Rohde & Schwarz FSWP8 (1322.8003.09)

Fastest Measurement Speed

(Save time and multiply measurement throughput)

The internal FSWP source enable measurement of highly sensitive oscillators such as DROs and OCXOs with a minimum number of cross correlations, saving considerable time.

Adding hardware accelerated signal processing to the FSWP phase noise analyzer enables real-time phase noise measurements.

Short measurement time is key since it speeds up the development to manufacturing process while increasing production throughput.

Unrivaled Sensitivity

(Highest sensitivity for phase and amplitude noise measurement)

The FSWP internal local oscillator surpasses phase-noise performance of almost any signal generator available on the market.

Thanks to the internal low-noise analyzer sources, just a few correlations are needed to measure a high-quality oscillator.

This allow for the fastest possible measurement times.

Highest Flexibility

(High-end phase noise analyzer and signal and spectrum analyzer in a single box)

Users can examine the spectrum and demodulate the signal to measure EVM or pulse characteristics in different measurement channels.

Designers of automatic test systems save space and money since they do not have to purchase an additional spectrum analyzer or vector signal analyzer.

The FSWP is a future-proof investment. It is based on the high-end FSW with its unique RF performance and high sensitivity.

Phase Noise of Pulsed Signals

(Easy analysis of pulsed signal sources)

Measuring the phase noise of pulsed sources used in radar applications has never been easier.

The FSWP captures the signal and calculates all pulse parameters instantaneously.

It offers cross-correlation for phase noise tests and automatically determines the trigger/gating parameters required for pulsed source measurements.

Gating enables the FSWP to achieve a larger dynamic range for pulsed phase noise measurements compared to other methods.

Residual/Additive Phase Noise Measurements

(Residual PN measurements on pulsed and CW signals)

For high-end radar applications, knowing the additional phase noise added by individual components (e.g. amplifiers) to the signal path is crucial, since these influence pulse-to -pulse phase stability.

The components have to be tested using pulsed signals under real-world conditions.

The FSWP has an internal signal source for measuring residual phase noise or pulse-to-pulse phase stability and it also provides additional inputs for other external sources.

VCO Characterization Made Easy

(Measure VCO parameters automatically)

The FSWP features extremely low-noise internal DC sources to supply and control voltage-controlled oscillators (VCO).

The FSWP measures not only the fundamental voltage but also the power of higher VCO harmonics relative to the turning voltage.

It also displays phase noise at various offset frequencies relative to the tuning voltage.

Transient Analysis

(Frequency and phase measurements in the time domain)

The FSWP offers up to 8 GHz bandwidth for analyzing frequency or phase characteristics versus time.

The FSWP also offers narrowband analysis down to 40 MHz to examine the transient response of PLLs in detail.

Amplitude and Phase Noise in Parallel

(Simultaneous measurement of amplitude noise and phase noise)

The FSWO allows concurrent measurement of amplitude and phase noise up to a frequency offset of 30 MHz.

It displays both results simultaneously in a single window or in separate windows.

Allan Variance

(Allan variance calculation from close-in phase noise)

To characterize oscillator frequency stability, the FSWP calculates the Allan variance from the phase noise and displays it for up to 1 million seconds (minimum offset: 1 µHz).

Unlike the time domain methods, this makes it easy to suppress undesired side effects that appear as spurious emissions in the phase noise spectrum.

Even short-term disturbances due to the phase noise from internal sources can be easily suppressed with cross-correlation.

< –166 dBc (1 Hz)

(f = 1 GHz, 10 kHz offset)

< –166 dBc (1 Hz)

(f = 1 GHz, 10 kHz offset)

< –166 dBc (1 Hz)

(f = 1 GHz, 10 kHz offset)