2″x2″ NaI(Tl) | Scintillator Detector

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2″x2″ NaI(Tl) | Scintillator Detector is a sealed gamma-ray detector assembled with a high-resolution Dia. 2″x2″ NaI(Tl) scintillator and a 2″ Hamamatsu PMT tepe (CR105) combined and are installed in an aluminum housing.

 

Description

2″x2″ NaI(Tl) | Scintillator Detector is a sealed gamma-ray detector assembled by combining a high-resolution Dia. 2″x2″ NaI(Tl) scintillator and a 2″ Hamamatsu PMT tepe (CR105) in an aluminum housing.

 

KEY FEATURES

  • Product Name: 2″x2″ NaI(Tl) Scintillation Detector
  • Detector Components:
    Scintillator:Dia. 2″x2″ NaI(Tl) Scintillator
    PMT: Hamamatsu Dia. 2″ CR105 (10-stage, 14-pin connector)
  • Aluminum Housing

 

Technical Specifications

Energy Resolution

<7.5%@662keV(Cs-137)

Working Temperature

-30~+50℃

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3″x3″ NaI(Tl) | Scintillator Detector

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3″x3″ NaI(Tl) | Scintillator Detector is a gamma-ray detector which can output scintillation directly as an electrical pulse.

Description

3″x3″ NaI(Tl) | Scintillator Detector is a sealed gamma-ray detector assembled with a high resolution Dia. 3″x3″ NaI(Tl) scintillator and a 3″ Hamamatsu photomultiplier tube(CR119), accommodated in an aluminum housing. It can output the scintillation caused by the input radiation directly as an electrical pulse.

 

KEY FEATURES

  • Product Name: 3″x3″ NaI(Tl) Scintillation Detector
  • Detector Components:
    Scintillator:Dia. 3″x3″ NaI(Tl) Scintillator
    PMT: Hamamatsu Dia. 3″ CR119(8-stage, 14-pin connector)
  • Aluminum Housing

Technical Specifications

Energy Resolution

<7.5%@662keV(Cs-137)

Working Temperature

-30~+50℃

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6Li-Glass | Scintillation Crystal

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6Li-glass | Scintillation Crystals are used for a variety of radiation detection applications such as alpha, beta, gamma and neutron detection and they are suitable for use in corrosive environments.

Description

6Li-Glass | Scintillation Crystal (cerium-activated lithium silicate glass scintillator) has been used for a variety of radiation detection applications such as alpha, beta, gamma and neutron detection. Neutron detection is based on a neutron and 6Li nuclear reaction. 6Li glass scintillator has advantages of short decay time, good temperature stability, and high slow-neutron detection efficiency. Additionally, it is non-deliquescent, acid and alkali resistant, and high/low temperature rapid-change resistant, so it can be used in an environment where corrosive liquids and vapors exist.

 

MAIN APPLICATIONS

  • Neutron flight time experiment
  • Petroleum well logging
  • Moisture content measurement
  • NDT and neutron photography

Technical Specifications

Li-6 Content

7.5~11.2w†%

Relative Light Output

12% (NaI:Tl)

Density

~2.3g/cm3

Decay Constant (UV Excitation)

53ns

Wavelength of Maximum Emission

416nm

Working Temperature

-50~200°C

Resolution of Thermal neutron

≤28%

Scintillator Size

50~100mm

n-γ Identifying Features

neutron peak equivalent electron energy
Co-60—1.54MeV
Cs-137—1.70MeV
Ba-133—2.67MeV

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AgGaS2 | Infrared Crystal

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AgGaS2 | Infrared Crystal is an excellent middle-infrared, nonlinear optical crystal which has many applications in the middle and deep-infrared wavelengths due to its unique features.

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Description

AgGaS2 | Infrared Crystal is an excellent middle-infrared, nonlinear optical crystal which has many applications in the middle and deep-infrared wavelengths due to its unique features. The crystal has a low absorption coefficient, large effective optical nonlinearity (d36=39pm/V), and wide broad-transparency range (0.73 to 21μm). It is especially useful in transmission ranges between 0.9 to 16μm, and wide-phase matchability provides benefits for OPO applications when pumped by a variety of currently available lasers.
MAIN APPLICATIONS
  • OPO pumped by YAG(Nd) laser
  • Difference-frequency mixing experiments using diode, Sapphire(Ti), YAG(Nd), and IR dye lasers covering a range of 3 to 12µm
  • Direct infrared countermeasure systems
  • SHG of CO2 laser

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Aluminum Plating | Reflector

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Aluminum Plating Reflector | Reflector

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Description

Aluminum Plating | Reflector

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Anaerobic Copper | Reflector

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Anaerobic Copper | Reflector is an oxygen-free, copper-base material which can support high laser power and is commonly used in industrial settings.

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Description

Anaerobic Copper | Reflector is an oxygen-free, copper-base material which can support high laser power and is commonly used in industrial settings. After proper installation and alignment it will provide the limit diffraction focusing function. Anaerobic copper reflector has high reflectance and with a durable Mo layer, it is very easy to clean and work with under poor conditions. X-Z LAB can also customize various shapes and drill the holes for the reflector.

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BaF2 | Infrared Crystal

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BaF2 | Infrared Crystal has been commonly used as a UV-IR window material due to its broad transmission spectrum (190-1200nm).

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Description

BaF2 | Infrared Crystal has been commonly used as a UV-IR window material due to its broad transmission spectrum (190-1200nm). It is characterized by high transmittance, slight hygroscopicity, and little dependence of the refractive index on the temperature. It is also a kind of scintillation material which has high energy resolution and time resolution, can simultaneously measure the energy spectrum and time spectrum, and shows excellent radiation hardness up to 106 rad or even more.

 

MAIN APPLICATIONS

  • High energy physics
  • Nuclear physics
  • Nuclear medicine
  • Etc.

 

 

Technical Specifications

Crystalsystem

Hexagonal Crystal

Density

4.89g/cm3

Radiation length

2.03cm

Melting Point

1280°C

Hardness

3Mho

Decay Constant

0.6~620ns

Peak Emission

220~310nm

Light Yield

10400 Photons/MeV

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BaF2 | Scintillation Crystal

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BaF2 | Scintillation Crystal has been commonly used in UV-IR windows due to its broad transmission spectrum and excellent radiation hardness.

Description

BaF2 | Scintillation Crystal has been commonly used as a UV-IR window material due to its broad transmission spectrum of 190nm-1200nm. It is characterized by high transmittance, slight hygroscopicity, and the refractive index has little dependence on temperature. It also has high energy and time resolutions, can simultaneously measure the energy and time spectrums, and it shows excellent radiation hardness, up to 106 rad or even more.

 

MAIN APPLICATIONS

  • High energy physics
  • Nuclear physics
  • Nuclear medicine
  • Etc.

Technical Specifications

Crystal System

Hexagonal Crystal

Density

4.89g/cm3

Radiation Length

2.03cm

Melting Point

1280°C

Hardness

3Mho

Decay Constant

0.6~620ns

Peak Emission

220~310nm

Light Yield

10400Photons/MeV

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BaMgF4 | Infrared Crystal

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BaMgF4 | Infrared Crystal is one of the most useful materials in UV applications.

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Description

BaMgF4 | Infrared Crystal is one of the most useful materials in UV applications. It has advantages of good stability, high beam-quality, and it can also be continuously adjustable in the UV and VUV. Its short UV cut-off wavelength (125nm) makes it applicable to the quasi phase matching (QPM) in vacuum UV lasers. In addition, it is now widely used in high-resolution rate spectroscopy, micro nano-processing decomposition, UV lithography, and medicine categories.

MAIN APPLICATIONS

  • Double-frequency produces deep UV lasers
  • Optical materials
  • Laser materials
  • Memorized materials

Technical Specifications

Nonlinear optical property

Double frequency produce deep UV lasers

Transmission range:125-13000nm

Optical material & Laser material

Ferroelectricity

Memorized material

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BBO | Non-Linear Crystal

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BBO | Non-Linear Crystal is an excellent non-linear crystal for frequency-doubling (SHG) of Visible and Near IR laser light, OPO/OPG/OPA pumped by ultrafast pulses of wavelengths in the Near IR to UV, and sum-frequency mixing (SFM) into the Visible to the deep UV.

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Description

BBO | Non-Linear Crystal is an excellent non-linear crystal for frequency-doubling (SHG) of Visible and Near IR laser light, OPO/OPG/OPA pumped by ultrafast pulses of wavelengths in the Near IR to UV, and sum-frequency mixing (SFM) into the Visible to the deep UV. BBO is also one of the few practical crystals for use below 500 nm in SHG and SFM and can be widely used in medical, military and meteorology fields.

 

ADVANTAGES

  • High damage threshold
  • Broad phase matchable range from 409.6nm to 3500nm
  • Wide transmission region from 190nm to 3500nm
  • High optical homogeneity with n10-6/cm
  • Wide temperature-bandwidth of about 55°C
  • Large effective second-hamonic-generation coefficient about 6 times greater than KDP crystal

 

MAIN APPLICATIONS

  • Second, third, fourth and fifth harmonic generation of YAG(Nd)
  • Frequency-doubling, -tripling and -mixing of dye lasers
  • Optical parametric amplifiers (OPA) and optical parametric oscillators (OPO)
  • Second, third, fourth and fifth harmonic generation of Ti: sapphire and alexandrite
  • Frequency-doubling of Argon ions, Cu vapor, and ruby lasers
  • External intra-cavity SHG

 

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BBO Pockels Cell | Q-Switch Crystal

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BBO Pockels Cell | Q-Switch Crystals are used to change the polarization state of light passing at wavelengths from the UV to more than 2 μm.

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Description

BBO Pockels Cell | Q-Switch Crystal is used to change the polarization state of light passing at wavelengths from the UV to more than 2μm. Low piezoelectric ringing makes this Pockels cell attractive for the control of high-power and high-pulse repetition rate lasers. The quarter-wave voltage is relative to the ratio of crystal length and electrode spacing. Thus, compact aperture devices tend to exhibit a lower quarter-wave. But even for 2.5 mm aperture tools, the quarter-wave voltage remains 4kV at 1064nm. Double-crystal design has been used to cut down the required voltages and also to enable operation in half-wave mode with quick switching times.

 

ADVANTAGES

  • High repetition rate
  • High peak-power damage resistance
  • Low absorption
  • UV transmission
  • Low acoustic noise

 

MAIN APPLICATIONS

  • High repetition rate DPSS Q-Switch
  • High repetition rate regenerative amplifier control
  • Laser cavity dumping
  • Beam chopper

 

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BGO | Scintillation Crystal

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The BGO | Scintillation Crystal is the most widely used oxide-based scintillator owing to its many strengths, including high density, ruggedness, and radiation hardness.

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SKU: SCN-BGO Category:

Description

BGO (Bi4Ge3O12) is a scintillation crystal used for gamma ray detection with a high effective atomic number and density.

BGO | Scintillation Crystal has an emission peak of 480 nm, coupling well with PMT and SiPM. Compared to other scintillation crystals, BGO has an unparalleled absorption rate at photopeak. Its energy resolution is about 12%. The scintillation characteristics of BGO changes linearly with temperature. Combined with digital signal processing (DSP), it can work under harsh conditions. With small volume, it can work stably under refrigeration.

BGO | Scintillation Crystal is a tried and tested scintillator with many ideal scintillation properties, including:

  • High density and atomic number
  • Good radiation hardness
  • No hygroscopicity
  • Mechanical ruggedness
  • Low afterglow

Growth method: Bridgman
Formula: Bi4Ge3O12

With access to the complete crystal finishing process, X-Z LAB has the means to provide custom crystals using state-of-the-art line cutting; fine grinding and polishing machines; and stable matrix assembly techniques.

 

MAIN APPLICATIONS

The most common oxide-based scintillator, BGO | Scintillation Crystal has been the popular choice for radiation detection. Because of its high detection efficiency and excellent physical properties, it has overtaken NaI(Tl) in higher energy applications, such as positron emission tomography (PET). Other applications include high-energy physics, nuclear medicine, geological prospecting, and gamma pulse spectroscopy.

Technical Specifications

Density

7.13 g/cm³

Melting Point

1,323 K

Refractive Index

2.15

Effective Atomic Number

73

Hardness

5 Mohs

Hygroscopicity

No

Cleavage

No

Wavelength

480 nm

Lower Wavelength Cutoff

320 nm

Decay Time

300 ns

Light Output

8–10 photons/keV

Photoelectron Yield

15–20% ∝ NaI(Tl)

Thermal Expansion Coefficient

7 x 10⁻⁶/°C

Temperature Response

-1.2%/°C

Afterglow

0.005% @ 3 ms

Energy Resolution

12.0%

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