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HO-ED-INT-10A Fabry - Perot Interferometer CCD BasedFabry Perot Interferometer CCD Based Computer interfaced Fabry Perot interferometer (Model No: HO ED INT 10A) is similar to projection type (model no: HO ED INT 10), apart from the fact that in this case, the interference pattern is captured by a CCD sensor and displayed on a computer monitor. The advantage of computer interface is that the pattern can be saved for future analysis. In addition, measurements can be taken directly from the monitor by
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Fabry - Perot Interferometer

CCD Based

Computer interfaced Fabry-Perot interferometer (Model No:HO-ED-INT-10A) is similar to projection type (model no:HO-ED-INT-10), apart from the fact that in this case, the interference pattern is captured by a CCD sensor and displayed on a computer monitor. The advantage of computer interface is that the pattern can be saved for future analysis. In addition, measurements can be taken directly from the monitor by using the software module provided.

In the etalon, distance between partially reflecting mirrors can be precisely varied in microns. One of the beam splitters can be kinematically adjusted for initial settings.

Experiment:

   To find the wavelength of monochromatic light

The wavelength of laser is calculated by,

λ  =  ( 2d / N ) Δ

where ‘d’ is the change in position that occurs for ‘N’ fringes to pass and Δ is the calibration constant of the micrometer

   To determine the spacing between the plates of fabry perot etalon from the fringe Pattern

The Spacing of the Etalon is given by,

 

t  =  nD2λ  /  χn2

where n is the order, ‘D ’ is the distance between the etalon and the screen, ‘λ’ is the wavelength of light used.

χn2  =  χm+n2  -  χm2

χm+n2 is the square of the radius of (m+n)th ring and χm2 that of mth ring.

   To find the finesse and free spectral range (FSR) of etalon from the fringe calibration at different cavity thickness

The Free Spectral Range of the Etalon is given by,

FSR  =  c / 2t,

Where c is the speed of light in air and t is the spacing of the Etalon

The finesse is a measure of the interferometer's ability to resolve closely spaced spectral lines.

The finesse F is defined by the following equation.

F  =  π √R / ( 1-R )

Where, R is the reflectivity of surfaces

Specifications:

  Spacing of Etalon     2 - 8 mm
    Ratio R/T     80 / 20
    Aperture     25 mm

Features:

Mercury vapor lamp is used as light source
    Compact design
    Fine tuning is possible in etalon
    High resolution CCD camera

Drawings:

Video:

Click HERE for Video

Related Topics:

Interference of light
    Fabry Perot etalon
    Finesse of etalon

 

Scope for Delivery:

Optical Rail
Fabri-Perot Interferometer
Kinematic Laser Mount
Colour Filter Mount
Plano Convex Lens with Mount Supply
Camera Lens Assembly with Mount
Colour Filters (Green, Blue)
Diode Laser with Power supply (Red)
CCD Camera
Mercury Vapor Lamp with Power Supply
Accessories

Allen Key
Instruction Manual

 

 

HO-ED-INT-10A Fabry - Perot Interferometer CCD Based

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