
At Pyramid we are constantly developing our range of products and services. Watch this page for information on new products, product applications and software releases. You can access older news items by clicking the links on the left-hand side.

A new clean manufacturing test area has been set up for our range of electronics and beamline instrumentation. The old manufacturing area is now dedicated for engineering development. Full segregation between production inventory and engineering materials is possible now. Please call by!

The CP10-A is optimized for use with fast inorganic scintillators like LaCl3, LaBr3 and YAP. The higher bandwidth CP10-B is intended for use with pulse-counting electron multipliers, channel plates and high-gain avalanche photodiode systems such as silicon photomultipliers.

These individual scintillation events from a LaCl3 detector illustrate the response of the two pre-amplifiers. The CP10-B on the right shows the individual avalanche structure of the event, but although this is interesting, it's not what you want for reliable pulse counting, so the CP10-A is the correct choice for this detector.


The C400 was developed in response to a requirement from FMB-Oxford (www.fmb-oxford.com) for synchrotron beamline diffraction detector electronics. Because this application can require clusters of fast photon-counting detectors operating in parallel, the C400 has trigger distrinution features to allow multiple units to operate in synchronization. It also includes a dedicated input for a position encoder, so that measured counts can be correlated directly with the position of a goniometer or similar motion device.
The C400 includes Ethernet, fiber optic and RS-232 / RS-485 interfaces. A fully-featured diagnostic host program is supplied which allows you to gather, display and log data, and control all the features of the device.
(Heidelberg Ion-Beam Therapy Center)
Particle therapy is an important tool in the fight against cancer. Beams of protons or heavier ions such as carbon 6+ are delivered to a precisely defined tumor volume in the patient's body. The ionizing radiation kills the cancer cells, and the particular energy deposition characteristic of the ions in the body means that healthy tissue is spared to a much greater extent than with the well-established X-ray therapy techniques. You can read an introduction to particle therapy by John Gordon published in the August 2010 issue of Physics World, or view it on-line here.
We are pleased in particular to be working with Dr Jay Flanz and his colleagues at the Francis H Burr Proton Therapy Center at Massachusetts General Hospital (MGH). This center is one of the leading sites in the world for the use and advancement of the technique. Pyramid developed and installed beam measurement and scan control systems at MGH to enable pencil-beam scanning treatments.
Pyramid brings its expertise with realtime systems, beamline diagnostics and beam scan control to particle therapy. We would be pleased to discuss your needs in any of the following particle beam technology areas:
Our customer at the University of Heidelberg requested that this facility be added to the PSI Diagnostic software. It is now available to all customers in version 4.62, which is available on the downloads page (here).
The software stores a compensation offset and gain factor for each channel, which are associated with a particular unit serial number. To measure the offsets, you simply ensure that the stimulus signal is absent, but that a representative background is present, and click the offsets button. Enter the value of the stimulus signal, which can be in any units you like, then apply the uniform flat field stimulus and click the gains button. The factors are calculated and stored.
The compensated values are accessed via a new "Comp" unit selection on the Data screen. In the following example, the first screenshot shows a flat field stimulus measured in absolute current units, in the normal way. The stimulus was used for a compensation calibration, and the second screenshot shows how it then appears when measured in compensated units. The response is flat, as required.
he F3200E can be triggered by the external sweep generator, or it can trigger the source itself. Data averaging schemes include block averaging of the incoming data for bandwidth narrowing, and averaging across multiple triggers in the manner of digital oscillscope waveform averaging. Even before averaging, the unloaded noise levels are less than 0.1% of full scale on each current range at 1 MSa/s conversion rate. The following plot shows RMS noise as a fraction of full scale, measured for the four current ranges, as a function of the number of ADC conversions averaged into each reading.
The F3200E is the first member of the enhanced G2 range of Pyramid products. It is compatible with the existing product line, including the A500 real-time loop controller, but adds significant on-board capability including an Ethernet interface, extended memory for data buffering and fully uploadable firmware. The Diagnostic host software is built on a RPC function library that is also available to customers who wish to create their own software.
Asked to comment on the F3200E, company president Dr Paul Boisseau would probably say "We are proud of the F3200E. It combines significant advances in analog and digital performance with a flexible, open software system. We expect that our customers will see features in their data, perhaps for the first time, that increase their understanding of their data and processes. That is the path to better results." Please look at the Products page here for further details of the F3200E.