MPhil thesis of Lo Chi Wa - Department of Electronic & Computer ...

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(b) I+ output (b) Q+ output(a) I+ output (a) Q+ outputFig. 77 IQ outputs of coupled LC oscillators (a) without common source connection and (b) withconnectionQuadrature phase controlA better phase matching can be obtained for the quadrature outputs of the proposed LCoscillator due to the better-matched output amplitudes and the current interactionbetween the two oscillators.Matched output amplitudesThe four coupling transistors force the two oscillators to oscillate at the same frequencyand 90-degree out-of-phase. However, the quadrature phase can be maintained only ifthe amplitudes of the two oscillators are the same. A simple simulation using the circuitshown in Fig. 78 can show this. When the applied voltages at the coupling transistorsare not matched, the quadrature phase difference cannot be maintained. Since the outputamplitudes of the two oscillators, which share the same current source, are morematched, the four coupling transistors can maintain the quadrature phase better.To the outputs of the two identical LC oscillators1 1 A AFig. 78 Circuit to verify imperfect control of the phase for different IQ amplitudes82
Current interactionThe two oscillators can supply extra current for each other when more current is neededto enhance both oscillations if they oscillate at the same frequency with quadraturephase difference. This effect favors them to oscillate at the same frequency and with a90-degree phase difference than any other condition. This mechanism can be proved bytwo identical oscillators with only the current sources being connected together butwithout four coupling transistors. After startup, they can automatically oscillate with90-degree out-of-phase (Fig. 79). Another evidence is that a pair of coupled oscillatorswith shared current source can always form the quadrature relationship between theoutputs much faster as shown in Fig. 80.Fig. 79 Output voltage waveform of two LC oscillators with common source node connection only83
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A 1.5-V 900-Mhz Monolithic CMOSFast
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A 1.5-V 900-Mhz Monolithic CMOS Fas
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Table of ContentsPageAcknowledgment
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Testing setup......................
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List of FiguresPageFig. 1 Block dia
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Fig. 76 Amplitudes and currents of
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Chapter 1 IntroductionBackgroundWir
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applications because it can provide
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existing monolithic frequency synth
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the receiver frequency band is from
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out-of-bandin-bandout-of-band0dBmin
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Based on the maximum interference,
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carrierdBcspur∆fFig. 8 Frequency
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Spurs requirement (dBc)Frequency of
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The frequency diversity can be perf
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Chapter 3 System DesignPhase-locked
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coarse tuning can be provided by th
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array is now possible. Moreover, th
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performance of the synthesizer 9 .
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signalquantizationnoisea) f b)signa
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esolution. The loop bandwidth is 80
Page 43 and 44: the output value between 0 and 0.5,
Page 45 and 46: The coupled-LC oscillators can be v
Page 47 and 48: 890MHzf25MHz243KHz865MHzFig. 23 Tun
Page 49 and 50: onoffCwellClinearCwellClinearCwellC
Page 51 and 52: spirals of similar sizes is around
Page 53 and 54: in Fig. 27a and Fig. 27b, the same
Page 55 and 56: conductance (Gm) and the reciprocal
Page 57 and 58: −19⎛ 900M⎞0.0259×1.6×10 ×
Page 59 and 60: GdoVinFig. 32 Gdo of the proposed L
Page 61 and 62: RzCzIcpCpR4C4a)IcpCzR4B.IcpCpRpC4b)
Page 63 and 64: Usually, capacitors in the filter o
Page 65 and 66: RVinFig. 38 Resistance of NMOS resi
Page 67 and 68: feedback path to prevent the proble
Page 69 and 70: 890MHz25MHz865MHzfA+∆A
Page 71 and 72: High-speed multi-modulus dividerThe
Page 73 and 74: CLKQBQDDBFig. 50 Schematic diagram
Page 75 and 76: ANDgateABclkclkclkclkQBFig. 54 Sche
Page 77 and 78: f o/2 /2,3 /2,3 /2 /2f div/4Combina
Page 79 and 80: next stage, as shown in the Fig. 59
Page 81 and 82: co10bDclkclkFig. 60 Schematic of th
Page 83 and 84: (1-Z -1 ) 23bDQBclkZ -1 (1-Z -1 )2b
Page 85 and 86: X 16clkDclkQBDclkQBFig. 66 Schemati
Page 87 and 88: ~90 oa) b) c)Fig. 68 Different meth
Page 89 and 90: (dotted line). As the oscillation c
Page 91 and 92: In practice, it is not desirable to
Page 93: and decrease in amplitude mismatch
Page 97 and 98: equirements. Fortunately, by connec
Page 99 and 100: LC oscillators are put apart to red
Page 101 and 102: Gain mismatch (in %)Two oscillators
Page 103 and 104: equals to1 . By doubling the height
Page 105 and 106: 30 is obtained. It is because the s
Page 107 and 108: The spiral inductor is designed and
Page 109 and 110: oscillators (shown in the upper and
Page 111 and 112: Synthesizer LayoutThe layout and th
Page 113 and 114: Die LayoutFig. 98 shows the die pho
Page 115 and 116: Testing setupThe testing setup show
Page 117 and 118: Resistance (ohms)Freq (Hz)Fig. 101
Page 119 and 120: Resistance (ohms)Freq (Hz)Fig. 105
Page 121 and 122: VaractorFig. 109 shows the testing
Page 123 and 124: Table 5 Summary of parameters of va
Page 125 and 126: Table 6 Summary of N-well substrate
Page 127 and 128: Fig. 120 Quality factor of the swit
Page 129 and 130: The decrease in quality factor is d
Page 131 and 132: Fig. 126 Schematic diagram of the p
Page 133 and 134: Output frequency(MHz)Number of swit
Page 135 and 136: Gain (MHz/V)Tuning voltage (v)Fig.
Page 137 and 138: on the process variation. Therefore
Page 139 and 140: voltage (Vos = Rp x Ios) appeared.
Page 141 and 142: Although the spurs are quite large,
Page 143 and 144: GMSK signals with 0.3 BT and a bit
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Power spectral density (dB)(b)(a)(c
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Summary of performanceA summary of
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Table 10 Comparison of performances
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As the voltage-controlled oscillato
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Bibliography1 Thomas H. Lee, The De
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