N31 Nd: Glass
N31 Nd:Glass case (1)
Size: φ10×100 mm;
Both apertures: Flat, laser quality polished (lambda/10), AR@1053nm(R<0.3%/surface);
AR coating LIDT: Durable at 30J, 0.5ms pulse, multimode, 0.02Hz(1PPM) repetition, 1053nm
N31 Nd:Glass case (2)
Size: φ7×148 mm;
Doping: 1 wt.%;
Coating: AR/AR R<0.25% @ 1053 nm, 0°, damage > 7 J/cm2 for 1 ns
N31 Nd:Glass case (3)
Size: φ25×256 mm;
Doping: 1.0 wt.%;
Coating: AR/AR R<0.25% @ 1053 nm, 0°, damage > 7 J/cm2 for 1 ns @ 1053 nm
N31 Nd:Glass case (4)
Size: φ50×267 mm;
Doping: 0.5 (±0.03) wt.%
Coating: AR/AR R<0.25% @ 1053 nm, 0°, damage > 7 J/cm2 for 1 ns @1053 nm
N31 phosphate glass is specially developed for high power laser facility. N31 is a good material which has the characteristics of high energy storage, large excitation cross section and long fluorescence lifetime. It is also easy to prepare glass with large size and good optical uniformity, so it is widely used in high-power laser systems. At present, it has been successfully applied in Shen Guang Ⅱ and Shen Guang Ⅲ systems.
- High energy storage
- Large excitation cross section
- Long fluorescence lifetime
- Low coefficient of nonlinearity
- High damage threshold
- High-power laser systems
Mainly used for inertial confinement fusion physics experimental research，can provide nearly 200,000 joules, 60TW ultraviolet radiation source
- Ultrashort pulse laser
Used for nonlinear laser microscopies， practical, fiber-based, high-power, wideband sources and practical optical frequency comb system
- Waveguide amplifier
Used for femtosecond laser writing method, optical communication
N31 Nd:Glass
Size: Φ10×178 mm
N31 Nd:Glass
Size: Φ25×254 mm
N31 Nd:Glass
Size: Φ50×254 mm
Want to get more information about what kind of Nd Glass crylink have supplied?
Parameter
| Nd2O3 (wt%) | 3.5 |
| Nd3+ conc.(1020ions/cm3) | 3.4±0.1 |
| Cross section for stimulated emission(10-20cm2) | 3.8±0.1 |
| Lifetime at 1053nm(μsec) | ≥370 (Nd2O3:0.5wt%) |
| ≥360 (Nd2O3:1.2wt%) | |
| ≥315 (Nd2O3:3.5wt%) | |
| ≥310 (Nd2O3:4.2wt%) | |
| Effective bandwidth(nm) | 25.4 |
| Fluorescence peak wavelength(nm) | 1053 |
| Absorption coefficient(cm-1) | ≤0.0015(1053nm) |
| ≤0.25(400nm) | |
| ≤1.5(3333nm) |
| Non-linear refractive index coeff.n2(×10-13e.s.u) | ≤1.2 |
| Refracive index(1053nm) | 1.535±0.003 |
| Abbe value | 65.6 |
| dn/dt(10-6/℃)(20~100℃） | -4.3 |
| Transformation temp.(℃） | 445 |
| Softening temp.(℃） | 485 |
| Coeff.of linear thermal expansion (10-7/K)(30~100℃） | 116 |
| Thermal coeff. Of optical path length(10-6/K)(50~100℃） | 1.4 |
| Thermal comductive (25℃)(W/Mk) | 0.59 |
| Specific heat(25℃)(J/Gk) | 0.75 |
| Density(g/cm3) | 2.87 |
| Young’s modulus(Gpa) | 58.3 |
| Posson’ rayio | 0.26 |
| Knoop hardness(kg/cm2) | 404 |
| Fracture toughness(Mpa.m1/2) | 0.58 |
*The homogeneeity is about 2×10-6
