I want to explain a particularly easy example of a motivic cellular decomposition: That of nn-dimensional projective space. We will have a look at the cohomology, the Chow groups and the algebraic K-theory of projective space -- a discussion probably interesting to non-motivic people as well. After these invariants, I will look at the motive and the A¹-homotopy type. Then I want to describe the decomposition of the motive (and the homotopy type) homotopy-theoretically, by means of cofiber sequences. (We will see that projective space is not isomorphic to a coproduct of motivic spheres with the same motive). Of course, nothing is new, I'm just working out exercises here.

In this part 1, I discuss only the cohomology of Pn\mathbb{P}^n. Part 2 contains a discussion of the intersection theory and bundles and part 3 contains the motivic stuff. I intentionally left out usage of projective bundle formulas, as I will discuss them separately.

CW structure on the associated analytic space

We can compute the Betti cohomology, i.e. the singular cohomology of the associated analytic space, by showing that the manifold CPn:=(Pn(C))an\mathbb{CP}^n := (\mathbb{P}^n(\mathbb{C}))^{an} admits a CW-structure and computing the cellular cohomology (which also satisfies the Eilenberg-Mac Lane axioms, hence is isomorphic).
For n=0n=0 this is easy, as CP0\mathbb{CP}^0 is just a single point. Suppose now we already have a CW-structure on CPn\mathbb{CP}^n, then we will construct CPn+1\mathbb{CP}^{n+1} by attaching one 2n+22n+2-cell Cn+1\mathbb{C}^{n+1} by the gluing map η:Cn+1{0}CPn\eta : \mathbb{C}^{n+1} \setminus \{0\} \to \mathbb{CP}^n given by quotienting out the C×\mathbb{C}^\times-action, i.e. I claim CPn+1CPnηCn+1\mathbb{CP}^{n+1} \simeq \mathbb{CP}^{n} \cup_{\eta} \mathbb{C}^{n+1}. The map η\eta is known under the name "Hopf map", and it is a surjective map.
The CW structure of CPn\mathbb{CP}^n, as we have just seen, is such that there is a single 2k2k-dimensional cell for each k=0,,nk = 0,\dots,n. The chain complex computing cellular cohomology thus has no differentials, so we can quickly see that
!Hcelli(CPn,Z)={Z, for i=2k,kn0else.! H^i_{cell}(\mathbb{CP}^n,\mathbb{Z}) = \begin{cases} \mathbb{Z}, & \text{ for } i=2k, k\leq n\\ 0 & \text{else.} \end{cases}

Smooth de Rham theory and ring structure

We can also look at the deRham cohomology of CPn\mathbb{CP}^n as a smooth 2n2n-dimensional real manifold. The advantage is that we would see the cup product structure (coming from the wedge of differential forms). From what we already know, there should be a closed smooth differential 2k2k-form ωk\omega_k which isn't exact for each k=0,,nk = 0,\dots,n. We know that ωn\omega_n will be a volume form and similarly ωk\omega_k can be chosen to be a volume form of CPk\mathbb{CP}^k when restricted to that subspace. Then we have ωkωj\omega_k \wedge \omega_j homologous to ωk+j\omega_{k+j} for k+jnk+j \leq n, so that the multiplicative structure in the cohomology can be described as [ωk]=[ω1]k[\omega_k] = [\omega_1]^k and by writing x=[ωk]x = [\omega_k] (of degree 22) we have the identity of graded rings
!HdR(CPn,R)=R[x]/(xn+1).! H^\bullet_{dR}(\mathbb{CP}^n,\mathbb{R}) = \mathbb{R}[x]/(x^{n+1}).

Some people like to describe the cohomology of projective space by choosing an arbitrary hyperplane HCPnH \subset \mathbb{CP}^n (so the complement is isomorphic to CPn1\mathbb{CP}^{n-1}) and then Hsing(CPn,Z)=Z[H]/(Hn+1),H^\bullet_{sing}(\mathbb{CP}^n,\mathbb{Z}) = \mathbb{Z}[H]/(H^{n+1}), with HH in degree 22. This description arises from the Poincaré duality map taking singular kk-cycles in CPn\mathbb{CP}^n to singular 2nk2n-k-cocycles, which takes any complex hyperplane HCPnH \subset \mathbb{CP}^n to the same cohomology class of degree 22 (since the real codimension of a complex hyperplane is 22).

Cup product with integer coefficients

Of course, it is unsatisfying to have the multiplicative structure only with real coefficients, so we can work a little bit more (or differently) and compute the cup product via Yoneda products in sheaf cohomology of the constant sheaf Z\underline{\mathbb{Z}}. I'm too lazy now, but in the end you get
!HBetti(Pn,Z)=H(CPn,ZCPn)=Z[x]/(xn+1).! H^\bullet_{Betti}(\mathbb{P}^n,\mathbb{Z}) = \mathbb{H}^\bullet(\mathbb{CP}^n, \underline{\mathbb{Z}}_{\mathbb{CP}^n}) = \mathbb{Z}[x]/(x^{n+1}).

Yet another way to get the cup product is the most "canonical" way with cellular cohomology (in my eyes), where we use only the diagonal morphism and the Künneth formula. I'm going to do that:
The diagonal PnPn×Pn\mathbb{P}^n \to \mathbb{P}^n \times \mathbb{P}^n induces a homomorphism Hcell(Pn×Pn)Hcell(Pn)H^\bullet_{cell}(\mathbb{P}^n \times \mathbb{P}^n) \to H^\bullet_{cell}(\mathbb{P}^n) and the Künneth formula tells us Hcell(Pn×Pn)Hcell(PnHcell(Pn))H^\bullet_{cell}(\mathbb{P}^n \times \mathbb{P}^n) \simeq H^\bullet_{cell}(\mathbb{P}^n \otimes H^\bullet_{cell}(\mathbb{P}^n)), so we can take classes α,βHcell(Pn)\alpha,\beta \in H^\bullet_{cell}(\mathbb{P}^n), form αβ\alpha \otimes \beta, move this through the Künneth isomorphism and the morphism induced by the diagonal and end up in Hcell(Pn)H^\bullet_{cell}(\mathbb{P}^n) again, where we call the result αβ\alpha \cup \beta. Since Künneth is a graded isomorphism, this map is graded and thus we have all properties of a cup product. All other constructions (via Yoneda Ext products or wedge products of differential forms) yield the same product (otherwise we wouldn't call it cup product).

Hodge theory

There is still something left out in this discussion, namely Hodge theory. Betti cohomology of a smooth projective variety carries a Hodge structure. For projective space, there isn't much to discuss, as the Hodge structure is trivial in the sense that every class in HB2k(Pn)H^{2k}_{B}(\mathbb{P}^n) is of Hodge type (k,k)(k,k), i.e. the Hodge diamond of Pn\mathbb{P}^n has only the Hodge numbers hk,k=1h^{k,k}=1 and all other Hodge numbers vanish. The computation can be found in Voisin's book, section 7.2 (page 167 of book one of the english edition).

The structure of a homogeneous space

Now, a little bit of general theory not necessary to proceed:
The nn-dimensional projective space parametrizes 1-dimensional linear subspaces LL of affine n+1n+1-space, which we can consider as partial flags of linear subspaces 0LAn+10 \leq L \leq \mathbb{A}^{n+1}. We have a natural GLn+1GL_{n+1}-action on An+1\mathbb{A}^{n+1} (hence on flags). Partial flags of linear subspaces in An+1\mathbb{A}^{n+1} are stabilized by certain parabolic subgroups PP of GLn+1GL_{n+1}, for example full flags are stabilized by a Borel subgroup. The quotient GLn+1/BGL_{n+1}/B thus parametrizes precisely full flags in An+1\mathbb{A}^{n+1}. The quotients GLn+1/PGL_{n+1}/P that parametrize partial flags of a certain shape (determined by PP) are called generalized Grassmannians.
I included this material here to give an outlook on how to proceed past projective space later on, in further calculations.

More concretely:
In GLn+1GL_{n+1} look at the subgroup PP given by block matrices with a block of size n×nn \times n just all of GLnGL_n (in the upper left corner) and a block of size 1×11 \times 1 (in the lower right corner) just GL1GL_1, i.e. Gm\mathbb{G}_m, and a block of size n×1n \times 1 just An\mathbb{A}^n (in the upper right corner), with a block of size 1×n1 \times n just zeroes (in the lower left corner). If we look at GLn+1/PGL_{n+1}/P, we see that, as a variety, the big n×nn \times n block in the upper left corner of GLn+1GL_{n+1} is killed and what remains is An+1{0}\mathbb{A}^{n+1} \setminus \{0\} from the right column of GLn+1GL_{n+1}, modulo the group action from Gm\mathbb{G}_m from the lower right corner of PP. So we really have
!GLn+1/P=(An+1{0})/Gm=Pn.! GL_{n+1}/P = (\mathbb{A}^{n+1} \setminus \{0\})/\mathbb{G}_m = \mathbb{P}^n.

The good thing about this description is that PP contains a maximal torus (the diagonal matrices) and then there is a nice general theory of Schubert calculus to be applied. Topologically, this also gives us a CW structure, isomorphic to the structure we built "manually" before.

Algebraic de Rham cohomology over the rationals

By definition, HdR(Pn)=H(Pn,ΩPn/Q)H^\bullet_{dR}(\mathbb{P}^n) = \mathbb{H}^\bullet(\mathbb{P}^n, \Omega^\bullet_{\mathbb{P}^n/\mathbb{Q}}), a sheaf cohomology group. A cup product structure comes from the wedge product on the de Rham complex ΩPn/Q\Omega^\bullet_{\mathbb{P}^n/\mathbb{Q}}. One can compute algebraic de Rham cohomology by the Hodge-to-de Rham spectral sequence, which is
!E1p,q:=Hq(Pn,ΩPn/Qp)HdRp+q(Pn).! E^{p,q}_1 := \mathbb{H}^q(\mathbb{P}^n,\Omega^p_{\mathbb{P}^n/\mathbb{Q}}) \Rightarrow H^{p+q}_{dR}(\mathbb{P}^n).
From Hq(Pn,Ωp)=0\mathbb{H}^q(\mathbb{P}^n,\Omega^p) = 0 for pqp \neq q and Hq(Pn,Ωp)Q\mathbb{H}^q(\mathbb{P}^n,\Omega^p) \simeq \mathbb{Q} for 0p=qn0 \leq p=q \leq n (this is Hartshorne's Exercise III.7.3) we see that the spectral sequence degenerates hence the odd-dimensional algebraic de Rham cohomology of Pn\mathbb{P}^n vanishes and HdR2k(Pn)QH^{2k}_{dR}(\mathbb{P}^n) \simeq \mathbb{Q} for k=1,,nk = 1,\dots,n.

In particular, we have HdR(P1)Q[x]/(x2)H^\bullet_{dR}(\mathbb{P}^1) \simeq \mathbb{Q}[x]/(x^2). With the Künneth formula we compute for an nn-fold product HdR(P1××P1)Q[x1,,xn]/(xi2)H^\bullet_{dR}(\mathbb{P}^1\times\cdots\times\mathbb{P}^1) \simeq \mathbb{Q}[x_1,\dots,x_n]/(x_i^2). The symmetric group SnS_n acts on this polynomial ring as well as on the nn-fold product (P1)×n(\mathbb{P}^1)^{\times n}. We let the symmetric group act trivially on Pn\mathbb{P}^n and the map (P1)×nPn(\mathbb{P}^1)^{\times n} \to \mathbb{P}^n becomes SnS_n-equivariant. It induces an SnS_n-equivariant injection HdR(Pn)HdR((P1)×n)H^\bullet_{dR}(\mathbb{P}^n) \to H^\bullet_{dR}((\mathbb{P}^1)^{\times n}), so after taking invariants we obtain
!HdR(Pn)Q[x]/(xn+1)! H^\bullet_{dR}(\mathbb{P}^n) \simeq \mathbb{Q}[x]/(x^{n+1}), where x=x1++xn,x = x_1 + \cdots + x_n,
with xx in degree 22. Observe just that SnS_n is the Weyl group of GLnGL_n, and its appearance here is no accident.

l-adic cohomology

I don't want to compute l-adic cohomology here, since even the definitions are a bit lengthy.

For example, Hk(Pn)0H^k_\ell(\mathbb{P}^n) \simeq 0 for odd kk and Hk(Pn)ZH^k_\ell(\mathbb{P}^n) \simeq \mathbb{Z}_\ell for even kk. There is a Galois action on Hk(Pn)H^k_\ell(\mathbb{P}^n) such that H2(Pn)H^2_\ell(\mathbb{P}^n) is equivariantly isomophic to T(μ)T_\ell(\mu), the limit over the roots of unity μnC\mu_{\ell^n} \subseteq \mathbb{C}. Also, H0(Pn)ZH^0_\ell(\mathbb{P}^n) \simeq \mathbb{Z}_\ell, where we equip Z\mathbb{Z}_\ell with a trivial Galois action. Note that there are many non-equivariant isomorphisms ZT(μ)\mathbb{Z}_\ell \to T_\ell(\mu).

Similar in spirit, there is crystalline cohomology (or rigid cohomology) but I don't know enough about the subject to compute anything, so I have to leave that out.

Counting points over finite fields & Zeta function

I have written about this before (although with a different aim), so I don't want to repeat it.

The Zeta function of projective space is Z(Pn,s)=k=0n(1pkt)1Z(\mathbb{P}^n,s) = \prod_{k=0}^n{(1-p^kt)^{-1}},
as you can compute by hand from the decomposition of Fq\mathbb{F}_q-rational points Pn(Fq)=An(Fq)An1(Fq)A0(Fq)\mathbb{P}^n(\mathbb{F}_q) = \mathbb{A}^n(\mathbb{F}_q) \cup \mathbb{A}^{n-1}(\mathbb{F}_q) \cup \cdots \cup \mathbb{A}^0(\mathbb{F}_q).

So far this is what I had to tell about the cohomology of projective space.