PicoScope 9000 系列采样示波器

先进功能
 

12 GHz带宽 PicoScope 9200A采样示波器采用顺序采样技术来测量快速重复信号而无需昂贵的实时采样硬件。包含一个12 GHz 的输入带宽，使之能够捕获上升时间为50 ps或更快的信号。精确的时基稳定性和精度，和200 fs 的分辨率，允许大多数高要求应用项目中抖动的特性。 紧凑和轻便 PicoScope 9200A 采样示波器使用我们PC示波器的架构设计出一款紧凑又轻量的仪器，可轻松放入你的电脑包。 10 GHz  prescaled 触发 PicoScope 9200A 采样示波器有一个内置的高频触发器和频率除法器。它的常规带宽达到 10 GHz  可测量具有超快数据速率的微波器件。 1 GHz全功能直接触发 该采样示波器有一个内置的直接触发器用于达到1 GHz重复率的信号而无需附加的触发器。 内置 2.7 Gb/s 时钟恢复 PicoScope 9211A, 9221A, 和 9231A 有一个专用的时钟恢复触发输入用于串行数据12.3 Mb/s  至 2.7 Gb/s。 脉冲参数测量 PicoScope 9200A 采样示波器可快速测量超过40个脉冲参数，所以你不需要数格子数和估算波形的位置。高达10个同时测量项或4个统计测量项可同时进行。这些测量项符合 IEEE 标准。 光转电转换器 PicoScope 9221A 和 9231A 有一个内置的8 GHz的光电转换器。可用于分析光信号例如SONET/SDH OC1 至 OC48, 光纤通道 FC133 至 FC4250, 和 G.984.2。该转换器输入接受单模式 (SM) 和多模式 (MM) 光纤，并且波长范围 750 至 1650 nm。 Bessel-Thomson 滤波器可单独购买。它用于特定光纤标准。
强大的数学分析 PicoScope 9000同时支持4个所采集波形的数学组合和函数转换。 你可以选择任何数学函数作为一个运算符施予操作数。一个波形的数学运算符是一个数学函数，要求一个或者两个源。包含两个波形源的运算符是：加，减，乘和除。包含一个波形源的运算符是：反数，绝对值，指数，对数，微分，积分，反函数，FFT，插值，光滑函数。观看视频 >
柱状图分析 柱状图是一个概率分布用于显示所采集数据的分布，显示在用户自定义的柱状图视窗内。柱状图收集的信息被用于做统计分析。 柱状图可以在波形上以垂直坐标或水平坐标构建。垂直柱状图最常用于测量和描绘所显示波形上的噪音，而水平柱状图最长用于测量和描绘所显示波形上的抖动。观看视频 >
眼图分析 PicoScope 9000系列快速测量超过30个基本参数用于绘制不归零 (NRZ)信号和归零 (RZ)信号的特性曲线。可以同时测量4个参数。观看视频 > 波罩测试 对于眼图波罩，例如SONET和SDH标准所指定的哪些，PicoScope 9000支持在板波罩显示以便可视化比较。可显示灰度或色阶以帮助分析眼图上的噪音和抖动。观看视频 >
FFT分析 所有PicoScope 9000系列采样示波器都能用一系列开窗函数对输入信号进行2个快速傅立叶变换。FFT特别适用于查找串扰问题，查找非线性放大器引起的模拟波形上的失真问题，调整滤波器电路用于过滤掉波形上的某些谐波，测试系统的脉冲响应，和识别与定位噪音和干扰源。观看视频 >     码型同步触发和眼线模式 PicoScope 9211A, 9221A 和 9231A 可内部生成一个码型同步触发，由比特率，码型长度，和触发分割率导出。使之能够从任何特定的位或位群按顺序创建一个眼图。 眼线模式适用于码型同步触发来隔离8个可能路径中的任何一个，称之为眼线，信号可经过整个眼图。这使仪器能够显示平均的眼图展现一个特定的眼线。观看视频 >

软件开发包

PicoScope 9000 软件可用作一个独立的示波器程序和一个ActiveX 控件。ActiveX 控件符合 Windows COM 模型，并且能够嵌入你的软件内。有Visual Basic (VB.NET), LabVIEW 和 Delphi的例程提供给你。但是任何支持COM标准的编程语言或标准都可使用，包括 JavaScript 和 C。

我们提供全面的编程指导书，详细说明了ActiveX 控件的每个功能。

SDK 可通过USB或LAN口控制示波器。

记住：你购买 PicoScope 采样示波器的钱已经包含了所有这些 - 我们不会为软件的功能或升级再收你的钱。

PicoScope 9211A和9231A TDR/TDT示波器专门用于时域反射(TDR)和时域透射(TDT)。它是一种低成本的测试方法，可测试线缆，连接器，电路板和IC包的不想要的反射和损耗。

PicoScope 9211A和9231A 发射脉冲到所测试的设备内，使用它的两个独立的可编程的，100-ps上升时间阶梯发生器中的一个。然后使用它的12 GHz采样输入，建立一个来自反射或者透射的脉冲的照片。结果可以显示为伏特，欧姆或者rho对时间或者距离。

下图显示PicoScope 9211A的TDR功能，用于分析一系列PCB间距5 mm上的via-holes。

提示: 你购买PicoScope采样示波器的价格包含所有功能 - 我们不会为软件的功能或者升级再向你收费。

注释: 只是PicoScope 9211A和9231A才有TDR和TDT测量和分析功能。

1. PicoScope 9200采样示波器与常规数字存储示波器有什么不同?

2. PicoScope 9201A/9211A是一个数字信号分析仪(DSA)吗?

3. 实时采样率和等效采样率之间有什么不同?

4. 我能把PicoScope 9201A/9211A用作常规测试和测量项目吗?

5. 直接触发和HF触发输入之间有什么不同?

6. 柱状图功能用来做什么?

7. 这么低的价格是否还有其它费用?

PicoScope 9200采样示波器与常规数字存储示波器有什么不同?

All digital storage oscilloscopes (DSOs) work by sampling the input signal. The standard type of DSO uses “real-time sampling”, which is illustrated in Fig. 1.

Fig. 1 – Real-time sampling. (a) The original signal. (b) The scope samples the signal in several places. (c) The samples are stored in memory. (d) The scope reconstructs the signal using the stored samples. (Straight-line interpolation is shown here, but other methods exist.)

A sampling oscilloscope is a special type of DSO that exclusively uses a technique called “sequential equivalent-time sampling” or just “sequential sampling”. This type of sampling is best suited to repetitive waveforms such as serial data streams, clock waveforms and pulses in digital circuits, some of the data patterns used in semiconductor testing, and amplifier pulse-response and rise-time tests. A sampling scope captures just one sample from one cycle of the waveform and then repeats the process over a large number of cycles, varying the timing of the sample in a known pattern from one sample to the next. The resulting collection of samples is then assembled into a picture of the whole waveform.

Fig. 2 – Sequential sampling. (a) One sample is taken from each of a number of similar waveforms. (b) The samples are assembled to form a composite waveform.

The advantage of a sampling scope is that its analogue-to-digital
converter (ADC) only needs to be fast enough to capture one
sample in each cycle of the waveform, rather than the tens or
hundreds of samples that a real-time scope would require. This
allows the scope to capture waveforms with much higher
bandwidths, up to 12 GHz in the case of the PicoScope 9201A/9211A,
and to capture each sample with higher precision. A real-time
DSO that could capture a single cycle of the same 12 GHz
waveform would be prohibitively expensive. For example the
12 GHz Agilent DSO91204A, with a real-time sample rate of
40 GS/s, has a base price of $96,000 – 8 times the price of the
PicoScope 9201A/9211A.

PicoScope 9201A/9211A是一个数字信号分析仪(DSA)吗?

Yes. Some manufacturers use that term for sampling scopes that are aimed at the digital signal market. We chose to call the PicoScope 9201A/9211A a sampling oscilloscope because it can do more than just measure digital signals: it can also be used to analyse repetitive analogue waveforms.

实时采样率和等效采样率之间有什么不同?

The real-time sampling rate of an oscilloscope is the rate at which its ADC can reliably sample the input waveform. If you wish to capture a single event such as a one-off glitch in a digital circuit, then the oscilloscope has only one chance to acquire enough samples to represent the waveform accurately. In such cases, there is no substitute for an oscilloscope with a high real-time sampling rate. A common rule of thumb is that at least 10 samples are needed for each cycle of the waveform. For example, if the signal in question is a 2 GHz square wave, then a scope with a real-time sampling rate of at least 20 GS/s would be needed to capture a realistic-looking picture. For accurate analysis of the timing and shape of the waveform, as required in mask testing, several hundred samples are needed. This would entail a real-time sampling rate of 200 GS/s or more, which is beyond the capabilities of today's off-the-shelf instruments and, even if such a scope existed, it would be prohibitively expensive.

The equivalent-time sampling (ETS) speed of a scope is not a measure of the speed of its ADC, but an estimate of the speed of an imaginary ADC that could capture a single-shot waveform at the same timebase, and with the same number of samples, as the sampling scope in question. If a sampling scope had perfectly accurate timing, then it could achieve an ETS rate as large as you wished just by waiting for the necessary number of cycles of the input waveform to pass by. In real life, however, the ETS rate of the scope is limited by the timing and trigger circuitry. The smaller the timing uncertainty (called jitter), the more non-overlapping samples the scope can take to form the final picture, and therefore the higher the equivalent-time sampling rate. Thanks to its low jitter, the PicoScope 9201A/9211A has a maximum ETS rate of 5 TS/s.

Many of today's DSOs list both real-time and equivalent-time, or sequential, sampling rates in their specifications. When choosing an oscilloscope, you need to make sure that both sampling rates are adequate for your application.

我能把PicoScope 9201A/9211A用作常规测试和测量项目吗?

The PicoScope 9201A/9211A is not intended to replace the general-purpose oscilloscope on your workbench. The main differences between the PicoScope 9201A/9211A and a general-purpose scope are as follows:

• SMA input connectors . General-purpose scopes usually have BNC connectors on their inputs, but these connectors do not have a well-defined impedance above about 2 GHz. SMA connectors are better suited to high-frequency signals and are widely used in microwave applications.

• 50 ohm inputs . The PicoScope 9201A/9211A has low-impedance inputs that do not work with passive high-impedance scope probes but work well with low-impedance probes. The low input impedance is necessary to match the scope to standard high-frequency signal cables and connectors without causing reflections. Most instruments designed for signals above about 500 MHz have input and output impedances of 50 ohms.

• ±2 volt safe input range . The sensitive, high-bandwidth input circuitry of the PicoScope 9201A/9211A does not allow the same wide range of input voltages as found on a general-purpose scope. If your signal is larger than ±1 volt (the maximum measuring range) then you must use an external attenuator. You must also protect the inputs against electrostatic discharges.

• 100 kS/s real-time sampling . The PicoScope 9201A/9211A is not designed to be used as a real-time sampling oscilloscope. Its precision ADC is optimised for equivalent-time sampling with very low jitter, allowing an equivalent-time sampling rate of up to 5 TS/s for repetitive signals.

• Dedicated software . The software supplied with the PicoScope 9201A/9211A is designed to work only with sampling oscilloscopes. It contains advanced display features such as eye diagrams and histograms, and specialised measurements and industry-standard mask tests that do not apply to real-time oscilloscopes. This software is very different from PicoScope 6, our general-purpose oscilloscope software, in both appearance and function, and data files cannot be exchanged between the two programs.

直接触发和HF触发输入之间有什么不同?

The Direct Trigger is a full-function trigger input with a bandwidth of 1 GHz, and is applied
directly to the trigger circuitry. This input allows variable slope, hysteresis and trigger level.
The HF Trigger input passes through an internal prescaler before being applied to the trigger
circuitry. This input has a higher bandwidth, up to 10 GHz, but lacks the adjustments available
on the Direct Trigger input.

柱状图功能用来做什么?

The PicoScope 9201A/9211A can collect large numbers of waveforms
and perform statistical analysis on them. The results of the
analysis can be displayed as histograms against voltage
(vertical histograms) or time (horizontal histograms).
A vertical histogram shows how much time the signal spends
at each voltage level, and is useful for visualising RMS
noise and noise margins; while a horizontal histogram
shows how fast the signal voltage changes during each
time interval, and shows RMS jitter and timing margins.
Histograms help you to visualise the quality of your signal,
but if you prefer you can also get statistics in numerical
form by using the built-in statistics functions.
 

这么低的价格是否还有其它费用?

There are no hidden extra costs. When you buy a PicoScope 9201A/9211A, you get a complete system: the front-end hardware to plug into your USB port, a mains power adapter, and Windows-based software for your PC. You just provide the computer. You also get valuable extra services: free, time-unlimited support from our technical specialists, and free software updates for as long as we continue to support the product.

Of course, every lab needs more than just a scope. You will need cables, connectors, and possibly coaxial splitters and attenuators, but these are all application-specific and you are likely to have them on your shelf anyway. To keep costs down, the PicoScope 9201A/9211A kit does not include probes, which are not needed if you have a 50-ohm signal source.

9000系列采样示波器附件

下列附件特别适用于PicoScope 9200采样示波器。(它们也适用于其它带SMA输入接头的高频示波器)

TA061: 1.5 GHz 示波器探头 x10

Features:

• Small size - 2.5 mm diameter at the probe tip

• New IC contact system for 0.5 to 1.27 mm pitch

• Interchangeable spring contact tip

• Ideal for measurements of SMT components

• Coaxial design

• Low input capacitance

A range of kits containing accessories and spare parts for the TA061 are available.

 ,

TA077: 3dB SMA-SMA Attenuator

Typical performance: Frequency (MHz) Attenuation (dB) Return loss (dB) 0.03 3.02 56.17 50.00 3.00 52.32 100.00 3.00 46.96 500.00 3.05 36.37 1000.00 3.10 32.48 2000.00 3.19 31.52 3000.00 3.31 35.67 4000.00 3.43 26.35 5000.00 3.58 19.50 6000.00 3.81 15.77   TA078: 6dB SMA-SMA Attenuator Typical performance: Frequency (MHz) Attenuation (dB) Return loss (dB) 0.03 6.06 47.85 50.00 6.01 52.94 100.00 6.02 47.09 500.00 6.10 38.55 1000.00 6.15 34.41 2000.00 6.23 34.50 3000.00 6.33 39.05 4000.00 6.39 24.30 5000.00 6.52 18.08 6000.00 6.94 14.73   TA140: 10 dB  SMA–SMA Attenuator Features: DC to 6,000 MHz 50 Ω, 1 W RoHS compliant Typical performance: Frequency (MHz) Attenuation (dB) VSWR(:1) 0.03 10.06 1.00 50.00 10.01 1.01 100.00 10.02 1.00 500.00 10.06 1.01 1000.00 10.06 1.02 2000.00 10.01 1.03 3000.00 9.89 1.07 4000.00 9.60 1.19 5000.00 9.51 1.31 6000.00 9.69 1.50   TA141: 20 dB  SMA–SMA Attenuator Features: DC to 6,000 MHz 50 Ω, 0.5 W RoHS compliant Typical performance: Frequency (MHz) Attenuation (dB) VSWR(:1) 0.03 20.08 1.01 20.00 20.03 1.00 50.00 20.01 1.00 100.00 20.02 1.00 500.00 20.11 1.00 1000.00 20.21 1.01 2000.00 20.32 1.06 3000.00 20.10 1.11 4000.00 19.53 1.17 5000.00 18.63 1.24     TA079: 4.2GHz 2 Way-0° Power Splitter/Combiner Features: Very wideband, DC to 4200 MHz Low insertion loss, 0.1 dB typical Excellent amplitude unbalance, 0.02 dB typical Rugged shielded case TA079 Specifications Frequency range DC to 4200 MHz Isolation DC to 100 MHz 100 MHz to fu/2 fu/2 to fu 6.2 dB Typical 6.5 dB Typical 7.0 dB Typical Insertion loss DC to 100 MHz 100 MHz to fu/2 fu/2 to fu Typical 0.1 dB 0.1 dB 0.4 dB Maximum 0.2 dB 0.5 dB 1.4 dB Phase unbalance DC to 100 MHz 100 MHz to fu/2 fu/2 to fu 1° maximum 3° maximum 5° maximum Amplitude unbalance DC to 100 MHz 100 MHz to fu/2 fu/2 to fu 0.1 dB maximum 0.2 dB maximum 0.5 dB maximum Impedance 50 Ω Operating temperature -55 °C to 100 °C Storage temperature -55 °C to 100 °C Power input (as a splitter) 750 mW maximum Internal dissipation 375 mW maximum Compliance RoHS compliant Note: fu = upper frequency.   Bessel–Thomson Reference Receiver Filters For use with the optical–to–electrical converter on the PicoScope 9221A and 9231A Reduces peaking and ringing Choice of filter depends on the bit rate of the signal under analysis Cat No Bit Rates TA120 51.8 Mb/s  (OC1/STM0) TA121 155 Mb/s  (OC3/STM1) TA122 622 Mb/s  (OC12/STM4) TA123 1.250 Gb/s  (GBE) TA124 2.488 Gb/s  (OC48/STM16) / 2.500 Gb/s  (Infiniband 2.5G)