JAJSDE7 June   2017 LMH6644-MIL

PRODUCTION DATA.  

  1. 特長
  2. アプリケーション
  3. 概要
    1.     各種の電源における閉ループ・ゲインと周波数との関係
  4. 改訂履歴
  5. 概要(続き)
  6. Pin Configuration and Functions
    1.     Pin Functions
  7. Specifications
    1. 7.1 Absolute Maximum Ratings
    2. 7.2 ESD Ratings
    3. 7.3 Recommended Operating Conditions
    4. 7.4 Thermal Information
    5. 7.5 3-V Electrical Characteristics
    6. 7.6 5-V Electrical Characteristics
    7. 7.7 ±5-V Electrical Characteristics
    8. 7.8 Typical Performance Characteristics
  8. Detailed Description
    1. 8.1 Overview
    2. 8.2 Functional Block Diagram
    3. 8.3 Feature Description
    4. 8.4 Device Functional Modes
  9. Application and Implementation
    1. 9.1 Application Information
    2. 9.2 Typical Application
      1. 9.2.1 Design Requirements
        1. 9.2.1.1 Input and Output Topology
        2. 9.2.1.2 Single-Supply, Low-Power Photodiode Amplifier
      2. 9.2.2 Detailed Design Procedure
      3. 9.2.3 Application Curves
  10. 10Power Supply Recommendations
  11. 11Layout
    1. 11.1 Layout Guidelines
    2. 11.2 Layout Example
  12. 12デバイスおよびドキュメントのサポート
    1. 12.1 ドキュメントの更新通知を受け取る方法
    2. 12.2 コミュニティ・リソース
    3. 12.3 商標
    4. 12.4 静電気放電に関する注意事項
    5. 12.5 Glossary
  13. 13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

Design Requirements

The circuit shown in Figure 55 is used to amplify the current from a photodiode into a voltage output. In this circuit, the emphasis is on achieving high bandwidth and the transimpedance gain setting is kept relatively low. Because of its high-slew-rate limit and high speed, the LMH6644-MIL lends itself well to such an application. This circuit achieves approximately 1 V/mA of transimpedance gain and capable of handling up to 1 mApp from the photodiode. Q1, in a common base configuration, isolates the high capacitance of the photodiode (Cd) from the op amp input in order to maximize speed. Input is AC coupled through C1 to ease biasing and allow single supply operation. With 5-V single supply, the device input/output is shifted to near half supply using a voltage divider from VCC. Note that Q1 collector does not have any voltage swing and the Miller effect is minimized. D1, tied to Q1 base, is for temperature compensation of Q1’s bias point. Q1 collector current was set to be large enough to handle the peak-to-peak photodiode excitation and not too large to shift the U1 output too far from mid-supply.