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About laser crystals

About laser crystals

In this post, we would like to educate you about laser crystals.

Er,Cr:YSGG Crystals

About laser crystals About laser crystals

Erbium- and chromium-doped yttrium-scandium-gallium garnet (Er, Cr: YSGG) is an effective laser crystal for lasing  with a wavelength of 2800 nm, which is an important water absorption band. Er, Cr: YSGG crystal has a high conversion efficiency, stable chemical properties, and a long fluorescence lifetime. These crystals are widely used in dentistry, environmental studies, communication systems, military industry and remote sensing technologies.


Special features:

– High conversion efficiency;

– Excellent optical properties;

– Lasing modes modes: continuous, free generation or Q-modulation;

– The lowest generation threshold among standard erbium-doped crystals;

– the highest differential quantum efficiency among standard erbium-doped crystals;

– Natural disorder leading to an increase in the width of the spectral pumping line and in strength;

– Flash lamp (chromium absorption bands) or diode (erbium bands) pumping;

– Long fluorescence lifetime.


Main properties of Er,Cr:YSGG crystals:

ParametersDescription and values
Crystal structurecubic, garne
Growing methodChokhralsky’s method
Chemical formulaY2.93Sc1.43 Ga3.64O12
Lattice parameters12.42 Å
Doping (atoms/cm3Cr:5×1020 , Er:×1021
Density5.67 g/cm3(Cr&Er doping)
Refraction index1.92 at 1000 nm
Coefficient of thermal expansion8.1×10-6/K
Thermal conductivity (W/mK)8
Mineralogical hardness8
Thermo-optic coefficients(dn/dT)(10-6/K)12.3
Emission cross-section (cm2)5.2×10-21
Fluorescence lifetime1400 µs


Nd:YVO4 Crystals

About laser crystalsAbout laser crystals

Neodymium-doped yttrium-vanadate crystals (Nd:YVO4) are some of the most effective laser crystals for coherent sources with diode pumping, especially for sources with low and middle power density. Their absorption and emission properties are even better than those of Nd:YAG crystals.

A laser diode pumped Nd:YVO4 crystal was combined with crystals with a high non-linearity factor (LBO, BBO  or KTP) to shift the frequency of the lasing output from the near-IR to the green, blue or even UV spectral region.  This combination in solid-state lasers is an ideal tool for most common laser applications, including material processing, spectroscopy, wafer quality control systems, laser printing, etc. It is proven that diode-pumped ND: YVO4 solid-state lasers quickly gain markets where water-cooled ion lasers and lamp-pumped lasers traditionally dominate, especially when a compact design and emission with a single longitudinal mode are required.


Advantages of Nd:YVO4 lasers over Nd:YAG:

– The absorption coefficient is 5 times greater in the whole wide pumping range around 808 nm (besides, the dependence on the pump wavelength is much lower, and there is also a strong tendency to form single-mode emission);

– The stimulated emission cross-section is 3 times larger at a wavelength of 1064 nm;

– Lower generation threshold and higher differential quantum efficiency;

– Uniaxial crystal with double refraction: linearly polarized radiation.


Special features:

– Doping: 0.1% – 3%;

– Doping material concentration tolerance: ±0.05% (atoms%<1%), ±0.1% (atoms%≥1%);

– Crystals of various sizes and of high quality;

– 10 000 items Nd:YVO4 per month 3x3x0.5 – 4x4x8 mm3 in size;

– Competing prices.

Nd:YVO4 crystal absorption curve ( 0.5% doping, 4 mm thick)

Nd:YVO4 crystal properties

ParametersDescription and values
Atoms concentration1.26×1020 atoms/cm3 (Nd 1.0%)
Crystals structure

Unit cell parameter

Zircon Tetragonal, space group D4h-I4/amd
a=b=7.1193Å, c=6.2892Å
Density4.22 g/cm3
Mineralogical hardness4-5 (glass)
Thermal expansion coefficient (300 K)αa=4.43×10-6/K
Thermal conductivity coefficient (300 K)∥C:0.0523 W/cm/К
⊥C:0.0510 W/cm/К
Laser wavelength1064 nm, 1342 nm
Thermo-optic coefficients (300 K)dno/dT=8.5×10-6/K
Stimulated emission cross-section25×10-19 cm2  at 1064 nm
Fluorescence lifetime90 ms (1%)
Absorption coefficient31.4 cm-1 at 810 nm
Inner losses0.02 cm-1 at  1064 nm
Amplification bandwidth0.96 nm at 1064 nm
Polarized laser radiationPolarized; Parallel to the optic axis (c-axis)
Pump efficiency as to laser optical efficiency>60%
Selmeyer’s equation (λ in um)no2=3.77834+0.069736/(λ2-0.04724)-0.010813λ2

Nd:YVO4 lasers properties 

1. One of the most appealing properties of Nd:YVO4 crystals is their absorption coefficient, which is 5 times bigger  than that of Nd:YAG crystals in a wide range with the peak around 808 nm, what corresponds to the standard wavelength of laser diodes of high power. It means that it is possible to use more compact crystals in lasers, resulting in size reduction of a coherent radiation source system as a whole. Besides, a lower power of a pumping laser diode is needed, which, in its turn, increases the laser diode lifetime. The absorption bandwidth of Nd:YVO4 may be 2.4 – 6.3 times bigger than that of Nd:YAG crystals. High efficiency of pumping allows choosing less expensive laser diodes for pumping.

2. Nd:YVO4 crystals have a wider cross-section of stimulated emission at both 1064 nm and 1342 nm wavelengths.  At 1064 nm wavelength lasing, this cross-section is 4 times as big as the cross-section of a similar Nd:YAG crystal; at  1340 nm lasing the cross-section is 18 times bigger. This enables Nd:YVO4 lasers to support powerful single mode radiation at both wavelengths.

3. Unlike Nd:YAG crystals with cubic symmetry, Nd:YVO4 crystals are single uniaxial, that makes it possible to generate linear polarized emission. Though, the service lifetime of Nd:YVO4 is 2.7 times shorter than that of  Nd:YAG, their differential quantum efficiency is rather high due to the high pumping efficiency.

Comparison of Nd:YVO4 and Nd:YAG characteristics is given below:

stimulated emission cross-section (σ), absorption coefficient (α), fluorescence lifetime (τ), absorption length (Lα), threshold power (Pth) and quantum efficiency of pumping (ηs).

Nd:YVO4 and Nd:YAG characteristics


(atoms %)


(×10-19 cm2)


























Comparison of Nd:YVO4 and diode-doped Nd:YAG lasers

CrystalSize (mm3)Pumping powerOutput emission (at 1064 nm)
Nd:YVO43×3×1850 mW350 mW
Nd:YVO43×3×515 W6 W
Nd:YAG3×3×2850 mW34 mW

Diode-pumped Nd:YVO4+KTP laser

– 8 W green light generated by an Nd:YVO4 (0.5% doping, 15 W pumping laser diode. KTP crystal inside the resonator.

– 200 mW green light generated by an Nd:YVO4 (2% doping, 1 W pumping laser diode.

– KTP crystal: 2x2x5 mm3, Nd:YVO4 crystal: 3x3x1 mm3.

Anti-reflective coating

– Both butt-ends with anti-reflective coating for 1064/808 nm, R<0.2% at 1064 nm, R<2% at 808 nm;

– 1 surface: high reflective coefficient coating at 1064&532 nm, with high transmittance coefficient for 808 nm, R>99.8% at 1064&532, T>90% at 808 nm;

– 2 surface: anti-reflective coating at 1064&532 nm, R<0.2% at 1064 nm; R<0.5% at 532 nm;

– 1 surface: high reflective coefficient coating at 1064 nm, with high transmittance coefficient for 808 nm, R>99.8% at 1064, T>95% at 808 nm;

– 2 surface: anti-reflective coating at 1064 nm, R<0.1% at 1064 nm;

– 1, 2 surface: anti-reflective coating, 3 surface: gilding / chrome plating;

– Both butt-ends with anti-reflective coating at 1064 nm, 3 surface anti-reflection coating for 808 nm;

– Other variants of coating at request.



Nd:GdVO4 crystals

About laser crystals

 Nd:GdVOcrystals are used as active substance in diode-pumped solid-state lasers. They have some advantages over Nd:YAG  crystals: wide emission cross-section, wide absorption band, polarized lasing output.


Special features:

– Wide cross-section of stimulated emission at the laser wavelength;

– High absorption coefficient and wide operation range at the pumping wavelength;

– Low pumping wavelength dependency;

– High thermal conductivity;

– Low lasing threshold, high differential quantum efficiency;

– High damage threshold;

– Highly polarized laser radiation;.

Main properties:

– Wavefront distortion: <λ/4 at 633 nm;

– Crystal dimension limit: (W±0.1 mm)x(H±0.1 mm)x(L+0.2/-0.1mm);

– Aperture: >90%;

– Flatness: λ/8 at 633 nm, λ/4 at 633 nm for crystals< 2 mm thick;

– Surface quality 10/5 Scratch/Dig (characteristic chip size) (MIL-PRF-13830B);

– Parallelism: < 20 arcseconds;

– Perpendicularity: ≤5 arcseconds;

– Angle tolerance: <±30′.

Nd:GdVO4 crystals characteristics+

ParametersDescription and values
Crystal structureTetragonal
Space groupI41/amd
Lattice parametersa=0.721 nm, b=0.635 nm
Lasing transition4F3/2 —-> 4I11/2
Laser wavelength1062.9 nm
Emission cross-section (at 1064 nm)7.6×10-19 cm2
Absorption cross-section (at 808 nm)4.9×10-19 сm2
Absorption coefficient (at 808 nm)74 см-1
Refraction index (at 1064 nm)no=1.972,ne=2.192
Thermal conductivity11.7 Вт/(м×K)
Density5.47 g/cm3
Nd (atomically) doping0.1%,0.2%,0.3%,0.5%,0.7%,1.0%,…

Nd:GdVO4 and Nd:YVO4 properties comparison

Crystal structure,  space groupTetragonal, I41/amdTetragonal, I41/amd
Lattice parameters (nm)a:0.721




Melting temperature (℃)17801825
Thermal expansion coefficient at 25℃, ×10-6/℃a1.5a4.43
Specific heat capacity at 25℃, cal/(mole·К)32.624.6

Comparison of neodymium laser material properties

Laser wavelength1064.3 nm,

1342.0 nm

1062.9 nm,

1340 nm

1064.2 nm

1338.2 nm

Emission bandwidth
(line width 1064 nm)
0.8 nmn/a0.45 nm
Effective emission cross-section
(Emission cross-section at 1064 nm)
15.6×10-19 cm27.6×10-19 cm26.5×10-19 cm2
PolarizationParallel to c axisParallel to c axisNon-polarized
Pumping wavelength808.5 nm808.4 nm807.5 nm
Pumping absorption peak at 1% doping~41 cm-1~57 cm-1
Thermal conductivity, W/m/K5.111.714
Doping concentration0.1-3.0%0.1-3.0%0.1-2.0%



Nd:YAG Crystals

About laser crystalsAbout laser crystals

Neodymium-doped aluminum yttrium garnet («YAG», Y3Al5O12) crystals are most popular and long-used laser crystals. As long as these crystals combine plenty of property advantages, Nd:YAG are used in almost every solid-state laser of the near IR range, as well as in modules for generation of second, third and higher harmonics.


Nd:YAG crystals advantages:

– High gain coefficient;

– Low lasing threshold;

– High efficiency;

– High optic characteristics;

– Low losses at 1064 nm;

– Good thermal conductivity and thermostability;

– High mechanical toughness;

– Lasing modes: continuous, pulse, Q modulation, mode synchronization.

Special features:

– Size: 15×180 mm– 40×2 mm2;

– Nd doping: 0.3~2.0(±0.1) % atoms;

– Diameter tolerance: ±0.05 mm;

– Length tolerance: ±0.5 mm;

– Perpendicularity: ≤5 angular minutes;

– Parallelism: <10 angular minutes;

– Wavefront distortion: λ/8;

– Flatness: λ/10;

– Surface quality: 10/5 (MIL-O-13830A);

– Highly reflective coating: R>99.8% at 1064 nm, R< 5% at 808 nm;

– Anti-reflective coating (one layer of MgF2): R<0.25% for each surface (at 1064 nm);

– Other reflective coatings for 1064/532 nm, 946 nm, 1319 nm, etc.;

– Damage threshold: >500 MW/ cm2.

Nd:YAG crystals main features

Parameters Description and values
Chemical formulaY3Al5O12
Crystal structureCubic
Lattice parameters12.01Å
Melting temperature1970°C
Density4.5 g/сm3
Reflection index1.82
Thermal expansion coefficient7.8×10-6 /K,0 – 250 ℃
Thermal conductivity14 ВW/m/К, 20 °C
10.5 W/m/К, 100 °C
Mineralogical hardness8.5
Stimulated emission cross-section2.8×10-19 cm-2
Loss coefficient0.003 cm-1 at 1064 nm
Line width0.6 nm
Laser junction lifetime550 ms

Nd:YAG crystals optic parameters

Diameter (mm)StandardHigh qualityTop quality
φ3-6.35≤0.5 interference band/inch≤0.25 interference band/inch≤0.1 interference band/inch
≥25 dB≥28 dB≥30 dB
φ7-10≤0.7 interference band/inch≤0.4 interference band/inch≤0.16 interference band/inch
≥22 dB≥25 dB≥28 dB
φ11-13≤1 interference band/inch≤0.6 interference band/inch≤0.2 interference band/inch
≥20 dB≥23 dB≥26 dB
φ14-16≤1.2 interference band/inch≤0.8 interference band/inch≤0.25 interference band/inch
≥18 dB≥20 dB≥23 dB

Optional Nd:YAG rods and sheets are available for ordering, Nd:YAG rods for 946 nm and 1319 nm. Er:YAG, Yb:YAG and other ion-doped YAG crystals are delivered at request.



Cr4+:YAG crystals

About laser crystalsAbout laser crystals

Chrome-doped aluminum-yttrium garnet («YAG», Y3Al5O12) crystals are very good for work with Nd:YAG, Nd:YLF, Nd:YVO4 lasers or coherent sources with Nd- and Yb-doped crystals, passive Q-switching and diode or lamp pumping in the wavelength range of 0.8 – 1.2 um. Due to their chemical stability, durability, UV resistance, good thermal conductivity and high radiation resistance (> 500 MW / cm2), these crystals will soon replace the traditionally used materials (LiF, organic dyes and color centers).

Cr 4+ :YAG crystals with doping in the range of 0.5 mole% – 3 mole% are available for ordering. Crystal sizes vary from 2×2 mm2 to 14×14 mm2 , from 0.1 mm to 12 mm long. The transmittance coefficient may vary from 10% to 92% according to the request.

Preliminary experiments with Cr 4+: YAG crystals showed that the pulse width of passively Q-switched lasers can be shorter than 5 ns for diode-pumped Nd: YAG lasers, and a pulse repetition rate of 10 kHz for diode-pumped Nd: YV lasers.

Cr 4+ :YAG crystals can be also used as laser crystals for lasers adjustable in the range of 1.35 – 1.55 um. When   Nd:YAG laser pumped at a wavelength of 1.064 um, this source can generate ultrashort pulses.

Attention: when ordering Cr 4+ :YAG crystals specify the size, coating type and crystal transmittance coefficient.

Cr 4+ :YAG crystals properties

ParametersDescription and values
Crystal structureCubic
Doping level0.5 mole% ~ 3 mole%
Radiation resistance> 500 MW/cm2
Reflection index1.82 at 1064 nm



Ho:Cr:Tm:YAG crystals

About laser crystalsAbout laser crystals

Ho:Cr:Tm:YAG crystals are highly efficient material for active laser medium, enabling lasing with a wavelength of 2.1 um. They are widely used in surgery, dentistry, atmospheric analysis, etc.

Specific features:

– High differential quantum efficiency;

– Lamp or diode pumping;

– Operation at room temperature;

– Operates at the eye-safe wavelength .

Ho:Cr:Tm:YAG crystals technical features

ParametersDescription and values
Lasing transition7 → 5 I 8
Laser wavelength2.097 um
Photon energy9.55 x 10-20 J
Emission cross-section7 x 10-21 cm2
Fluorescence lifetime8.5 ms
Refraction index1.80 at 2.08 um
Absorption line width4 nm
Diode pumping line781 nm
Pumping band400~800 nm
Doping elements concentrationHo:~0.35 atoms%, Tm:~5.8 atoms%, Cr:~1.5 atoms%
Wavefront distortion≤ 0.125λ/inch (at 1064 nm)
Extinction coefficient≥25 дБ
Rod sizeDiameter: 3~6 mm, length: 50~120 mm

at request

Size toleranceDiameter: +0.00/-0.05 mm, length: ± 0.5 mm
SurfacingLapping: 400# Grit
Surface quality10/5
Angularity0.006″±0.002″ at 45°± 5°
Antireflective coatingReflection ≤ 0.25% (at 2094 nm)



Nd:Ce:YAG Crystals

About laser crystals About laser crystals

In neodymium- and cerium-doped aluminum yttrium garnet (Nd:Ce:YAG) cerium is chosen as a neodymium ions  (Nd3+) sensibilizer because of its strong UV-range absorption at lamp pumping and effective energy transfer to Nd3+ excitation. As a result, thermal deformations in Nd: Ce: YAG crystals are much smaller, and the output radiation energy is much greater than that of Nd: YAG crystals under similar pumping conditions. These properties make it possible to create high power lasers based on Nd: Ce: YAG crystals with excellent beam quality. The wavelength of such a laser will be 1064 nm. The radiation resistance and thermal conductivity of Nd: Ce: YAG crystals are similar to those of Nd: YAG crystals.


Special features:

– High efficiency;

– Low lasing threshold;

– UV exposure resistance;

– High thermal resistance;

– High quality.

Optic and spectral properties of Nd:Ce:YAG crystals

ParametersDescription and values
Lasing transition4 F 3/2–> 4 I 11/2
Laser wavelength1.064 um
Photon energy1.86×10-19 J at 1.064 um
Emission bandwidth4.5Å at 1.064 um
Emission cross-section (Nd 1 atoms %)2.7~8.8×10-19 cm-2
Fluorescence lifetime230 ms
Refraction index1.8197 at 1064 nm
Doping elements concentrationNd:1.1~1.4 atoms%, Ce:0.05~0.1 atoms%
Wavefront distortion≤ 0.2λ/inch
Extinction coefficient≥28 dB
Rod sizeDiameter:3~6 mm, length: 40~80 mm

At request

Size toleranceDiameter: +0.000“/-0.002”, length: ±0.02″
SurfacingLapping: 400# Grit
Surface quality10/5 (MIL-PRF-13830B)
Angularity0.006″±0.002″ at 45°± 5°
Anti-reflective coating. Reflection≤ 0.25% (at 1064 nm)




Yb:YAG Crystals

About laser crystalsAbout laser crystals

Ytterbium-doped aluminum yttrium garnet (Yb:YAG) crystals are one of the most prospective materials better suited for diode doping than neodymium-doped (Nd) crystals. As compared to more popular Nd:YAG crystals, Yb:YAG crystals have a wider absorption band, which reduces requirements for thermal control systems, have a longer lifetime, and a 3-4 times less thermal capacity. Yb:YAG crystals emit radiation with a wavelength of 1030 nm and are excellent replacement for Nd:YAG crystals (1064 nm). The second harmonic wave of Yb:YAG laser radiation (515 nm) can serve as an alternative to argon (Ar) lasers (514 nm).

Characteristic features:

– Heating: less than 11 %;

– High differential quantum efficiency;

– Wide absorption band: 8 nm at 940 nm;

– No absorption from excited state;

– Reliable InGaAs diode pumping at 940 nm (or 970 nm);

– High  thermal conductivity and endurance;

– Excellent optic qualities.

Yb:YAG crystals technical features

ParametersDescription and  values
Doping elements concentrationYb: 5~15 at. %
Wavefront distortion≤ 0.125λ/inch
Extinction coefficient≥28 dB
Rod sizeDiameter: 2~20 mm, length: 5~150 mm

at request

Dimension limitDiameter: +0.00“/-0.002” mm, length: ± 0.02″
SurfacingLapping: 400# Grit
Surface quality10/5 (MIL-PRF-13830B)
Angularity0.006″±0.002″ at 45°± 5°
Anti-reflective coating. Reflection≤ 0.25% (at 1030 nm)
Losses per pass<3×10-3 cm-1
Lasing transition2 F 5/22 F 7/2
Laser wavelength1030 nm
Photon energy1.93×10-19 J (at 1030 nm)
Emission bandwidth9 nm
Emission cross-section2.0×10-20 cm2
Fluorescence lifetime1.2 ms
Diode pumping line940 nm or 970 nm
Absorption bandwidth of pumping radiation8 nm
Reflection index1.82
Thermo-optic coefficient9×10-6/℃
Loss factor0.003 cm-1



Er:YAG Crystals

About laser crystalsAbout laser crystals

Erbium-doped aluminum yttrium garnet (Er:YAG) crystals are very good for lasers with a wavelength of 2940 nm. Radiation with this wavelength corresponds to the water and hydroxylapatite absorption lines. These crystals are widely used for medical purposes, particularly, in dentistry, orthopedics etc.

Specific features

– High differential quantum efficiency;

– Very good for operation at room temperature;

– Works at a relatively eye-safe spectral wavelength range.

Technical features of Er:YAG crystals

ParametersDescription and values
Doping elements concentrationEr: ~50 at. %
Wavefront distortion≤0.125λ/inch (at 1064 nm)
Extinction coefficient≥25 dB
Rod sizeDiameter: 3~6 mm, length: 50~120 mm

at request

Dimensional limitDiameter: +0.000″/-0.002″,

length: ± 0.02″

SurfacingLapping: 400# Grit
Surface quality10/5 (MIL-PRF-13830B)
Angularity0.006″±0.002″ at 45°± 5°
Anti-reflective coating. Reflection≤ 0.25% (at 2940 nm)
Lasing transition4 I 11/2 – 4 I 13/2
Laser wavelength2940 nm
Photon energy6.75×10-20 J (at 2940 nm)
Emission cross-section3×10-20 cm2
Refraction index1.79 при 2940 nm
Pumping range600~800 nm





Nd:YLF Crystals

About laser crystalsAbout laser crystals

Top-quality basic materials for crystal growth, crystal interferometry and strict quality control by way of He-Ne laser beam diffusion analyzing allow using of all these elements for solving tasks with highest level requirements.

Special features:

– Rod size (diameter), 1 – 150 mm(long);

– Rod axis  orientation  against crystal axis:  around 1;

– Polished  surface or anti-reflective coating;

– Doping elements concentration  (Nd): 0.4 – 1.2 at. %;

– Other doping elements sizes and concentrations are available at request.

 Nd:YLF crystal optical  properties

ParametersDescription and values
Transparency range180-6700 nm
Stimulated emission cross-section1.8×10-19/cm(E∥c) at 1047 nm
1.2×10-19/cm(E⊥c) at 1053 nm
Fluorescence lifetime485 ms for 1% Nd-doped
Diffusion loss<0.2%/cm
Absorption coefficient (for 1.2% neodymium)α= 10.8 cm-1 (792.0 nm E∥c)
α= 3.59 cm-1 (797.0 nm E⊥c)
Laser wavelength1047 nm (∥c, a-cross-section)
1053 nm (⊥c, a or c-cross-section)

Nd:YLF crystals physical properties

ParametersDescription and values
Chemical formulaLiY 1.0-x Nd x F4
Space groupI41/a
Nd atoms/cm31.40 x 1020 atoms/cm3  for 1% Nd doped
Youngs’s modulus85 hPa
Crystal structureTetragonal
Unit cell parametersa=5.16 Å, c=10.85 Å
Melting temperature819℃
Mineralogical hardness4~5
Density3.99 g/cm3
Thermal conductivity0.063 W/cm/K
Specific heat0.79 J/g/K
Thermal expansion coefficients8.3×10-6/k∥c
13.3×10-6/ k⊥c

Refraction index of Nd:YLF crystals

Wavelength (nm)none

Thermo-optic coefficients of Nd:YLF dn/dT crystals

Wavelength (nm)E∥cE⊥c

Sellmeyer’s ratio (λ in um)



Nd:YLF laser crystals specification

ParametersDescription and values
Standard concentration of doping elements1.1 ± 0.1%
Wavefront distortion<λ/4 per inch at 633 nm
Parallelism<10 ″
Perpendicularity<5 ′
Angularity0.13± 0.07 mm at 45°
Surface quality10/5
CoatingR<0.15% at 1047/1053 nm
Surface flatnessλ/8 at 632.8 nm



Cr:LiSAF Crystals

About laser crystals About laser crystals

They are very good for laser active medium, as they have high differential quantum efficiency. These crystals are also suitable for work with ultrashort pulses of high power. Today, gadgets based on Cr:LiSAF are widely used in systems with diode and lamp pumping.

Specific features:

– Sizes:  from 2 to 6 mm (rod diameter), 1 – 180 mm (rod length);

– Doping elements concentration (Cr): 0.5~1.0 mole%;

– Parallelism: <10 ″;

– Perpendicularity: <5 ′;

– Angularity: 0.13±0.07 mm ×45°;

– Surface quality: 10/5 (MIL-PRF-13830B);

– Flatness: λ/8 at 632.8 nm;

– Anti-reflective coating: R<0.10% at 850 nm.

Other rod sizes and crystals with non-standard doping elements concentration are available at request.

Cr:LiSAF crystals physical properties

ParametersDescription and  values
Chemical formulaCr 3+ :LiSrAlF6
Lattice parametera=5.084 Å,c=10.21 Å
Crystal structureTrigonal
Cr atoms/cm3 at 1% doping8.75×1019
Fracture toughness (mPas)0.40(||c)
Melting temperature766℃
Density3.45 g/cm3
Young’s module109 hPa
Thermal expansion coefficient-10(||c)
Thermo-optic coefficient (10-6 / K)25(⊥c)
Thermal conductivity (W/m/К)3.3(||c)
Specific heat (J/g·K) (at 25℃)0.842

Cr:LiSAF crystal optic properties:

ParametersDescription and values
Emission peak846 nm
Stimulated emission max. cross-section (×10-20 cm2 )4.8(||c)
Spontaneous fluorescence lifetime67 ms
Dispersion loss<0.2%/cm
dn/dT(×10-6/ ℃)-4.8(||c)

Sellmeyer’s equations (λ in um)



CrystalWavelength (nm)ncna
















Nd:KGW Crystals

About laser crystalsAbout laser crystals

Neodymium-doped potassium gadolinium tungstate (Nd:KGd(WO4)2 or Nd:KGW) crystals are suitable to be used as laser active medium due to its low lasing threshold and wide emission cross-section.   The effect of concentration quenching of fluorescence with neodymium ions (Nd3+) in KGW crystals can be weakened by a covalent W – O bond, therefore, this crystal has a higher concentration of active ions. Moreover, the Nd3+ absorption band at 808 nm in KGW crystals 12 nm wide (FWHM) matches well the emission wavelength of modern commercial laser diodes.


Nd:KGW: crystals main properties

Parameter sDescription and values
Crystal structureMonoclinous
Space groupC2h(2/c)-C 2/c
Unit cell parametersa=8.087Å; b=10.374 Å;c=7.588 Å
Refraction index at 1067 nmng = 2.049; np = 1.978;nm = 2.014
Mineral hardness5
Density (radiant emission)7.27 g/cm3
Meting temperature1075 ℃
Thermal conductivity at 373K,
W x cm-1 x K-1
K[100] = 0.026;K[010] = 0.038;K[001] = 0.034
Young’s  module, gPaE[100] = 115.8;E[010] = 152.5;E[001] = 92.4
Thermal expansion coefficients, at 373Kα[100] = 4 x 10-6 K-1; α[010] = 1.6 x 10-6 K-1; α[001] = 8.5 x 10-6 K-1
Laser wavelength911 nm, 1067 nm, 1351 nm
Absorption band808 nm (FWHM 12 nm)
Fluorescence lifetime110 ms (3% doping), 90 ms (8% doping)

Nd:KGW crystals properties:

3% Nd:KGWWavelength1070 nm
Emission bandwidth15 nm
Stimulated emission cross-section σ(x10-20 cm2)1.48
Fluorescence  lifetime (ms)109
Amplification bandwidth15 nm
Absorption wavelength810 nm
Absorption bandwidth14 nm
Absorption cross-section σα (x10-20 сm2)1.28

Nd:KGW crystals specific features

ParametersDescription and values
Standard concentration of doping elements (atoms%)3%,5%,8%
Max. length50 mm
Length tolerance, mm+1.0/-0.0
Diameter tolerance, mm+/-0.1
Surface quality20/10

Crystal transmittance curve  Nd:KGW

Crystal emission spectrum 3% Nd:KGWCrystal absorption spectrum 3% Nd:KGW




Yb:KGW Crystals

About laser crystalsAbout laser crystals

Ytterbium-doped potassium gadolinium tungstate (Yb:KGd(WO4)2 or Yb:KGW) crystals are suitable to be used as laser active medium and have distinct advantages over Nd3+ -doped KGW crystals. They are as follows: a wide emission spectrum in the range of 1023 – 1060 nm, the ability to generate short pulses (fs, ps), a wide absorption spectrum at 980 nm, аs well as a high pumping emission absorption coefficient that allows to effectively use the pumping radiation of laser diodes. As compared to YAG crystals, KGW crystals have a wider absorption cross-section, which reduces the required value of pumping intensity.

Yb:KGW crystals main features  

ParametersDescription and values
Crystal structureMonoclinic
Point groupC2/c
Unit cell parametersa = 8.09Å; b = 10.43Å; c = 7.588Å
Refraction index at 1067 nmng=2.033;np=2.037;nm=1.986
Mineralogical hardness5
Density7.27 г/см3
Melting temperature1075℃
Thermal conductivity at 373K, W/cm/КK[100] = 0.026; K[010] = 0.038; K[001] = 0.034
Thermal expansion coefficient at 373Kα[100] = 4 x 10-6 K-1; α[010] = 1.6 x 10-6 K-1;
α [001] = 8.5 x 10-6 K-1
Laser wavelength1023 – 1060 nm
Absorption band981 nm (FWHM: 3.7 nm)
Fluorescence lifetime600 ms (5% doping)
Doping elements  standard concentration (atoms%)5%
Max. length50 mm
Length tolerance, mm+1.0/-0.0
Diameter tolerance, mm+/-0.1
Surface quality20/10



Titanium-sapphire (Ti:Sapphire) Crystals

About laser crystalsAbout laser crystals

Titanium-doped sapphire (Ti:Sapphire) crystals are widely used to create tuneable coherent sources with ultra-shot pulses, high gain coefficient and power. Azimut Photonics company supplies titanium-sapphire crystals, grown by thermal gradient method. The crystals have big dimensions (30 x30 mm), high quality  (without diffusion), and density dislocation of less 102сm-2. Sapphire crystals grown by thermal gradient method are characterized with oriented growth (0001), high doping level (α490 = 4.0 cm-1), high gain coefficient and damage threshold.


– Tuneable wavelength in the range of 700 – 1000 nm makes Ti:Sapphire lasers a perfect alternative to dye lasers;

– Ti:Sapphire lasers can be used for UV generation of far UV band (up to 193 nm) with the pulse length up to 10 fs using non-linear crystals (e.g. BBO) to double frequency;

– Ti:Sapphire lasers are also widely used as pumping radiation sources for OPO (optical parametric oscillators) to increase the adjustment range.

Special features:

– Orientation: the optical axis С is perpendicular to the rod axis;

– Concentration of Ti2O3: 0.06 – 0.2 mass %;

– Quality index (FOM): 100~250 (>250 at request);

– α490: 1.0~4.0 cm-1;

– Diameter: 2~30 mm or as required;

– Optical path length: 2~30 mm or as required;

– Butt-end configuration: flat or Brewster angled;

– Flatness: <λ/10 at 633 nm;

– Parallelism: 10 angular seconds;

– Surface quality: :<40/20 scratch/dig (MIL-PRF-13830B);

– Wavefront distortion: <λ/4 per inch.

Notes: Anti-reflective coating at request.

Main properties of Ti:sapphire crystals

ParametersDescription and values
Chemical formulaTi3+:Al2O3
Crystal structureHexagonal
Lattice parametersa=4.758 Å,c=12.991 Å
Density3.98 g/cm3
Melting temperature2040 ℃
Mineral hardness9
Thermal conductivity52 W/m/К
Specific heat0.42 J/g/K
Laser functioning principle4-level scheme
Fluorescence lifetime3.2 ms (T=300 К)
Tuning range660 – 1050 nm
Absorption400 – 600 nm
Emission peak795 nm
Absorption peak488 nm
Refraction index1.76 at 800 nm
Max. cross-section3~4×10-19 сm2
Thermal expansion coefficient8.40×10-6/℃



Diffusion-Bonded Crystals

About laser crystals

Diffusion-bonded (diffusion-spliced) crystals consist of one laser crystal and one or two crystals without doping additives. The combination of crystals is carried out by the method of optical contact and further exposure to high temperature. Diffusion-bonded crystals help significantly reduce the lens effect that occurs when crystals are heated.

There are 3 type of diffusion-bonded crystals: YVO4+Nd:YVO4+YVO4, YAG+ Nd:YAG+YAG, Cr:YAG+Nd:YAG

Diffusion-bonded crystals

MaterialDoping elements concentrationAperture


Laser crystal length



The following crystals are available to order:

Diffuse-bonded crystals with different structure configuration are supplied by request.



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