Beam Profiling-Advanced Physics-Lab Report, Exercises of Advanced Physics

This is lab report for Advanced Physics Course. It was submitted to Prof. Dhirendra Kapoor at Alliance University. Its main points are: Profiling, Beam, Physics, Sharp, Diameter, Height, Guassian, Sigma, Intersects, Laser, Propagation, Measurement, Radiation

Typology: Exercises

2011/2012

Uploaded on 07/16/2012

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Calculation of beam diameter of He-Ne Laser
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In every laser application, whether in medical, industrial, laser printing, marking, welding and
cutting, or fiber optics, the beam profile provides valuable information for the most efficient use
of the laser. Beam profiles are very commonly the principal measurement in practical
applications found in industry. The beam profile tells all about the beam’s spatial characteristics,
which in turn describe the propagation, beam quality and utility of the beam. In addition, it can
tell how effectively optics are succeeding in modifying and shaping the laser’s output. Profiling
is particularly helpful in building optical systems for laser printers and fiber optic collimators.
What is Beam Profiling?
Spatial characteristics describe the distribution of radiant energy across the wave front of an
optical beam. The radiation can be shown as a plot of the relative intensity of points across a
plane that intersects projected path of the beam. The most basic measurement of the beam’s
irradiance is a single number defining its width or diameter. Since optical beams do not actually
have sharp physical edges, the beam width is made between two points that contain a selected
percentage of the “useful” energy. When beams are Gaussian, or at least approximately
Gaussian, the common value for this measurement is at the 1/e2 diameter. This is the point at
which the beam contains 4-sigma of the energy distribution and occurs where the beam’s power
is at 13.5% of the maximum height. Another common measurement is at the full-width-half
maximum (FWHM) level, where the power drops to one half of the maximum. The beam
diameter measurement, by either method, allows one to determine other important features of the
spatial irradiance pattern of the beam. According to wave front propagation theory, light waves
diverge, causing the beam diameter to increase as it travels along the beam path. The rate at
which the beam diverges is an angular term known as the divergence, denoted as θ (theta). The
point at which a beam width is at its minimum size is known as the beam waist (D0). By
measuring the beam diameter at various points along the axis of propagation, known as the z-
axis, the divergence and waist characteristics of the beam can be determined. Beam profiling is
the act of sampling the beam size along the z-axis and thereby determining its spatial
characteristics. The net result of profiling yields an image of the beam’s energy pattern.
Techniques to make these measurements have included mode cups, phosphors, infrared cards,
Plexiglas blocks, burn papers and film. These crude techniques do not provide numerical values
and thus require a subjective evaluation of the image. More precise instruments for measuring a
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In every laser application, whether in medical, industrial, laser printing, marking, welding and

cutting, or fiber optics, the beam profile provides valuable information for the most efficient use

of the laser. Beam profiles are very commonly the principal measurement in practical

applications found in industry. The beam profile tells all about the beam’s spatial characteristics,

which in turn describe the propagation, beam quality and utility of the beam. In addition, it can

tell how effectively optics are succeeding in modifying and shaping the laser’s output. Profiling

is particularly helpful in building optical systems for laser printers and fiber optic collimators.

What is Beam Profiling?

Spatial characteristics describe the distribution of radiant energy across the wave front of an

optical beam. The radiation can be shown as a plot of the relative intensity of points across a

plane that intersects projected path of the beam. The most basic measurement of the beam’s

irradiance is a single number defining its width or diameter. Since optical beams do not actually

have sharp physical edges, the beam width is made between two points that contain a selected

percentage of the “useful” energy. When beams are Gaussian, or at least approximately

Gaussian, the common value for this measurement is at the 1/e2 diameter. This is the point at

which the beam contains 4-sigma of the energy distribution and occurs where the beam’s power

is at 13.5% of the maximum height. Another common measurement is at the full-width-half

maximum (FWHM) level, where the power drops to one half of the maximum. The beam

diameter measurement, by either method, allows one to determine other important features of the

spatial irradiance pattern of the beam. According to wave front propagation theory, light waves

diverge, causing the beam diameter to increase as it travels along the beam path. The rate at

which the beam diverges is an angular term known as the divergence, denoted as θ ( theta). The

point at which a beam width is at its minimum size is known as the beam waist (D0). By

measuring the beam diameter at various points along the axis of propagation, known as the z-

axis, the divergence and waist characteristics of the beam can be determined. Beam profiling is

the act of sampling the beam size along the z-axis and thereby determining its spatial

characteristics. The net result of profiling yields an image of the beam’s energy pattern.

Techniques to make these measurements have included mode cups, phosphors, infrared cards,

Plexiglas blocks, burn papers and film. These crude techniques do not provide numerical values

and thus require a subjective evaluation of the image. More precise instruments for measuring a

laser beam are scanning apertures and CCD array cameras. These sensors are preferred because

they give a true numerical output that makes it easier to accurately quantify the nature of the

beam.

Experimental Procedure

Results

Diameter

distance Vs Normalized intensity Distance(mm) Normalized Intensity

  • d(mm) I I-0. Observations and Calculations - 0 7.97 7.956 Intensity
    • 0.01 7.97 7.956
    • 0.02 7.97 7.956
    • 0.03 7.97 7.956
    • 0.04 7.97 7.956
    • 0.05 7.97 7.956
    • 0.06 7.97 7.956
    • 0.07 7.97 7.956
    • 0.08 7.96 7.946 0.
    • 0.09 7.96 7.946 0.
      • 0.1 7.96 7.946 0.
    • 0.11 7.96 7.946 0.
    • 0.12 7.96 7.946 0.
    • 0.13 7.96 7.946 0.
    • 0.14 7.96 7.946 0.
    • 0.15 7.96 7.946 0.
    • 0.16 7.96 7.946 0.
    • 0.17 7.96 7.946 0.
    • 0.18 7.96 7.946 0.
    • 0.19 7.96 7.946 0.
      • 0.2 7.96 7.946 0.
    • 0.21 7.96 7.946 0.
    • 0.22 7.96 7.946 0.
    • 0.23 7.96 7.946 0.
    • 0.24 7.96 7.946 0.
    • 0.25 7.96 7.946 0.
    • 0.26 7.96 7.946 0.
    • 0.27 7.96 7.946 0.
    • 0.28 7.95 7.936 0.
    • 0.29 7.95 7.936 0.
      • 0.3 7.95 7.936 0.
    • 0.31 7.95 7.936 0.
    • 0.32 7.95 7.936 0.
    • 0.33 7.94 7.926 0.
    • 0.34 7.94 7.926 0.
    • 0.35 7.94 7.926 0.
    • 0.36 7.94 7.926 0.
    • 0.37 7.94 7.926 0.
  • 0.38 7.93 7.916 0.
  • 0.39 7.93 7.916 0.
    • 0.4 7.93 7.916 0.
  • 0.41 7.92 7.906 0.
  • 0.42 7.92 7.906 0.
  • 0.43 7.92 7.906 0.
  • 0.44 7.91 7.896 0.
  • 0.45 7.91 7.896 0.
  • 0.46 7.9 7.886 0.
  • 0.47 7.89 7.876 0.
  • 0.48 7.88 7.866 0.
  • 0.49 7.87 7.856 0.
    • 0.5 7.84 7.826 0.
  • 0.51 7.57 7.556 0.
  • 0.52 7.18 7.166 0.
  • 0.53 6.3 6.286 0.
  • 0.54 5.65 5.636 0.
  • 0.55 5.6 5.586 0.
  • 0.56 4.87 4.856 0.
  • 0.57 4.38 4.366 0.
  • 0.58 3.75 3.736 0.
  • 0.59 3.34 3.326 0.
    • 0.6 3.11 3.096 0.
  • 0.61 2.65 2.636 0.
  • 0.62 2.37 2.356 0.
  • 0.63 2.03 2.016 0.
  • 0.64 1.73 1.716 0.
  • 0.65 1.57 1.556 0.
  • 0.66 1.38 1.366 0.
  • 0.67 1.28 1.266 0.
  • 0.68 1.08 1.066 0.
  • 0.69 0.89 0.876 0.
    • 0.7 0.78 0.766 0.
  • 0.71 0.72 0.706 0.
  • 0.72 0.64 0.626 0.
  • 0.73 0.56 0.546 0.
  • 0.74 0.51 0.496 0.
  • 0.75 0.45 0.436 0.
  • 0.76 0.41 0.396 0.
  • 0.77 0.38 0.366 0.
  • 0.78 0.35 0.336 0.
  • 0.79 0.34 0.326 0.
    • 0.8 0.31 0.296 0.
  • 0.81 0.29 0.276 0.
  • 0.82 0.25 0.236 0. - 0.83 0.22 0.206 0. - 0.84 0.19 0.176 0. - 0.85 0.19 0.176 0. - 0.86 0.17 0.156 0. - 0.87 0.17 0.156 0. - 0.88 0.17 0.156 0. - 0.89 0.16 0.146 0. - 0.9 0.15 0.136 0. - 0.91 0.15 0.136 0. - 0.92 0.15 0.136 0. - 0.93 0.14 0.126 0.
      • 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9