The Agilent 1161A miniature passive probe is a small, rugged, general purpose probe for use with the Agilent 54835A, 54845A/B, and 54846A/B Infiniium oscilloscopes. It is fully compatible with the Agilent AutoProbe interface which completely configures the Agilent Infiniium oscilloscope for the probe.
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The Agilent 1159A is a FET input differential probe with 1 GHz bandwidth and greater than 19 dB CMRR (Common Mode Rejection Ratio) at 500 MHz. The 1159A offers the 1:1 attenuation, making it ideal for characterizing high bandwidth, low-voltage signals.
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The Agilent 1158A 4 GHz active probe offers R & D engineers the performance they need to probe small geometries in hard-to-reach areas on the DUT. These probes were designed specifically for the Infiniium Series oscilloscopes. As the speeds in your design increase, you may notice more overshoot, ringing, and other perturbations. when connecting an oscilloscope probe. Probes form a resonant circuit where they connect to the device. If this resonance is within the bandwidth of the oscilloscope probe you are using, it will be difficult to determine if the measurement perturbations are due to your circuit or the probe. Agilent is the only company that has overcome the resonance formed by the connection of a probe to a device. The Agilent 1158A probes optimize performance to make your job easier. Combined with the Agilent 54846A Infiniium scope, the 1158A 4 GHz probe offers you a full 2.25 GHz of system bandwidth, giving you accurate insight into your high-speed devices.
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The Agilent 1156A, 1157A, and 1158A family of active probes offers R & D engineers the performance they need to probe small geometries in hard-to-reach areas on the DUT. These probes were designed specifically for the Infiniium 54800 Series oscilloscopes. As the speeds in your design increase, you may notice more overshoot, ringing, and other perturbations when connecting an oscilloscope probe. Probes form a resonant circuit where they connect to the device. If this resonance is within the bandwidth of the oscilloscope probe you are using, it will be difficult to determine if the measurement perturbations are due to your circuit or the probe. Agilent is the only company that has overcome the resonance formed by the connection of a probe to a device. The Agilent 1156/7/8A probes optimize performance to make your job easier.
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The Agilent 1156A active probes offer R & D engineers the performance they need to probe small geometries in hard-to-reach areas on the DUT. These probes were designed specifically for the Infiniium Series, and 6000 Series 300 MHz – 1 GHz oscilloscopes. As the speeds in your design increase, you may notice more overshoot, ringing, and other perturbations when connecting an oscilloscope probe. Probes form a resonant circuit where they connect to the device. If this resonance is within the bandwidth of the oscilloscope probe you are using, it will be difficult to determine if the measurement perturbations are due to your circuit or the probe. Agilent is the only company that has overcome the resonance formed by the connection of a probe to a device. The Agilent 1156A probes optimize performance to make your job easier.
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The Agilent 1155A is a two-channel low mass active probe for Agilent Infiniium oscilloscopes. It combines a probe tip that weighs less than 1 gram with the superior performance of an active probe. It’s a powerful combination ideal for attaching to fine-pitch ICs and probing surface mount components.
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The Agilent 1154A is a FET input differential probe with 500 MHz bandwidth and greater than 40 dB CMRR (Common Mode Rejection Ratio) at 10 MHz. The 1154A offers the flexibility of 10X gain and 10:1 attenuation for a maximum of 100:1 attenuation.
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The Agilent 1153A is a 1:1 FET differential probe with 200 MHz bandwidth and 3000:1 CMRR (Common Mode Rejection Ratio) at 1 MHz. The probe has an input resistance of 1 MO and low input capacitance of 7 pF to minimize circuit loading.
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The Agilent 1152A active probe’s bandwidth, superior accuracy, and reliability make it an ideal companion for the Agilent 54845A 1.5 GHz bandwidth oscilloscope. The low input capacitance of the active probe eliminates distortion caused by excessive loading. As frequency increases, probe tip capacitance decreases the impedance of the probe by Xc=1/(2pi*fC), resulting in measurement error, depending on the source impedance of the output device. The Agilent 1152A’s low tip capacitance becomes a distinct advantage as frequency increases. Nonintrusive, reliable probing provides faithful reproduction of signals.
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