Specifications

Table Of Contents
Version 1.1 rev Jan 2013
Page 38
iXon Ultra
Features and Functionality
During an acquisition using a conventional Frame Transfer CCD (FT CCD), the image area is exposed to light and an
image is captured. This image, in the form of an electronic charge, is then automatically shifted downwards behind the
masked region of the chip before being read out. To read out the sensor, charge is moved vertically into the readout
register, and then horizontally from the readout register into the output node of the amplier. As stated previously,
the readout register is extended to include the multiplication (gain) register. The amplication occurs in this register
through the scheme highlighted in Figure 8 below. When moving charge through a register, there is a very tiny, but nite
probability that the charges being transferred can create additional charge by a process known as “impact ionization”.
Impact ionization occurs when a charge is clocked and has sufcient energy to create another electron-hole pair in the
conduction band and by this process amplication occurs. To make this process viable, EMCCD’s optimize the process
in two ways:
1. The probability of any one charge creating a secondary electron is increased by giving the initial electron charge
more energy. This is typically done by replacing one of the electrodes (phases) of this readout section with two
electrodes. The rst is held at a xed potential, and the second is operated as normal, except that much higher
voltages are used than are necessary for charge transfer alone. The large electric eld generated between
the xed voltage electrode and the clocked electrode is sufciently high for the electrons to cause “impact
ionization” as they transfer. This impact ionization causes the generation of new electrons, i.e. multiplication or
gain.
2. The EMCCD is designed with hundreds of cells or pixels in which impact ionization can occur and although the
probability of amplication or multiplication in any one pixel is small (only around x1.01 to x1.015 times) over
the entire length of the EM register, the probability is very high and substantial gains of up to thousands can be
achieved.
Figure 8: Gain register operation