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GB2330199A - Wavelength measuring device for short duration laser pulses - Google Patents

Wavelength measuring device for short duration laser pulses Download PDF

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Publication number
GB2330199A
GB2330199A GB9820626A GB9820626A GB2330199A GB 2330199 A GB2330199 A GB 2330199A GB 9820626 A GB9820626 A GB 9820626A GB 9820626 A GB9820626 A GB 9820626A GB 2330199 A GB2330199 A GB 2330199A
Authority
GB
United Kingdom
Prior art keywords
wavelength
measuring device
laser pulses
wavelength measuring
light
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Withdrawn
Application number
GB9820626A
Other versions
GB9820626D0 (en
Inventor
Markus Rech
Harry Schlemmer
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Zeiss Eltro Optronic GmbH
Original Assignee
Zeiss Eltro Optronic GmbH
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Zeiss Eltro Optronic GmbH filed Critical Zeiss Eltro Optronic GmbH
Publication of GB9820626D0 publication Critical patent/GB9820626D0/en
Publication of GB2330199A publication Critical patent/GB2330199A/en
Withdrawn legal-status Critical Current

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Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J11/00Measuring the characteristics of individual optical pulses or of optical pulse trains
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J9/00Measuring optical phase difference; Determining degree of coherence; Measuring optical wavelength
    • G01J9/02Measuring optical phase difference; Determining degree of coherence; Measuring optical wavelength by interferometric methods
    • G01J9/0246Measuring optical wavelength

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  • Physics & Mathematics (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • General Physics & Mathematics (AREA)
  • Spectrometry And Color Measurement (AREA)
  • Photometry And Measurement Of Optical Pulse Characteristics (AREA)

Abstract

A device for measuring the wavelength of the narrow band low intensity stray light from short duration laser pulses (eg from laser range finders) wherein the light is split and directed along two light intensity measuring channels (FO1/2, ST1/2, Detector1/2) with differing spectral transmission characteristics (eg by a spectral filter 4). The wavelength of the light is then determined computationally from these two intensity measurements.

Description

Wavelength Measuring Device for Short Laser Pulses The invention relates to a wavelength measuring device for short laser pulses. In particular it relates to wavelength measuring device for short laser pulses of narrow-band stray light with low intensity whereby a specific visual field is simultaneously monitored by a supplementary optical element.
In the present state of the art, all tunable Fabry-Perot filters, graded interference filters, monochromators etc. are temporally always ready to receive only in one wavelength, and therefore the probability of detecting single short pulses is very small without temporal synchronisation.
Simultaneously measuring diode line spectrometers work with an on-chip integration of the measured signal, and with the long measurement times compared to the nanosecond pulses the background signal is problematic, since its noise covers the low intensity of the pulses to be measured. With the usual low pixel dimensions, moreover, it is difficult to simultaneously obtain a sufficiently large visual field and a large entrance pupil, since this leads to exactly opposed requirements for the focal length.
Preferably the present invention provides a measuring device of the aforementioned type, which enables and assures determination of the wavelength of narrow-band stray light generated by short laser pulses - e.g. by laser range finders.
Accordingly, the present invention provides wavelength measuring device for short laser pulses of narrow-band stray light with low intensity whereby a specific visual field is simultaneously monitored by a supplementary optical element, characterised in that the incident light is spatially split and distributed onto a specific number of measuring channels, these measuring channels having sensitivities differing spectrally from one another, which are generated by spectral filters arranged in the optical path of a collection optical system or different detectors, and the wavelength of the incident light is computationally determined from the measured values of the different measuring channels.
Configurations and further developments are specified in the sub-claims and an example is explained in the following description in conjunction with the figures of the drawings: Figure 1 shows the essential structure of an embodiment of a beam splitter with two detectors in schematic representation; Figure 2 is a diagram showing a transmission curve of a spectral filter.
An embodiment of a wavelength measuring device according to the invention for narrow-band light pulses such as those occurring in the case of stray light generated by laser range finders, for example, is described below. Both a short pulse duration and a very low intensity should be given as situation features.
The pulse duration typically lies in the ns range.
Furthermore, the instant of time of the pulse and the exact direction is unknown, and therefore all wavelengths in the spectral range of interest must preferably be monitored simultaneously and a specific visual field must preferably also be monitored with a suitable supplementary optical element.
The general concept of the invention therefore envisages spatially splitting the incident light pulse and distributing it onto a specific number - at least two - of measuring channels. These measuring channels are marked by spectrally different sensitivities and the sensitivity curves as a function of the wavelength are thereby assumed to be monotonically sloping upwards or downwards, ideally to be linear.
The wavelength of the respectively incident light may be computationally clearly determined from the individual measured values, at least by quotient formation. The suitable spectral sensitivity curves are formed by different spectral filters and different detectors.
An embodiment of the above-mentioned wavelength measuring device is sketched in Figure 1 and shows a light-collecting objective lens comprising mirror or lens elements with a spectral filter 4 arranged in its collection beam axis, which divides the collection beam into two part-beams ST1 and ST2 in a manner dependent on wavelength, which are respectively dIrected onto the detectors 1 and 2 allocated to them via a focussing optical system FOl and FO2.
The diagram in Figure 2 illustrates an example of a favourable transmission curve of the spectral filter used. It is evident from this that the detectors observe different signal strengths relative to one another depending upon the wavelengths. The signal I of detector 1 is: I = T * 1o and the signal of detector 2 is: I2 = R * I.
The wavelength X results, for example, from I1/I2 = T/R (\) independently of the intensity 1o of the incident light.
As a result of proposed measures not hitherto recognised by the prior art, determination of the wavelength of narrow-band stray light of short laser pulses is now assured in a surprisingly simple manner.

Claims (4)

  1. Patent - Claims: 1. Wavelength measuring device for short laser pulses of narrow-band stray light with low intensity whereby a specific visual field is simultaneously monitored by a supplementary optical element, characterised in that the incident light is spatially split and distributed onto a specific number of measuring channels, these measuring channels having sensitivities differing spectrally from one another, which are generated by spectral filters arranged in the optical path of a collection optical system or different detectors, and the wavelength of the incident light is computationally determined from the measured values of the different measuring channels.
  2. 2. Wavelength measuring device according to Claim 1, wherein a mirror or lens optical element is used as collection optical system.
  3. 3. Wavelength measuring device according to Claim 1 or 2, wherein a focussing optical system and a corresponding detector are allocated to each measuring channel of spectrally different sensitivity generated by the spectral filter or filters.
  4. 4. A wavelength measuring device substantially as any one embodiment herein described with reference to the accompanying drawings.
GB9820626A 1997-10-09 1998-09-22 Wavelength measuring device for short duration laser pulses Withdrawn GB2330199A (en)

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
DE1997144565 DE19744565C2 (en) 1997-10-09 1997-10-09 Wavelength measuring device for short laser pulses

Publications (2)

Publication Number Publication Date
GB9820626D0 GB9820626D0 (en) 1998-11-18
GB2330199A true GB2330199A (en) 1999-04-14

Family

ID=7845027

Family Applications (1)

Application Number Title Priority Date Filing Date
GB9820626A Withdrawn GB2330199A (en) 1997-10-09 1998-09-22 Wavelength measuring device for short duration laser pulses

Country Status (3)

Country Link
DE (1) DE19744565C2 (en)
FR (1) FR2769710A1 (en)
GB (1) GB2330199A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102018108809B4 (en) 2018-04-13 2020-02-06 Hensoldt Optronics Gmbh camera system

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4904088A (en) * 1984-08-10 1990-02-27 U.S. Philips Corporation Method and apparatus for determining radiation wavelengths and wavelength-corrected radiation power of monochromatic light sources
GB2226127A (en) * 1988-12-16 1990-06-20 Stc Plc Optical frequency monitor
WO1991001466A1 (en) * 1989-07-14 1991-02-07 Caterpillar Inc. A high pressure tube assembly and method of manufacture
GB2288013A (en) * 1993-03-01 1995-10-04 Marconi Gec Ltd Optical wavelength meter

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4308456A (en) * 1979-11-19 1981-12-29 Versatile Integrated Modules Method and apparatus for measuring the frequency of radiation
US4772118A (en) * 1986-07-14 1988-09-20 Gte Laboratories Incorporated Methods of and apparatus for measuring picosecond semiconductor laser pulse duration using the internally generated second harmonic emission accompanying the laser output
US4792230A (en) * 1986-09-08 1988-12-20 Nippon Telegraph And Telephone Corporation Method and apparatus for measuring ultrashort optical pulses

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4904088A (en) * 1984-08-10 1990-02-27 U.S. Philips Corporation Method and apparatus for determining radiation wavelengths and wavelength-corrected radiation power of monochromatic light sources
GB2226127A (en) * 1988-12-16 1990-06-20 Stc Plc Optical frequency monitor
WO1991001466A1 (en) * 1989-07-14 1991-02-07 Caterpillar Inc. A high pressure tube assembly and method of manufacture
GB2288013A (en) * 1993-03-01 1995-10-04 Marconi Gec Ltd Optical wavelength meter

Also Published As

Publication number Publication date
FR2769710A1 (en) 1999-04-16
DE19744565A1 (en) 1999-05-06
GB9820626D0 (en) 1998-11-18
DE19744565C2 (en) 2000-02-03

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WAP Application withdrawn, taken to be withdrawn or refused ** after publication under section 16(1)