The InfiniiMax II Series 1168B 10 GHz probing system for Infiniium oscilloscopes provides full real-time bandwidth to 10 GHz. The award-winning InfiniiMax probing system supports even the most demanding mechanical access requirements without sacrificing performance.
With only 3.4:1 of attenuation ratio, the 1168A/69A provides the lowest probe noise floor among InfiniiMax probes, making it ideal for signal integrity measurements that require high sensitivity. The 1168A/69A probe system supports a wide variety of real-world applications with an extensive line up of probe heads and accessories. Unrivaled InfiniiMax probe accessories support browsing, solder-in, socketed, ZIF tip, QuickTip (magnetic tip), soft touch head and SMA head solutions with various options to choose from.
The 1168B is the RoHS compliant version of the 1168A. The 1168B is 100% form, fit, function and price equivalent to the 1168A.
Key Features |
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Bandwidth | 10 GHz |
Range | Dynamic Range: 3.3 V peak-to-peak
DC Offset Range: +/- 16V
Maximum Voltage: +/- 30V
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Input Impedance | Differential Input R: 50 kOhm
Differential Input C: 0.21 pF
Single Ended Input R: 25 kOhm
Single Ended Input C: 0.35 pF
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Recommended Probe Heads | MX0100A 25 GHz Micro Probe Head
MX0106A 23 GHz Solder-in Probe Head
MX0105A 20 GHz SMA Probe Head
N2839A 21 GHz Browser Probe Head
N5425B 18 GHz ZIF Probe Head
N2851A 12 GHz QuickTip Probe Head
E2678B 12 GHz Socketed Probe Head
N5381B 12 GHz Solder-in Probe Head
N5380B 12 GHz SMA Probe Head
E2677B 12 GHz Solder-in Probe Head
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Oscilloscope Connectivity | MXR, EXR oscilloscopes
S-Series oscilloscopes
90000A oscilloscopes
UXR 3.5mm oscilloscope with N5442A
UXR 1&1.85mm oscilloscope with N5442A and N2852A adapters
90000X, Q, V, Z-series oscilloscopes with N5442A
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Specifications |
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High-Frequency Differential Active Probes ≥ 10 GHz |
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Model Overview |
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Model | Bandwidth | Impedance Profile1 | Diff Input Impedance | Probe Noise2 | Probe-to-Scope Interface | InfiniiMode3 | Input Range | Probe Offset | Attenuation Range4 |
N2803A | 30 GHz | RCRC | 100 kΩ /0.32 pF
| 23.9 nV/rt(Hz) | AutoProbe2 | No | ±1.25 V
| ±16 V
| 6:1 |
MX0025A | 25 GHz | RC | 50 kΩ/0.17 pF | 25.0 nV/rt(Hz) | AutoProbe2 | Yes | ±2.5 V | ±16 V | 1:1/4:1/8:1 |
MX0023A | 25 GHz | RC | 50 kΩ/0.17 pF | 25.0 nV/rt(Hz) | AutoProbe2
| No | ±1.25 V | ±16 V | 1:1/4:1
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N2802A | 25 GHz | RCRC | 100 kΩ /0.32 pF | 23.9 nV/rt(Hz) | AutoProbe2
| No | ±1.25 V | ±16 V | 6:1 |
MX0024A | 20 GHz | RC | 50 kΩ/0.17 pF | 25.0 nV/rt(Hz) | AutoProbe2 | Yes | ±2.5 V | ±16 V | 1:1/4:1/8:1 |
N2801A | 20 GHz | RCRC | 100 kΩ /0.32 pF | 23.9 nV/rt(Hz) | AutoProbe2
| No | ±1.25 V | ±16 V | 6:1 |
N7003A | 20 GHz | RCRC | 100 kΩ /0.32 pF | 33.5 nV/rt(Hz) | AutoProbe2
| Yes | ±2.5 V | ±16 V | 5:1/10:1 |
MX0022A | 16 GHz | RC | 50 kΩ/0.17 pF | 25.0 nV/rt(Hz) | AutoProbe2 | Yes | ±2.5 V | ±16 V | 1:1/4:1/8:1 |
N7002A | 16 GHz | RCRC | 100 kΩ /0.32 pF | 33.5 nV/rt(Hz) | AutoProbe2
| Yes | ±2.5 V | ±16 V | 5:1/10:1
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MX0021A | 13 GHz | RC | 50 kΩ/0.17 pF | 25.0 nV/rt(Hz) | AutoProbe2 | Yes | ±2.5 V | ±16 V | 1:1/4:1/8:1 |
N7001A | 13 GHz | RCRC | 100 kΩ /0.32 pF | 33.5 nV/rt(Hz) | AutoProbe2
| Yes | ±2.5 V | ±16 V | 5:1/10:1 |
N2832A | 13 GHz | RCRC | 100 kΩ /0.32 pF | 33.5 nV/rt(Hz) | AutoProbe1
| Yes | ±2.5 V | ±16 V | 5:1/10:1 |
1169B | 13 GHz | RC | 50 kΩ /0.21 pF | 25.0 nV/rt(Hz) | AutoProbe1
| No | ±1.65 V | ±16 V | 3.45:1 |
MX0020A | 10 GHz | RC | 50 kΩ/0.17 pF | 25.0 nV/rt(Hz) | AutoProbe2 | Yes | ±2.5 V | ±16 V | 1:1/4:1/8:1 |
1168B | 10 GHz | RC | 50 kΩ /0.21 pF | 25.0 nV/rt(Hz) | AutoProbe1
| No | ±1.65 V | ±16 V | 3.45:1 |
Notes:
¹ Input Impedance Profile: RCRC architecture is the best choice for signals with low source impedance and RC architecture is the best choice for measuring signals that transition to low power modes because it has lower loading.
² Probe noise listed is the most common setup. Probe noise can vary with multiple factors such as attenuation ratio, probe head, and probe mode.
³ Measure differential, single-ended, and common mode signals.
⁴ Auto selected based on volts/division (all modes).