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Basic properties of dlt pairs

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Classical vanishing theorems and some applications

3.13. Basic properties of dlt pairs

In this section, we prove some basic properties of dlt pairs. We note that the notion of dlt pairs plays very important roles in the recent developments of the minimal model program after [KoMo]. We also note that the notion of dlt pairs was introduced by Shokurov [Sh2].

First, let us prove the following well-known theorem.

Theorem 3.13.1. Let (X, D) be a dlt pair. Then X has only ra- tional singularities.

For the proof of Theorem 3.13.1, the following formulation of the Kawamata–Viehweg vanishing theorem is useful.

3.13. BASIC PROPERTIES OF DLT PAIRS 85

Theorem3.13.2 (Kawamata–Viehweg vanishing theorem). Let f : Y X be a projective surjective morphism onto a variety Y and let M be a Cartier divisor on Y. Letbe a boundary R-divisor on Y such that Supp ∆ is a normal crossing divisor on Y. Assume that M (KY + ∆) is f-ample. Then

RifOY(M) = 0 for every i >0.

It is obvious that Theorem 3.13.2 contains Norimatsu’s vanishing theorem: Theorem 3.2.12.

Proof of Theorem 3.13.2. We put D=M (KY + (1−ε)∆) for some small positive number ε. ThenD is an f-ampleR-divisor on Y such that dDe = M −KY and that Supp{D} is a normal crossing divisor on Y. By Theorem 3.2.9, we obtain RifOY(KY +dDe) = 0 for every i >0. This means that RifOY(M) = 0 for every i >0.

Let us give a proof of Theorem 3.13.1 based on Theorem 3.12.5, which was first obtained in [F17, Theorem 4.9]. For a related result, see [Nak2, Chapter VII, 1.1.Theorem].

Proof of Theorem 3.13.1. By the definition of dlt pairs, we can take a resolution f : Y X such that Exc(f) and Exc(f) Suppf1Dare both simple normal crossing divisors on Y and that

KY +f1D=f(KX +D) +E

with dEe ≥ 0. We can take an effective f-exceptional divisor A on Y such −A is f-ample (see, for example, Remark 2.3.18 and [F12, Proposition 3.7.7]). Then

dEe −(KY +f1D+{−E}+εA) = −f(KX +D)−εA is f-ample for ε > 0. If 0 < ε 1, then f1D+{−E}+εA is a boundary R-divisor whose support is a simple normal crossing divisor on Y. Therefore, RifOY(dEe) = 0 for i > 0 by Theorem 3.13.2 and fOY(dEe)' OX. Note that dEeis effective andf-exceptional. Thus, the composition

OX →RfOY →RfOY(dEe)' OX

is a quasi-isomorphism in the derived category. So,X has only rational

singularities by Theorem 3.12.5.

Remark 3.13.3. It is curious that Theorem 3.13.1 is missing in [Kv3]. As we saw in the proof of Theorem 3.13.1, it easily follows from Kov´acs’s characterization of rational singularities (see Theorem

86 3. CLASSICAL VANISHING THEOREMS AND SOME APPLICATIONS

3.12.5 and [Kv3, Theorem 1]). In [Kv3, Theorem 4], Kov´acs only proved the following statement. Let X be a variety with log terminal singularities. ThenX has only rational singularities.

3.13.4 (Weak log-terminal singularities). The proof of Theorem 3.13.1works for weak log-terminal singularities (see Definition2.3.21).

Thus, we can recover [KMM, Theorem 1-3-6], that is, we obtain the following statement.

Theorem3.13.5 (see [KMM, Theorem 1-3-6]). All weak log-terminal singularities are rational.

We do not need the difficult vanishing theorem due to Elkik and Fujita (see Theorem3.14.1) to obtain the above theorem. In Theorem 3.13.1, if we assume that (X, D) is only weak log-terminal singularities, then we can not always make Exc(f) and Exc(f)Suppf1D simple normal crossing divisors. We can only make themnormal crossing di- visors. However, Theorem 3.13.2works in this setting. Thus, the proof of Theorem 3.13.1 works for weak log-terminal singularities. Anyway, the notion of weak log-terminal singularities is not useful in the recent minimal model program.

The following theorem generalizes [Koetal, 17.5 Corollary], where it was only proved that S is semi-normal and satisfies Serre’sS2 condi- tion. Theorem3.13.6was first obtained in [F17] in order to understand [Koetal, 17.5 Corollary].

Theorem3.13.6 ([F17, Theorem 4.14]). LetXbe a normal variety and let S+B be a boundary R-divisor such that (X, S+B) is dlt, S is reduced, and bBc = 0. Let S = S1 +· · · +Sk be the irreducible decomposition. We put T = S1 +· · ·+Sl for some l with 1 l k. Then T is semi-normal, Cohen–Macaulay, and has only Du Bois singularities.

Proof. Let f :Y →X be a resolution of singularities such that KY +S0+B0 =f(KX +S+B) +E

with the following properties (see Remark 2.3.18):

(i) S0 (resp. B0) is the strict transform of S (resp.B).

(ii) Supp(S0+B0)Exc(f) and Exc(f) are simple normal crossing divisors onY.

(iii) f is an isomorphism over the generic point of any log canonical center of (X, S+B).

(iv) dEe ≥0.

3.13. BASIC PROPERTIES OF DLT PAIRS 87

We write S = T +U. Let T0 (resp. U0) be the strict transform of T (resp. U) on Y. We consider the following short exact sequence

0→ OY(−T0+dEe)→ OY(dEe)→ OT0(dE|T0e)0.

Since −T0+E R,f KY +U0+B0 and E R,f KY +S0+B0, we have

−T0+dEe ∼R,f KY +U0+B0+{−E} and

dEe ∼R,f KY +S0 +B0+{−E}. By Theorem 3.2.11, we obtain

RifOY(−T0+dEe) = RifOY(dEe) = 0 for every i >0. Therefore, we have

0→fOY(−T0+dEe)→ OX →fOT0(dE|T0e)0

and RifOT0(dE|T0e) = 0 for every i > 0. Note that dEe is effective and f-exceptional. Thus we obtain

OT 'fOT0 'fOT0(dE|T0e).

Since T0 is a simple normal crossing divisor,T is semi-normal. By the above vanishing result, we obtainRfOT0(dE|T0e)' OT in the derived category. Therefore, the composition

OT →RfOT0 →RfOT0(dE|T0e)' OT

is a quasi-isomorphism. Apply

RHomT( , ωT) to

OT →RfOT0 → OT. Then the composition

ωT →RfωT0 →ωT

is a quasi-isomorphism by Grothendieck duality. Hence, we have hi(ωT)⊆RifωT0 'Ri+dfωT0,

where d= dimT = dimT0.

Claim (see also Lemma 5.6.1). RifωT0 = 0 for every i >0.

Proof of Claim. We use induction on the number of the irre- ducible components ofT0. If T0 is irreducible, then Claim follows from the Grauert–Riemenschneider vanishing theorem: Theorem 3.2.7. Let Si0 be the strict transform of Si on Y for every i. Let W be any irre- ducible component of Si0

1 ∩ · · · ∩Si0m for {i1,· · · , im} ⊂ {1,2,· · · , k}. Thenf :W →f(W) is birational by the construction off. Therefore,

88 3. CLASSICAL VANISHING THEOREMS AND SOME APPLICATIONS

every Cartier divisor onW isf-big. We putT0 =S10 +T00 and consider the short exact sequence

0→ OT00(−S10)→ OT0 → OS10 0.

By taking ⊗ωT0, we obtain 0→ωT0

0 →ωT0 →ωS0

1 ⊗ OS01(T0|S10)0.

Then we have the following long exact sequence

· · · →RifωT0

0 →RifωT0 →RifOS01(KS0

1 +T0|S01)→ · · · . By Theorem 3.2.11, RifOS01(KS0

1 +T0|S01) = 0 for every i > 0. By induction on the number of the irreducible components, we obtain that RifωT00 = 0 for everyi >0. Therefore, we obtain the desired vanishing

theorem.

Therefore, by Claim, hi(ωT) = 0 for i 6= −d. Thus, T is Cohen–

Macaulay. This argument is the same as the proof of Theorem 3.12.5.

Since T0 is a simple normal crossing divisor, T0 has only Du Bois sin- gularities (see, for example, Lemma5.3.8). Note that the composition

OT →RfOT0 → OT

is a quasi-isomorphism. It implies thatT has only Du Bois singularities (see [Kv1, Corollary 2.4]). Since the composition

ωT →fωT0 →ωT

is an isomorphism, we obtain fωT0 T. By Grothendieck duality, RfOT0 'RHomT(RfωT0, ωT)'RHomT(ωT, ωT)' OT. So, we have RifOT0 = 0 for every i >0.

We obtained the following vanishing theorem in the proof of Theo- rem 3.13.6.

Corollary 3.13.7. Under the notation in the proof of Theorem 3.13.6, RifOT0 = 0 for every i >0 and fOT0 ' OT.

As a special case, we have:

Corollary 3.13.8 ([KoMo, Corollary 5.52]). Let (X, S+B)be a dlt pair as in Theorem 3.13.6. Then Si is normal for every i.

Proof. We put T =Si. ThenSi is normal since fOT0 ' OT (see

Corollary 3.13.7).

Let us discuss a nontrivial example. This example shows the sub- tleties of the notion of dlt pairs.

3.13. BASIC PROPERTIES OF DLT PAIRS 89

Example 3.13.9 (cf. [KMM, Remark 0-2-11. (4)]). We consider the P2-bundle

π :V =PP2(OP2 ⊕ OP2(1)⊕ OP2(1))P2.

Let F1 = PP2(OP2 ⊕ OP2(1)) and F2 = PP2(OP2 ⊕ OP2(1)) be two hy- persurfaces of V which correspond to projections

OP2 ⊕ OP2(1)⊕ OP2(1)→ OP2 ⊕ OP2(1)

given by (x, y, z)7→(x, y) and (x, y, z)7→(x, z). Let Φ : V →W be the flipping contraction that contracts the negative section of π:V P2, that is, the section corresponding to the projection

OP2 ⊕ OP2(1)⊕ OP2(1)→ OP2 0.

LetC P2 be an elliptic curve. We put Y =π1(C),D1 =F1|Y, and D2 = F2|Y. Let f : Y X be the Stein factorization of Φ|Y : Y Φ(Y). Then the exceptional locus of f isE =D1∩D2. We note that Y is smooth, D1 +D2 is a simple normal crossing divisor, and E 'C is an elliptic curve. Let g :Z →Y be the blow-up along E. Then

KZ +D01+D20 +D=g(KY +D1+D2),

where D01 (resp. D02) is the strict transform of D1 (resp. D2) and D is the exceptional divisor of g. Note that D'C×P1. Since

−D+ (KZ+D10 +D20 +D)(KZ+D10 +D20) = 0,

we obtain that Rif(gOZ(−D+KZ +D01 +D02+D)) = 0 for every i > 0 by Theorem 5.7.3 below. We note that f ◦g is an isomorphism outside D. We consider the following short exact sequence

0→ IE → OY → OE 0,

where IE is the defining ideal sheaf of E. Since IE = gOZ(−D), we obtain that

0→f(IE ⊗ OY(KY +D1+D2))→fOY(KY +D1+D2)

→fOE(KY +D1+D2)0 byR1f(IE ⊗ OY(KY +D1+D2)) = 0. By adjunction,

OE(KY +D1 +D2)' OE. Therefore,OY(KY +D1+D2) is f-free. In particular,

KY +D1+D2 =f(KX +B1+B2),

whereB1 =fD1 andB2 =fD2. Thus, −D−(KZ+D10 +D20)fg 0.

So, we have

RifIE =Rif(gOZ(−D)) = 0

90 3. CLASSICAL VANISHING THEOREMS AND SOME APPLICATIONS

for every i > 0 by Theorem 5.7.3 below. This implies that RifOY ' RifOE for every i >0. Thus,R1fOY 'C(P), where P =f(E). We consider the following spectral sequence

Ep,q =Hp(X, RqfOY ⊗ OX(−mA))⇒Hp+q(Y,OY(−mA)), where A is an ample Cartier divisor on X and m is any positive in- teger. Since H1(Y,OY(−mfA)) = H2(Y,OY(−mfA)) = 0 by the Kawamata–Viehweg vanishing theorem (see Theorem 3.2.1), we have

H0(X, R1fOY ⊗ OX(−mA))'H2(X,OX(−mA)).

If we assume that X is Cohen–Macaulay, then we have H2(X,OX(−mA)) = 0

for everym 0 by Serre duality and Serre’s vanishing theorem. On the other hand, H0(X, R1fOY ⊗ OX(−mA))' C(P) because R1fOY ' C(P). This is a contradiction. Thus, X is not Cohen–Macaulay. In particular, (X, B1 +B2) is log canonical but not dlt. We note that Exc(f) = E is not a divisor on Y.

Let us recall that Φ : V W is a flipping contraction. Let Φ+ : V+ →W be the flip of Φ. We can check that

V+=PP1(OP1 ⊕ OP1(1)⊕ OP1(1)⊕ OP1(1))

and the flipped curveE+'P1 is the negative section ofπ+ :V+P1, that is, the section corresponding to the projection

OP1 ⊕ OP1(1)⊕ OP1(1)⊕ OP1(1) → OP1 0.

LetY+be the strict transform ofY onV+. ThenY+is Gorenstein, log canonical alongE+ ⊂Y+, and smooth outsideE+. LetD1+ (resp.D2+) be the strict transform of D1 (resp. D2) on Y+. If we take a Cartier divisor B on Y suitably, then

(Y, D1+D2)_ _ _ _ _ _ _//

fLLLLLLL%%

LL

LL (Y+, D+1 +D+2)

xxpppppppppppp

X

is the B-flop of f : Y X. In this example, the flopping curve E is a smooth elliptic curve and the flopped curve E+ is P1. We note that (Y, D1 +D2) is dlt. However, (Y+, D+1 +D2+) is log canonical but not dlt.

We close this section with Kov´acs’s vanishing theorem.

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