Lambda-ring
A pre--ring is a commutative ring R with identity element 1 and a set of mappings \lambda^n : R \rightarrow R, n = 0,1,2,\ldots such that
i) \lambda^0(x) = 1 for all x \in R;
ii) \lambda^1(x) = x for all x \in R;
iii) \lambda^n(x+y) = \sum_{i+j=n} \lambda^i(x) \lambda^j(y).
Examples are, for instance, the topological K-groups K(M) and K_G(M), G a compact Lie group (cf. K-theory), and the complex representation ring R(G) of a finite group G (cf. Representation of a compact group). In all these cases the \lambda^n are induced by taking exterior powers. For instance, for M = \text{pt}, K(M) = \mathbf{Z} and the \lambda-structure is given by \lambda^n(m) = \binom{m}{n} (binomial coefficients; the formula \binom{m_1+m_2}{n} = \sum_{i+j=n} \binom{m_1}{i} \binom{m_2}{j} follows by the binomial expansion theorem from (X+Y)^{m_1+m_2} = (X+Y)^{m_1} (X+Y)^{m_2}.
Let R be any commutative ring with unit element 1. Consider the set \Lambda(R) = 1 + t R[[t]] of power series in t over R with constant term 1. Multiplication of power series turns \Lambda(R) into an Abelian group. A pre-\lambda-ring structure on \Lambda(R) defines a homomorphism of Abelian groups \lambda_t : R \rightarrow \Lambda(R), \lambda_t(x) = \lambda^0(x) + \lambda^1(x) t + \lambda^2(x) t^2 + \cdots, and vice versa.
Let \alpha(t) = 1 + a_1 t + a_2 t^2 + \cdots, \beta(t) = 1 + b_1 t + b_2 t^2 + \cdots be two elements of \Lambda(R). Formally, write \alpha(t) = \prod_{i=1}^\infty \left({ 1 - \xi_i t }\right) \beta(t) = \prod_{i=1}^\infty \left({ 1 - \eta_i t }\right) and consider the expressions \prod_{i,j=1}^\infty \left({ 1 - \xi_i \eta_j t }\right) = 1 + P_1 t + P_2 t^2 + \cdots \ , \prod_{i_1 < i_2 < \cdots < i_n}^\infty \left({ 1 - \xi_{i_1} \xi_{i_2} \cdots \xi_{i_n} t }\right) = 1 + L_{1,n} t + L_{2,n} t^2 + \cdots \ .
The P_i and L_{i,n} are symmetric polynomial expressions in the \xi's and \eta's and hence can be written as universal polynomial expressions in the a's and b's. Now define a multiplication on \Lambda(R) by \alpha(t) * \beta(t) = 1 + P_1(a,b) t + P_2(a,b) t^2 + \cdots (a = (a_1,a_2,\ldots), b = (b_1,b_2,\ldots)), and define operations (mappings) \lambda^n : \Lambda(R) \rightarrow \Lambda(R) by \lambda^n \alpha(t) = 1 + L_{1,n}(a,b) t + L_{2,n}(a,b) t^2 + \cdots \ .
The ring \Lambda(R) with these operations is a pre-\lambda-ring. Given two pre-\lambda-rings R_1, R_2, a \lambda-ring homomorphism \phi : R_1 \rightarrow R_2 is a homomorphism of rings such that \phi(\lambda^n(x)) = \lambda^n(\phi(x)) for all x \in R_1, n = 0,1,2,\ldots.
A pre-\lambda-ring R is a \lambda-ring if \lambda_{-t} : R \rightarrow \Lambda(R), \lambda_{-t}(x) = 1 - \lambda^1(x) t + \lambda^2(x) t^2 - \cdots, is a homomorphism of pre-\lambda-rings. The ring \Lambda(R) is always a \lambda-ring and so are the standard examples K(M), K_G(M), R(G) of pre-\lambda-rings mentioned above.
On the other hand, consider a finite group G. A finite G-set is a finite set together with a group action of G. Using disjoint union and Cartesian products with diagonal action, the isomorphism classes of finite G-sets form a semi-ring, A^+(G). The associated Grothendieck ring A(G) is called the Burnside ring. On A^+(G), define operations \lambda^n : A^+(G) \rightarrow A^+(G) by taking \lambda^n(S) to be the set ofn-element subsets of S with the natural induced G-action. This generalizes the \lambda-operations \lambda^n on \mathbf{N} \subset \mathbf{Z}, \lambda^n(m) = \binom{m}{n}. Using iii), the \lambda^n extend to A(G), making the Burnside ring into a pre-\lambda-ring. As a rule this pre-\lambda-ring is not a \lambda-ring, [a9].
Instead of pre-\lambda-ring and \lambda-ring one also finds, respectively, the phrases \lambda-ring and special \lambda-ring in the literature.
Let R be a pre-\lambda-ring. One defines new operations \psi^i : R \rightarrow R by the formula -t \frac{d}{dt} \log \lambda_{-t} (x) = \sum_{i=1}^\infty \psi^i(x) t^i \ .
These operations are called the Adams operations on the pre-\lambda-ring R. They were introduced in the case R = K(M) by J.F. Adams ([a10]).
The Adams operations satisfy
iv) \Psi^1(x) = x;
v) \Psi^n(x+y) = \Psi^n(x) + \Psi^n(y).
Let R be a torsion-free pre-\lambda-ring; then R is a \lambda-ring if and only if the Adams operations satisfy in addition
vi) \Psi^i(1) = 1;
vii) \Psi^n(xy) = \Psi^n(x) \Psi^n(y);
viii) \Psi^{ij}(x) = \Psi^i(\Psi^j(x)).
A ring R with operations \Psi^i satisfying iv)–viii) is sometimes called a \Psi-ring.
The ring \Lambda(R) is isomorphic to the ring W(R) of (big) Witt vectors (cf. (the editorial comments to) Witt vector): \bar E : W(R) \rightarrow \Lambda(R) (a_1,a_2,\ldots) \mapsto \prod_{i=1}^\infty \left({ 1 - a_i t^i }\right)
Under this isomorphism the Adams operations \Psi^n on \Lambda(R) correspond to the Frobenius operations \mathbf{f}_n : W(R) \rightarrow W(R).
The \lambda-structures on the rings \Lambda(R) define a functorial morphism of ring-valued functors \lambda_{-t}(\cdot) : \Lambda(\cdot) \rightarrow \Lambda(\Lambda(\cdot)) . Together with \Lambda(R) \rightarrow R, 1 + a_1 t + a_2 t^2 + \cdots \mapsto a_1, this defines a co-triple structure on the functor \Lambda, and the \lambda-rings are precisely the co-algebras of this co-triple.
Via the isomorphism \bar E one finds "exponential homomorphisms" E : W(R) \rightarrow W(W(R)) E' : W(R) \rightarrow \Lambda(W(R)) which should be seen as (generalizing) the so-called Artin–Hasse exponential ([a11], [a12]).
Let w_n(R) : W(R) \rightarrow R be the ring homomorphism w_n (a_1,a_2,\ldots) = \sum_{d|n} d a_d^{n/d} \ . Then the Artin–Hasse exponential E(R) : W(R) \rightarrow W(W(R)) is functorially characterized by w_n(W(R)) \circ E(R) = \mathbf{f}_n(R) where \mathbf{f}_n is the Frobenius homomorphism.
Let V : \lambda\textsf{-Ring} \rightarrow \textsf{Ring} be the forgetful functor. Then the functor \Lambda : \textsf{Ring} \rightarrow \lambda\textsf{-Ring} is right adjoint (cf. Adjoint functor) to V: \textsf{Ring}(V(S),R) \equiv \lambda\textsf{-Ring}(S,\Lambda(R)) (cf. [a5], p. 20).
There are (besides the identity) three natural automorphisms of the Abelian group \Lambda(R) = 1 + t R[[t]], given by the substitution t \mapsto -t, the "inversion" \alpha(t) \mapsto \alpha(t)^{-1}, and the combination of the two. Correspondingly there are four natural ways to introduce a ring structure on \Lambda(R); the corresponding unit elements are 1-t, 1+t, (1-t)^{-1}, (1+t)^{-1}. All four occur in the literature. The most frequently occurring have 1-t or 1+t as their unit element — here, in the above, 1-t is the unit element —, and (1+t)^{-1} seems to be the most rare case.
\lambda-rings were introduced by A. Grothendieck in an algebraic-geometric setting [a2] and were first used in group representation theory by M.F. Atiyah and D.O. Tall ([a1]).
In case x \in R is one-dimensional, i.e. \lambda^n(x) = 0 for n \ge 2, the terminology derives from the case R = K(M) or R = R(G); one has \Psi^n(x) = x^n, whence the name power operations for the \Psi^n. On the \Lambda(R) the operations \Psi^n are directly defined by \Psi^n \left({ \prod_{i=1}^\infty (1 - \xi_i t) }\right) = \prod_{i=1}^\infty (1 - \xi_i^n t) \ .
References
[a1] | M.F. Atiyah, D.O. Tall, "Group representations, \lambda-rings and the J-homomorphism" Topology , 8 (1969) pp. 253–297 MR244387 |
[a2] | A. Grothendieck, "La théorie des classes de Chern" Bull. Soc. Math. France , 86 (1958) pp. 137–154 MR0116023 Zbl 0091.33201 |
[a3] | A. Grothendieck, "Classes de faisceaux et théorème de Riemann–Roch" , Sem. Géom. Algébrique , 6 , Springer (1972) pp. 20–77 Zbl 0229.14008 |
[a4] | M. Hazewinkel, "Formal groups and applications" , Acad. Press (1978) pp. 144ff MR0506881 MR0463184 Zbl 0454.14020 |
[a5] | D. Knutson, "\lambda-rings and the representation theory of the symmetric group" , Springer (1974) MR0364425 Zbl 0272.20008 |
[a6] | P. Berthelot, "Généralités sur les \lambda-anneaux" , Sem. Géom. Algébrique , 6 , Springer (1972) pp. 297–365 |
[a7] | W. Fulton, S. Lang, "Riemann–Roch algebra" , Springer (1985) MR0801033 Zbl 0579.14011 |
[a8] | T. tom Dieck, "Transformation groups and representation theory" , Springer (1979) Zbl 0445.57023 |
[a9] | C. Siebeneicher, "\lambda-Ringstrukturen auf dem Burnsidering der Permutationsdarstellungen einer endlichen Gruppe" Math. Z. , 146 (1976) pp. 223–238 MR0390035 Zbl 0306.20011 |
[a10] | J.F. Adams, "Vectorfields on spheres" Ann. of Math. , 75 (1962) pp. 603–632 DOI 10.2307/1970213 Zbl 0112.38102 |
[a11] | M. Hazewinkel, "Twisted Lubin–Tate formal group laws, ramified Witt vectors and (ramified) Artin–Hasse exponentials" Trans. Amer. Math. Soc. , 259 (1980) pp. 47–63 MR0561822 Zbl 0437.13014 |
[a12] | E. Artin, H. Hasse, "Die beide Ergänzungssätze zum Reciprozitätsgesetz der \ell^n-ten Potenzreste im Körper der \ell^n-ten Einheitswurzeln" Abh. Math. Sem. Univ. Hamburg , 6 (1928) pp. 146–162 |
[a13] | G. Whaples, "Generalized local class field theory III: Second form of the existence theorem, structure of analytic groups" Duke Math. J. , 21 (1954) pp. 575–581 MR73645 |
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