| Catalog No. | CY2448 |
|---|---|
| Size | 10*10*0.5 mm or customized |
| Density | 8.1 g/cm3 |
| Orientation | <100>, <110>, <111> |
| Curie Temperature | 135-150°C |
PMN-PT crystal substrate is the core material of a new generation of nonlinear optical devices and photodetector devices. Stanford Advanced Materials (SAM) offers an industry-leading variety of scintillator crystal materials for radiation detection and nuclear identification.
PMN-PT crystal substrate has excellent piezoelectric properties, nonlinear optical properties, and pyroelectric properties. PMN-PT crystal substrate can meet the application needs and become the core material of a new generation of nonlinear optical devices and photodetector devices. PMN-PT single crystal also provides a good scientific Research vehicle.
|
Chemical Formula |
(PbMg0.33Nb0.67O3 )1-x:(PbTiO3)x |
|
Structure |
R3m, Rhombohedral |
|
Lattice |
a0 ~4.024Å(pseudo-cubic, varieswith composition ) |
|
Melting Point |
1280 oC |
|
Density |
8.1 g/cm3 |
|
Piezo-electric modulusd33 ： |
>2000 pC/N |
|
Kt(thickness mode)： |
59-62% |
|
K33’(beam mode)： |
84-88% |
|
Permittivity E(at 1kHz after poling)： |
4000 ~ 6000 |
|
Dielectric loss |
Tan d<0.9 |
|
Curie Temperature |
135-150°C |
|
Remanent Polarization |
20uC/cm2 |
PMN-PT crystal substrate can be used in:
– High-performance piezoelectric transducers
– None-linear optical devices
– Photodetector devices
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