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UNIT-7
 FIBER OPTICS.
 HOLOGRAPHY.




                  1
APPLIED PHYSICS

 CODE : 07A1BS05
     I B.TECH
CSE, IT, ECE & EEE
     UNIT-7: CHAPTER 1.
NO. OF SLIDES :19

                          2
UNIT INDEX

S.No.          Module         Lecture PPT Slide No.
                              No.

    1   Introduction.         L -1    4-10
            Acceptance angle.
            Numerical
            aperture
    2   Types of optical      L -2    11-17
        fibres

   3.   Attenuation in optical L-3    18-19
        fibres
                                                  3
Lecture-1


        INTRODUCTION

Optical fibers are long, thin
strands of very pure glass about
the diameter of a human hair.

 They are arranged in bundles
called optical cables and used to
transmit light signals over long
distances.                          4
Optical Fiber
There are 3 parts in optical fiber. They are

1.Core

           2.Cladding.

                       3.Buffer coating.
                                               5
OPTICALFIBER STRUCTURE




                         6
L
              e
              c
              t
Core:         u
              r

   - Thin glass center of the fiber where the
              e
              -
  light travels
              1

Cladding :
 Outer optical material surrounding the core

  that reflects the light back into the core
Buffer coating:
Plastic coating that protects the fiber fom
  damage and moisture.
                                            7
Acceptance angle




                   8
“The maximum angle of incidence at
 the core of the optical fiber for which
 the rays undergo totall internal
 reflections and travel along the
 fiber” is called acceptance angle.
 The acceptance angle is given by


    α m = Sin-1[(√n12-n22)/n0]         9
L

    NUMERICAL APERTURE
              e
              c
              t
              u
 Numerical aperture of a fiber is a
              r
              e

  measure of its light gathering
              -
              1

  capacity.
 The numerical aperture (NA) is

  defined as the sin of the acceptance
  angle.
 (NA) = Sinα = (√n 2-n 2)/n
                m       1  2  0
                                         10
Lecture-2


Single-mode fibers:
 If the core diameter is small it
  allows only one mode to travel
  through it. Then the fiber is called
  single mode or monomode fiber.
 The monomode fiber has very small
  core diameter less than
  10micrometers.
 They Transmit infrared laser light
  (wavelength = 1,300 to 1,550
  nanometers).                           11
Multi-mode fibers
 If a fiber allows more number of
  modes, then it is called multimode
  fiber.
 It has larger core diameter than single

  mode fiber.



                                        12
 The relative refractive index
  difference is also larger than single
  mode fiber.
 It transmits infrared light

  (wavelength = 850 to 1,300 nm) from
  light-emitting diodes (LEDs).

                                      13
Step index Fiber
 The refractive index of core is
  constant through out the core.
 Different rays reach the exit end

  at different times. Therefore, the
  pulsed signal received at the exit
  end gets broadened. This is called
  ‘intermodal dispersion’.         14
Graded Index Fiber
 If the core has a non-uniform refractive
  index that gradually decreases from the
  center towards the core-cladding
  interface, the fiber is called graded index
  fiber.
 The light travels at different speeds in

  different directions.

                                                15
 A ray is continuously bent and
  travels a periodic path along the axis
  in the form of helical or skew rays.
 There is no chance of intermodal

  dispersion.
 Bandwidth is high.


                                           16
Plasticfibers
Some optical fibers can be made
 from plastic. These fibers have a
 large core (0.04 inches or 1 mm
 diameter)
transmit visible red light
 (wavelength = 650 nm) from
 LEDs
                                     17
Lecture-3
   L
   e
            ATTENUATION
   c
   t
uAttenuation is the loss of power
   r
  suffered by the optical signal as it
   e
   -
  propagates through the fiber.
   2


 It is also called fiber loss.

 Signal attenuation is defined as the

  ratio of the input optical power Pi
  into the fiber to the output received
  optical power Po from the fiber.        18
   The attenuation coefficient of the
    signal per unit length is given as
           α =10/L log (Pi/Po) dB/km
   The mechanisms through which
    attenuation takes place are
               1.Absorption losses
               2.Scattering losses       19
UNIT INDEX

S.No.         Module          Lectur PPT Slide
                              e      No.
                              No.
   1    Basic principles of   L -4   3-6
           Holography
   2    Construction and      L -5   7-18
        reconstruction
        Images
            On hologram.
   3.   Applications of       L-6    19-23
        Holography.
                                                 20
Lecture-4
                    Holography
      L
      e
•   Holographyis about the photographic
      c
      t
    technique.
      u
      r
      e
•   The technic is called HOLOGRAPHY after
      -
      3
    the greek words HOLOS, and GRAPHOS,
    which mean ‘complete’, and ‘writing’
    respectively.

•   It is the science of producing holograms.

•    It is a form of photography that allows an
    image to be recorded in three dimensions.     21
   The technique of holography can also be used
    to optically store, retrieve, and process
    information.

   It is common to confuse volumetric displays
    with holograms, particularly in science fiction
    works such as Star Trek, Star Wars,
    Red Dwarf, and Quantum Leap.

                                                   22
Technical description
   The difference between holography and
    photography is best understood by considering
    what a black and white photograph .It is a
    point-to-point recording of the intensity of
    light rays that make up an image. Each point
    on the photograph records just one thing, the
    intensity (i.e. the square of the amplitude of
    the electric field) of the light wave that
    illuminates that particular point.
                                                 23
   In the case of a colour photograph, slightly
    more information is recorded (in effect the
    image is recorded three times viewed through
    three different colour filters), which allows a
    limited reconstruction of the wavelength of the
    light, and thus its colour.

   the holograms are recorded
    monochromatically.
                                                  24
Holographic recording process
   To produce a recording of the phase of the
    light wave at each point in an image,
    holography uses a reference beam which is
    combined with the light from the scene or
    object (the object beam).

    If these two beams are coherent, optical
    interference between the reference beam and
    the object beam, due to the superposition of
    the light waves, produces a series of intensity
    fringes that can be recorded on standard
    photographic film.                              25
    These fringes form a type of
    diffraction grating on the film, which is called
    the hologram.

   The central goal of holography is that when
    the recorded grating is later illuminated by a
    substitute reference beam, the original object
    beam is reconstructed, producing a 3D image.

                                                       26
Lecture-5

                Construction process




                                       27
Holographic reconstruction process

   When the processed holographic film is
    illuminated once again with the reference
    beam, diffraction from the fringe pattern on
    the film reconstructs the original object beam
    in both intensity and phase (except for rainbow
    holograms where the depth information is
    encoded entirely in the zoneplate angle).


                                                 28
   Because many viewpoints are stored, each of
    the viewer's eyes sees the image from a
    slightly different angle, so the image appears
    three-dimensional. This is known as stereopsis
    .

   The viewer can move his or her viewpoint and
    see the image rotate
                                                 29
Reconstruction process




                         30
   HOLOGRAPHY-CONSTRUTION PROCESS
                                     L
                                     e
                                     c
                                     t
                                     u
                                     r
                                     e
                                     -
                                     5




                                     31
   HOLOGRAPHY-CONSTRUCTION PROCESS




                                  32
   CONSTRUCTION PROCESS




                           33
Holograms as diffraction grating


   A diffraction grating is a transparent or
    reflective sheet with thin slits, the distance
    between them and their diameter being on the
    order of the wavelength of the light. Light rays
    travelling towards it are bent at an angle
    determined by the distance between the slits
    and the wavelength of the light.


                                                   34
   When holograms are constructed, the reference
    beam and the object beam interfere with one
    another and the dark and light fringes of the
    interference pattern are recorded.
   When this photograph is developed, the light
    parts become clear and the dark parts opaque.



                                               35
   The clear, light parts become like the slits of a
    diffraction grating, and the angle at which they
    bend incoming light (the reconstruction beam)
    is determined by the spacing between them,
    which in turn was determined originally by the
    object beam and reference beam, when the
    hologram's interference pattern was made.
    Thus the slits bend the reconstruction beam to
    be the exact angles at each point that the object
    beam was going at.

                                                   36
APPLICATIONS                    Lecture-6


 Holography can be applied to a variety of uses
  other than recording images.
1 Holographic data storage is a technique that
  can store information at high density inside
  crystals or photopolymers.
 The ability to store large amounts of

  information in some kind of media is of great
  importance, as many electronic products
  incorporate storage devices.


                                                37
   As current storage techniques such as Blu-ray
    reach the denser limit of possible data density
    (due to the diffraction-limited size of the
    writing beams), holographic storage has the
    potential to become the next generation of
    popular storage media.
   The advantage of this type of data storage is
    that the volume of the recording media is used
    instead of just the surface.

                                                  38
APPLICATIONS
2. Digital holography
   An alternate method to record holograms is to
    use a digital device like a CCD camera instead
    of a conventional photographic film. This
    approach is often called digital holography.
    In this case, the reconstruction process can be
    carried out by digital processing of the
    recorded hologram by a standard computer.
   A 3D image of the object can later be
    visualized on the computer screen or TV set.


                                                   39
APPLICATIONS
3.Use of holography in banknotes
 Holograms are used widely as a security device

  in many currencies such as the Brazilian real 20
  note, British pound 5/10/20 notes, Canadian
  dollar 5/10/20/50/100 notes, Euro
  5/10/20/50/100/200/500 notes, South Korean
  won 5000/10000 notes, Japanese yen
  5000/10000 notes, etc.


                                                 40
4. Holography in art
 Early on artists saw the potential of

  holography as a medium and gained access to
  science laboratories to create their work.
  Holographic art is often the result of
  collaborations between scientists and artists,
  although some holographers would regard
  themselves as both an artist and scientist.


                                                   41

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7

  • 2. APPLIED PHYSICS CODE : 07A1BS05 I B.TECH CSE, IT, ECE & EEE UNIT-7: CHAPTER 1. NO. OF SLIDES :19 2
  • 3. UNIT INDEX S.No. Module Lecture PPT Slide No. No. 1 Introduction. L -1 4-10 Acceptance angle. Numerical aperture 2 Types of optical L -2 11-17 fibres 3. Attenuation in optical L-3 18-19 fibres 3
  • 4. Lecture-1 INTRODUCTION Optical fibers are long, thin strands of very pure glass about the diameter of a human hair.  They are arranged in bundles called optical cables and used to transmit light signals over long distances. 4
  • 5. Optical Fiber There are 3 parts in optical fiber. They are 1.Core 2.Cladding. 3.Buffer coating. 5
  • 7. L e c t Core: u r  - Thin glass center of the fiber where the e - light travels 1 Cladding :  Outer optical material surrounding the core that reflects the light back into the core Buffer coating: Plastic coating that protects the fiber fom damage and moisture. 7
  • 9. “The maximum angle of incidence at the core of the optical fiber for which the rays undergo totall internal reflections and travel along the fiber” is called acceptance angle.  The acceptance angle is given by α m = Sin-1[(√n12-n22)/n0] 9
  • 10. L NUMERICAL APERTURE e c t u  Numerical aperture of a fiber is a r e measure of its light gathering - 1 capacity.  The numerical aperture (NA) is defined as the sin of the acceptance angle.  (NA) = Sinα = (√n 2-n 2)/n m 1 2 0 10
  • 11. Lecture-2 Single-mode fibers:  If the core diameter is small it allows only one mode to travel through it. Then the fiber is called single mode or monomode fiber.  The monomode fiber has very small core diameter less than 10micrometers.  They Transmit infrared laser light (wavelength = 1,300 to 1,550 nanometers). 11
  • 12. Multi-mode fibers  If a fiber allows more number of modes, then it is called multimode fiber.  It has larger core diameter than single mode fiber. 12
  • 13.  The relative refractive index difference is also larger than single mode fiber.  It transmits infrared light (wavelength = 850 to 1,300 nm) from light-emitting diodes (LEDs). 13
  • 14. Step index Fiber  The refractive index of core is constant through out the core.  Different rays reach the exit end at different times. Therefore, the pulsed signal received at the exit end gets broadened. This is called ‘intermodal dispersion’. 14
  • 15. Graded Index Fiber  If the core has a non-uniform refractive index that gradually decreases from the center towards the core-cladding interface, the fiber is called graded index fiber.  The light travels at different speeds in different directions. 15
  • 16.  A ray is continuously bent and travels a periodic path along the axis in the form of helical or skew rays.  There is no chance of intermodal dispersion.  Bandwidth is high. 16
  • 17. Plasticfibers Some optical fibers can be made from plastic. These fibers have a large core (0.04 inches or 1 mm diameter) transmit visible red light (wavelength = 650 nm) from LEDs 17
  • 18. Lecture-3 L e ATTENUATION c t uAttenuation is the loss of power r suffered by the optical signal as it e - propagates through the fiber. 2  It is also called fiber loss.  Signal attenuation is defined as the ratio of the input optical power Pi into the fiber to the output received optical power Po from the fiber. 18
  • 19. The attenuation coefficient of the signal per unit length is given as α =10/L log (Pi/Po) dB/km  The mechanisms through which attenuation takes place are 1.Absorption losses 2.Scattering losses 19
  • 20. UNIT INDEX S.No. Module Lectur PPT Slide e No. No. 1 Basic principles of L -4 3-6 Holography 2 Construction and L -5 7-18 reconstruction Images On hologram. 3. Applications of L-6 19-23 Holography. 20
  • 21. Lecture-4 Holography L e • Holographyis about the photographic c t technique. u r e • The technic is called HOLOGRAPHY after - 3 the greek words HOLOS, and GRAPHOS, which mean ‘complete’, and ‘writing’ respectively. • It is the science of producing holograms. • It is a form of photography that allows an image to be recorded in three dimensions. 21
  • 22. The technique of holography can also be used to optically store, retrieve, and process information.  It is common to confuse volumetric displays with holograms, particularly in science fiction works such as Star Trek, Star Wars, Red Dwarf, and Quantum Leap. 22
  • 23. Technical description  The difference between holography and photography is best understood by considering what a black and white photograph .It is a point-to-point recording of the intensity of light rays that make up an image. Each point on the photograph records just one thing, the intensity (i.e. the square of the amplitude of the electric field) of the light wave that illuminates that particular point. 23
  • 24. In the case of a colour photograph, slightly more information is recorded (in effect the image is recorded three times viewed through three different colour filters), which allows a limited reconstruction of the wavelength of the light, and thus its colour.  the holograms are recorded monochromatically. 24
  • 25. Holographic recording process  To produce a recording of the phase of the light wave at each point in an image, holography uses a reference beam which is combined with the light from the scene or object (the object beam).  If these two beams are coherent, optical interference between the reference beam and the object beam, due to the superposition of the light waves, produces a series of intensity fringes that can be recorded on standard photographic film. 25
  • 26. These fringes form a type of diffraction grating on the film, which is called the hologram.  The central goal of holography is that when the recorded grating is later illuminated by a substitute reference beam, the original object beam is reconstructed, producing a 3D image. 26
  • 27. Lecture-5  Construction process 27
  • 28. Holographic reconstruction process  When the processed holographic film is illuminated once again with the reference beam, diffraction from the fringe pattern on the film reconstructs the original object beam in both intensity and phase (except for rainbow holograms where the depth information is encoded entirely in the zoneplate angle). 28
  • 29. Because many viewpoints are stored, each of the viewer's eyes sees the image from a slightly different angle, so the image appears three-dimensional. This is known as stereopsis .  The viewer can move his or her viewpoint and see the image rotate 29
  • 31. HOLOGRAPHY-CONSTRUTION PROCESS L e c t u r e - 5 31
  • 32. HOLOGRAPHY-CONSTRUCTION PROCESS 32
  • 33. CONSTRUCTION PROCESS 33
  • 34. Holograms as diffraction grating  A diffraction grating is a transparent or reflective sheet with thin slits, the distance between them and their diameter being on the order of the wavelength of the light. Light rays travelling towards it are bent at an angle determined by the distance between the slits and the wavelength of the light. 34
  • 35. When holograms are constructed, the reference beam and the object beam interfere with one another and the dark and light fringes of the interference pattern are recorded.  When this photograph is developed, the light parts become clear and the dark parts opaque. 35
  • 36. The clear, light parts become like the slits of a diffraction grating, and the angle at which they bend incoming light (the reconstruction beam) is determined by the spacing between them, which in turn was determined originally by the object beam and reference beam, when the hologram's interference pattern was made. Thus the slits bend the reconstruction beam to be the exact angles at each point that the object beam was going at. 36
  • 37. APPLICATIONS Lecture-6  Holography can be applied to a variety of uses other than recording images. 1 Holographic data storage is a technique that can store information at high density inside crystals or photopolymers.  The ability to store large amounts of information in some kind of media is of great importance, as many electronic products incorporate storage devices. 37
  • 38. As current storage techniques such as Blu-ray reach the denser limit of possible data density (due to the diffraction-limited size of the writing beams), holographic storage has the potential to become the next generation of popular storage media.  The advantage of this type of data storage is that the volume of the recording media is used instead of just the surface. 38
  • 39. APPLICATIONS 2. Digital holography  An alternate method to record holograms is to use a digital device like a CCD camera instead of a conventional photographic film. This approach is often called digital holography.  In this case, the reconstruction process can be carried out by digital processing of the recorded hologram by a standard computer.  A 3D image of the object can later be visualized on the computer screen or TV set. 39
  • 40. APPLICATIONS 3.Use of holography in banknotes  Holograms are used widely as a security device in many currencies such as the Brazilian real 20 note, British pound 5/10/20 notes, Canadian dollar 5/10/20/50/100 notes, Euro 5/10/20/50/100/200/500 notes, South Korean won 5000/10000 notes, Japanese yen 5000/10000 notes, etc. 40
  • 41. 4. Holography in art  Early on artists saw the potential of holography as a medium and gained access to science laboratories to create their work. Holographic art is often the result of collaborations between scientists and artists, although some holographers would regard themselves as both an artist and scientist. 41