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Photomultiplier Tubes
Photomultiplier Tubes’ invention is based upon two primary
discoveries:
 The Photoelectric Effect
 The Secondary Emission
Basic Introduction
Photomultiplier tubes are types of photo-detectors and
they are highly sensitive device towards light especially
whose wavelength lies in the range of UV, Visible and IR
region of the electromagnetic spectrum. Their basic use is
to amplify the signal input signal. Photomultiplier tubes
are widely used in Spectroscopy as a detector.
Construction and Working
The photomultiplier tubes are just similar in
construction to phototubes. A phototube consists of a semi-
cylindrical photocathode and an anode wire fixed inside an
evacuated glass tube.
When a voltage is applied across the two electrodes
and when light electromagnetic waves falls on the
photocathode, the emission of electrons takes place and
these electrons tend to move towards anode and hence the
photocurrent is observed.
Photomultiplier tubes are similar to that of phototube
that gives electrical signal on exposure of electromagnetic
waves.
The electrons emitted from photocathode start drifting towards anode (dynode) which
is maintained at up to 100 volt more positive with respect to cathode.
Primary Electrons
The electrons emitted after the strike of photons to
photocathodes are called ‘primary electrons’.
Secondary Electrons
The electrons ejected from dynode D1 by the fall of
primary electrons on it are called ‘secondary electrons’ and
similarly when these electrons fall on the surface of dynode D2,
more electrodes are emitted than earlier. These are all called
secondary electrons.
In this way by the successive striking of electrons on dynodes surface yield a large
number of electrons which are easily detectable as represented by the output
current.
Look at the diagram below:
Note that in the above diagram, dynode D1 is ~100 volt more
positive with respect to photocathode, D2 is 100 volt more
positive than D1, D3 is at 100 volt more positive than D2 and so
on. In this way amplification of electrons which is our gain
takes place we can imagine this multiplication process by an
estimation that each Photon results in the emission of about
107 electrons.
Muhammad Hamza Tahir
mhamzatahir481@gmail.com
+923126958957

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Photomultiplier tubes

  • 1. Photomultiplier Tubes Photomultiplier Tubes’ invention is based upon two primary discoveries:  The Photoelectric Effect  The Secondary Emission Basic Introduction Photomultiplier tubes are types of photo-detectors and they are highly sensitive device towards light especially whose wavelength lies in the range of UV, Visible and IR region of the electromagnetic spectrum. Their basic use is to amplify the signal input signal. Photomultiplier tubes are widely used in Spectroscopy as a detector.
  • 2. Construction and Working The photomultiplier tubes are just similar in construction to phototubes. A phototube consists of a semi- cylindrical photocathode and an anode wire fixed inside an evacuated glass tube. When a voltage is applied across the two electrodes and when light electromagnetic waves falls on the photocathode, the emission of electrons takes place and these electrons tend to move towards anode and hence the photocurrent is observed. Photomultiplier tubes are similar to that of phototube that gives electrical signal on exposure of electromagnetic waves.
  • 3. The electrons emitted from photocathode start drifting towards anode (dynode) which is maintained at up to 100 volt more positive with respect to cathode. Primary Electrons The electrons emitted after the strike of photons to photocathodes are called ‘primary electrons’. Secondary Electrons The electrons ejected from dynode D1 by the fall of primary electrons on it are called ‘secondary electrons’ and similarly when these electrons fall on the surface of dynode D2, more electrodes are emitted than earlier. These are all called secondary electrons.
  • 4. In this way by the successive striking of electrons on dynodes surface yield a large number of electrons which are easily detectable as represented by the output current. Look at the diagram below:
  • 5. Note that in the above diagram, dynode D1 is ~100 volt more positive with respect to photocathode, D2 is 100 volt more positive than D1, D3 is at 100 volt more positive than D2 and so on. In this way amplification of electrons which is our gain takes place we can imagine this multiplication process by an estimation that each Photon results in the emission of about 107 electrons. Muhammad Hamza Tahir mhamzatahir481@gmail.com +923126958957