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| '''Photomultipliers''', or photomultiplier tubes (PMT) or phototubes for short, are extremely sensitive detectors of light in the ], ] and near ]. These detectors multiply the signal produced from the incident light from which single ] are detectable. | '''Photomultipliers''', or photomultiplier tubes (PMT) or phototubes for short, are extremely sensitive detectors of light in the ], ] and near ]. These detectors multiply the signal produced from the incident light from which single ] are detectable. | ||
| ] | |||
| Photomultipliers are constructed from a glass ] which houses a ] and an ]. Incident ] strike the ] material which is present as a thin deposit on the entry window of the device, with ] being produced as a consequence of the ]. These electrons are directed by the focusing ] towards the ], where electrons are multiplied by the process of secondary emission. | Photomultipliers are constructed from a glass ] which houses a ] and an ]. Incident ] strike the ] material which is present as a thin deposit on the entry window of the device, with ] being produced as a consequence of the ]. These electrons are directed by the focusing ] towards the ], where electrons are multiplied by the process of secondary emission. | ||
| The electron multiplier consists of a number of ]s, called dynodes. Each dynode is held at a more positive voltage than the previous one. The ]s leave the photocathode, having the energy of the incoming photon. As they move towards the first dynode they are accelerated by the electric field and arrive with much greater energy. On striking the first dynode, more low energy electrons are emitted and these, in turn, are accelerated toward the second dynode. The geometry of the dynode chain is such that a cascade occurs with an ever-increasing number of electrons being produced at each stage. Finally the anode is reached where the accumulation of charge results in a sharp current pulse indicating the arrival of a photon at the photocathode. | ].]] The electron multiplier consists of a number of ]s, called dynodes. Each dynode is held at a more positive voltage than the previous one. The ]s leave the photocathode, having the energy of the incoming photon. As they move towards the first dynode they are accelerated by the electric field and arrive with much greater energy. On striking the first dynode, more low energy electrons are emitted and these, in turn, are accelerated toward the second dynode. The geometry of the dynode chain is such that a cascade occurs with an ever-increasing number of electrons being produced at each stage. Finally the anode is reached where the accumulation of charge results in a sharp current pulse indicating the arrival of a photon at the photocathode. | ||
| ⚫ | Amplification can be as much as 10<sup>8</sup> meaning that measurable pulses can be obtained from single ]s. The combination of high gain, low noise, high frequency response and large area of collection have meant that these devices still find applications in ] and ], ], ] and motion picture film scanning (]). ]s like ]s have replaced photomultipliers in some applications, but photomultipliers are still used in most cases. | ||
| ] | ] | ||
| ⚫ | Amplification can be as much as 10<sup>8</sup> meaning that measurable pulses can be obtained from single ]s. The combination of high gain, low noise, high frequency response and large area of collection have meant that these devices still find applications in ] and ], ], ] and motion picture film scanning (]). ]s like ]s have replaced photomultipliers in some applications, but photomultipliers are still used in most cases. | ||
| While powered, photomultipliers must be shielded from ambient light to prevent their destruction through overexcitation. If used in a location with high magnetic fields (which will curve electron paths), they are usually shielded by a layer of ]. | While powered, photomultipliers must be shielded from ambient light to prevent their destruction through overexcitation. If used in a location with high magnetic fields (which will curve electron paths), they are usually shielded by a layer of ]. | ||
Revision as of 02:11, 8 March 2006
Photomultipliers, or photomultiplier tubes (PMT) or phototubes for short, are extremely sensitive detectors of light in the ultraviolet, visible and near infrared. These detectors multiply the signal produced from the incident light from which single photons are detectable.
Photomultipliers are constructed from a glass vacuum tube which houses a dynode and an anode. Incident photons strike the photocathode material which is present as a thin deposit on the entry window of the device, with electrons being produced as a consequence of the photoelectric effect. These electrons are directed by the focusing electrode towards the electron multiplier, where electrons are multiplied by the process of secondary emission.
The electron multiplier consists of a number of electrodes, called dynodes. Each dynode is held at a more positive voltage than the previous one. The electrons leave the photocathode, having the energy of the incoming photon. As they move towards the first dynode they are accelerated by the electric field and arrive with much greater energy. On striking the first dynode, more low energy electrons are emitted and these, in turn, are accelerated toward the second dynode. The geometry of the dynode chain is such that a cascade occurs with an ever-increasing number of electrons being produced at each stage. Finally the anode is reached where the accumulation of charge results in a sharp current pulse indicating the arrival of a photon at the photocathode.
Amplification can be as much as 10 meaning that measurable pulses can be obtained from single photons. The combination of high gain, low noise, high frequency response and large area of collection have meant that these devices still find applications in nuclear and particle physics, astronomy, medical imaging and motion picture film scanning (telecine). Semiconductor devices like avalanche photodiodes have replaced photomultipliers in some applications, but photomultipliers are still used in most cases.
While powered, photomultipliers must be shielded from ambient light to prevent their destruction through overexcitation. If used in a location with high magnetic fields (which will curve electron paths), they are usually shielded by a layer of mu-metal.
See also
References
- Engstrom, Ralph W., Photomultiplier Handbook, RCA (1980).
- anon, Photomultiplier Tubes: Principles and Applications, Philips Photonics, Brive, France, (1994).
- anon, Photomultiplier Tubes: Basics and Applications (Second Edition), Hamamatsu Photonics, Hamamatsu City, Japan, (1999).
- Flyckt, S.O. and Marmonier, C., Photomultiplier Tubes: Principles and Applications, Photonis, Brive, France, (2003).
External links
- Electron Multiplier Simulation of electron multiplier tube
- Molecular expressions A java simulation and tutorial on photomultiplier tubes
- Photomultiplier Tubes Basics and Applications from Hamamatsu Photonics
- Photomultiplier Handbook from Burle Industries, essentially the Engstrom-RCA Handbook reprinted
- Photomultiplier Tubes: Principles and Applications the Photonis applications book
- Photomultiplier Technical Papers from Electron Tubes Ltd