Detectors

The standard detection system for full-field X-ray tomography consists of three main components:

  • Scintillator
  • Optical microscope
  • Visible light camera

The scintillator converts the X-ray image produced by the transmission and refraction of the X-ray beam through the sample, also called the shadowgraph or radiograph, into visible light. This visible light image is then magnified by the optical microscope, which is focused at the imaging plane of the scintillator. The magnified image is finally digitally recorded by a highly sensitive visible light camera. 

Various combinations of different scintillators, microscopes, and cameras are available at TOMCAT to achieve the optimal image quality for a given experimental setup. The choice of equipment depends mainly on the desired magnification, spatial resolution, and field of view, as well as the X-ray energy to be used and the required acquisition speed. 

The table below lists the most relevant microscope-camera combinations, showing the achievable pixel sizes and maximum fields-of-view (max. FOVs), and sorted according to the maximum horizontal field of view (max. FOV H mm) from largest to smallest. The maximum FOVs were calculated from the effective pixel size and camera pixel resolution, but please note that the vertical beam size at S-TOMCAT is limited to ~4 mm, and that the beam size at I-TOMCAT is limited to 1.5 mm x 1.5 mm. The actual maximum FOVs are therefore reduced depending on which beamline the detector will be used.

Detailed descriptions and specifications of the microscopes and cameras on the table can be found at the bottom of the page.

Microscope

Magnification (×)

Camera

Effective Pixel Size (µm)

Max. FOV H (mm)

Max. FOV V (mm)

Microscope 2

1

GigaFRoST

11.00

22.18

~4

Microscope 2

1

pco.edge 10

4.60

20.31

~4

Microscope 2

1

pco.edge 5.5

6.50

16.64

~4

Microscope 1

1.25

pco.edge 5.5

5.20

13.31

~4

Microscope 2

1

pco.edge 4.2

6.50

13.31

~4

Microscope 1

2

pco.edge 5.5

3.25

8.32

~4

Macroscope 5

4

GigaFRoST

2.75

5.54

~4

Macroscope 5, 1

4

pco.edge 5.5

1.63

4.16

3.51

Microscope 6, 7

10

GigaFRoST

1.10

2.22

2.22

Microscope 6, 7

10

pco.edge 10

0.46

2.03

1.09

Microscope 7

10

pco.edge 10

0.46

2.03

1.09

Microscope 1, 6, 7

10

pco.edge 5.5

0.65

1.66

1.40

Microscope 8

13.5

GigaFRoST

0.81

1.64

1.64

Microscope 8

13.5

pco.edge 10

0.34

1.50

0.81

Microscope 8

13.5

pco.edge 5.5

0.48

1.23

1.04

Microscope 6

20

GigaFRoST

0.55

1.11

1.11

Microscope 6

20

pco.edge 10

0.23

1.02

0.54

Microscope 1, 6

20

pco.edge 5.5

0.33

0.83

0.70

Microscope 8

27

GigaFRoST

0.41

0.82

0.82

Microscope 8

27

pco.edge 10

0.17

0.75

0.40

Microscope 8

27

pco.edge 5.5

0.24

0.62

0.52

Microscope 1

40

pco.edge 5.5

0.16

0.42

0.35

Please remember that pixel size DOES NOT EQUAL spatial resolution! As a general rule-of-thumb, two pixels are necessary to define an edge and three pixels are necessary to define a feature. So, depending on your goals, the true spatial resolution is typically 2-3 times the effective pixel size.

The following sections give an overview of the most commonly used scintillators, and an exhaustive list of microscopes and cameras routinely used at TOMCAT.

Depending on user requirements (optimizing for scanning speed and/or spatial resolution), several scintillators are available. The LuAG:Ce scintillators are most frequently used for our standard experiments as they provide a good compromise between speed and resolution. The following table lists the most commonly used scintillators:

ScintillatorThickness (μm)Spatial ResolutionScanning Speed
LSO:Tb5.9Excellent (<1μm)Slow
LuAG:Ce20Good (~1μm)Fast
LuAG:Ce100-150Medium (>3μm)Faster
LuAG:Ce300Poor (>10μm)Fastest

Note that the thickness of the scintillator affects the overall spatial resolution! The thicker a scintillator, the poorer the spatial resolution due to light scattering within the scintillator material. The thickness should thus be matched with the effective pixel size of the optical system. 

Other scintillator options are available. If you need a specialized setup, please contact beamline staff in advance of your experiments. Users are also welcome to bring their own scintillators, but should contact beamline staff in advance to ensure that the scintillator fits onto the microscope and a proper mount is available and ready to use.

TOMCAT has a pool of optical microscopes that are compatible with all of our standard cameras. The following paragraphs give a detailed information on each microscope.

Microscope 1: Standard High-resolution Microscope (Optique Peter)

This microscope is based on a revolver system that can accommodate up to three objectives at the same time. The diffraction-limited objective type and magnifications available are listed in the table below. It is not compatible with high X-ray photon flux, i.e. filtered white beam and monochromatized undulator beam. 

Objective

Magnification

PLAPO1.25x

1.25x

PLAPO2x

2x

UPLAPO4x

4x

UPLAPO10x

10x

UPLAPO20x

20x

UPLAPO40x

40x

Microscope 2: 1:1 Optics (Optique Peter)

This system is based on a high numerical aperture, tandem 1:1 configuration, accepting a diagonal up to 40 mm. It is typically used for the DPC (differential phase contrast) imaging setup or for large samples that do not require high spatial resolution. It can be used in combination with all our cameras and can be operated using both polychromatic and monochromatic radiation. This is the microscope offering the largest effective pixel size option. 

Lens

Magnification

Focal length

KinoOptik

1.0

150 mm

Macroscope 5: High Numerical Aperture 4x White-Beam Macroscope (Optique Peter)

This novel, high quality, custom-made macroscope offers a 4x magnification and has a very high numerical aperture of 0.35, making it highly efficient. The macroscope is modular, flexible and can be mounted both in a horizontal and vertical configuration, to best match the sample environment and imaging requirements. It has been designed for high-resolution time-resolved X-ray tomographic microscopy and can be operated using both polychromatic and monochromatic radiation, coupled either to a pco.edge camera or a GigaFRoST detector. The macroscope has a tunable aperture which can be used to optimize the spatial resolution for different imaging setups. The high efficiency and superior image quality of the macroscope have made tomographic studies with a time resolution of 20 Hz and beyond at TOMCAT a reality. A detailed description of the macroscope performance can be found here (DOI: 10.1107/S1600577519004119).

Microscope 6: Dual-Head (10x and 20x) White-Beam Macroscope (Optique Peter) 

This is a dual-head, high-magnification, white beam microscope from Optique Peter. Our model is equipped with long working distance objectives offering a 10x (NA=0.28) and 20x (NA=0.42) magnification with integrated lead glass. Each head has it’s own scintillator support. It can be operated using both polychromatic and monochromatic radiation, coupled either to the pco cameras or GigaFRoST detector. A detailed specification of this microscope is listed below.

Lens  

Magnification  

Numerical Aperture 

Lead Glass 

Working Distance 

Tube length  

X10 

10x

0.28 

4.5mm 

26.9mm 

200 mm  

X20 

20x

0.42 

3mm 

15.2mm 

200 mm  

Microscope 7: High Numerical Aperture 10x White-Beam Microscope (Optique Peter) 

This is the latest long-working distance generation of white beam, single-objective microscope from Optique Peter. Our model is offering a 10x magnification with a numerical aperture of 0.4. The macroscope is modular, flexible and can be mounted both in a horizontal and vertical configuration, to best match the sample environment and imaging requirements. It has been designed for high-resolution, time-resolved X-ray tomographic microscopy and can be operated using both polychromatic and monochromatic radiation, coupled either to the pco cameras or GigaFRoST detector. The special head design allows the beam to go through and perform multi-scale imaging at the same time. A detailed specification of this microscope is listed below.

Lens  

Magnification  

Numerical Aperture 

Tube length  

X10 

10x

0.4 

200 mm  

Microscope 8: Single-Head (13.5x or 27x) White-Beam Macroscope (Optique Peter) 

This is a single head, high magnification, white beam microscope from Optique Peter. Our model is equipped with long working distance objectives which can be exchanged between 10x (NA=0.28) and 20x (NA=0.42) high magnification lenses with integrated lead glass. In combination with a tube lens, it offers a magnification of 13.5x and 27x, respectively. It can be operated using both polychromatic and monochromatic radiation, coupled either to the pco cameras or GigaFRoST detector. A detailed specification of this microscope is listed below.

Lens  

Magnification  

Numerical Aperture 

Lead Glass 

Working Distance 

Tube length  

X10 

13.5x  

0.28 

4.5mm 

26.9mm 

270 mm 

X20 

27x  

0.42 

3mm 

15.2mm 

270 mm 

The following detectors are routinely in use at TOMCAT and fully supported in the data acquisition and controls system. The choice of detector is governed mostly by the requirements in terms of the achievable pixel size, field of view, image quality and acquisition speed. The table below gives the key specifications for these cameras, while the paragraphs below contain more specific information about each camera model.

 pco.edge 4.2  pco.edge 5.5  pco.edge 10 bi CLHS  pco.dimax  GigaFRoST  
Manufacturer  PCO PCO PCO PCO PSI in-house  
Pixel size [μm]  6.5  6.5  4.6 11.0  11.0  
Sensor size [pixels] (h x v)  2048 x 2048  2560 x 2160  4416 x 2368 2016 x 2016  2016 x 2016  
Sensor size [Megapixels]  4.2  5.5  10.4 4.1  4.1  
Max frame rate (full frame)  100 fps (FS) 
35 fps (SS)  
100 fps (FS,RS) 
33 fps (SS,RS)  
122 fps (RS)  1255 fps  1255 fps  
Max frame buffer (full frame)  3'000  3'000   6’307  71’860  
Exposure time  100μs - 10s  500μs - 2s  

6.8 μs - 1 s @ fast scan 

27.5 μs - 1 s @ slow scan  

2μs - 40ms  2μs - 40ms  
Shutter mode  RS  RS/GS  RS  GS  GS  
Bit-depth  16-bit  16-bit  16-bit  12-bit  12-bit  
Dynamic range [dB]  90.4  88.6  83.7 65.8  65.8  
Peak QE  >70%  >60%  >85%  >50%  >50%  
Dark current [e- 1.0  1.2  0.4 e-/pixel/s @ +10 °C <20  <20  
Cooling  water (chiller)  water (chiller)  forced air & water air (fan)  air (fan)  

Legend RS: Rolling Shutter, GS: Global Shutter, FS: Fast scan, SS: Slow scan

pco.edge 5.5

This is the low noise and large field of view camera by pco, and the work-horse camera for standard measurements at TOMCAT. It is built on sCMOS technology and features a sensor size of 2560 x 2160 pixels, 6.5μm pixel size and a 16-bit nominal dynamic range → technical specifications.

pco.edge 4.2

This is the slightly smaller brother of the pco.edge 5.5, featuring even slightly lower noise levels, but at the expense of a reduced sensor size (2048 x 2048 pixels). It is also based on sCMOS technology with a 6.5μm pixel size and a 16-bit nominal dynamic range → technical specifications.

pco.edge 10  

This is the latest generation camera, featuring a large sensor size (4416 x 2368 pixels) and small pixel size (4.6 μm). It is also based on sCMOS technology and a 16-bit nominal dynamic range with a high QE.  → technical specifications 

pco.dimax

The pco.dimax is the high-speed camera offered by pco. The imaging chip is built on CMOS technology and features 2016 x 2016 pixels, 11μm pixel size and a 12-bit nominal dynamic range. The camera has an on-board memory of 36 GB and is read out via a USB2.0 connection (slow!) → technical specifications

This camera is rarely used at present and mostly replaced by the GigaFRoST camera.

GigaFRoST

The GigaFRoST camere is a PSI in-house development incorporating the same imaging chip as the pco.dimax, but featuring a novel readout system providing continuous and sustained data streaming at up to ~8GB/s to a dedicated high-performance data backend server. This allows for the high-speed acquisition of long time series to observe dynamic phenomena in a time-resolved manner during long perdiods of time. 

For an in-depth description of the GigaFRoST camera system refer to R. Mokso, C. M. Schlepütz, G. Theidel, H. Billich, E. Schmid, T. Celcer, et al., "GigaFRoST: The Gigabit Fast Readout System for Tomography", J. Synchrotron Rad., 24 (6), 1250-1259 (2017). DOI: 10.1107/S1600577517013522.