- Source: Highly structured ring spectrum
In mathematics, a highly structured ring spectrum or
A
∞
{\displaystyle A_{\infty }}
-ring is an object in homotopy theory encoding a refinement of a multiplicative structure on a cohomology theory. A commutative version of an
A
∞
{\displaystyle A_{\infty }}
-ring is called an
E
∞
{\displaystyle E_{\infty }}
-ring. While originally motivated by questions of geometric topology and bundle theory, they are today most often used in stable homotopy theory.
Background
Highly structured ring spectra have better formal properties than multiplicative cohomology theories – a point utilized, for example, in the construction of topological modular forms, and which has allowed also new constructions of more classical objects such as Morava K-theory. Beside their formal properties,
E
∞
{\displaystyle E_{\infty }}
-structures are also important in calculations, since they allow for operations in the underlying cohomology theory, analogous to (and generalizing) the well-known Steenrod operations in ordinary cohomology. As not every cohomology theory allows such operations, not every multiplicative structure may be refined to an
E
∞
{\displaystyle E_{\infty }}
-structure and even in cases where this is possible, it may be a formidable task to prove that.
The rough idea of highly structured ring spectra is the following: If multiplication in a cohomology theory (analogous to the multiplication in singular cohomology, inducing the cup product) fulfills associativity (and commutativity) only up to homotopy, this is too lax for many constructions (e.g. for limits and colimits in the sense of category theory). On the other hand, requiring strict associativity (or commutativity) in a naive way is too restrictive for many of the wanted examples. A basic idea is that the relations need only hold up to homotopy, but these homotopies should fulfill again some homotopy relations, whose homotopies again fulfill some further homotopy conditions; and so on. The classical approach organizes this structure via operads, while the recent approach of Jacob Lurie deals with it using
∞
{\displaystyle \infty }
-operads in
∞
{\displaystyle \infty }
-categories. The most widely used approaches today employ the language of model categories.
All these approaches depend on building carefully an underlying category of spectra.
Approaches for the definition
= Operads
=The theory of operads is motivated by the study of loop spaces. A loop space ΩX has a multiplication
Ω
X
×
Ω
X
→
Ω
X
{\displaystyle \Omega X\times \Omega X\to \Omega X}
by composition of loops. Here the two loops are sped up by a factor of 2 and the first takes the interval [0,1/2] and the second [1/2,1]. This product is not associative since the scalings are not compatible, but it is associative up to homotopy and the homotopies are coherent up to higher homotopies and so on. This situation can be made precise by saying that ΩX is an algebra over the little interval operad. This is an example of an
A
∞
{\displaystyle A_{\infty }}
-operad, i.e. an operad of topological spaces which is homotopy equivalent to the associative operad but which has appropriate "freeness" to allow things only to hold up to homotopy (succinctly: any cofibrant replacement of the associative operad). An
A
∞
{\displaystyle A_{\infty }}
-ring spectrum can now be imagined as an algebra over an
A
∞
{\displaystyle A_{\infty }}
-operad in a suitable category of spectra and suitable compatibility conditions (see May, 1977).
For the definition of
E
∞
{\displaystyle E_{\infty }}
-ring spectra essentially the same approach works, where one replaces the
A
∞
{\displaystyle A_{\infty }}
-operad by an
E
∞
{\displaystyle E_{\infty }}
-operad, i.e. an operad of contractible topological spaces with analogous "freeness" conditions. An example of such an operad can be again motivated by the study of loop spaces. The product of the double loop space
Ω
2
X
{\displaystyle \Omega ^{2}X}
is already commutative up to homotopy, but this homotopy fulfills no higher conditions. To get full coherence of higher homotopies one must assume that the space is (equivalent to) an n-fold loopspace for all n. This leads to the in
∞
{\displaystyle \infty }
-cube operad of infinite-dimensional cubes in infinite-dimensional space, which is an example of an
E
∞
{\displaystyle E_{\infty }}
-operad.
The above approach was pioneered by J. Peter May. Together with Elmendorf, Kriz and Mandell he developed in the 90s a variant of his older definition of spectra, so called S-modules (see Elmendorf et al., 2007). S-modules possess a model structure, whose homotopy category is the stable homotopy category. In S-modules the category of modules over an
A
∞
{\displaystyle A_{\infty }}
-operad and the category of monoids are Quillen equivalent and likewise the category of modules over an
E
∞
{\displaystyle E_{\infty }}
-operad and the category of commutative monoids. Therefore, is it possible to define
A
∞
{\displaystyle A_{\infty }}
-ring spectra and
E
∞
{\displaystyle E_{\infty }}
-ring spectra as (commutative) monoids in the category of S-modules, so called (commutative) S-algebras. Since (commutative) monoids are easier to deal with than algebras over complicated operads, this new approach is for many purposes more convenient. It should, however, be noted that the actual construction of the category of S-modules is technically quite complicated.
= Diagram spectra
=Another approach to the goal of seeing highly structured ring spectra as monoids in a suitable category of spectra are categories of diagram spectra. Probably the most famous one of these is the category of symmetric spectra, pioneered by Jeff Smith. Its basic idea is the following:
In the most naive sense, a spectrum is a sequence of (pointed) spaces
(
X
0
,
X
1
,
…
)
{\displaystyle (X_{0},X_{1},\dots )}
together with maps
Σ
X
i
→
X
i
+
1
{\displaystyle \Sigma X_{i}\to X_{i+1}}
, where ΣX denotes the suspension. Another viewpoint is the following: one considers the category of sequences of spaces together with the monoidal structure given by a smash product. Then the sphere sequence
(
S
0
,
S
1
,
…
)
{\displaystyle (S^{0},S^{1},\dots )}
has the structure of a monoid and spectra are just modules over this monoid. If this monoid was commutative, then a monoidal structure on the category of modules over it would arise (as in algebra the modules over a commutative ring have a tensor product). But the monoid structure of the sphere sequence is not commutative due to different orderings of the coordinates.
The idea is now that one can build the coordinate changes into the definition of a sequence: a symmetric sequence is a sequence of spaces
(
X
0
,
X
1
,
…
)
{\displaystyle (X_{0},X_{1},\dots )}
together with an action of the n-th symmetric group on
X
n
{\displaystyle X_{n}}
. If one equips this with a suitable monoidal product, one gets that the sphere sequence is a commutative monoid. Now symmetric spectra are modules over the sphere sequence, i.e. a sequence of spaces
(
X
0
,
X
1
,
…
)
{\displaystyle (X_{0},X_{1},\dots )}
together with an action of the n-th symmetric group on
X
n
{\displaystyle X_{n}}
and maps
Σ
X
i
→
X
i
+
1
{\displaystyle \Sigma X_{i}\to X_{i+1}}
satisfying suitable equivariance conditions. The category of symmetric spectra has a monoidal product denoted by
∧
{\displaystyle \wedge }
. A highly structured (commutative) ring spectrum is now defined to be a (commutative) monoid in symmetric spectra, called a (commutative) symmetric ring spectrum. This boils down to giving maps
X
n
∧
X
m
→
X
n
+
m
,
{\displaystyle X_{n}\wedge X_{m}\to X_{n+m},}
which satisfy suitable equivariance, unitality and associativity (and commutativity) conditions (see Schwede 2007).
There are several model structures on symmetric spectra, which have as homotopy the stable homotopy category. Also here it is true that the category of modules over an
A
∞
{\displaystyle A_{\infty }}
-operad and the category of monoids are Quillen equivalent and likewise the category of modules over an
E
∞
{\displaystyle E_{\infty }}
-operad and the category of commutative monoids.
A variant of symmetric spectra are orthogonal spectra, where one substitutes the symmetric group by the orthogonal group (see Mandell et al., 2001). They have the advantage that the naively defined homotopy groups coincide with those in the stable homotopy category, which is not the case for symmetric spectra. (I.e., the sphere spectrum is now cofibrant.) On the other hand, symmetric spectra have the advantage that they can also be defined for simplicial sets. Symmetric and orthogonal spectra are arguably the simplest ways to construct a sensible symmetric monoidal category of spectra.
= Infinity-categories
=Infinity-categories are a variant of classical categories where composition of morphisms is not uniquely defined, but only up to contractible choice. In general, it does not make sense to say that a diagram commutes strictly in an infinity-category, but only that it commutes up to coherent homotopy. One can define an infinity-category of spectra (as done by Lurie). One can also define infinity-versions of (commutative) monoids and then define
A
∞
{\displaystyle A_{\infty }}
-ring spectra as monoids in spectra and
E
∞
{\displaystyle E_{\infty }}
-ring spectra as commutative monoids in spectra. This is worked out in Lurie's book Higher Algebra.
= Comparison
=The categories of S-modules, symmetric and orthogonal spectra and their categories of (commutative) monoids admit comparisons via Quillen equivalences due to work of several mathematicians (including Schwede). In spite of this the model category of S-modules and the model category of symmetric spectra have quite different behaviour: in S-modules every object is fibrant (which is not true in symmetric spectra), while in symmetric spectra the sphere spectrum is cofibrant (which is not true in S-modules). By a theorem of Lewis, it is not possible to construct one category of spectra, which has all desired properties. A comparison of the infinity category approach to spectra with the more classical model category approach of symmetric spectra can be found in Lurie's Higher Algebra 4.4.4.9.
Examples
It is easiest to write down concrete examples of
E
∞
{\displaystyle E_{\infty }}
-ring spectra in symmetric/orthogonal spectra. The most fundamental example is the sphere spectrum with the (canonical) multiplication map
S
n
∧
S
m
→
S
n
+
m
{\displaystyle S^{n}\wedge S^{m}\to S^{n+m}}
. It is also not hard to write down multiplication maps for Eilenberg-MacLane spectra (representing ordinary cohomology) and certain Thom spectra (representing bordism theories). Topological (real or complex) K-theory is also an example, but harder to obtain: in symmetric spectra one uses a C*-algebra interpretation of K-theory, in the operad approach one uses a machine of multiplicative infinite loop space theory.
A more recent approach for finding
E
∞
{\displaystyle E_{\infty }}
-refinements of multiplicative cohomology theories is Goerss–Hopkins obstruction theory. It succeeded in finding
E
∞
{\displaystyle E_{\infty }}
-ring structures on Lubin–Tate spectra and on elliptic spectra. By a similar (but older) method, it could also be shown that Morava K-theory and also other variants of Brown-Peterson cohomology possess an
A
∞
{\displaystyle A_{\infty }}
-ring structure (see e.g. Baker and Jeanneret, 2002). Basterra and Mandell have shown that Brown–Peterson cohomology has even an
E
4
{\displaystyle E_{4}}
-ring structure, where an
E
4
{\displaystyle E_{4}}
-structure is defined by replacing the operad of infinite-dimensional cubes in infinite-dimensional space by 4-dimensional cubes in 4-dimensional space in the definition of
E
∞
{\displaystyle E_{\infty }}
-ring spectra. On the other hand, Tyler Lawson has shown that Brown–Peterson cohomology does not have an
E
∞
{\displaystyle E_{\infty }}
structure.
Constructions
Highly structured ring spectra allow many constructions.
They form a model category, and therefore (homotopy) limits and colimits exist.
Modules over a highly structured ring spectrum form a stable model category. In particular, their homotopy category is triangulated. If the ring spectrum has an
E
2
{\displaystyle E_{2}}
-structure, the category of modules has a monoidal smash product; if it is at least
E
4
{\displaystyle E_{4}}
, then it has a symmetric monoidal (smash) product.
One can form group ring spectra.
One can define the algebraic K-theory, topological Hochschild homology, and so on, of a highly structured ring spectrum.
One can define the space of units, which is crucial for some questions of orientability of bundles.
See also
Commutative ring spectrum
En-ring
References
= References on E∞-ring spectra
=Elmendorf, A.D.; Kriz, I.; Mandell, M.A.; May, J.P. (2007). Rings, modules, and algebras in stable homotopy theory. AMS. ISBN 978-0-8218-4303-1.
May, J. Peter (1977).
E
∞
{\displaystyle E_{\infty }}
-ring spaces and
E
∞
{\displaystyle E_{\infty }}
-ring spectra. Springer.
May, J. Peter (2009). "What precisely are
E
∞
{\displaystyle E_{\infty }}
ring spaces and
E
∞
{\displaystyle E_{\infty }}
ring spectra?". Geometry & Topology Monographs. 16: 215–282. arXiv:0903.2813. doi:10.2140/gtm.2009.16.215.
= References about structure of E∞-ring spectra
=Basterra, M.; Mandell, M.A. (2005). "Homology and Cohomology of E-infinity Ring Spectra" (PDF)
Lawson, T. (2017). "Calculating obstruction groups for
E
∞
{\displaystyle E_{\infty }}
-ring spectra". arXiv:1709.09629 [math.AT].
= References about specific examples
=Baker, A.; Jeanneret, A. (2002). "Brave new Hopf algebroids and extensions of MU-algebras". Homology, Homotopy and Applications. 4 (1): 163–173. doi:10.4310/HHA.2002.v4.n1.a9.
Basterra, M.; Mandell, M.A. (June 2013). "The multiplication on BP" (PDF). Journal of Topology. 6 (2): 285–310. arXiv:1101.0023. doi:10.1112/jtopol/jts032. S2CID 119652118. Archived from the original (PDF) on 2015-02-06.
= General references on related spectra
=Lurie, J. "Higher Algebra" (PDF). Archived from the original (PDF) on 2015-02-06.
Mandell, M.A.; May, J.P.; Schwede, S.; Shipley, B. (2001). "Model Categories of Diagram Spectra" (PDF). Proc. London Math. Soc. 82 (2): 441–512. doi:10.1112/S0024611501012692. S2CID 551246.
Richter, B. (2017). "Commutative ring spectra". arXiv:1710.02328 [math.AT].
Schwede, S. (2001). "S-modules and symmetric spectra" (PDF). Math. Ann. 319 (3): 517–532. doi:10.1007/PL00004446. S2CID 6866612.
Schwede S. Schwede, S. (2007). "An untitled book project about symmetric spectra" (PDF).