WO2018082020A1 - 一种扫描头瞄准光曝光解决系统 - Google Patents

一种扫描头瞄准光曝光解决系统 Download PDF

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Publication number
WO2018082020A1
WO2018082020A1 PCT/CN2016/104627 CN2016104627W WO2018082020A1 WO 2018082020 A1 WO2018082020 A1 WO 2018082020A1 CN 2016104627 W CN2016104627 W CN 2016104627W WO 2018082020 A1 WO2018082020 A1 WO 2018082020A1
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pin
control circuit
scanning head
aiming
grounded
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PCT/CN2016/104627
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English (en)
French (fr)
Inventor
王冬生
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深圳盈达信息科技有限公司
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Priority to US15/743,233 priority Critical patent/US10509929B2/en
Priority to SG11201805711WA priority patent/SG11201805711WA/en
Priority to PCT/CN2016/104627 priority patent/WO2018082020A1/zh
Priority to EP16920581.2A priority patent/EP3537333B1/en
Publication of WO2018082020A1 publication Critical patent/WO2018082020A1/zh

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    • G—PHYSICS
    • G06—COMPUTING; CALCULATING OR COUNTING
    • G06K—GRAPHICAL DATA READING; PRESENTATION OF DATA; RECORD CARRIERS; HANDLING RECORD CARRIERS
    • G06K7/00—Methods or arrangements for sensing record carriers, e.g. for reading patterns
    • G06K7/10—Methods or arrangements for sensing record carriers, e.g. for reading patterns by electromagnetic radiation, e.g. optical sensing; by corpuscular radiation
    • G06K7/10544—Methods or arrangements for sensing record carriers, e.g. for reading patterns by electromagnetic radiation, e.g. optical sensing; by corpuscular radiation by scanning of the records by radiation in the optical part of the electromagnetic spectrum
    • G06K7/10554—Moving beam scanning
    • G06K7/10564—Light sources
    • G—PHYSICS
    • G06—COMPUTING; CALCULATING OR COUNTING
    • G06K—GRAPHICAL DATA READING; PRESENTATION OF DATA; RECORD CARRIERS; HANDLING RECORD CARRIERS
    • G06K7/00—Methods or arrangements for sensing record carriers, e.g. for reading patterns
    • G06K7/10—Methods or arrangements for sensing record carriers, e.g. for reading patterns by electromagnetic radiation, e.g. optical sensing; by corpuscular radiation
    • G06K7/10544—Methods or arrangements for sensing record carriers, e.g. for reading patterns by electromagnetic radiation, e.g. optical sensing; by corpuscular radiation by scanning of the records by radiation in the optical part of the electromagnetic spectrum
    • G06K7/10821—Methods or arrangements for sensing record carriers, e.g. for reading patterns by electromagnetic radiation, e.g. optical sensing; by corpuscular radiation by scanning of the records by radiation in the optical part of the electromagnetic spectrum further details of bar or optical code scanning devices
    • G06K7/10851—Circuits for pulse shaping, amplifying, eliminating noise signals, checking the function of the sensing device
    • G—PHYSICS
    • G06—COMPUTING; CALCULATING OR COUNTING
    • G06K—GRAPHICAL DATA READING; PRESENTATION OF DATA; RECORD CARRIERS; HANDLING RECORD CARRIERS
    • G06K7/00—Methods or arrangements for sensing record carriers, e.g. for reading patterns
    • G06K7/10—Methods or arrangements for sensing record carriers, e.g. for reading patterns by electromagnetic radiation, e.g. optical sensing; by corpuscular radiation
    • G—PHYSICS
    • G06—COMPUTING; CALCULATING OR COUNTING
    • G06K—GRAPHICAL DATA READING; PRESENTATION OF DATA; RECORD CARRIERS; HANDLING RECORD CARRIERS
    • G06K7/00—Methods or arrangements for sensing record carriers, e.g. for reading patterns
    • G06K7/10—Methods or arrangements for sensing record carriers, e.g. for reading patterns by electromagnetic radiation, e.g. optical sensing; by corpuscular radiation
    • G06K7/14—Methods or arrangements for sensing record carriers, e.g. for reading patterns by electromagnetic radiation, e.g. optical sensing; by corpuscular radiation using light without selection of wavelength, e.g. sensing reflected white light
    • G06K7/1404—Methods for optical code recognition
    • G06K7/1408—Methods for optical code recognition the method being specifically adapted for the type of code
    • G06K7/1417—2D bar codes
    • H—ELECTRICITY
    • H03—ELECTRONIC CIRCUITRY
    • H03K—PULSE TECHNIQUE
    • H03K19/00—Logic circuits, i.e. having at least two inputs acting on one output; Inverting circuits
    • H03K19/20—Logic circuits, i.e. having at least two inputs acting on one output; Inverting circuits characterised by logic function, e.g. AND, OR, NOR, NOT circuits

Definitions

  • the invention relates to the technical field of two-dimensional code scanning heads, in particular to a scanning head aiming light exposure solving system.
  • the camera is equipped with a fill light and an aiming light
  • the camera is used for taking the code
  • the fill light is used to provide the fill light
  • the aiming light is used to guide the operator to scan the code. It is usually used when the fill light and the aiming light are turned on while the camera is taking the code.
  • the disadvantage of this type of scanning head is that the aiming light needs to be aligned with the scanned one-dimensional code or two-dimensional code, and the aiming light as a positioning guide must have a small-area light source, and in most cases will cover the identified one-dimensional Code or QR code, so the camera will form a partial overexposure.
  • the premise of camera decoding is to take the picture clearly. The partial overexposure not only corrects the decoding accuracy, stability, recognition rate, decoding speed but also the power of the scan head. Consumption has a huge impact.
  • the present invention provides the following technical solutions:
  • a scanning head aiming light exposure solving system comprises a control circuit of an aiming lamp, wherein the control circuit of the aiming lamp is composed of 5 pin ends, wherein pin 1 and pin 2 are input terminals of the AND circuit, and pins 4 is the output terminal of the non-gate circuit, and the high-level Vcc is connected to the pin 5 end of the control circuit, and is grounded at the pin 3 end of the control circuit; the pin 1 and the pin 2 of the control circuit are respectively connected for scanning.
  • the signal and the field sync signal are connected to the resistor R1 and grounded on the field sync signal; connected to the gate of the field effect transistor at the pin 4 end of the control circuit; the drain of the field effect transistor is connected to the high level Vcc; The source of the transistor is connected to the resistor R2 and the light emitting diode and grounded.
  • the field effect transistor is an N-type MOS transistor.
  • control circuit is a U1 controller.
  • the present invention has the beneficial effects:
  • the scanning head is aimed at the light exposure solution system, and the camera is driven to output the field synchronization signal.
  • the field sync signal is input to the control circuit, and the control circuit separates the start point and the end point of the blanking time of the field sync signal, the start point is used as the turn-on signal of the aiming light, and the end point is used as the close signal of the aiming light.
  • the camera acquisition time is completed in the effective picture interval of the on-field synchronization signal, so that the camera's code acquisition time and the aiming lamp illumination time can be completely separated, thereby completely avoiding local overexposure caused by the aiming light.
  • the scanning head aiming at the light exposure solving system compared with the existing scanning head on the market, the invention can completely eliminate the problem of partial overexposure of the aiming light, and the decoding precision, stability, recognition rate, decoding speed and even the scanning head are even Power consumption has been greatly improved, and it is easy to achieve low cost.
  • 1 is a timing diagram of a field sync signal of the present invention
  • FIG. 2 is a control circuit diagram of the aiming lamp of the present invention.
  • a scanning head aiming light exposure solving system includes a control circuit 1 of an aiming lamp, and the control circuit 1 of the aiming lamp is composed of 5 pin ends, and the control circuit 1
  • the control circuit 1 For the U1 controller, where pin 1 and pin 2 are the input terminals of the AND circuit, pin 4 is the output terminal of the NOT circuit, and the high level Vcc is connected to the pin 5 of the control circuit 1 in the control.
  • the pin 3 end of the circuit 1 is grounded; the pin 1 and the pin 2 of the control circuit 1 are respectively connected to the scan signal and the field sync signal, and the resistor R1 is connected to the ground sync signal and grounded, and the scan signal (SCAN_ENABLE) and The field sync signal (vsync) is used as the input end of the AND circuit, and the output is used as the control signal of the aiming lamp; the pin 4 of the control circuit 1 is connected to the gate of the field effect transistor Q1, and the field effect transistor Q1 is the N type MOS transistor.
  • the drain of the field effect transistor Q1 is connected to the high level Vcc; the source of the field effect transistor Q1 is connected to the resistor R2 and the light emitting diode D1, and is grounded.
  • the present invention utilizes a camera driver to output a field sync signal (vsync) to the outside.
  • vsync field sync signal
  • the control circuit 1 separates the start point and the end point of the blanking time of the field sync signal, the start point as an open signal of the aiming light, and the end point as a close signal of the aiming light.
  • the camera acquisition time is completed in the effective picture interval of the on-field synchronization signal, so that the camera's code acquisition time and the aiming lamp illumination time can be completely separated, thereby completely avoiding local overexposure caused by the aiming light.

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  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Electromagnetism (AREA)
  • Artificial Intelligence (AREA)
  • Toxicology (AREA)
  • General Health & Medical Sciences (AREA)
  • Health & Medical Sciences (AREA)
  • Computer Vision & Pattern Recognition (AREA)
  • General Physics & Mathematics (AREA)
  • Theoretical Computer Science (AREA)
  • Studio Devices (AREA)
  • Facsimile Scanning Arrangements (AREA)
  • Stroboscope Apparatuses (AREA)
  • Exposure And Positioning Against Photoresist Photosensitive Materials (AREA)
  • Image Input (AREA)

Abstract

一种扫描头瞄准光曝光解决系统，包括瞄准灯的控制电路(1)，瞄准灯的控制电路(1)由5个引脚端构成，其中引脚1和引脚2为与门电路的输入端，引脚4为非门电路的输出端，在控制电路(1)的引脚5端接入高电平Vcc，在控制电路(1)的引脚3端接地；控制电路(1)的引脚1和引脚2分别接入扫描信号(SCAN_ENABLE)和场同步信号(vsync)，在场同步信号(vsync)上接入电阻R1并接地。与市场上现有的扫描头相比，可以完全消除瞄准光局部过曝的问题，对扫描头解码精度、稳定性、识别率、解码速度乃至功耗都有很大改善，而且容易实现成本低廉。

Description

一种扫描头瞄准光曝光解决系统 技术领域
本发明涉及二维码扫描头技术领域，尤其是一种扫描头瞄准光曝光解决系统。
背景技术
随着移动互联网和物流行业的蓬勃发展，一维码，二维码无论在工作还是生活中都是无处不在，因此对扫描头技术提出了更高的要求，解码精度、稳定性、低功耗、识别率、识别速度等方面都有有着严格要求。
现有二维码扫描头方案中都是采取摄像头配合补光灯以及瞄准灯，摄像头是用来取码，补光灯则是用来提供补光，瞄准灯用来指引操作者扫码。通常使用是情况是，打开补光灯和瞄准灯同时摄像头进行取码。这种扫描头的缺点就是，瞄准光需要对准被扫描的一维码或者二维码，而瞄准灯作为定位指引，必定小面积的光源，而且大多数情况下都会覆盖在被识别的一维码或者二维码上，因此摄像头取码就会形成局部过曝，摄像头解码的前提就是取码图片要清晰，局部过曝不仅对扫描头的解码精度、稳定性、识别率、解码速度乃至功耗都有极大的影响。
发明内容
本发明的目的在于提供一种扫描头瞄准光曝光解决系统，以解决上述背景技术中提出的问题。
为实现上述目的，本发明提供如下技术方案：
一种扫描头瞄准光曝光解决系统，包括瞄准灯的控制电路，所述瞄准灯的控制电路由5个引脚端构成，其中引脚1和引脚2为与门电路的输入端，引脚4为非门电路的输出端，在控制电路的引脚5端接入高电平Vcc，在控制电路的引脚3端接地；所述控制电路的引脚1和引脚2分别接入扫描信号和场同步信号，在场同步信号上接入电阻R1并接地；在控制电路的引脚4端接到场效应晶体管的栅极；所述场效应晶体管的漏极接入高电平Vcc；场效应晶体管的源极接入电阻R2和发光二极管，并接地。
作为本发明进一步的方案：所述场效应晶体管为N型MOS管。
作为本发明进一步的方案：所述控制电路为U1控制器。
与现有技术相比，本发明有益效果：
1、本扫描头瞄准光曝光解决系统，利用摄像头驱动使其对外输出场同步信 号(vsync)。将场同步信号输入到控制电路中，控制电路将场同步信号的消隐时间的开始点和结束点分离出来，开始点作为瞄准灯的开启信号，结束点作为瞄准灯的关闭信号。而摄像头取码时间是在在场同步信号的有效图片区间内完成，这样就可以将摄像头的取码时间和瞄准灯点亮时间完全分开，从而完全避免了因瞄准光而造成的局部过曝。
2、本扫描头瞄准光曝光解决系统，与市场上现有的扫描头相比，本发明可以完全消除瞄准光局部过曝的问题，对扫描头解码精度、稳定性、识别率、解码速度乃至功耗都有很大改善，而且容易实现成本低廉。
附图说明
图1为本发明的场同步信号的的时序关系图；
图2为本发明的瞄准灯的控制电路图。
图中：1-控制电路；Q1-场效应晶体管；D1-发光二极管；D2-二极管。
具体实施方式
下面将结合本发明实施例中的附图，对本发明实施例中的技术方案进行清楚、完整地描述，显然，所描述的实施例仅仅是本发明一部分实施例，而不是全部的实施例。基于本发明中的实施例，本领域普通技术人员在没有做出创造性劳动前提下所获得的所有其他实施例，都属于本发明保护的范围。
请参阅图1-2，本发明实施例中，一种扫描头瞄准光曝光解决系统，包括瞄准灯的控制电路1，所述瞄准灯的控制电路1由5个引脚端构成，控制电路1为U1控制器，其中引脚1和引脚2为与门电路的输入端，引脚4为非门电路的输出端，在控制电路1的引脚5端接入高电平Vcc，在控制电路1的引脚3端接地；所述控制电路1的引脚1和引脚2分别接入扫描信号和场同步信号，在场同步信号上接入电阻R1并接地，将扫描信号(SCAN_ENABLE)和场同步信号(vsync)作为与门电路的输入端，输出端作为瞄准灯的控制信号；在控制电路1的引脚4端接到场效应晶体管Q1的栅极，场效应晶体管Q1为N型MOS管；所述场效应晶体管Q1的漏极接入高电平Vcc；场效应晶体管Q1的源极接入电阻R2和发光二极管D1，并接地。
综上所述：能够完美的解决瞄准光造成的局部过曝问题。本发明利用摄像头驱动使其对外输出场同步信号(vsync)。将场同步信号输入到控制电路1中， 控制电路1将场同步信号的消隐时间的开始点和结束点分离出来，开始点作为瞄准灯的开启信号，结束点作为瞄准灯的关闭信号。而摄像头取码时间是在在场同步信号的有效图片区间内完成，这样就可以将摄像头的取码时间和瞄准灯点亮时间完全分开，从而完全避免了因瞄准光而造成的局部过曝。
对于本领域技术人员而言，显然本发明不限于上述示范性实施例的细节，而且在不背离本发明的精神或基本特征的情况下，能够以其他的具体形式实现本发明。因此，无论从哪一点来看，均应将实施例看作是示范性的，而且是非限制性的，本发明的范围由所附权利要求而不是上述说明限定，因此旨在将落在权利要求的等同要件的含义和范围内的所有变化囊括在本发明内。不应将权利要求中的任何附图标记视为限制所涉及的权利要求。
此外，应当理解，虽然本说明书按照实施方式加以描述，但并非每个实施方式仅包含一个独立的技术方案，说明书的这种叙述方式仅仅是为清楚起见，本领域技术人员应当将说明书作为一个整体，各实施例中的技术方案也可以经适当组合，形成本领域技术人员可以理解的其他实施方式。

Claims (3)

  1. 一种扫描头瞄准光曝光解决系统，包括瞄准灯的控制电路(1)，其特征在于：所述瞄准灯的控制电路(1)由5个引脚端构成，其中引脚1和引脚2为与门电路的输入端，引脚4为非门电路的输出端，在控制电路(1)的引脚5端接入高电平Vcc，在控制电路(1)的引脚3端接地；所述控制电路(1)的引脚1和引脚2分别接入扫描信号和场同步信号，在场同步信号上接入电阻R1并接地；在控制电路(1)的引脚4端接到场效应晶体管(Q1)的栅极；所述场效应晶体管(Q1)的漏极接入高电平Vcc；场效应晶体管(Q1)的源极接入电阻R2和发光二极管D1，并接地。
  2. 根据权利要求1所述的一种扫描头瞄准光曝光解决系统，其特征在于：所述场效应晶体管(Q1)为N型MOS管。
  3. 根据权利要求1所述的一种扫描头瞄准光曝光解决系统，其特征在于：所述控制电路(1)为U1控制器。
PCT/CN2016/104627 2016-11-04 2016-11-04 一种扫描头瞄准光曝光解决系统 WO2018082020A1 (zh)

Priority Applications (4)

Application Number Priority Date Filing Date Title
US15/743,233 US10509929B2 (en) 2016-11-04 2016-11-04 Scan head's aiming beam exposure solution system
SG11201805711WA SG11201805711WA (en) 2016-11-04 2016-11-04 A Scan head’s Aiming Beam Exposure Solution System
PCT/CN2016/104627 WO2018082020A1 (zh) 2016-11-04 2016-11-04 一种扫描头瞄准光曝光解决系统
EP16920581.2A EP3537333B1 (en) 2016-11-04 2016-11-04 System for resolving exposure of aiming beams of scanning head

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PCT/CN2016/104627 WO2018082020A1 (zh) 2016-11-04 2016-11-04 一种扫描头瞄准光曝光解决系统

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CN109460686A (zh) * 2018-09-25 2019-03-12 深圳盈达信息科技有限公司 一种用于瞄准装置瞄准光消隐的方法及系统
CN109460686B (zh) * 2018-09-25 2022-06-14 深圳盈达信息科技有限公司 一种用于瞄准装置瞄准光消隐的方法及系统

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