JAJSDE6 June   2017 LMH6624-MIL

PRODUCTION DATA.  

  1. 1 特長
  2. 2 アプリケーション
  3. 3 概要
  4. 4 改訂履歴
  5. 5 Pin Configuration and Functions
  6. 6 Specifications
    1. 6.1 Absolute Maximum Ratings
    2. 6.2 ESD Ratings
    3. 6.3 Recommended Operating Conditions
    4. 6.4 Thermal Information
    5. 6.5 Electrical Characteristics ±2.5 V
    6. 6.6 Electrical Characteristics ±6 V
    7. 6.7 Typical Characteristics
  7. 7 Detailed Description
    1. 7.1 Overview
    2. 7.2 Feature Description
      1. 7.2.1 Bias Current Cancellation
      2. 7.2.2 Total Input Noise vs Source Resistance
      3. 7.2.3 Noise Figure
      4. 7.2.4 Low-Noise Integrator
      5. 7.2.5 High-Gain Sallen-Key Active Filters
      6. 7.2.6 Low-Noise Magnetic Media Equalizer
    3. 7.3 Device Functional Modes
      1. 7.3.1 Single Supply Operation
  8. 8 Application and Implementation
    1. 8.1 Application Information
    2. 8.2 Typical Application
      1. 8.2.1 Design Requirements
      2. 8.2.2 Detailed Design Procedure
      3. 8.2.3 Application Curve
  9. 9 Power Supply Recommendations
  10. 10Layout
    1. 10.1 Layout Guidelines
    2. 10.2 Layout Example
  11. 11デバイスおよびドキュメントのサポート
    1. 11.1 ドキュメントのサポート
      1. 11.1.1 関連資料
    2. 11.2 ドキュメントの更新通知を受け取る方法
    3. 11.3 コミュニティ・リソース
    4. 11.4 商標
    5. 11.5 静電気放電に関する注意事項
    6. 11.6 Glossary
  12. 12メカニカル、パッケージ、および注文情報

パッケージ・オプション

メカニカル・データ（パッケージ｜ピン）
  • Y|0
サーマルパッド・メカニカル・データ
発注情報

8 Application and Implementation

NOTE

Information in the following applications sections is not part of the TI component specification, and TI does not warrant its accuracy or completeness. TI’s customers are responsible for determining suitability of components for their purposes. Customers should validate and test their design implementation to confirm system functionality.

8.1 Application Information

A transimpedance amplifier is used to convert the small output current of a photodiode to a voltage, while maintaining a near constant voltage across the photodiode to minimize non-linearity. Extracting the small signal requires high gain and a low-noise amplifier, and therefore, the LMH6624-MIL device is ideal for such an application in order to maximize SNR. Furthermore, because of the large gain (RF value) needed, the device used must be high speed so that even with high-noise gain (due to the interaction of the feedback resistor and photodiode capacitance), bandwidth is not heavily impacted.

Figure 39 implements a high-speed, single supply, low-noise transimpedance amplifier commonly used with photo-diodes. The transimpedance gain is set by RF.

8.2 Typical Application

LMH6624-MIL modified_sbd_v6.gif Figure 49. Application Schematic

8.2.1 Design Requirements

Figure 50 shows the Noise Gain (NG) and transfer function (I-V Gain). As with most transimpedance amplifiers, it is required to compensate for the additional phase lag (noise gain zero at fZ) created by the total input capacitance: CD (diode capacitance) + CCM (CM input capacitance) + CDIFF (DIFF input capacitance) looking into RF. This is accomplished by placing CF across RF to create enough phase lead (Noise Gain pole at fP) to stabilize the loop.

LMH6624-MIL 30068002.gif Figure 50. Transimpedance Amplifier Noise Gain and Transfer Function

8.2.2 Detailed Design Procedure

The optimum value of CF is given by Equation 8 resulting in the I-V –3dB bandwidth shown in Equation 9, or around 124 MHz in this case, assuming GBWP = 1.5 GHz, CCM (CM input capacitance) = 0.9 pF, and CDIFF (DIFF input capacitance) = 2 pF. This CF value is a “starting point” and CF needs to be tuned for the particular application as it is often less than 1 pF and thus is easily affected by board parasitics.

Optimum CF Value:

Equation 8. LMH6624-MIL 30068039.gif

Resulting –3dB Bandwidth:

Equation 9. LMH6624-MIL 30068040.gif

Equation 10 provides the total input current noise density (ini) equation for the basic transimpedance configuration and is plotted against feedback resistance (RF) showing all contributing noise sources in Figure 51. The plot indicates the expected total equivalent input current noise density (ini) for a given feedback resistance (RF). This is depicted in the schematic of Figure 52 where total equivalent current noise density (ini) is shown at the input of a noiseless amplifier and noiseless feedback resistor (RF). The total equivalent output voltage noise density (eno) is ini*RF. Noise Equation for Transimpedance Amplifier:

Equation 10. LMH6624-MIL 30068037.gif
LMH6624-MIL 30068028.gif Figure 51. Current Noise Density vs Feedback Resistance
LMH6624-MIL 30068012.gif Figure 52. Transimpedance Amplifier Equivalent Input Source Mode

From Figure 53, it is clear that with the LMH6624-MIL extremely low-noise characteristics, for RF < 3 kΩ, the noise performance is entirely dominated by RF thermal noise. Only above this RF threshold, the input noise current (in) of LMH6624-MIL becomes a factor and at no RF setting does the LMH6624-MIL input noise voltage play a significant role. This noise analysis has ignored the possible noise gain increase, due to photo-diode capacitance, at higher frequencies.

8.2.3 Application Curve

LMH6624-MIL 20058928.gif Figure 53. Current Noise Density vs Feedback Resistance