Laser-Pumped Lamps | Optics and Laser Elements

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Laser-Pumped Lamps | Optics and Laser Elements include the laser-pumped pulsed xenon lamp and laser-pumped continuous krypton lamp, which are based on the high-quality cut-off UV quartz tube as lamp materials.

Description

Laser-Pumped Lamps | Optics and Laser Elements include the laser-pumped pulsed xenon lamp and laser-pumped continuous krypton lamp, which are based on the high-quality cut-off UV quartz tube as lamp materials. The reserve-type electrode is the lamp emitter electrode. They also have high load strength, high pump efficiency, good beam quality, and long lifetimes.

 

MAIN APPLICATIONS

  • YAG lamp-pump lasers
  • Precision welding, cutting, and drilling applications in the electronic, medical, automotive, and fine-mechanics market.

 

 

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LBO | Non-Linear Crystal

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LBO | Non-Linear Crystal is an excellent nonlinear optical crystal for frequency doubling (SHG) and tripling (THG) of YAG(Nd), YLF(Nd), and YVO4(Nd) lasers.

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Description

LBO | Non-Linear Crystal is an excellent nonlinear optical crystal for frequency doubling (SHG) and tripling (THG) of YAG(Nd), YLF(Nd), and YVO4(Nd) lasers. Its transmission range is from 0.21 um to 2.3 um and it is one of the most useful nonlinear optical materials in ultraviolet and visible laser applications. In addition, it allows temperature-controllable non-critical phase matching for 1.0-1.3 um, type I SHG, and also provides room temperature NCPM for Type II SHG at 0.8-1.1um.

 

ADVANTAGES

  • Broad transparency range from 160nm to 2.6um
  • High optical homogeneity (dn»10-6/cm) and free of inclusion
  • Relatively large effective SHG coefficient (about three times that of KDP)
  • Wide acceptance angle and small walk-off
  • Type I and type II non-critical phase matching in a wide wavelength range
  • Spectral NCPM near 1300nm
  • High damage threshold

 

MAIN APPLICATIONS

  • Medical and industrial field of YAG(Nd) lasers, Sapphire(Ti) and LiSAF(Cr) lasers
  • Scientific research and military field of high power YAG(Nd), YLF(Nd) lasers
  • OPO and OPA, SHG, THG for high power 1340nm YAP(Nd) lasers

 

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LiF | Infrared Crystal

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LiF | Infrared Crystal is a type of cubic crystal which can be cleaved along 100 and less commonly 110.

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Description

LiF | Infrared Crystal is a type of cubic crystal which can be cleaved along 100 and less commonly 110. It has high optical transmittance from the vacuum ultraviolet to the infrared spectrum region (0.11 to 7μm) and shows excellent transmittance in the VUV regions. Modest precautions should be taken against moisture and high energy radiation damage. LiF is effected by atmospheric moisture at 400 °C and softens at 600 °C. It is sensitive to thermal shock and irradiation produces color centers.

 

MAIN APPLICATIONS

  • Windows
  • Lenses
  • Polarizers
  • Prisms
  • UV-sources
  • Receivers
  • Excimer lasers
  • X-ray fluorescence instruments

 

 

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LiIO3 | Non-Linear Crystal

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LiIO3 | Non-Linear Crystal is an uniaxial non-linear crystal with high non-linear optical coefficients and wide transparency range.

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Description

LiIO3 | Non-Linear Crystal is an uniaxial non-linear crystal with high non-linear optical coefficients and wide transparency range.  It is used for frequency doubling of the low and medium power Sapphire(Ti) and other lasers, and in some cases, it is used for frequency doubling and tripling of YAG(Nd) lasers and auto-correlators to measure ultra-short pulse width. In addition, it has wide prospect in the aviation, chemical, metallurgy, and oil industries.

 

ADVANTAGES

  • Large nonlinear coefficients, broad angular, and temperature bandwidth
  • Low dielectric constants and low ionic conductivities
  • Lower absorption in the 3-4 μm spectrum range than KTP
  • Highly resistant to high-intensity laser radiation

 

MAIN APPLICATIONS

  • From the SHG to FHG of the fundamental laser emission in the range from 0.69 to 2.0μm
  • OPO of the tuned radiation in ranges from 0.8 to 4.0μm
  • Frequency multiplication and mixing in transparency crystal range from 0.28 to 5.5μm
  • Measurement of parameters of ultra-short laser pulses, including the single ones
  • Visualization of IR radiation to obtain the object image by non-linear optical methods

 

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LiNO3 | Piezo-Electrical Crystal

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LiNO3 | Piezo-Electrical Crystal has excellent electro-optic, acousto-optic, piezoelectric, and nonlinear properties and is widely used in civil and military fields.

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LiNO3 | Piezo-Electrical Crystal has excellent electro-optic, acousto-optic, piezoelectric, and nonlinear properties and is widely used in civil and military fields. With the development of photoelectric technology, LiNbO3 crystal is increasingly emphasized in the application of defense technology. It is an important multifunctional crystal with good nonlinear properties and has a relatively large nonlinear optical coefficient, which can realize the critical phase matching. As an electro-optic crystal, it serves as an important optical waveguide material and as a piezo-electric crystal, it can be used to make middle and low frequency SAW filters as well as high power and high temperature ultrasonic transducers, etc. LiNbO3 material also has wide applications; LN(Mg) crystal can greatly improve the anti-laser damage threshold; LN(Mg)(Nd) crystal can realize the frequency doubling effect; LN(Fe) crystal can be used in optical holographic storage.

 

MAIN APPLICATIONS

  • Pockel Cells
  • Q-switches
  • Phase modulators
  • Waveguide substrate
  • Surface acoustic wave (SAW) wafers
  • Etc.

 

 

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LiTaO3 | Piezo-Electrical Crystal

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LiTaO3 | Piezo-Electrical Crystal is an important multi-functional material with excellent piezoelectric, ferroelectric, acousto-optic, and electro-optic effects.

Description

LiTaO3 | Piezo-Electrical Crystal is an important multi-functional material with excellent piezoelectric, ferroelectric, acousto-optic, and electro-optic effects. It is a basic functional material in SAW devices, optical communication, and laser and photoelectron fields. X-Z LAB supplies high quality LiTaO3 boules, wafers, or slices with the specifications for standard applications. We can also offer other specifications upon request.

 

MAIN APPLICATIONS

  • Resonators
  • SAW filters
  • Energy converters
  • Electronic communication devices
  • Mobile phones
  • Interphones
  • Satellite communications
  • Aerospace
  • High-end communications

 

 

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LN&MgOLN | Q-Switch Crystal

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LN&MgOLN | Q-Switch Crystal is a low-cost photoelectric material with good mechanical and physical properties, as well as high optical homogeneity.

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Description

LN&MgOLN | Q-Switch Crystal is a low-cost photoelectric material with good mechanical and physical properties, as well as high optical homogeneity. It has been widely used as frequency doublers for wavelengths greater than 1mm and optical parametric oscillators (OPOs) pumped at 1064nm, as well as quasi-phase-matched (QPM) devices. With preferable E-O coefficients, LiNbO3 crystal has become the most commonly used material for Q-switches and phase modulators, waveguide substrate, and surface acoustic wave (SAW) wafers, etc. Compared with LiNbO3, LiNbO3(MgO) crystal exhibits a higher damage threshold.

 

ADVANTAGES

  • Large nonlinear optical coefficient
  • The receiving angle is large and the angle of the angle is small.
  • Wide temperature and spectral bandwidth
  • High photoelectric coefficient and low dielectric constant
  • No water absorption
  • Chemical and mechanical properties

 

MAIN APPLICATIONS

  • Military laser radar
  • Industrial application of YAG(Nd) laser systems
  • Medium-sized laser power devices
  • Etc.

 

 

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LSO(Ce) | Scintillation Crystal

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LSO(Ce) | Scintillation Crystal is a new type of high-quality inorganic scintillation crystal, which is especially suited for gamma ray detection.

Description

LSO(Ce) | Scintillation Crystal is a new type of inorganic scintillation crystal with high light output, fast decay time, excellent radio resistance, high detection efficiency, is non-hygroscopic, and is stable. Its emission peak matches the photomultiplier receiving range and is especially suited for gamma ray detection.

 

MAIN APPLICATIONS

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

Technical Specifications

Crystal System

Monoclinic

Density

7.3~7.4g/cm3

Hardness

5.8Mohs

Decay Constant

≤47ns

Peak Emission

410nm

Light Yield

26000Photons/MeV

Energy Resolution

≤13%

Index of Refraction

1.82

Radiation Hardness

>1x108rad

Melting Point

2070°C

Light Output

75% (Relative to NaI)

Hygroscopicity

None

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LuAG(Ce) | Scintillation Crystal

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LuAG(Ce) | Scintillation Crystal is a rugged, mechanically and chemically stable scintillator ideal for photodiode and avalanche diode readout.

SKU: SCN-LUAG-CE Category:

Description

LuAG(Ce) | Scintillation Crystal is a rugged, mechanically and chemically stable scintillator ideal for photodiode and avalanche diode readout.

LuAG(Ce) | Scintillation Crystal is a relatively dense and fast scintillation material. Its characteristics include fast decay time, high density, and mechanical and chemical stability. LuAG(Ce) can be machined into a variety of shapes and sizes, including prisms, spheres, and very thin plates. The wavelength of scintillation emission is about 535 nm, which is ideal for photodiode and avalanche diode readout. The material can also be used for imaging screens, similar to YAG(Ce). A particular advantage of LuAG(Ce) is its higher density, resulting in thinner screens with higher spatial resolution.

 

KEY FEATURES

  • Mechanical resistance and stability
  • High density
  • Fast decay time
  • Non-hygroscopicity

 

MAIN APPLICATIONS

  • Positron emission tomography (PET)
  • Gamma and charged particle detection
  • Electron and X-ray imaging screens

 

Technical Specifications

Density

6.7 g/cm³

Melting Point

2223 K

Refractive Index

1.84

Hardness

8.5 Mohs

Radiation Length

1.3 cm

Hygroscopicity

No

Cleavage

No

Wavelength

535 nm

Decay Time

70 ns

Light Output

12.5 photons/keV

Energy Resolution

≤ 7.5%

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LuAG(Pr) | Scintillation Crystal

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LuAG(Pr) | Scintillation Crystal is a dense, mechanically robust scintillator with a fast decay time suitable for fast particle image, TOF-PET, and positron emission mammography.

SKU: SCN-LUAG-PR Category:

Description

LuAG(Pr) | Scintillation Crystal is a dense, mechanically robust scintillator noted for its fast decay time.

LuAG(Pr) | Scintillation Crystal is an excellent scintillator with high density, fast response time, and high light yield. It is mainly characterized by a high light output of 20 photons/keV, a short decay time constant of 20 ns, and a large effective atomic number of 62.9. LuAG(Pr) with a Pr doping concentration of 3% has slightly higher fluorescence intensity, but the position of the excitation peak does not change for different concentrations.

 

KEY FEATURES

  • High density
  • High energy resolution
  • High light output
  • Fast decay time
  • Non-hygroscopicity

 

MAIN APPLICATIONS

  • Fast particle imaging
  • Time-of-flight positron emission tomography (TOF-PET)
  • Positron emission mammography (PEM)

Technical Specifications

Density

6.7 g/cm³

Melting Point

2223 K

Refractive Index

2.03 @ 310 nm

Effective Atomic Number

62.9

Hardness

8 Mohs

Radiation Length

1.41 cm

Hygroscopicity

No

Cleavage

No

Wavelength

310 nm

Decay Time

20 ns

Light Output

20–22 photons/keV

Photoelectron Yield

20% ∝ NaI(Tl)

Thermal Expansion Coefficient

8.8 × 10⁻⁶/°C

Energy Resolution

≤ 5%

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LYSO(Ce) | Scintillation Crystal

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The LYSO(Ce) | Scintillation Crystal by X-Z LAB is a new type of scintillation material with excellent scintillation properties, including high light output, short decay time, high density, and anti-radiation hardness.

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SKU: SCN-LYSO-CE Category:

Description

LYSO (Lu1-xYxSi2O5) belongs to the monoclinic system. LYSO(Ce) | Scintillation Crystal is a scintillation crystal with the best combination of properties available at present.

LYSO(Ce) | Scintillation Crystal emits 420 nm light and couples well with PMT under the stimulation of high energy. It also has the advantage of high light yield, short decay time, high density, non-deliquescence, and all around stable physical and chemical properties. Owing to its excellent time and energy resolution, LYSO(Ce) | Scintillation Crystal is widely used in nuclear medicine and nuclear physics.

LYSO(Ce) | Scintillation Crystal is a new type of scintillation material with excellent scintillation properties, including:

  • High light output
  • Short decay time
  • High density and anti-radiation hardness
  • Stable chemical and physical properties

Growth method: Czochralski
Formula: Lu1-xYxSi2O5
Dimensions: Max diameter 65 mm x 180 mm length (maximum boule)
Available items: Monolithic and pixelated LYSO

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

 

MAIN APPLICATIONS

LYSO(Ce) | Scintillation Crystal is the ideal positron emission tomography (PET) and scintillator crystal. It has improved energy and timing resolution compared to traditional crystals, such as BGO (bismuth germanate). This is vital to get a clear image and shorten the scanning process.

The global market for PET has been estimated to be around $1 billion worldwide, including the USA, Europe, and Asia, where most of the growth is occurring. The current main PET service suppliers are GE Healthcare, Positron Corporation, Philips Healthcare, Siemens Healthcare, and Raytest.

Technical Specifications

Density

7.1 g/cm³

Melting Point

2,323 K

Refractive Index

1.81

Effective Atomic Number

60

Hardness

5.8 Mohs

Radiation Length

1.16 cm

Hygroscopicity

No

Cleavage

No

Wavelength

420 nm

Decay Time

41 ns

Light Output

> 28 photons/keV

Photoelectron Yield

75% ∝ NaI(Tl)

Temperature Response

-0.28%/°C

Energy Resolution

10%

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MgF2 | Infrared Crystal

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MgF2 | Infrared Crystal is a positive, uni-axial crystal with a very high optical transmittance from the vacuum UV to IR.

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Description

MgF2 | Infrared Crystal is a positive, uni-axial crystal with a very high optical transmittance from the vacuum UV to IR. Its useful transmission range is 0.12 to 8.5μm and irradiation does not lead to color centers. MgF2 is a chemically stable, hard material which is resistant to thermal and mechanical shock. It is a positive birefringent crystal grown normally to a large diameter by the vacuum stockbroker technique, seeding along the c-axis.

 

MAIN APPLICATIONS

  • UV and excimer laser windows
  • Polarizers
  • Prisms
  • Lenses
  • Wedges
  • Windows
  • Other optical components

 

 

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