|  Group Theory | 
In General
  > s.a. types of groups [including generalizations].
  * History:
    The theory was invented by Galois in the early XIX century.
  $ Def: A group is a
    pair (G, \(\circ\)), with G a set and \(\circ\) an
    operation \(\circ\) : G × G → G,
    which is associative, has a neutral element, and such that each element
    has an inverse; I.e., a group is a monoid with inverse.
  * Specifying a group:
    For finite groups, one can give the full multiplication table;
    In general, one gives a list of elements and a composition law in some
    representation, or a group presentation; The fundamental problem of group
    theory is the isomorphism problem, that of deciding whether
    any two finite presentations correspond to isomorphic groups; It was
    proved unsolvable in the late 1950s;
    > s.a. Combinatorial Group Theory;
    Group Presentation; Isomorphism;
    representations.
  * Main branches:
    Abstract group theory; representation theory.
  @ II: Falicov 66;
    Leech & Newman 69;
    Armstrong 88;
    Moody 94;
    Mirman 95 [II/III];
    Snaith 03 [and rings, etc];
    Ronan 06 [esp Monster group];
    Reis 11.
  @ III: Weyl 46;
    Kurosh 55;
    Hall 59;
    Hamermesh 62;
    Scott 64;
    Rotman 65;
    Suzuki 82;
    Zassenhaus 99;
    Roman 12;
    Machì 12 [many exercises].
  @ Geometric group theory:
    de la Harpe 00;
    Chiswell in Bullett et al 17.
  @ Books, special emphasis:
    Babakhanian 72 [cohomological methods];
    Asche 89 [with software];
    Geoghegan 08 [topological methods];
    Steeb et al 12 [problems and solutions].
  @ Related topics: Stillwell BAMS(82) [isomorphism problem].
  > Applications: see algebraic topology;
    ordinary and partial differential equations;
    Group Theory in Physics below.
  > Online resources:
    see Wikipedia page.
Related Concepts and Structure
  > s.a. Center; Coset; group
  action on a set; lie group [metric]; measure;
  Rank; Word.
  * Conjugate elements: Two elements
    g1, g2
    in G (two subgroups H1,
    H2 of G) are conjugate if there exists
    a g in G such that g1 = g
    g2 g−1
    (H1 = g H2
    g−1); This is an equivalence relation.
  * Conjugacy Classes:
  * Subgroups: Only if N
    is a normal subgroup is G/N a group; The order of a subgroup
    must be a divisor of the order of the group (think about cosets).
  * Sylvester graph of a group:
    > see, e.g., matter.
  @ References: Balantekin AIP(10)-a1011 [character expansions of products of invariant functions on G].
Operations on Groups > s.a. lie
  algebras [group contractions]; Semidirect Product.
  * Extension of a group A by a
    group C: A new group B ⊃ A with B/A
    = C; Expressed by the exact sequence
0 → A → B → C → 0 .
* Free product:
Subgroups > s.a. group actions [stabilizer];
  Little Group; Torsion Subgroup.
  * Normal: (H \(\triangleleft\) G)
    An H such that for all g in G,
    g−1Hg = H;
    Alternatively, H is the kernel of some homomorphism.
  * Normalizer of a subset S:
    The subgroup of G defined by NG(S):=
    {g ∈ G | g−1Sg = S}
    ≡ {g ∈ G | Sg = gS}, i.e., the biggest subgroup of G
    in which S is normal; If S is a subgroup, S \(\triangleleft\) N(S),
    and S \(\triangleleft\) G is equivalent to N(S) = G;
    Special cases: If S = {s}, one element, N(S)
    = C(S), but in general C(S) ⊂ N(S).
  * Commutant: The normal subgroup Q
    of elements of the form q = q1
    q2 ... qm,
    where qi
    = gg'g−1g'−1;
    Remark: The quotient group G/Q is Abelian.
  * Centralizer of a subset
    S: The subgroup of G defined by
CG(S):= {g ∈ G | g−1sg = s , ∀s ∈ S} ≡ {g ∈ G | gs = sg , ∀g ∈ S} .
And Physics > s.a. gauge theory; general
  relativity; lie groups; quantum theory
  and canonical approach; symmetries.
  * Idea: It is a very effective way
    of formulating and exploiting the symmetries of a system; The knowledge of a symmetry
    group gives the level scheme, branching ratios and selection rules; Symmetries are
    usually broken, but the approximation is still useful.
  * History: Symmetry in physics was
    introduced with special relativity and the Lorentz group; Noether's theorem; 1932,
    Heisenberg joins p and n into an SU(2) doublet and postulates an
    SU(2)-invariant Lagrangian; 1954, local symmetries introduced with Yang-Mills theory.
  @ Books and overviews: Kahan 65;
    Wybourne 74;
    Balachandran & Trahern 84;
    Cornwell 84;
    Tung 85 (and
    Aivazis 91);
    Isham 89;
    Sternberg 91;
    Fässler & Stifel 92;
    Ludwig & Falter 96;
    Teodorescu & Nicorovici 04;
    Ma & Gu 04 [problems and solutions];
    Bonolis RNC(04) [history];
    Dresselhaus et al 08 [in condensed matter, r PT(08)nov];
    Ramond 10;
    Balachandran et al 10 [and Hopf algebras];
    Jeevanjee 11 [r PT(12)apr];
    Belhaj a1205-ln;
    Coddens 15 [spin and quantum mechanics];
    Zee 16 [in a nutshell];
    Martin-Dussaud GRG(19)-a1902 [lqg and spin foams];
    Ma 19;
    Wilson a2009 [group-theorist's perspective].
  @ For particle physics: 
    Barnes 10 [standard model];
    Haywood 10 [symmetries and conservation laws];
    Costa & Fogli 12;
    Saleem & Rafique 12.
  @ And dynamics:
    Aldaya & Azcárraga FdP(87).
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