Magnetic crystal for electromagnetic wave absorbing material and electromagnetic wave absorber
First Claim
1. A magnetic crystal for use in an electromagnetic wave absorbing materials having absorbing capability in a high frequency band of 25 to 160 GHZ, the magnetic crystal having a structure of ε
- -MxFe2-xO3 with 0<
x<
1, and further having the same space group as that of an ε
-Fe2O3 crystal and in which M is substituted for a portion of the Fe sites of the ε
-Fe2O3 crystal;
wherein M is a trivalent element having an effect of lowering a coercive force Hc of the magnetic oxide comprising an ε
-Fe2O3 crystal when M is substituted for a portion of the Fe sites of the ε
-Fe2O3 crystal.
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Accused Products
Abstract
Disclosed is a magnetic crystal for electromagnetic wave absorbing materials, having a structure of ε-MxFe2-xO3 with 0<x<1, which has the same space group as that of an ε-Fe2O3 crystal and which is derived from an ε-Fe2O3 crystal by substituting a part of the Fe site therein with M. In this, M is a trivalent element having an effect of lowering the coercive force Hc of ε-Fe2O3 crystal by the substitution. Concretely, the element M includes Al and Ga. An electromagnetic wave absorber having a packed structure of particles having such a substituent element M-added “M-substituted ε-Fe2O3 crystal” as the magnetic phase may control the electromagnetic wave absorption peak frequency depending on the degree of substitution with the element M, and for example, the invention gives an electromagnetic wave absorber applicable to a 76 GHz band for on-vehicle radars.
18 Citations
12 Claims
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1. A magnetic crystal for use in an electromagnetic wave absorbing materials having absorbing capability in a high frequency band of 25 to 160 GHZ, the magnetic crystal having a structure of ε
- -MxFe2-xO3 with 0<
x<
1, and further having the same space group as that of an ε
-Fe2O3 crystal and in which M is substituted for a portion of the Fe sites of the ε
-Fe2O3 crystal;wherein M is a trivalent element having an effect of lowering a coercive force Hc of the magnetic oxide comprising an ε
-Fe2O3 crystal when M is substituted for a portion of the Fe sites of the ε
-Fe2O3 crystal. - View Dependent Claims (2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12)
- -MxFe2-xO3 with 0<
Specification