| Motore di ricerca datesheet componenti elettronici |
|
HMC1061LC5TR-R5 Scheda tecnica(PDF) 14 Page - Analog Devices |
|
|
|||||||||||||||||||||||||||||
HMC1061LC5TR-R5 Scheda tecnica(HTML) 14 Page - Analog Devices |
|
14 / 18 page ![]() HMC1061LC5 Data Sheet Rev. B | Page 14 of 18 Additionally, the common-mode output level may be adjusted within the range of approximately ±0.5 V by adjusting the VCCOB power supply according to the approximate relation VOCM = (VCCOB-2) ÷ 2 where VOCM is the output common mode voltage and VCCOB can be varied in the range of +1 V < VCCOB < +3 V. The bandwidth of the output amplifier that buffers the track- and-hold amplifier signal between the hold node and the 50 Ω outputs is approximately 7 GHz. The broad output buffer band- width is maintained to support the fast settling times required for users operating at high clock rates. However, because of the broad bandwidth, the output amplifier noise contribution to the total output noise is significant. Users operating at lower clock rates (such as < 1 GHz) may optimize their signal-to-noise ratio (SNR) by filtering the output to a lower bandwidth than the output amplifier bandwidth of 7 GHz. Such an output filter does not reduce the sampled front-end noise (which is frozen into the signal samples and represents the majority of the track-and-hold amplifier noise because of the wide front-end bandwidth) but it can reduce the output amplifier noise contribution. The user can filter the output to the lowest bandwidth that still retains the maximum settling time required to support the chosen clock rate. Typically this optimal bandwidth is of the order of 2 to 3 times the clock rate and it can be realized with a simple single-pole resistor circuit (RC) filter if desired (for example, a shunt capaci- tance on the outputs). A user operating at a clock rate of 350 MHz with a 1 GHz noise bandwidth output filter can achieve approxi- mately 1 dB lower noise relative to the unfiltered output condition. The output has very sharp transitions at the clock edges due to the broad output amplifier bandwidth. The user must be aware that any significant length of cable between the chip output and the load causes frequency response roll off and dispersion that can produce low amplitude tails with relatively long time constants in the settling of the output waveform into the load. This effect is most noticeable when operating in a lab setting with output cables of a few feet length, even with high quality cable. Output cables between the track-and-hold amplifier and the load must be of very high quality and 2 feet or less in length. Reflections between the load and the part degrades the hold mode response. The output cable length can be adjusted to minimize the reflection perturbations to some extent. In general, the round trip transit time of the cable must be an integer number of clock periods to obtain the minimal reflection perturbation in the hold mode portion of the waveform. The optimal perfor- mance is obtained when the track-and-hold amplifier is within 50 ps or less of the load since this gives a reflection duration equal to the approximate settling time of the device. In ADC applications, the track-and-hold amplifier must be placed as close as possible to the ADC to minimize reflection effects on the path between the track-and-hold output and the input of the ADC. LINEARITY MEASUREMENT When characterizing the linearity of a track-and-hold amplifier, the transfer function linearity of the held samples (referred to as track-and-hold mode linearity) is usually the quantity of most interest to the user. These samples contain the signal information that is ultimately digitized by the downstream ADC. A linearity measurement issue unique to the track-and-hold device is the need for output waveform frequency response correction. In the case of a dual rank track-and-hold amplifier, the output waveform resembles a square wave with duration equal to the clock period. Mathematically, the output can be viewed as the convolution of an ideal delta function sample train with a single square pulse of duration equal to one clock period. This weights the output spectral content with a sin(πf/fs)/(πf/fs)(Sinc) function frequency response envelope which has nulls at harmonics of the clock frequency, fs, and substantial response reduction beyond half the clock frequency. This spectral content and envelope function are observed during spectrum analyzer measurement because the analyzer simply reproduces the entire spectrum of the incoming waveform. However, the spectral content of the held samples without the envelope weighting is required for proper measurement of the linearity, as measured by a downstream ADC converter that samples a time instant in the held waveform. Either the impact of the response envelope must be corrected in the data, or a measurement method must be used that heterodynes the relevant nonlinear harmonic products to low frequencies to avoid significant envelope response weighting. This latter method is referred to as the low frequency beat product technique. The low frequency beat product technique is commonly used for high speed track-and-hold amplifier linearity measurements, although the measurement does impose restrictions on the specific input signal and clock frequencies that can be used. For example, with a clock frequency of 512.5 MHz, a single-tone input at 995 MHz beats with the second harmonic of the sampling frequency (through the sampling process) to produce a first-order beat product at 30 MHz. Likewise, the second and third harmonics of the input signal (generated via distortion in the track-and-hold amplifier) beat with the fourth and sixth harmonics of the sampling frequency, respectively, to produce second and third-order beat products at 60 MHz and 90 MHz. In this manner, the track-and-hold nonlinearity in the vicinity of 1 GHz can be measured even though the 995 MHz fundamental and the 1.99 GHz and 2.985 GHz nonlinear harmonics are well beyond the 256 MHz 4 dB bandwidth of the sinx/x response envelope. The possible input frequency choices are overly limited when the low frequency beat product technique is used at high clock rates. A related high frequency beat product measurement using correction for the sinx/x envelope weighting must be employed to measure linearity over a wide range of input frequencies. Analog Devices, Inc., uses both low frequency and high frequency beat product methods to measure linearity for a wide range of clock and signal frequencies. High frequency beat |
|
|
Link URL |
| Lei ha avuto il aiuto da alldatasheet? [ DONATE ] |
Di alldatasheet | Richest di pubblicita | contatti | Privacy Policy | Collegamento alla scheda tecnica | scambio Link | Ricerca produttore All Rights Reserved©Alldatasheet.com |
| Russian : Alldatasheetru.com | Korean : Alldatasheet.co.kr | Spanish : Alldatasheet.es | French : Alldatasheet.fr | Italian : Alldatasheetit.com Portuguese : Alldatasheetpt.com | Polish : Alldatasheet.pl | Vietnamese : Alldatasheet.vn Indian : Alldatasheet.in | Mexican : Alldatasheet.com.mx | British : Alldatasheet.co.uk | New Zealand : Alldatasheet.co.nz |
|
Family Site : ic2ic.com |
icmetro.com |