Specifications
Table Of Contents
- iXon Ultra
- SAFETY AND WARNINGS INFORMATION
- SAFETY AND WARNINGS SYMBOLS
- MANUAL HANDLING
- SHIPPING AND STORAGE PRECAUTIONS
- SECTION 1 - INTRODUCTION TO IXON ULTRA HARDWARE
- 1.1 - TECHNICAL SUPPORT
- 1.2 - DISCLAIMER
- 1.3 - TRADEMARKS AND PATENT INFORMATION
- 1.4 - COMPONENTS
- 1.4.1 - Camera description
- 1.4.2 - Camera Power Supply Unit
- 1.4.3 - SOFTWARE
- 1.5 - SPECIFICATIONS
- 1.6 - ACCESSORIES
- 1.7 - SAFETY PRECAUTIONS AND MAINTENANCE
- 1.7.1 - Care of the camera
- 1.7.2 - Regular checks
- 1.7.3 - Annual electrical safety checks
- 1.7.4 - Replacement parts
- 1.7.5 - Fuse replacement
- 1.7.6 - Working with electronics
- 1.7.7 - Condensation
- 1.7.8 - Dew Point graph
- 1.7.9 - EM Gain ageing
- 1.7.10 - Minimizing particulate contamination
- 2.1 - INSTALLING THE HARDWARE
- 2.1.1- PC requirements
- 2.2 - INSTALLING ANDOR SOLIS SOFTWARE - WINDOWS O/S(XP/VISTA/SEVEN)
- 2.3 - NEW HARDWARE WIZARD
- 2.5 - WATER PIPE CONNECTORS
- 2.6 - MOUNTING POSTS
- 2.7 - COOLING
- 2.8 - START-UP DIALOG
- 3.1 - EMCCD OPERATION
- 3.1.1 - Structure of an EMCCD
- 3.1.2 - EM Gain & Read Noise
- 3.1.3 - EM Gain ON vs EM Gain OFF
- 3.1.4 - Multiplicative Noise Factor and Photon Counting
- 3.1.5 - EM Gain dependence and stability
- 3.1.6 - RealGain: Real and Linear gain
- 3.1.7 - EM Gain Ageing: What causes it and how is it countered?
- 3.1.8 - Gain and signal restrictions
- 3.1.9 - EMCAL
- 3.2 - COOLING
- 3.2.1 - Cooling options
- 3.2.2 - Heat generated in the EMCCD
- 3.2.3 Heatsink “hot side“ temperature
- 3.2.4 - Fan settings
- 3.3 - SENSOR READOUT OPTIMIZATION
- 3.3.1 - Sensor Pre-amp options
- 3.3.2 - Variable Horizontal Readout Rate
- 3.3.3 - Variable Vertical Shift Speed
- 3.3.4 - Output amplifier selection
- 3.3.5 - Baseline Optimization
- 3.3.5.1 - Baseline Clamp
- 3.3.6 - Binning and Sub Image options
- 3.4 - ACQUISITION OPTIONS
- 3.4.1 - Capture Sequence in Frame Transfer (FT) Mode
- 3.4.1.1 - Points to consider when using FT Mode
- 3.4.2 - Capture Sequence in Non-Frame Transfer Mode (NFT) with an FT EMCCD
- 3.4.2.1 - Points to note about using an FT EMCCD as a standard EMCCD
- 3.4.3 - Capture Sequence for Fast Kinetics (FK) with an FT EMCCD
- 3.4.3.1 - Points to consider when using Fast Kinetics mode
- 3.4.4 - Keep Clean Cycles
- 3.5 - TRIGGERING OPTIONS
- 3.5.1 - Triggering options in Frame Transfer (FT) mode
- 3.5.1.1 - Internal Triggering (FT)
- 3.5.1.2 - External Triggering (FT)
- 3.5.1.3 - External Exposure (FT)
- 3.5.2 - Triggering options in Non-Frame Transfer (NFT) mode
- 3.5.2.1 - Internal (NFT)
- 3.5.2.2 - External & Fast External (NFT)
- 3.5.2.3 - External Exposure (NFT)
- 3.5.2.4 - Software trigger (NFT)
- 3.5.3 - Trigger options in Fast Kinetics (FK) mode
- 3.5.3.1 - Internal (FK)
- 3.5.3.2 - External (FK)
- 3.5.3.3 - External Start (FK)
- 3.6 - SHUTTERING
- 3.7 - COUNT CONVERT
- 3.8 - OPTACQUIRE
- 3.8.1 - OptAcquire modes
- 3.9 - PUSHING FRAME RATES WITH CROPPED SENSOR MODE
- 3.9.1 - Cropped Sensor Mode Frame Rates
- 3.10 - ADVANCED PHOTON COUNTING IN EMCCDs
- 3.10.1 - Photon Counting by Post-Process
- 3.11 - SPURIOUS NOISE FILTER
- 4.1 - EMCCD TECHNOLOGY
- 4.1.1 - What is an Electron Multiplying CCD?
- 4.1.2 - Does EMCCD technology eliminate Read Out Noise?
- 4.1.3 - How sensitive are EMCCDs?
- 4.1.4 - What applications are EMCCDs suitable for?
- 4.1.5 - What is Andor Technology's experience with EMCCDs?
- 4.2 - EMCCD SENSOR
- 4.3 - VACUUM HOUSING
- 4.3.1 - Thermoelectric cooler
- 4.4 – USB 2.0 INTERFACE
- 4.5 - OUTGASSING
- 4.6 - EXTERNAL I/O
- 4.7 - SIGNAL DIAGRAMS
- 4.8 - CAMERALINK
- SECTION 5: TROUBLESHOOTING
- 5.1 - UNIT DOES NOT SWITCH ON
- 5.2 - SUPPORT DEVICE NOT RECOGNISED WHEN PLUGGED INTO PC
- 5.3 - TEMPERATURE TRIP ALARM SOUNDS (CONTINUOUS TONE)
- 5.4 - CAMERA HIGH FIFO FILL ALARM
- 5.5 - USE OF MULTIPLE HIGH SPEED USB 2.0 I/O ON ONE CAMERA
- A.1 - GLOSSARY
- A.1.1 - Readout sequence of an EMCCD
- A.1.2 - Accumulation
- A.1.3 - Acquisition
- A.1.4 - A/D Conversion
- A.1.5 - Background
- A.1.6 - Binning
- A.1.7 - Counts
- A.1.8 - Dark Signal
- A.1.9 - Detection Limit
- A.1.10 - Exposure Time
- A.1.11 - Frame Transfer
- A.1.12 - NOISE
- A.1.12.1 - Pixel Noise
- A.1.12.1.1 - Readout Noise
- A.1.12.1.2 - Shot Noise
- A.1.12.1.2.A - Shot Noise from the Signal
- A.1.12.1.2.B - Shot Noise from the Dark Signal
- A.1.12.1.3 - Calculation of Total Pixel Noise
- A.1.12.2 - Fixed Pattern Noise
- A.1.13 - Quantum Efficiency/Spectral Response
- A.1.14 - Readout
- A.1.15 - Saturation
- A.1.16 - Scans (Keep Clean and Acquired)
- A.1.17 - Shift Register
- A.1.18 - Signal To Noise Ratio
- B - MECHANICAL DIMENSIONS
- C - DECLARATION OF CONFORMITY
- D - HARDWARE AND SOFTWARE WARRANTY SERVICE
- D.1 - SERVICE DESCRIPTION
- D.2 - Access to Service
- D.3 - Hardware Remediation
- D.4 - Software Remediation
- E - THE WASTE ELECTRONIC AND ELECTRICAL EQUIPMENT REGULATIONS 2006 (WEEE)

Version 1.1 rev Jan 2013
Page 44
iXon Ultra
Features & Functionality
3.1.5 - EM Gain dependence and stability
EM Gain is a function of the EM voltage and of the sensor operating temperature. When the user applies gain
through the software, it is the EM voltage in the gain register that is varied. As can be seen from Figure 12 below, the
dependence of EM Gain on EM voltage is sharp (note the logarithmic scale). This arises because the signal electrons
acquire energy as they are accelerated through the EM electric eld, and once this eld strength reaches the threshold
needed to overcome the bandgap energy, the impact ionization rate rises rapidly. Historically, this sharp dependence
has meant that the software control of EM Gain in all EMCCD cameras has been via a non-linear scale with most of
the amplication occurring within a relatively small portion at the top of the overall scale. Thus considerable ne tuning
by the user to determine an optimal gain setting has been required, and even then the actual gain is determined only
through measurement of a stable light source, with and without gain applied.
Figure 12: EM Gain vs EM clock voltage
The effect of sensor temperature on EM Gain is shown in Figure 13. This dependence arises primarily from photon
scattering of electrons when they are accelerating in the EM electric eld. The scattering causes a loss of energy, which
increases with temperature. To make up this loss and maintain EM Gain, a larger EM electric eld must be used at higher
temperatures. As can be seen from Figure 13, EM Gains well in excess of x1000 can be achieved at low temperatures.
However, it is not recommended to use gains above x1000 because such high gains can cause signicant ageing of the
gain register (see EM Gain Ageing in Section 3.1.7).
Figure 13: EM Gain vs sensor cooling temperature










