normalized phase noise in ultracmos devices - psemi · the phase noise is very close to the...

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Phase Noise is a measure of the spectral purity of a signal in an oscillator system. It quantifies the short-term random variation of the frequency of the signal, and is a product of thermal noise and low frequency flicker noise within the system. Most RF systems require an overall integrated phase noise specification to be met, as phase noise can corrupt both the up-converted and down-converted signal paths. For digital systems, the integrated phase noise can be converted and expressed as phase jitter. In the frequency domain, phase noise is typically quantified at various frequency offsets from the carrier frequency. Expressed as a ratio in units of dBc/Hz, the noise power in a 1 Hz bandwidth is measured at each offset frequency and divided into the carrier power. If noise sidebands on either side of the carrier are measured, the phase noise at each offset can be expressed as a double-sideband value instead of a single-sideband value. Phase Noise in PLL Frequency Synthesizers A frequency synthesizer is used to generate multiple output frequencies from a single reference frequency. Used in a Phase-Locked Loop (PLL), a divided down output can be compared to a scaled reference, generating an error signal that drives the loop to achieve both frequency and phase lock (Fig 1). W hat is Phase Noise? Figure 1. Block Diagram of PLL Frequency Synthesizer Loop Filter VCO f VCO f c Crystal Reference REF divider ÷R Main divider ÷N Phase detector Phased-Locked Loop (PLL) phase noise is shaped by several noise contributors including reference noise, phase detector noise, and VCO noise. The loop bandwidth defines the range over which the output tracks the input. Within the loop bandwidth, the phase detector drives the VCO to track the reference, and the phase detector noise dominates the overall phase noise. At very large-frequency offsets, outside the loop bandwidth, the loop does not track the reference and the VCO noise dominates the overall phase noise. Ideally, the PLL loop bandwidth is designed so that the phase detector noise floor equals the free-running VCO noise. Normalized Phase Noise in UltraCMOS ® Devices Low Phase Noise

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Phase Noise is a measure of the spectral purity of a signal in an oscillator system. It quantifies the short-term random variation of the frequency of the signal, and is a product of thermal noise and low frequency flicker noise within the system. Most RF systems require an overall integrated phase noise specification to be met, as phase noise can corrupt both the up-converted and down-converted signal paths. For digital systems, the integrated phase noise can be converted and expressed as phase jitter.

In the frequency domain, phase noise is typically quantified at various frequency offsets from the carrier frequency. Expressed as a ratio in units of dBc/Hz, the noise power in a 1 Hz bandwidth is measured at each offset frequency and divided into the carrier power. If noise sidebands on either side of the carrier are measured, the phase noise at each offset can be expressed as a double-sideband value instead of a single-sideband value.

Phase Noise in PLL Frequency SynthesizersA frequency synthesizer is used to generate multiple output frequencies from a single reference frequency. Used in a Phase-Locked Loop (PLL), a divided down output can be compared to a scaled reference, generating an error signal that drives the loop to achieve both frequency and phase lock (Fig 1).

What is Phase Noise?

Figure 1. Block Diagram of PLL Frequency Synthesizer

LoopF ilter VC O

fVC O

fc

C rys ta lR eference

R EF d ivider÷R

Main d ivider÷N

Phasedetec tor

Phased-Locked Loop (PLL) phase noise is shaped by several noise contributors including reference noise, phase detector noise, and VCO noise. The loop bandwidth defines the range over which the output tracks the input. Within the loop bandwidth, the phase detector drives the VCO to track the reference, and the phase detector noise dominates the overall phase noise. At very large-frequency offsets, outside the loop bandwidth, the loop does not track the reference and the VCO noise dominates the overall phase noise. Ideally, the PLL loop bandwidth is designed so that the phase detector noise floor equals the free-running VCO noise.

Normalized Phase Noisein UltraCMOS® Devices

Low Phase Noise

the phase noise is very close to the calculated value. At this point in the loop, the 1/f noise has rolled off and the phase detector noise is the dominant contributor.

For a given normalized phase noise, the phase detector phase noise can be reduced by 3 dB by doubling the comparison frequency:

With fvco = 4 GHz and fc = 100 MHz, the phase detector phase noise can be calculated as

Phase Detector Phase Noise (dBc/Hz) = -230 dBc/Hz + 10log (100 MHz) + 20log (4 GHz/10 MHz) = -118 dBc/Hz

In this fashion, the user can easily make tradeoffs to determine if the PLL can meet the overall phase noise requirements.

Reference: Peregrine Semiconductor Application Note 16:“Using Peregrine Phase-Locked Loop Integrated Circuits in Reference and System Clock Applications."

http://www.psemi.com/pdf/app_notes/an16.pdf

Figure 2. Typical Phase Noise for the PE33241. VDD = 2.8 V, Temp = 25oC, fvco = 4 GHz, fc = 50 MHz, Loop Bandwidth = 500 kHz

Normalized Phase NoiseOften datasheets, selection guides, or technical collateral from PLL component vendors advertise phase noise Figures of Merit (FOM). Peregrine Semiconductor uses normalized phase noise in benchmarking its PLL products. By normalizing the phase detector noise floor to 1 Hz, the phase noise within the loop bandwidth (dominated by the phase detector) can be easily calculated for any comparison frequency and VCO frequency. The mathematical relationship is specified as follows:

Phase Detector Phase Noise (dBc/Hz) = Normalized Phase Detector Noise Floor (dBc/Hz) +10log (fc) + 20log (N)

where

fc = comparison frequencyfvco = VCO output frequencyN = fvco/fc

Take for example, the PE33241 5 GHz Integer-N PLL synthesizer. Fabricated in UltraCMOS® technology, the PE33241 enables low phase noise frequency synthesizers for specialized applications. The datasheet specifies a FOM

Floor of -230 dBc/Hz, a

significant improvement over prior generations. The EVK reference design can be used to calculate the phase noise as follows:

With fvco = 4 GHz and fc = 50 MHz,

Phase Detector Phase Noise (dBc/Hz) = -230 dBc/Hz + 10log (50 MHz) + 20log(4 GHz/50 MHz) = -115 dBc/Hz

Figure 2 shows the measured phase noise for the standard EVK reference design.

Observing the plot at a frequency offset within loop where the phase detector noise dominates (100 kHz),

© 2013 Peregrine Semiconductor Corporation. All rights reserved. The Peregrine name, logo and UltraCMOS are registered trademarks, and HaRP and DuNE are trademarks of Peregrine Semiconductor Corporation. All other trademarks are the property of their respective owners. All information on these pages are subject to change without notice. Consult website for latest specifications. Peregrine products are protected under one or more of the following U.S. Patents: http://patents.psemi.com

100 100K

Frequency O�set (Hz)

Typical Phase Noise for PE97240

Phas

e N

oise

(dBc

/Hz)

1M 10M 100M

-80

-90

-100

-110

-120

-130

-140

-160

-70

-150

-1701K 10K

PE33241 Integer-N PLL � Normalized phase noise floor figure of merit: -230 dBc/Hz

� Low power consumption of 80 µA @ 2.8 V

� Dual modulus prescaler: 10/11 to 5 GHz and 5/6 to 4 GHz