32.
    发明专利
    未知

    公开(公告)号:DE3684097D1

    公开(公告)日:1992-04-09

    申请号:DE3684097

    申请日:1986-11-12

    Abstract: The method of measuring mode field radius in single-mode optical fibres comprises the modulation of an optical beam by means of a spatial filter with radial-distribution of transmittivity of Gaussian type. Modulated beam intensity is measured in correspondence with the beam axis for different widths of the Gaussian curve, and the mode field radius is derived from both such intensity values and a parameter dependant on the Gaussian width. The apparatus which implements the method is also provided.

    33.
    发明专利
    未知

    公开(公告)号:DE3583926D1

    公开(公告)日:1991-10-02

    申请号:DE3583926

    申请日:1985-12-09

    Abstract: A method and an apparatus are provided wherein a light beam is passed through a slit (7) oscillating with respect to the beam, and a periodic signal is obtained from the beam portion traversing the slit and is split into its spectral components. Moment values are derived from the values of the amplitudes of such components.

    34.
    发明专利
    未知

    公开(公告)号:DE3675992D1

    公开(公告)日:1991-01-17

    申请号:DE3675992

    申请日:1986-04-16

    Abstract: An optical beam is injected into a single-mode (FO) fibre of a given length and outgoes from an end face of the fibre, is reflected by a reflecting optical system into said fibre; the optical power of the reflected beam guided backward by the fibre is measured. Said end face of the fibre is placed in the optical centre of the reflecting system to obtain the maximum reflected power, and is then deviated from said position detecting the occurring reductions of the reflected optical power.A device and variants to implement the method are also described.

    38.
    发明专利
    未知

    公开(公告)号:IT1155284B

    公开(公告)日:1987-01-28

    申请号:IT6714982

    申请日:1982-02-10

    Abstract: The invention is based on phase difference measurements. A Zeeman effect laser (3) generates a light beam (4) containing two radiations with slightly different frequencies whose beat is generated at the end of a path external to the material (1, 2a, 101). The same beam is split into the two component radiations (4c, 4d); the beats are generated between the first radiation, which is made to follow a path outside the material, and two radiations obtained by making the second radiation follow two different paths inside the material. The phase differences of these two beats with respect to the first are measured by a phase-comparison system (20, 21), and the refractive-index values as well as the thickness values are obtained by suitable computing means.

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