![generic header](/nsls2/images/generic-template-short.jpg)
Detector Group
MAIA Detector
Maia is an advanced system designed specifically for scanning X-ray fluorescence microprobe applications. It consists of a large array of photodiode detectors and associated signal processing, closely coupled to an FPGA based control and analysis system.
![MAIA Detector](../images/maia-detector-720px.jpg)
MAIA Detector
![MAIA Detector](images/maia-finished-350px.jpg)
Finished product
![MAIA Detector](images/maia-cross-section-350px.jpg)
The cross-section of MAIA
MAIA Detector Development
The planar diode sensors in MAIA limit the energy resolution. Also the noise performance of the current ASIC needs to be improved To obtain a low capacitance sensor, we are exploring the option of Silicon Drift Detectors or SDDs and samples are being fabricated. A new amplifier MARS has been designed to provide lower noise together with these low-capacitance detectors.
![MAIA Detector structure: old and new](images/maia-structure-old-and-new-720px.jpg)
The comparison between old (a) and new (b) MAIA structure—note the complexity of the new improved version
VIPIC (Vertically Integrated Photon Imaging Chip)
VIPIC is a small 64 x 64 pixels sensor for soft X-ray. It explores the possibilities of three-dimensional integration for x-ray imaging applications. VIPIC operates without any readout dead-time. Each detected photon is immediately read out as a time- and position-stamped event
![VIPIC chip](images/vipic-chip-720px.jpg)
VIPIC chip mounted on PCB
![VIPIC Scattering Pattern](images/vipic-scattering-pattern-350px.jpg)
Time-integrated image of scattering pattern recorded by VIPIC
HEXID (Hyperspectral Energy-resolving X-ray Imaging Detector)
HEXID can be thought of as a true color X-Ray camera! It is an imaging detector for x-rays, which provides spectroscopic data for each pixel. It would be the basis for a full-field elemental microscope, and also could reinvigorate the Laue white-beam diffraction method of crystallographic structure determination. We have fabricated a prototype of such a detector consisting of a 16 x 16 array of hexagonal pixels. The hexagonal array provides some reduction in the complexity of the charge-combining algorithm. In addition, there are fewer ways in which the charge can be split in a hexagonal array. In particular, the charge is at most divided into three pixels, not four as is the case for a square array. These two features both help in making the reconstruction of split charges easier and potentially lower noise (i.e. better energy resolution).
![HEXID prototype chips](images/hexid-chips-720px.jpg)
HEXID prototype chips