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CsI(Tl) Scintillator Crystals (Low After Glow)

  • High light yield 
  • Rugged and robust, durable against mechanical shock
  • A low afterglow version (0.05~0.39% @20ms, the value could be tailored upon request)
  • Applications: Nuclear Radiation Detection, Security and Industrial Inspection, Medical CT, etc.
  • CsI(Tl) Bulk Crystals, CsI(Tl) Scintillation Screens, and CsI(Tl) Scintillator Arrays are available
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Basic Properties:

Density(g/cm3)4.51Melting Point (K)894
Cleavage PlaneNoneHardness(Mohs)2
HygroscopicSlightlyRefractive Index at Emission Peak1.79
Emission Peak Wavelength (nm)550Lower Wavelength Cutoff (nm)320
Decay Time (ns)1000Light Yield (% of NaI(Tl) )40
Afterglow(%@20ms)0.05~0.39

CsI(Tl) or Thallium-activated Cesium Iodide crystals are among the brightest scintillator materials. Its emission peak sits at 550nm within the broad emission spectrum of 350-700nm, which matches well with photodiode readouts. And because photodiodes can be used, the sizes of the scintillator detectors can be reduced, with the additional advantage that one might need to use high-voltage supplies. Furthermore, photodiodes are less affected by magnetic fields. CsI(Tl) has a high light output of 54 photons/Kev, leading to a photoelectron yield to gamma radiations that amounts to 45% of the value of Na(I), making them one of the brightest scintillators ever known. CsI(Tl) is also well suited for detecting heavy charged particles utilizing particle pulse analysis technique as the ratio of its multiple decay time component is variant to the ionization capacity.  CsI(Tl) has a naturally larger photoabsorption cross-section compared to many other scintillator materials. This property in combination with its high radiation hardness and good stopping power made it great for applications like gamma spectroscopy and imaging.

Physically, CsI(Tl) is robust and has excellent mechanical properties because it has no cleavage plane, contributing to its reliable strength under various conditions. CsI(Tl) can be utilized in medical applications such as jaw and head scanning, security X-radiation inspection, well-logging, space research, etc. However, it is worth noting that CsI(Tl) is a slow scintillator, which limits its potential when fast speed is critical.

Afterglow is defined as the fraction of scintillation light that persists for a specific time after the excitation source has stopped. In most applications, afterglow is undesirable because it can interfere with the detector’s performance. For example, in X-ray scanning, afterglow can retard the decay of illumination, leading to image blurring and reduced clarity. Low afterglow CsI(Tl) inherit high light yield from normal CsI(Tl) while restraining the afterglow phenomenon with high effectiveness, enhancing the image quality.

Hangzhou Shalom EO offers custom Low Afterglow CsI(Tl) scintillators; the products highlight a low afterglow of 0.05~0.39% @20ms; we could tailor the value of afterglow upon your request. The products are available as CsI(Tl) blanks, polished crystals, encapsulated scintillators, CsI(Tl) arrays, CsI(Tl) array +PD assemblies, and 2-dimensional arrays upon customer's request. Our CsI(Tl) scintillation crystals and CsI(Tl) arrays feature excellent radiation hardness, high light output, and reliable robustness. Our CsI(Tl) crystals could be applied in diverse fields, including nuclear radiation detection, high energy physics, security X-radiation scanning machines, Industrial inspection, and medical equipment of Computerized Tomographic (CT) Scanning. 


Figure 1. shows a pair of comparison curves of the afterglow of normal CsI(Tl) and our low afterglow CsI(Tl)

                                                             


Figure 2. shows a sample image obtained using our low afterglow CsI(Tl)

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CsI(Tl) Scintillator Crystals

CsI(Tl) Scintillator Crystals

  • Maximum size reaching 400mm x 400mm x 100 mm
  • We can provide CsI(Tl) in many special shapes and designs, such as CsI(Tl) with a hole bore in the center/well-shaped CsI(Tl), CsI(Tl) scintillators with single or multiple windows
  • Superiorly high light output, 52 photons keV average
  • Good γ-ray stopping power and radiation hardness
  • Emission peak at 550nm, matches well with photodiodes
  • Robust physical properties
  • Low afterglow CsI(Tl) available. and besides the CsI(Tl) bulk crystals, we also provide CsI(Tl) Scintillation Screens, and CsI(Tl) Scintillator Arrays are available
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CsI Scintillation Crystals

CsI Scintillation Crystals

  • Fast decay time: 16ns
  • Emission peak at 315nm
  • Lower light output than CsI(Tl) and CsI(Na)
  • Grown using the Bridgman method, maximum size diameter 90mm x 300mm length and above
  • High stopping power
  • CsI one-dimensional line arrays, CsI two-dimensional plane arrays, CsI(Tl), and CsI(Na) also available
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