MICROWAVE MATERIALS

The properties of gyromagnetic materials come from the electron spin in a static magnetic field. The transformation is fast and the high-frequency loss is small. Therefore, it can be used in high-frequency microwave communications such as isolators, circulators and phase shifters. Because these materials contain magnetic ions, they have both dielectric properties and magnetic properties. This unique combination makes them a necessity for a wide variety of high frequency applications.





Instructions
HIMAG
Material
Characteristic
Garnet Materials
H-1800(NLW)  4πMs : 1750±5% Gs   ΔH : 55±20% Oe   εr : 15.2±10%)
H-1900(NLW)  4πMs : 1880±5% Gs   ΔH : 55±20% Oe   εr : 15.2±10%)
H-400-Gd  4πMs : 450±5% Gs   ΔH : 220±20% Oe   εr : 14.5±10%)
H-700-Gd  4πMs : 700±5% Gs   ΔH : 85±20% Oe   εr : 15.2±10%)
H-850-Gd  4πMs : 842±5% Gs   ΔH : 105±20% Oe   εr : 14.75±10%)
H-1500-Ho  4πMs : 1600±5% Gs   ΔH : 90±20% Oe   εr : 15.12±10%)
 Ho doping ,Improved loss performance

Spinel

 Materials

H-1600  4πMs : 1600±5% Gs   ΔH : 230±20% Oe   εr : 12.05±10%)
 Mg ferrite 

H-1800  4πMs : 1750±5% Gs   ΔH : 290±20% Oe   εr : 12.3±10%)
 Mg ferrite 

H-3000  4πMs : 3200±5% Gs   ΔH : 300±20% Oe   εr : 13.2±10%)
 Ni ferrite 

H-5000  4πMs : 4650±5% Gs   ΔH : 300±20% Oe   εr : 13.6±10%)
 Ni ferrite 
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