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905 Series NaI (Tl) scintillation radiation detector

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905 Series NaI (Tl) scintillation radiation detector image

905 Series NaI (Tl) scintillation radiation detector

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Brief description:Gamma rays interacting with the scintillator produce light pulses that are converted into electrical pulses by a photomultiplier tube (PMT)

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Detailed introduction

905 Series NaI(Tl) Scintillation Radiation Detector with DigiBASE Photomultiplier Base
Gamma rays interacting with the scintillator produce pulses of light that are converted into electrical pulses by a photomultiplier tube (PMT). PMT consists of a photocathode, a focusing electrode, and 10 or more dynodes that are used to multiply the number of electrons on each dynode. A series of resistors, usually located in the plug-in header assembly, will bias the anode and dynode. Complete components including scintillator and PMT are available.
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    • Download link 905 Series Brochure
    • Download link 905 Series Brochure (A4)
  • More information +


    Scintillation materials used to produce good detectors have characteristics such as transparency, large size, and large light output proportional to the gamma ray energy. Few materials have good properties for use in detectors. Commonly used materials are activated [NaI(Tl)] and cesium iodide [CsI(Tl)] crystals, as well as a variety of plastics. CsI(Tl) and plastic have much faster light decay times than NaI(Tl) and are primarily used in timing applications.

    The high Z iodine in the NaI(Tl) crystal ensures high efficiency in gamma ray detection. For 137Cs, resolution is typically around 7% for 3" diameter and 3" long crystals, slightly worse for larger sizes. The light decay time constant of NaI(Tl) crystal is about 0.23 μs. A typical charge-sensitive preamplifier converts this into an output voltage pulse with a rise time of approximately 0.5 μs. Fast coincidence measurements cannot achieve short resolution times with plastic scintillator, especially at low gamma ray energies.

    The 905 Series has Nal (TI) detectors in various sizes. These detectors are assembled and supplied to ORTEC by several companies specializing in the production of Nal (TI) detectors.

    Typical total counting efficiency given in percent for a 1-μCi 137Cs source centered at a 10-cm distance is as follows:
    905-1 (1" x 1"): 0.17 @0.5 MeV and 0.09 @2.0 MeV
    905-3 (2" x 2"): 0.75 @0.5 MeV and 0.45 @2.0 MeV
    905-4 (3" x 3"): 2.00 @0.5 MeV and 1.30 @2.0 MeV

    Note: Special sizes and configurations such as Wells, Thin Window X-rays, Thyroid Counters and Large Plates are available for special order.

  • Specifications +


    NOTE: Specifications will vary slightly due to original manufacturer.

    905-1 NaIscintillation detector,1 x 1inch crystal,2inch tube
    905-1 NaI(Tl) Scintillation Radiation Detector
    905-3 NaIscintillation detector,2 x 2inch crystal,2inch tube
    905-3 NaI(Tl) Scintillation Radiation Detector
    905-4 NaIscintillation detector,3 x 3inch crystal,3inch tube
    905-4 NaI(Tl) Scintillation Radiation Detector
    905-16 NaIscintillation detector,4 x 4inch crystal,3inch tube
    905-16 NaI(Tl) Scintillation Radiation Detector
    lead shieldG-5 Desktop lead shielded with cable duct. Supplied clamping mechanism to secure detector/PMTcomponent and forORTEC PMTThe base provides enough space to connect toPMT(see picture). Shipping weight: 300pounds (with905-16Detector is not compatible).
    Lead Shield G-5 Table top lead shield with cable-way for Scintillation Radiation Detector
  • Ordering information +


    Model

    Description

    905-1

    NaIscintillation detector,1 x 1inch crystal,2inchesPMT

    905-3

    NaIscintillation detector,2 x 2inch crystal,2inchesPMT

    905-4

    NaIscintillation detector,3 x 3inch crystal,3inchesPMT

    905-16

    NaIscintillation detector,4 x 4inch crystal,3inchesPMT。

    lead shieldG-5

    Desktop lead shield with cable duct.

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