Abstract:
A thermoelectric material having a high Seebeck coefficient and a large output factor and excellent in shock resistance, thermal strain resistance, and formability, and a thermoelectric element are disclosed. The thermoelectric material and thermoelectric element is composed of a multilayered body made up of a laminar body of a semimetal, a metal, or a synthetic resin and a laminar body of a semimetal. The average thickness of the laminar bodies ranges from 0.3 nm to 1000 nm. Examples of the combination of the laminar bodies are Bi-Al, Bi-polyamide resin, and Ag-Fe. Such a multilayered body is manufactured by forming an initial multilayered body composed of all the types of laminar bodies constituting the multilayered body and rolling or uniaxially pressing a stack of such initial multilayered bodies.
Abstract:
Disclosed is a magnetic material for a high frequency wave which has high magnetic permeability and small eddy-current loss, particularly a magnetic material for a high frequency wave which can be used suitably in an information device which works in a high frequency field of 1 GHz or higher. Specifically disclosed is a composite magnetic material for a high frequency wave, which comprises a (rare earth element)-(iron)-(nitrogen)-based magnetic material and a (rare earth element)-(iron)-(nitrogen)-based magnetic material whose surface is coated with a ferrite magnetic material.
Abstract:
A magnetic material represented by the formula R alpha Fe(100- alpha - beta - gamma - delta )N beta H gamma O delta wherein R is at least one rare earth element inclusive of Y; alpha is from 5 to 20 atomic percent, beta is from 5 to 25 atomic percent, gamma is from 0.01 to 5 atomic percent and delta is from 3 to 15 atomic percent. From this magnetic material, a bonded magnet can advantageously be obtained, while maintaining excellent magnetic properties of the magnetic material used for the production thereof.
Abstract:
A magnetic material represented by the formula R alpha Fe(100- alpha - beta - gamma - delta )N beta H gamma O delta wherein R is at least one rare earth element inclusive of Y; alpha is from 5 to 20 atomic percent, beta is from 5 to 25 atomic percent, gamma is from 0.01 to 5 atomic percent and delta is from 3 to 15 atomic percent. From this magnetic material, a bonded magnet can advantageously be obtained, while maintaining excellent magnetic properties of the magnetic material used for the production thereof.
Abstract:
A magnetic material represented by the formula R alpha Fe(100- alpha - beta - gamma - delta )N beta H gamma O delta wherein R is at least one rare earth element inclusive of Y; alpha is from 5 to 20 atomic percent, beta is from 5 to 25 atomic percent, gamma is from 0.01 to 5 atomic percent and delta is from 3 to 15 atomic percent. From this magnetic material, a bonded magnet can advantageously be obtained, while maintaining excellent magnetic properties of the magnetic material used for the production thereof.
Abstract:
A thermoelectric material having a high Seeback coefficient and a large power factor and excellent in shock resistance, thermal strain resistance, and formability, and a thermoelectric element are disclosed. The thermoelectric material and thermoelectric element is composed of a multilayered body made up of a laminar body of a semimetal, a metal, or a synthetic resin and a laminar body of a semimetal. The average thickness of the laminar bodies ranges from 0.3 nm to 1000 nm. Embodiments of the combination of the laminar bodies are Bi-Al. Bi-polyamide series resin, and Age-Fe. Such a multilayered body is manufactured by forming an initial multilayered body composed of all the types of laminar bodies constituting the multilayered body and rolling or uniaxially pressing a stack of such initial multilayered bodies.
Abstract:
A magnetic material represented by the formula R alpha Fe(100- alpha - beta - gamma - delta )N beta H gamma O delta wherein R is at least one rare earth element inclusive of Y; alpha is from 5 to 20 atomic percent, beta is from 5 to 25 atomic percent, gamma is from 0.01 to 5 atomic percent and delta is from 3 to 15 atomic percent. From this magnetic material, a bonded magnet can advantageously be obtained, while maintaining excellent magnetic properties of the magnetic material used for the production thereof.
Abstract:
PURPOSE:To enhance the magnetic characteristics and oxidation resistance by a method wherein R-Fe-M-N base material having a rhombohedral system or hexagonal system crystal structure is made to coexist with a material ele ment. CONSTITUTION:A magnetic material is expressed by Ralpha(Fe(1-gamma)Mgamma)(100-alpha-beta)NB, where R represents at least one kind of rare earth elements including Y, M represents at least one kind of elements out of Si, Ge, P, As, Sb, Be, alpha, beta satisfy the inequalities of 3