The Poetical Works of John Milton, 1권T. Noble, 1845 |
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66 페이지
... field theory should be thought of as taking place on Lorentz manifolds . We allow field theories on Riemannian mani- folds and also on manifolds with less rigid structure . A field theory based on Riemannian manifolds is called a Euclidean ...
... field theory should be thought of as taking place on Lorentz manifolds . We allow field theories on Riemannian mani- folds and also on manifolds with less rigid structure . A field theory based on Riemannian manifolds is called a Euclidean ...
69 페이지
... field and 24 with the magnetic field . This identification is different from the usual one ( in Maxwell's theory , is identified with the electric field and pq ( P , q = 1 , 2 , 3 ) with the mag- netic field ) . We shall see however ...
... field and 24 with the magnetic field . This identification is different from the usual one ( in Maxwell's theory , is identified with the electric field and pq ( P , q = 1 , 2 , 3 ) with the mag- netic field ) . We shall see however ...
82 페이지
... field B can be replaced by non - interacting composite fermions in effective field B * . The essence of this theory may be described in simple words . a ) However large may be the ratio of Landau spacing to the Coulomb energy , we do ...
... field B can be replaced by non - interacting composite fermions in effective field B * . The essence of this theory may be described in simple words . a ) However large may be the ratio of Landau spacing to the Coulomb energy , we do ...
101 페이지
... field analysis through examination of what he describes as the relative autonomy of the field. To recap, according to Bourdieu, any field is structured between poles he defines as autonomous and heteronomous (figure 1.5). At the ...
... field analysis through examination of what he describes as the relative autonomy of the field. To recap, according to Bourdieu, any field is structured between poles he defines as autonomous and heteronomous (figure 1.5). At the ...
138 페이지
... fields ✈ ( 8.15 ) and the electromagnetic field A in ( 8.13 ) is called a " local gauge transformation " . QED is thus a locally gauge invariant theory . Its " gauge field " is the electromagnetic field Au ; its field quanta , the so ...
... fields ✈ ( 8.15 ) and the electromagnetic field A in ( 8.13 ) is called a " local gauge transformation " . QED is thus a locally gauge invariant theory . Its " gauge field " is the electromagnetic field Au ; its field quanta , the so ...
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