Groups generated by two operators $(s\sb 1,s\sb 2)$ satisfying the equation $s\sb 1s\sp 2\sb 2=s\sb 2s\sp 2\sb 1$
نویسندگان
چکیده
منابع مشابه
Chapter 1 More SSB , then Higgs
This lagrangian is, of course, invariant under SO(N), rotations of φ in the N dimensional internal space. φj(x) → Ojkφk(x), with O an orthogonal matrix, which leaves ∑ φ invariant. Notice that the mass term has the wrong sign. Had that sign been minus, with a + in the potential energy, the potential’s absolute minimum would have been at ~ φ = 0, the classical vacuum would be at ~ φ = 0, and the...
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متن کاملChapter 16 More SSB , then
This lagrangian is, of course, invariant under SO(N), rotations of φ in the N dimensional internal space. φj(x) → Ojkφk(x), with O an orthogonal matrix, which leaves ∑ φ invariant. Notice that the mass term has the wrong sign. Had that sign been minus, with a + in the potential energy, the potential’s absolute minimum would have been at ~ φ = 0, the classical vacuum would be at ~ φ = 0, and the...
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ژورنال
عنوان ژورنال: Transactions of the American Mathematical Society
سال: 1910
ISSN: 0002-9947
DOI: 10.1090/s0002-9947-1910-1500867-7