Invention Publication
EP1472643A1 ANORDNUNG UND VERFAHREN ZUR MESSUNG AN EINEM RESONANTEN SCHWINGER UND SEINER STEUERUNG UND EINSTELLUNG EINER PIXELBREITE 有权
系统和方法用于测量共振主席和其控制和调节的像素宽度的

  • Patent Title: ANORDNUNG UND VERFAHREN ZUR MESSUNG AN EINEM RESONANTEN SCHWINGER UND SEINER STEUERUNG UND EINSTELLUNG EINER PIXELBREITE
  • Patent Title (English): Arrangement and method for measurement on a resonant oscillator, control thereof and setting of a pixel width
  • Patent Title (中): 系统和方法用于测量共振主席和其控制和调节的像素宽度的
  • Application No.: EP03706457.3
    Application Date: 2003-02-07
  • Publication No.: EP1472643A1
    Publication Date: 2004-11-03
  • Inventor: WENZEL, Mike
  • Applicant: Jenoptik Ldt GmbH
  • Applicant Address: Fasaneninsel 1 07548 Gera DE
  • Assignee: Jenoptik Ldt GmbH
  • Current Assignee: Jenoptik Ldt GmbH
  • Current Assignee Address: Fasaneninsel 1 07548 Gera DE
  • Agency: Breit, Ulrich
  • Priority: DE10205207 20020208
  • International Announcement: WO2003067509 20030814
  • Main IPC: G06K7/10
  • IPC: G06K7/10 G02B7/182 H04N9/31 G02B26/10 H04N1/053 G01D5/30
ANORDNUNG UND VERFAHREN ZUR MESSUNG AN EINEM RESONANTEN SCHWINGER UND SEINER STEUERUNG UND EINSTELLUNG EINER PIXELBREITE
Abstract:
The invention relates to an arrangement and a method for measurement on a resonant oscillator with a mirror surface (8), which is displaced about an oscillation axis (2) with a period of duration (T), a laser diode (4) which emits a measuring beam (3) onto the first mirror surface (8), whereby a beam axis (21) of the measuring beam (3) intersects the oscillation axis (2). A photo receiver (6) is arranged opposing the first mirror surface (8) at a separation (a) from the beam axis (21) and a separation (b) from the mirror surface (8). The deflected measuring beam (5) moves within a quarter of a period (0 .... T/4) of an oscillation and over the photo-receiver (6) within a following quarter (T/4 .... T/2) of the period. The photo-receiver (6) is connected to an analytical circuit (11) which calculates the timepoints (t1, t2) from the impulses from the photo-receiver (6) and calculates a time period within the one half-wave (Δt = t2 - t1) from the above. The analytical circuit (11) calculates an actual value of the maximum amplitude with the equation:(I). The time duration Δt corresponds to a line dead time on writing sequential lines of a video image.
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