25°C, CL=15 pF SSC Block Diagram: Spread spectrum technology can be simplified and expressed as follow. Modulation carrier frequency in KHz range ÷ Ref. Frequency Input ÷ Phase Detector ÷ ø Low Pass Filter VCO SSC output Title: Low EMI oscillators MERCURY www.mercury-crystal.com Product: HM series Date: March 3, 2004 Revision: 2 TN No.: TN-020 Page 7 of 7 Jitter Due to Frequency Modulation: Although the SST modulation is processed in the background and the modulation carrier is at least one thousand times slower compared with the nominal frequency, one still concerns the jitter contributed to the whole system due to the instantaneous frequency. A comparison between clocks with and without SST modulation shows that the modulation process contributes less than 0.05% of the cycle-to-cycle jitter to the system. This negligible jitter contribution makes the spread spectrum oscillators gain more popularity. Mercury 3HM57 series has 250 ps typical and 300 ps max. for the group “R” and ±100 ps max. for the group “P”. Concerns of using SSC on PLL Most of the PLLs can work with SST clocks without any timing problem. However, downstream PLLs (defined as PLLs that receive clock signal from other PLLs in the circuit) requires extra precaution in terms of tracking skew. There are PLLs (Zero delay buffers ) available in the market specifically designed to work with spread spectrum clocks. Another area to be concerned is the tracking rate of a PLL needs to be faster than the modulation rate of the SST. All Mercury HM series has modulation carrier frequency below 60 KHz, downstream PLLs with 6 u sec tracking capability will work fine. Power Supply to the SSC Power supply filtering plays important role to the EMI reduction and optimum jitter performance. Circuit below shows the recommended power supply filtering configuration. This lowpass “Ð (PI)” filter can remove power supply noise and prevent clock noise from feeding back to the supply. C1 is low frequency supply decoupling capacitor, a tantalum type and 22 uF is recommended. C2 is high frequency supply decoupling capacitor, a 0.1 uF ceramic chip capacitor is recommended. C3, a decoupling capacitor for the SSC, can be a 0.1 uF ceramic chip capacitor. If ferrite bead, C1 and C2 are not available, tantalum type capacitor is preferred for the C3. All capacitors should be placed as close to the SSC as possible, otherwise the increased trace inductance will negate its decoupling capability. Ferrite Bead System Power Supply ++ C1 22uF Tantalum Cap. C2 0.1uF Ceramic Chip Cap. C3 5.00±0.15 VDD to SSC Rs SSC Output 0.1uF Ceramic Chip Cap. Series Termination Resistor (Rs) SSC output traces over one inch should use series termination. The output impedance of group “P” and group “R” SSCs is 30 ohms. Therefore, for typical 50 ohm trace impedance boards, a 22 ohm chip resistor is recommended. 47 ohm is recommended for 75 ohm trace impedance boards. The series resistor should be placed in series with the clock line and as close to the SSC output pin as possible. The series resistor helps to maintain the signal integrity and enhance the EMI emissions reduction.