1 Introduction

Let Y be a smooth manifold of dimension n. Assume that $$\mu _1,\ldots ,\mu _r$$ are cycles on Y of pure codimensions $$\kappa _1,\ldots ,\kappa _r$$, respectively, let , and let V be the set-theoretic intersection $$V=|\mu _1|\cap \cdots \cap |\mu _r|$$. If intersect properly, that is, if $$\mathrm{codim\,}V=\kappa$$, then there is a well-defined intersection cycle

where are the irreducible components of V and are integers. In the nonproper case there is no canonical intersection cycle. However, following Fulton–MacPherson, see [12], there is an intersection product $$\mu _1\cdot _Y\cdots \cdot _Y\mu _r$$, which is an element in the Chow group $${{\mathscr {A}}}_{n-\kappa }(V)$$; that is, the product is represented by a cycle on V of dimension $$n-\kappa$$ that is determined up to rational equivalence. For instance, the self-intersection of a line L in $${\mathbb {P}}^{\,n}$$ is obtained by intersecting L with a perturbation of L. If $$n=2$$ one gets an arbitrary point on L, whereas if $$n\hbox {\,\char 062\,}3$$ the intersection is empty.

In case $$Y={\mathbb {P}}^{\,n}$$ there is an intersection product due to Stückrad and Vogel [16, 18], that in general consists of components of various dimensions. For instance the self-intersection of a line is actually the line itself independently of n. However, in general a nonproper intersection has so-called moving components, that are only determined up to rational equivalence. There is a relation to the classical (Fulton–MacPherson) intersection product via van Gastel’s formulas [14], see also [11].

Tworzewski [17], introduced, for $$x\in V$$, local intersection numbers

\begin{aligned} \epsilon _\ell (\mu _1,\ldots ,\mu _r, x), \quad \ell =0,\ldots , \dim V, \end{aligned}
(1.1)

see also [1, 2, 13] and Sect. 3 below. In the proper case $$\epsilon _\ell (\mu _1,\ldots ,\mu _r, x)$$ is precisely the multiplicity at x of the proper intersection $$\mu _1\cdot _Y \cdots \cdot _Y \mu _r$$ for $$\ell =\dim V$$ and 0 otherwise. In the nonproper case the intersection numbers may be nonzero also for $$\ell <\dim V$$. In general no representative of the classical intersection product, cf. [6, Remark 1.4], or representative of the Stückrad–Vogel product, can represent these numbers at all points.

The main objective of this paper is to introduce a product of cycles in $${\mathbb {P}}^{\,n}$$ that at each point carries the local intersection numbers and at the same time have reasonable global properties, such as respecting the Bézout formula. To this end we must extend the class of cycles, and our construction is based on the $${{\mathbb {Z}}}$$-module $${\mathscr {GZ}}(X)$$ of generalized cycles on a (reduced) analytic space X introduced in [4]. It is the smallest class of currents on analytic spaces that is closed under multiplication by components of Chern forms and under direct images under proper holomorphic mappings. It turns out that generalized cycles inherit a lot of geometric properties and preferably can be thought of as geometric objects. Actually we are primarily interested in a certain natural quotient group $${{\mathscr {B}}}(X)$$ of $${\mathscr {GZ}}(X)$$. Each $$\mu$$ in $${\mathscr {GZ}}(X)$$ has a well-defined Zariski support $$|\mu |\subset X$$ that only depends on its class in $${{\mathscr {B}}}(X)$$. For a subvariety $$V\hookrightarrow X$$ there is a natural identification of $${{\mathscr {B}}}(V)$$ with elements in $${{\mathscr {B}}}(X)$$ that have Zariski support on V. The group of cycles $${{\mathscr {Z}}}(X)$$ is naturally embedded in $${{\mathscr {B}}}(X)$$. Given $$\mu \in {{\mathscr {B}}}(X)$$ also its restriction $$\mathbf{1}_V\mu$$ to the subvariety V is an element in $${{\mathscr {B}}}(X)$$. Each element in $${\mathscr {GZ}}(X)$$, and in $${{\mathscr {B}}}(X)$$, has a unique decomposition into sums of irreducible components. Each irreducible element has in turn a unique decomposition into components of various dimensions. We let $${{\mathscr {B}}}_k(X)$$ denote the elements in $${{\mathscr {B}}}(X)$$ of pure dimension k. We also introduce a notion of effective generalized cycle $$\mu$$ in $${\mathscr {GZ}}(X)$$, and class in $${{\mathscr {B}}}(X)$$, generalizing the notion of effective cycle. Each $$\mu$$ in $${\mathscr {GZ}}(X)$$, and in $${{\mathscr {B}}}(X)$$, has a well-defined multiplicity, $$\text {mult}_x\,\mu$$, at each point $$x\in X$$, that is an integer and nonnegative if $$\mu$$ is effective. Moreover, for each $$\mu$$ in $${\mathscr {GZ}}_k(X)$$, or in $${{\mathscr {B}}}_k(X)$$, there is a unique decomposition

\begin{aligned} \mu =\mu _{\mathrm{fix}}+\mu _{\mathrm{mov}}, \end{aligned}
(1.2)

where $$\mu _{\mathrm{fix}}$$ is an ordinary cycle of dimension k, whose irreducible components are called the fixed components of $$\mu$$, and $$\mu _{\mathrm{mov}}$$, whose irreducible components, the moving components, have Zariski support on varieties of dimension strictly larger than k.

Each $$\mu$$ in $${\mathscr {GZ}}_k({\mathbb {P}}^{\,n})$$, or in $${{\mathscr {B}}}_k(\mathbb P^{\,n})$$, has the degree

(1.3)

where $$\omega$$ is the first Chern class of $${\mathscr {O}}(1)\rightarrow {\mathbb {P}}^N$$, for instance represented by the Fubini–Study metric form. If $$\mu =\mu _0+\mu _1+\cdots$$, where $$\mu _k$$ has pure dimension k, then

For each point $$x\in {\mathbb {P}}^{\,n}$$ and $$\mu _1,\ldots ,\mu _r\in {{\mathscr {B}}}({{\mathscr {U}}})$$ for some open subset $${{\mathscr {U}}}\subset {\mathbb {P}}^{\,n}$$ there are $${{\mathbb {Z}}}$$-valued functions $$\epsilon _\ell (\mu _1,\ldots ,\mu _r,x)$$, $$\ell =0,1,\ldots$$, that are $${{\mathbb {Z}}}$$-multilinear in , only depend on the germs of at x, and which coincide with the local intersection numbers (1.1) if are cycles. We say that $$\epsilon _\ell (\mu _1,\ldots ,\mu _r,x)$$ are the local intersection numbers of $$\mu _1,\ldots ,\mu _r$$ at x. If are effective, then these numbers are nonnegative.

Our main result concerns a $${{\mathbb {Z}}}$$-multilinear mapping

(1.4)

We say that the image is the $$\bullet$$-product of $$\mu _1,\ldots ,\mu _r$$. It is obtained, roughly speaking, in the following way: We first choose representatives for the $${{\mathscr {B}}}$$-classes $$\mu _1, \ldots , \mu _r$$, then form a Stückrad–Vogel-type product of them. Even for cycles, this product depends on several choices. Taking a suitable mean value, we get a generalized cycle that turns out to define an element in $${{\mathscr {B}}}({\mathbb {P}}^{\,n})$$ that is independent of all choices. If are cycles, then the fixed components in the Stückrad–Vogel product appear as fixed components of . The formal definition, Definition 6.6, is expressed in terms of a certain Monge–Ampère type product, that can be obtained as a limit of quite explicit expressions, see Sect. 6. Here is our main result.

Theorem 1.1

The $${{\mathbb {Z}}}$$-multilinear mapping (1.4) has the following properties. To begin with, , is commutative, and

(1.5)

where $$( \ )_\ell$$ denotes the component of dimension $$\ell$$. If have pure dimensions and

(1.6)

then

(1.7)

If are effective, then is effective and

(1.8)

If $$\mu _1, \ldots , \mu _r$$ are cycles that intersect properly, then

(1.9)

One should keep in mind that the $$\bullet$$-product of r factors is not a repeated $$\bullet$$-product of two factors. In general, the $$\bullet$$-product of two factors is not associative, see Example 8.10.

Notice that $$\rho$$ equals $$n-(n-\dim \mu _1 +\cdots +n-\dim \mu _r)$$, which is the “expected dimension” of the intersection. The Bézout formula (1.7) may hold even if $$\rho <0$$: For instance, if are different lines through the point a, then their $$\bullet$$-product is a so that both sides of (1.8) are 1, see Example 8.8. Moreover, if we take a linear embedding $${\mathbb {P}}^{\,n}\hookrightarrow \mathbb P^{\,n'}$$, $$n'\!>n$$, and consider as elements in $${{\mathscr {B}}}({\mathbb {P}}^{\,n'})$$, then the product is unchanged. In particular, the -self-intersection of a k-plane is always the k-plane itself.

The -self-intersection of the cuspidal curve $$Z=\{x_1^3-x_0x_2^2=0\}$$ in $${\mathbb {P}}^2$$ is in the classical sense represented by nine points on Z obtained as the divisor of a generic meromorphic section of $${\mathscr {O}}_{{\mathbb {P}}^2}(3)$$ restricted to Z. The fixed part of the self-intersection in the Stückrad–Vogel sense is the curve itself plus 3 times the point $$a=[1,0,0]$$, whereas the moving part consists of another three points on Z that are determined up to rational equivalence on Z. Our product consists of the the fixed part $$Z+3a$$ of the Stückrad–Vogel (SV)-product and a moving component $$\mu$$ of dimension zero and degree 3; we think of $$\mu$$ as three points “moving around” on Z, cf. Example 8.13. In this case the local intersection numbers are carried by the fixed components. In general also moving components can contribute, see, e.g., Example 8.6.

We also consider another intersection product that is a $${{\mathscr {B}}}$$-variant of the classical nonproper intersection product in [12]: For any regular embedding i, in [4] we introduced a $${{\mathscr {B}}}$$-analogue of the Gysin mapping $$i^!$$ used in [12], see Sect. 2.7 below. Let be the diagonal embedding in $$({\mathbb {P}}^{\,n})^r$$. In analogy with the classical intersection product in [12] we define, for pure-dimensional ,

in $${{\mathscr {B}}}({\mathbb {P}}^{\,n})$$. We have the following relation to the $$\bullet$$-product.

Theorem 1.2

Assume that $$\mu _1,\ldots , \mu _r\in {{\mathscr {B}}}({\mathbb {P}}^{\,n})$$ have pure dimensions. Let and let $$\rho$$ be as in (1.6). Then

In particular, if $$\mu _1, \ldots , \mu _r$$ are cycles that intersect properly, see (1.9).

In [4, Section 10] we introduced cohomology groups $${\widehat{H}}^{*,*}(V)$$ for a reduced subvariety $$V\hookrightarrow {\mathbb {P}}^{\,n}$$ of pure dimension d that coincide with usual de Rham cohomology $$H^{*,*}(V)$$ when V is smooth. There are natural mappings $${{\mathscr {A}}}_k(V)\rightarrow \widehat{H}^{d-k,d-k}(V)$$ and $${{\mathscr {B}}}_k(V)\rightarrow {\widehat{H}}^{d-k,d-k}(V)$$.

Theorem 1.3

Assume that $$Z_1,\ldots , Z_r$$ are cycles in $${\mathbb {P}}^N$$ and let . The images in $$\widehat{H}^{*,*}(V)$$ of the Chow class and the $${{\mathscr {B}}}$$-class coincide.

The plan of the paper is as follows. Sections 2 through 4 mainly contain material from [4] and well-known facts from [12], as well as the definition of local intersection numbers and of the notion of an effective generalized cycle. The product $$\cdot _{{{\mathscr {B}}}(Y)}$$ is introduced in Sect. 5. In Sect. 6 we define the $$\bullet$$-product and prove Theorem 1.1, whereas the connection to the $$\cdot _{{{\mathscr {B}}}({\mathbb {P}}^{\,n})}$$-product is worked out in Sect. 7. Finally we have collected several examples in Sect. 8.

2 Preliminaries

Throughout this section X is a reduced analytic space of pure dimension n. We will recall some basic notions from intersection theory that can be found in [12], and some notions and results from [4]; however the material in Sect. 2.4 and Lemma 2.1 are new. We formulate statements in terms of coherent sheaves, rather than schemes.

2.1 Currents and cycles

We say that a current $$\mu$$ on X of bidegree $$(n-k, n-k)$$ has (complex) dimension k. If $$f:X'\!\rightarrow X$$ is a proper mapping of analytic spaces, then $$f^*$$ is well-defined on smooth forms, and $$f_*$$ is well-defined on currents and preserves dimension, see [7, III Corollary 2.4.11] or [5]. If $$\mu$$ is a current on $$X'$$ and $$\eta$$ is a smooth form on X, then

(2.1)

If $$\mu$$ has order zero then $$f_*\mu$$ has order zero. If $$V\hookrightarrow X$$ is a subvariety, then

\begin{aligned} \mathbf{1}_V f_*\mu =f_*\big (\mathbf{1}_{f^{-1} V} \mu \big ). \end{aligned}
(2.2)

If $$V\hookrightarrow X$$ has dimension k, then its associated Lelong current (current of integration) [V] has dimension k. We will often identify V and [V]. An analytic k-cycle $$\mu$$ on X is a formal locally finite linear combination , where and are irreducible analytic sets of dimension k. We denote the $${{\mathbb {Z}}}$$-module of analytic k-cycles on X by $${{\mathscr {Z}}}_k(X)$$. The support $$|\mu |$$ of $$\mu \in {{\mathscr {Z}}}_k(X)$$ coincides with the support of its associated Lelong current. Recall that $$\mathrm{mult}_x \mu =\ell _x \mu$$, where $$\ell _x\mu$$ denotes the Lelong number (of the Lelong current) of $$\mu \in {{\mathscr {Z}}}_k(X)$$ at x, and $$\mathrm{mult}_x\mu$$ is the multiplicity of $$\mu$$ at x, see [9, Chapter 2.11.1].

If $$f:X'\!\rightarrow X$$ is a proper mapping, then we have a mapping

\begin{aligned} f_*:{{\mathscr {Z}}}_k(X')\rightarrow {{\mathscr {Z}}}_k(X), \end{aligned}
(2.3)

and the Lelong current of the direct image $$f_*\mu$$ is the direct image of the Lelong current of $$\mu$$. If $$i:V\hookrightarrow X$$ is a subvariety, then $$\mu \in {{\mathscr {Z}}}_k(V)$$ can be identified with the cycle $$i_*\mu \in {{\mathscr {Z}}}_k(X)$$. The cycle $$\mu \in {{\mathscr {Z}}}_k(X)$$ is rationally equivalent to 0 on X, $$\mu \sim 0$$, if there are finitely many subvarieties of dimension $$k+1$$ and non-trivial meromorphic functions on such thatFootnote 1

We denote the Chow group of cycles $${{\mathscr {Z}}}_k(X)$$ modulo rational equivalence by $${{\mathscr {A}}}_k(X)$$. If $$f:X'\!\rightarrow X$$ is a proper morphism and $$\mu \sim 0$$ in $${{\mathscr {A}}}_k(X')$$, then $$f_*\mu \sim 0$$ in $${{\mathscr {A}}}_k(X)$$ and there is an induced mapping $$f_*:{{\mathscr {A}}}_k(X')\rightarrow {{\mathscr {A}}}_k(X)$$.

2.2 Chern and Segre forms

Recall that to any Hermitian line bundleFootnote 2$$L\rightarrow X$$ there is an associated (total) Chern formFootnote 3$${\widehat{c}}(L)=1+{\widehat{c}}_1(L)$$ and that two Hermitian metrics give rise to Chern forms whose difference is $$dd^c \gamma$$ for a smooth form $$\gamma$$ on X. We let c(L) denote the associated cohomology class.

Assume that $$E\rightarrow X$$ is a Hermitian vector bundle, and let $$\pi :{\mathbb {P}}(E)\rightarrow X$$ be the projectivization of E, i.e., the projective bundle of lines in E. Let $$L={\mathscr {O}}(-1)$$ be the tautological line bundle in the pullback $$\pi ^*\!E\rightarrow {\mathbb {P}}(E)$$, and let $${\widehat{c}}(L)$$ be the induced Chern form on $${\mathbb {P}}(E)$$. Since $$\pi$$ is a submersion, is a smooth form on X called the Segre form of E. If E is a line bundle, then $${\mathbb {P}}(E)\simeq X$$ and hence

\begin{aligned} {\widehat{c}}(E)=1/{\widehat{s}}(E). \end{aligned}
(2.4)

For a general Hermitian $$E\rightarrow X$$ we take (2.4) as the definition of its associated Chern form. If $$f:X'\!\rightarrow X$$ is a proper mapping, then

\begin{aligned} {\widehat{c}}_\ell (f^*\!E)=f^*{\widehat{c}}_\ell (E). \end{aligned}
(2.5)

Since $$\pi$$ is a submersion two different metrics on E give rise to Segre forms and Chern forms that differ by $$dd^c\gamma$$ for a smooth form $$\gamma$$ on X. The induced cohomology classes are denoted by s(E) and c(E), respectively. There are induced mappings

\begin{aligned} {{\mathscr {A}}}_k(X)\rightarrow {{\mathscr {A}}}_{k-\ell }(X),\quad \alpha \mapsto c_\ell (E)\cap \alpha . \end{aligned}

2.3 Generalized cycles

Generalized cycles on X were introduced in [4] and all statements in this subsection except Lemma 2.1 are proved in [4, Sections 3 and 4]. We say that a current $$\mu$$ is a generalized cycle if it is a locally finite linear combination over $${{\mathbb {Z}}}$$ of currents of the form $$\tau _* \alpha$$, where $$\tau :W\rightarrow X$$ is a proper map, W is smooth and connected, and $$\alpha$$ is a product of components of Chern forms for various Hermitian vector bundles over W, i.e.,

(2.6)

where are Hermitian vector bundles over W. One can just as well use components of Segre forms, and one can in fact assume that all are line bundles.

Notice that a generalized cycle is a real closed current of order zero with components of bidegree $$(*,*)$$. We let $${\mathscr {GZ}}_k(X)$$ denote the $${{\mathbb {Z}}}$$-module of generalized cycles of (complex) dimension k (i.e., of bidegree $$(n-k,n-k)$$) and we let $${\mathscr {GZ}}(X)=\bigoplus {\mathscr {GZ}}_k(X)$$. If $$\mu \in {\mathscr {GZ}}(X)$$ and $$\gamma$$ is a component of a Chern form on X, then $$\gamma {\wedge }\mu \in {\mathscr {GZ}}(X)$$. If $$E\rightarrow X$$ is a Hermitian vector bundle we thus have mappings $${\mathscr {GZ}}_k(X)\rightarrow {\mathscr {GZ}}_{k-\ell }(X)$$ defined by $$\mu \mapsto {\widehat{c}}_\ell (E){\wedge }\mu$$.

If $$i:V\hookrightarrow X$$ is a subvariety and $$\mu \in {\mathscr {GZ}}(X)$$, then $$\mathbf{1}_V\mu \in {\mathscr {GZ}}(X)$$. More precisely, if

(2.7)

where , then

Each subvariety of X is a generalized cycle so we have an embedding

\begin{aligned} {{\mathscr {Z}}}_k(X)\rightarrow {\mathscr {GZ}}_k(X). \end{aligned}

Given $$\mu \in {\mathscr {GZ}}(X)$$ there is a smallest variety $$|\mu |\subset X$$, the Zariski support of $$\mu$$, such that $$\mu$$ vanishes outside $$|\mu |$$. If $$f:X'\!\rightarrow X$$ is proper, then we have a natural mapping

\begin{aligned} f_*:{\mathscr {GZ}}_k(X')\rightarrow {\mathscr {GZ}}_k(X) \end{aligned}

that coincides with (2.3) on $${{\mathscr {Z}}}_k$$. If $$i:V \hookrightarrow X$$ is a subvariety, then

\begin{aligned} i_*:{\mathscr {GZ}}_k(V)\rightarrow {\mathscr {GZ}}_k(X) \end{aligned}
(2.8)

is an injective mapping whose image is precisely those $$\mu \in {\mathscr {GZ}}_k(X)$$ such that $$|\mu |\subset V$$. Thus we can identify $${\mathscr {GZ}}(V)$$ with generalized cycles in X that have Zariski support on Z. We have

Dimension principle

Assume that $$\mu \in {\mathscr {GZ}}_k(X)$$ has Zariski support on a variety V. If $$\dim V =k$$, then $$\mu \in {{\mathscr {Z}}}_k(X)$$. If $$\dim V<k$$, then $$\mu =0$$.

A nonzero generalized cycle $$\mu \in {\mathscr {GZ}}(X)$$ is irreducible if $$|\mu |$$ is irreducible and $$\mathbf{1}_V\mu =0$$ for any proper analytic subvariety $$V\hookrightarrow |\mu |$$. If $$\mu$$ has Zariski support $$V\subset X$$ it is irreducible if and only if V is irreducible and $$\mu$$ has a representation (2.7) where for each j. An irreducible $$\mu \in {\mathscr {GZ}}(X)$$ has the decomposition $$\mu =\mu _p+ \cdots + \mu _1 +\mu _0, \, \mu _k\in {\mathscr {GZ}}_k(X)$$, where p is the dimension of $$|\mu |$$. Each $$\mu \in {\mathscr {GZ}}(X)$$ has a unique decomposition

\begin{aligned} \mu =\sum _\ell \mu _\ell , \end{aligned}

where $$\mu _\ell$$ are irreducible with different Zariski supports.

If $$0\rightarrow S\rightarrow E\rightarrow Q\rightarrow 0$$ is a short exact sequence of Hermitian vector bundles over X, then we say that is a B-form. If $$\beta$$ is a component of a B-form, then there is a smooth form $$\gamma$$ on X such that $$dd^c\gamma =\beta$$. We say that $$\mu \in {\mathscr {GZ}}_k(X)$$ is equivalent to 0 in X, $$\mu \sim 0$$, if $$\mu$$ is a locally finite sum of currents of the form

(2.9)

where $$\tau :W\rightarrow X$$ is proper, $$\beta$$ is a component of a B-form, $$\alpha$$ is a product of components of Chern or Segre forms, and $$\gamma$$ is a smooth form on W. If $$\mu =\mu _0+\cdots +\mu _n$$, where $$\mu _k\in {\mathscr {GZ}}_k(X)$$, we say that $$\mu \sim 0$$ if $$\mu _k\sim 0$$ for each k. Let $${{\mathscr {B}}}(X)$$ denote the $${{\mathbb {Z}}}$$-module of generalized cycles on X modulo this equivalence. A class $$\mu \in {{\mathscr {B}}}(X)$$ has pure dimension k, $$\mu \in {{\mathscr {B}}}_k(X)$$, if $$\mu$$ has a representative in $${\mathscr {GZ}}_k(X)$$. Thus $${{\mathscr {B}}}(X)=\bigoplus _k{{\mathscr {B}}}_k(X)$$. The mapping $${{\mathscr {Z}}}(X)\rightarrow {{\mathscr {B}}}(X)$$ is injective so we can consider $${{\mathscr {Z}}}(X)$$ as a subgroup of $${{\mathscr {B}}}(X)$$.

If $$\mu \in {{\mathscr {B}}}(X)$$ and $${\widehat{\mu }}\in {\mathscr {GZ}}(X)$$ is a representative for $$\mu$$, then the Zariski support $$|\mu |\subset X$$ of $$\mu$$ is the union of the Zariski supports of the irreducible components of $${\widehat{\mu }}$$ that are nonzero in $${{\mathscr {B}}}(X)$$. Moreover, $$\mu \in {{\mathscr {B}}}(X)$$ is irreducible if there is a representative $${\widehat{\mu }}\in {\mathscr {GZ}}(X)$$ that is irreducible. The decomposition into irreducible components, as well as the decomposition into components of different dimensions, extend from $${\mathscr {GZ}}(X)$$ to $${{\mathscr {B}}}(X)$$.

If $$0\rightarrow S\rightarrow E\rightarrow Q\rightarrow 0$$ is a short exact sequence of Hermitian vector bundles and $${\widehat{\mu }}\in {\mathscr {GZ}}(X)$$, then

(2.10)

In particular, if E and $$E'$$ are the same vector bundle with two different Hermitian metrics, then so we have mappings

\begin{aligned} {{\mathscr {B}}}_k(X)\rightarrow {{\mathscr {B}}}_{k-\ell }(X), \quad \mu \mapsto c_\ell (E){\wedge }\mu . \end{aligned}

If $$f:X'\!\rightarrow X$$ is a proper mapping, then we have a natural mapping

\begin{aligned} f_* :{{\mathscr {B}}}(X')\rightarrow {{\mathscr {B}}}(X). \end{aligned}

If $$i:V\hookrightarrow X$$ is a subvariety, then

\begin{aligned} i_*:{{\mathscr {B}}}(V)\rightarrow {{\mathscr {B}}}(X) \end{aligned}
(2.11)

is injective, and we can identify its image with the elements in $${{\mathscr {B}}}(X)$$ that have Zariski support on V.

Each $$\mu \in {{\mathscr {B}}}_k(X)$$ (and $$\mu \in {\mathscr {GZ}}_k(X)$$) has a unique decomposition (1.2) where $$\mu _{\mathrm{fix}}$$ is a cycle of pure dimension k and the irreducible components of $$\mu _{\mathrm{mov}}$$ have Zariski supports of dimension strictly larger than k. We say that the irreducible components of $$\mu _{\mathrm{fix}}$$ are fixed and that the irreducible components of $$\mu _{\mathrm{mov}}$$ are moving.

We will need the following simple lemma.

Lemma 2.1

Assume that $$\mu _1,\ldots , \mu _r$$ are generalized cycles on reduced analytic spaces $$X_1,\ldots , X_r$$. Let be the natural projections. Then

is a generalized cycle on . If $$\mu _{j}\sim 0$$ in $$X_{j}$$ for some j, then in .

In particular, for $$\mu _{j}\in {{\mathscr {B}}}(X_{j})$$, $$j=1,\ldots , r$$, there is a well-defined .

Proof

Assume that , where are proper and are products of components of Chern forms. Let be the natural projections. Then $$\pi _1^*\alpha _1{\wedge }\cdots {\wedge }\pi _r^*\alpha _r$$ is a product of components of Chern forms on and

and hence it is a generalized cycle on . If, say, $$\mu _1\sim 0$$, we may assume, cf. (2.9), that $$\mu _1=(\tau _1)_*(\beta {\wedge }\alpha _1)$$, where $$\beta$$ is a component of a B-form. Then also $$\pi _1^*\beta$$ is a component of a B-form. Now is the push-forward of $$\pi _1^*\beta {\wedge }\pi _1^*\alpha _1{\wedge }\pi _2^*\alpha _2{\wedge }\cdots {\wedge }\pi _r^*\alpha _r$$ and therefore it is equivalent to 0 in by definition.$$\square$$

2.4 Effective generalized cycles

We say that a generalized cycle $$\mu$$ is effective if it is a positive current, see, e.g., [10, Chapter III, Definition 1.13]. Clearly effectivity is preserved under direct images.

Lemma 2.2

Let $$\mu =\mu _1+\mu _2+\cdots$$ be the decomposition of $$\mu \in {\mathscr {GZ}}(X)$$ into its irreducible components. Then $$\mu$$ is effective if and only if each is effective.

Proof

The if-part is clear. For the converse, let V be an irreducible subvariety of X. We already know that $$\mathbf{1}_V\mu$$ is a generalized cycle. It is not hard to see that it is positive if $$\mu$$ is positive. It is also part of the Skoda–El Mir theorem, see, e.g., [10, Chapter III, Theorem 2.3]. Now let be the Zariski supports of the various and assume that $$V_k$$ has minimal dimension. Then has positive codimension in for each $$j\ne k$$. By the definition of irreducibility it follows that $$\mathbf{1}_{V_k}\mu =\mathbf{1}_{V_k}\mu _k=\mu _k$$. We conclude that $$\mu _k$$ is positive for each k such that $$V_k$$ has minimal dimension. Let $$V'$$ be the union of these $$V_k$$ and let $$\mu '$$ be the sum of the remaining irreducible components. Clearly $$\mu '$$ is positive in . Let for smooth (1, 0)-forms $$a_{j}$$ and some r. It follows that $$A{\wedge }\mu '$$ is positive outside $$V'$$ by definition. However, $$\mathbf{1}_{V'}\mu '\!=0$$ and so $$A{\wedge }\mu '\!=A{\wedge }\mathbf{1}_{X{\setminus } V'}\mu '$$ is positive. Since A is arbitrary, we conclude that $$\mu '$$ is positive. Now the lemma follows by induction. $$\square$$

We say that $$\mu \in {{\mathscr {B}}}(X)$$ is effective if it has a representative $${\widehat{\mu }} \in {\mathscr {GZ}}(X)$$ that is effective. It follows that $$\mu$$ is effective if and only each of its irreducible components is effective. Moreover, the multiplicities of an effective $$\mu \in {{\mathscr {B}}}(X)$$ are nonnegative.

2.5 The Segre and $${{\mathscr {B}}}$$-Segre class

The material in this subsection is found in [4, Section 5] or in [12]. Let $${{\mathscr {J}}}\rightarrow X$$ be a coherent ideal sheaf over X with zero set Z. First assume that X is irreducible. If $${{\mathscr {J}}}=0$$ on X, then we define the Segre class $$s({{\mathscr {J}}},X)=s_0({{\mathscr {J}}},X)=\mathbf{1}_X\in {\mathscr {A}}_n(X)$$. Otherwise, let $$\pi :X'\!\rightarrow X$$ be a modification such that $$\pi ^*{{\mathscr {J}}}$$ is principalFootnote 4. For instance $$X'$$ can be the blow-up of X along $${{\mathscr {J}}}$$, or its normalization. Let D be the exceptional divisor, and let $$L_D$$ be the associated line bundle that has a section $${\sigma }^0$$ that defines D and hence generates $$\pi ^*{{\mathscr {J}}}$$. Then

it is a well-defined element in $${{\mathscr {A}}}_*(X)$$. If X has irreducible components $$X_1, X_2, \ldots$$, then $$s({{\mathscr {J}}},X)=s({{\mathscr {J}}},X_1)+s({{\mathscr {J}}},X_2)+\cdots$$. Notice that $$s({{\mathscr {J}}},X)$$ has support in Z so that it can be identified with an element $$s({{\mathscr {J}}},X)$$ in $${{\mathscr {A}}}_*(Z)$$. If $${{\mathscr {J}}}$$ is the sheaf associated with the subscheme V of X, then $$s({{\mathscr {J}}}, X)$$ coincides with the classical Segre class s(VX), cf. [12, Corollary 4.2.2].

We can define the $${{\mathscr {B}}}$$-Segre class $$S({{\mathscr {J}}},X)$$ in an analogous way by just interpreting $$\cap$$ as the ordinary wedge product. However, we are interested in more explicit representations and also in a definition of a $${{\mathscr {B}}}$$-Segre class on $$\mu \in {{\mathscr {B}}}(X)$$. To this end we assume that the ideal sheaf $${{\mathscr {J}}}\rightarrow X$$ is generated by a holomorphic section $${\sigma }$$ of a Hermitian vector bundle $$E\rightarrow X$$. If X is projective one can always find such a $${\sigma }$$ for any coherent ideal sheaf $${{\mathscr {J}}}\rightarrow X$$. We shall consider Monge–Ampère products on a generalized cycle $$\mu$$.

Theorem 2.3

Assume that $${\sigma }$$ is a holomorphic section of $$E\rightarrow X$$ and let $${{\mathscr {J}}}$$ be the associated coherent ideal sheaf with zero set Z. For each $$\mu \in {\mathscr {GZ}}(X)$$ the limits

exist and are generalized cycles with Zariski support on $$|\mu |$$. The generalized cycles

have Zariski support on $$Z\cap |\mu |$$. If $$\mu \sim 0$$, then . If g is a holomorphic section of another vector bundle that also defines $${{\mathscr {J}}}$$, then .

In case $$\mu =\mathbf{1}_X$$ we write $$M^{\sigma }_k$$ rather than $$M^{{\sigma }}_k\mathbf{1}_X$$. We let .

Definition 2.4

Assume that $${{\mathscr {J}}}\rightarrow X$$ is defined by the section $${\sigma }$$ of the Hermitian vector bundle $$E\rightarrow X$$. Given $$\mu \in {{\mathscr {B}}}(X)$$ and a representative $${\widehat{\mu }}\in {\mathscr {GZ}}(X)$$, we let the $${{\mathscr {B}}}$$-Segre class $$S_k({{\mathscr {J}}},\mu )$$ be the class in $${{\mathscr {B}}}(X)$$ defined by . We let $$S({{\mathscr {J}}},\mu )=S_0({{\mathscr {J}}},\mu )+S_1({{\mathscr {J}}},\mu )+\cdots$$.

Notice that has support in $$Z\cap |\mu |$$ so that we may identify $$S({{\mathscr {J}}},\mu )$$ with an element in $${{\mathscr {B}}}(Z\,{\cap }\, |\mu |)$$, in $${{\mathscr {B}}}(Z)$$, or in $${{\mathscr {B}}}(|\mu |)$$. If $$\mu =\mathbf{1}_X$$ we denote $$S({{\mathscr {J}}}, \mu )$$ by $$S({{\mathscr {J}}}, X)$$.

Remark 2.5

If , then

\begin{aligned} S({{\mathscr {J}}}, \mu )=S_\kappa ({{\mathscr {J}}},\mu )+S_{\kappa +1}({{\mathscr {J}}},\mu )+\cdots + S_{\dim \mu }({{\mathscr {J}}},\mu ). \end{aligned}

Indeed, $$S_\ell ({{\mathscr {J}}},\mu )$$ has dimension $$\text {dim}\,\mu -\ell$$ and Zariski support $$Z\cap |\mu |$$, so $$S_\ell ({{\mathscr {J}}},\mu )=0$$ if $$\text {dim}\, Z\cap \mu < \text {dim}\,\mu -\ell$$ by the dimension principle. Moreover, clearly $$S_\ell ({{\mathscr {J}}},\mu )=0$$ for degree reasons if $$\ell >\dim \mu$$.

If $${{\mathscr {J}}}$$ vanishes identically on $$|\mu |$$, then it follows from the definition that $$S({{\mathscr {J}}},\mu )=\mu$$.

One can define by a limit procedure without applying $$\mathbf{1}_Z$$, see [4, Proposition 5.7 and Remark 5.9].

Proposition 2.6

Let $${\sigma }$$ be a holomorphic section of a Hermitian bundle $$E\rightarrow X$$ and let

If $$\mu \in {\mathscr {GZ}}(X)$$, then

(2.12)

Moreover, is the value at $$\lambda =0$$, via analytic continuation from $$\mathrm{Re\, }\lambda \gg 0$$, of

Example 2.7

If $$\mu \in {\mathscr {GZ}}(X)$$ and , where $${{\mathscr {U}}}\subset X$$ is open and $$\gamma$$ is a smooth form in $${{\mathscr {U}}}$$, then by (2.12)

(2.13)

in $${{\mathscr {U}}}$$.

Example 2.8

If $$f:X'\! \rightarrow X$$ is proper, $$\mu '\!\in {\mathscr {GZ}}(X')$$, and $$\mu =f_*\mu '$$, then (2.1) and (2.12) imply that

(2.14)

Let $$\xi$$ be a section of a vector bundle in a neighborhood $${{\mathscr {U}}}\subset X$$ of x such that $$\xi$$ defines the maximal ideal at x. Notice that if $$\mu \in {\mathscr {GZ}}_k(X)$$, then by Theorem 2.3, is a generalized cycle with Zariski support at x and its image in $${{\mathscr {B}}}(X)$$ is independent of the choice of section $$\xi$$ defining the maximal ideal. In view of the dimension principle, see Sect. 2.3, for some real number a. We say that a is the multiplicity, $$\mathrm{mult}_x\mu$$, of $$\mu$$ at x, i.e.,

(2.15)

It is an integer that is independent of the choice of neighborhood $${{\mathscr {U}}}$$ and only depends on the class of $$\mu$$ in $${{\mathscr {B}}}(X)$$. If $$\mu$$ is effective (i.e., represented by a positive current), then $$\mathrm{mult}_x\mu$$ is the Lelong number of $$\mu$$ at x and hence nonnegative, see [4, Section 6].

Example 2.9

If $$\mu \in {\mathscr {GZ}}(X)$$ is of the form $$\mu =\gamma {\wedge }\mu '$$ in a neighborhood of x, where $$\gamma$$ is a closed smooth form of positive degree and $$\mu '\!\in {\mathscr {GZ}}(X)$$, then $$\mathrm{mult}_x\mu =0$$. In fact, by (2.13), which must vanish by the dimension principle, since has support at x and $$\gamma$$ has positive degree.

2.6 Segre numbers

Let $${{\mathscr {J}}}\rightarrow X$$ be a coherent ideal sheaf over X of codimension p. In [13, 17] Tworzewski, and Gaffney and Gassler, independently introduced, at each point $$x\in X$$, a list of numbers $$(e_p({{\mathscr {J}}},X,x),\ldots , e_n({{\mathscr {J}}},X,x))$$, called Segre numbers in [13]. The Segre numbers generalize the Hilbert–Samuel multiplicity at x in the sense that if $${{\mathscr {J}}}$$ has codimension n at x then $$e_n({{\mathscr {J}}},X,x)$$ is the Hilbert–Samuel multiplicity at x. The definitions in [13, 17], though slightly different, are both of geometric nature. There is also a purely algebraic definition, [1, 2]. In [6] were introduced semi-global currents whose Lelong numbers are precisely the Segre numbers. These currents are generalized cycles.

We can define Segre numbers for $${{\mathscr {J}}}$$ over a generalized cycle $$\mu \in {\mathscr {GZ}}(X)$$: In a neighborhood $${{\mathscr {U}}}$$ of a given point x we can take a section $${\sigma }$$ of a trivial Hermitian bundle such that $${\sigma }$$ generates $${{\mathscr {J}}}$$ and define the Segre numbers

where $$\kappa$$ is as in Remark 2.5. In view of Theorem 2.3, these numbers are independent of the choice of neighborhood $${{\mathscr {U}}}$$ and of section $${\sigma }$$, and only depend on the class of $$\mu$$ in $${{\mathscr {B}}}(X)$$. If $$\mu =\mathbf{1}_X$$, then $$e_k({{\mathscr {J}}},\mu ,x)$$ coincides with $$e_k({{\mathscr {J}}}, X, x)$$, see [6, Theorem 1.1].

2.7 Regular embeddings and Gysin mappings

Assume now that X is smooth and that $${{\mathscr {J}}}\rightarrow X$$ is locally a complete intersection of codimension $$\kappa$$. This means that $$\iota :Z_{{\mathscr {J}}}\hookrightarrow X$$ is a regular embedding, where $$Z_{{\mathscr {J}}}$$ is the non-reduced space of codimension $$\kappa$$ defined by $${{\mathscr {J}}}$$. Then the normal cone $$N_{{\mathscr {J}}}X$$ is a vector bundle over the reduced space $$i:Z\hookrightarrow X$$ and hence there is a well-defined cohomology class $$c(N_{{\mathscr {J}}}X)$$ on Z. Therefore there is a well-defined mapping, the classical Gysin mappingFootnote 5

\begin{aligned} \iota ^!:{{\mathscr {A}}}_k(X)\rightarrow {{\mathscr {A}}}_{k-\kappa }(Z),\quad i_*\iota ^!\mu = (c(N_{{\mathscr {J}}}X) \,{\cap }\, s({{\mathscr {J}}}, \mu ))_{k-\kappa }, \end{aligned}
(2.16)

where the lower index $$k-\kappa$$ denotes the component of dimension $$k-\kappa$$. We have the analogous $${{\mathscr {B}}}$$-Gysin mapping

\begin{aligned} \iota ^!:{{\mathscr {B}}}_k(X)\rightarrow {{\mathscr {B}}}_{k-\kappa }(Z),\quad i_*\iota ^!\mu = (c(N_{{\mathscr {J}}}X){\wedge }S({{\mathscr {J}}}, \mu ))_{k-\kappa }. \end{aligned}
(2.17)

Our main interest is when $${{\mathscr {J}}}$$ defines a submanifold; in this case $$Z=Z_{{\mathscr {J}}}$$ and $$i=\iota$$.

By suitable choices we can represent (2.17) by a mapping on $${\mathscr {GZ}}(X)$$: Assume that $${{\mathscr {J}}}$$ is defined by a section $${\sigma }$$ of a Hermitian vector bundle $$E\rightarrow X$$ and let $$E'$$ be the pull-back to Z. There is a canonical holomorphic embedding $$\varphi :N_{{\mathscr {J}}}X\rightarrow E'$$, see [4, Section 7]. Let us equip $$N_{{\mathscr {J}}}X$$ with the induced Hermitian metric and let $${\widehat{c}}(N_{{\mathscr {J}}}X)$$ be the associated Chern form, cf. Sect. 2.2. Then we have the concrete mapping

which induces the mapping (2.17). We recall [4, Propositions 1.4 and 1.5].

Proposition 2.10

If $${{\mathscr {J}}}\rightarrow X$$ defines a regular embedding, then

\begin{aligned} S({{\mathscr {J}}},X)=s(N_{{\mathscr {J}}}X){\wedge }[Z_{{\mathscr {J}}}], \quad S_k({{\mathscr {J}}},X)=s_{k-\kappa }(N_{{\mathscr {J}}}X){\wedge }[Z_{{\mathscr {J}}}] \end{aligned}

in $${{\mathscr {B}}}(X)$$, where $$[Z_{{\mathscr {J}}}]$$ is (the Lelong current of) the fundamental cycle associated to $${{\mathscr {J}}}$$. If $$\sigma$$ defines $${{\mathscr {J}}}$$, then

\begin{aligned} M^{\sigma }\!= {\widehat{s}}(N_{{\mathscr {J}}}X){\wedge }[Z_{{\mathscr {J}}}], \quad M_k^{\sigma }= \widehat{s}_{k-\kappa }(N_{{\mathscr {J}}}X){\wedge }[Z_{{\mathscr {J}}}] \end{aligned}

in $${\mathscr {GZ}}(X)$$.

Example 2.11

Let $$i:Z\rightarrow X$$ be the inclusion of a smooth submanifold of codimension $$\kappa$$ and suppose that $$\mu \in {\mathscr {GZ}}_k(X)$$ is a smooth form. Then, in view of Proposition 2.10,

Thus, $$i^!\mu =i^*\!\mu$$ is the usual pullback.

2.8 Intersection with divisors and the Poincaré–Lelong formula on a generalized cycle

See [4, Section 8] for proofs of the statements in this subsection. Let h be a meromorphic section of a line bundle $$L\rightarrow X$$. We say that $$\mathrm{div}\,h$$ intersects the generalized cycle $$\mu$$ properly if h is generically holomorphic and nonvanishing on the Zariski support of each irreducible component of $$\mu$$. If $$\mathrm{div}\,h$$ and $$\mu$$ intersect properly there is a generalized cycle with Zariski support on $$|\mathrm{div}\,h|\cap |\mu |$$ that we call the proper intersection of $$\mathrm{div}\,h$$ and $$\mu$$.

If $$\tau :W\rightarrow X$$ such that $$\mu =\tau _*\alpha$$, where $$\alpha$$ is a product of components of Chern or Segre forms, then Then if $$\mu \sim 0$$ so that the intersection has meaning for $$\mu \in {{\mathscr {B}}}(Y)$$. If h is holomorphic, i.e., $$\mathrm{div}\,h$$ is effective, then, in a local frame for L,

(2.18)

where is the norm of the holomorphic function obtained from any fixed local frame for L so that is well-defined. It follows that is effective if both $$\mathrm{div}\,h$$ and $$\mu$$ are effective. In light of (2.18) it is natural to write as $$[\mathrm{div}\, h]{\wedge }\mu$$.

Proposition 2.12

(The Poincaré–Lelong formula on a generalized cycle) Let h be a nontrivial meromorphic section of a Hermitian line bundle $$L\rightarrow X$$. Assume that $$\mathrm{div}\,h$$ intersects $$\mu$$ properly. Then

\begin{aligned} dd^c(\log |h|^2 \mu )=[\mathrm{div}\, h]{\wedge }\mu -{\widehat{c}}_1(L){\wedge }\mu . \end{aligned}

Remark 2.13

If $$\mathrm{div}\,h$$ does not intersect $$\mu$$ properly we define where $$\mu '_{j}$$ are the irreducible components of $$\mu$$ that $$\mathrm{div}\,h$$ intersects properly, see [4, Section 9].

2.9 Mappings into cohomology groups

In this subsection we assume that X is projective, in particular compact, cf. [4, Section 10]. Let $${\widehat{H}}^{k,k}(X)$$ be the equivalence classes of d-closed (kk)-currents $$\mu$$ on X of order zero such that $$\mu \sim 0$$ if there is a current $$\gamma$$ of order zero such that $$\mu =d\gamma$$. If X is smooth there is a natural isomorphism $${\widehat{H}}^{n-k,n-k}(X)\rightarrow H^{n-k,n-k}(X,{{\mathbb {C}}})$$; the surjectivity is clear and the injectivity follows since a closed current of order zero locally has a potential of order zero. If $$i:X\hookrightarrow M$$ is an embedding into a smooth manifold M of dimension N, then there is a natural mapping $$i_*:{\widehat{H}}^{n-k,n-k}(X)\rightarrow H^{N-k,N-k}(M,{{\mathbb {C}}})$$ induced by the push-forward of currents.

There are natural cycle class mappings

\begin{aligned} A_X:{{\mathscr {A}}}_k(X)\rightarrow {\widehat{H}}^{n-k,n-k}(X), \quad k=0,1, \ldots , \end{aligned}
(2.19)

and, [4, Equation (10.8)],

\begin{aligned} A_X (c(E)\,{\cap }\, \mu )=c(E){\wedge }A_X\mu , \end{aligned}

in $${\widehat{H}}(X)$$, where the right-hand side is represented by the wedge product of a smooth form and a current. There are natural mappings

\begin{aligned} B_X:{{\mathscr {B}}}_k(X)\rightarrow {\widehat{H}}^{n-k,n-k}(X), \quad k=0,1, \ldots , \end{aligned}
(2.20)

and clearly .

Example 2.14

Assume that h is a meromorphic section of a Hermitian line bundle $$L\rightarrow X$$ such that $$\mathrm{div}\,h$$ intersects $$\mu \in {\mathscr {GZ}}_k(X)$$ properly. It follows from Proposition 2.12 that $$[\mathrm{div}\,h]{\wedge }\mu$$ and $${\widehat{c}}_1(L){\wedge }\mu$$ coincide in $${\widehat{H}}^{n-k+1,n-k+1}(X)$$.

Let us recall [4, Proposition 1.6], that the images of $${{\mathscr {A}}}_k(X)$$ and $${{\mathscr {B}}}_k(X)$$ in $${\widehat{H}}^{n-k,n-k}(X)$$ coincide. We have the commutative diagram

Example 2.15

It follows from the dimension principle that $${{\mathscr {A}}}_n(X)={{\mathscr {Z}}}_n(X)={{\mathscr {B}}}_n(X)$$. If X has the irreducible components $$X_1, X_2, \ldots$$, then the image in $${\widehat{H}}^{0,0}(X)$$ of the cycle $$a_1X_1+a_2X_2+\cdots$$ on X is the d-closed (0, 0)-current $$a_1\mathbf{1}_{X_1}+a_2\mathbf{1}_{X_2}+\cdots$$. It follows that the mappings into $${\widehat{H}}^{0,0}(X)$$ are injective.

More generally, we have [4, Proposition 1.7].

Proposition 2.16

Assume that $${{\mathscr {J}}}\rightarrow X$$ defines a regular embedding $$Z_{{\mathscr {J}}}\hookrightarrow X$$ of codimension $$\kappa$$ and let $$\mu$$ be a cycle. The images in $${\widehat{H}}^{*,*}(Z)$$ of the Gysin and the $${{\mathscr {B}}}$$-Gysin mappings of $$\mu$$, (2.16) and (2.17), coincide.

3 Local intersection numbers

Let Y be a smooth manifold, let $$\mu _1, \ldots ,\mu _r$$ be generalized cycles on Y of pure dimensions and let $$d=\dim \mu _1+\cdots +\dim \mu _r$$. Following the ideas of Tworzewski [17] we define the local intersection numbers at x, cf. Lemma 2.1 and Sect. 2.6,

where is the parametrization $$x\mapsto (x,\ldots , x)$$ of the diagonal $${\Delta }$$ in $$Y^r$$ and $${{\mathscr {J}}}_\Delta \rightarrow Y^r$$ is the ideal sheaf that defines $${\Delta }$$. Notice that if is a Hermitian vector bundle and $${\sigma }$$ is a section of E that generates $${{\mathscr {J}}}_\Delta$$, then is a global generalized cycle such that

(3.1)

for $$\ell \hbox {\,\char 054\,}d$$. More invariantly we have, cf. Definition 2.4,

(3.2)

Given a point x, (3.1) holds as soon as $${\sigma }$$ defines $${{\mathscr {J}}}_\Delta$$ in a neighborhood of the point i(x) so we can assume that $${\sigma }$$ is a section of a trivial bundle. If the are cycles, therefore these numbers coincide with the local intersection numbers (1.1) introduced by Tworzewski in [17], cf. Sect. 2.6 and [6, Section 10].

Remark 3.1

Tworzewski, [17], proved that there is a unique global cycle $$\mu$$ such that the sum of its multiplicities, of its components of various dimensions, at each point $$x\in V$$ coincides with the sum of the local intersection numbers at x. Since this definition is local, it cannot carry global information. For instance, the self-intersection, in this sense, of any smooth curve Z in $${\mathbb {P}}^2$$ is just the curve itself, and therefore the Bézout formula, cf. (1.7), is not satisfied unless Z is a line.

4 The $$\pmb {{{\mathscr {B}}}}$$-Stückrad–Vogel class in $${\mathbb {P}}^M$$

Let $${\mathbb {P}}^M$$ be the projectivization of $${{\mathbb {C}}}_{x_0,\ldots ,x_M}^{M+1}$$. Let $$\eta =(\eta _1,\ldots ,\eta _m)$$ be a tuple of linear forms on $${{\mathbb {C}}}^{M+1}$$ in general position. As usual we identify the with sections of the line bundle $$L={\mathscr {O}}(1)\rightarrow {\mathbb {P}}^M$$ and $$\eta$$ with a section of . Similarly to Sect. 2.8 we let be the norm of the holomorphic tuple obtained from any fixed local frame for L so that is well-defined. Let Z be the plane of codimension m that $$\eta$$ defines and let $${{\mathscr {J}}}\rightarrow {\mathbb {P}}^M$$ be the associated radical ideal sheaf.

Let $$\mu$$ be a fixed generalized cycle in $${\mathbb {P}}^M$$ of pure dimension d. For a generic choice of $$a=(a_1,\ldots ,a_d)\in (\mathbb {P}^{m-1})^d$$, the successive intersectionsFootnote 6 by divisors, cf. Sect. 2.8, in

(4.1)

for $$k=0,\ldots ,d$$ are proper, and

(4.2)

is the resulting Stückrad–Vogel (SV) cycle, cf. [4, Section 9].

Proposition 4.1

If we take the mean value of (4.2) over $$(\mathbb P^{\,m-1})^d$$, with respect to normalized Haar measure, then we get the generalized cycle

Proof

With the convention in Remark 2.13 we can write

Now the proposition follows from [4, Proposition 9.3].$$\square$$

By [4, Proposition 9.5], the class of in $${{\mathscr {B}}}({\mathbb {P}}^M)$$ only depends on $${{\mathscr {J}}}$$, L, and $$\mu$$ and not on the choice of generators $$\eta$$.

Definition 4.2

For $$\mu \in {{\mathscr {B}}}({\mathbb {P}}^M)$$, we let $$V({{\mathscr {J}}},L,\mu )$$, the $${{\mathscr {B}}}$$-SV-class of L and $${{\mathscr {J}}}$$ on $$\mu$$, be the class of in $${{\mathscr {B}}}({\mathbb {P}}^M)$$.

Notice that has support in $$Z\cap |\mu |$$ so that we may identify $$V({{\mathscr {J}}},L,\mu )$$ with an element in $${{\mathscr {B}}}(Z\,{\cap }\, |\mu |)$$, cf. [4, Definition 9.6].

Let $${{\mathscr {U}}}\subset {\mathbb {P}}^M$$ be an open set where we have a local frame e for L. For instance, each nontrivial section of L vanishes on a hyperplane H and thus gives rise to a local frame in the open set . In $${{\mathscr {U}}}$$ we have that

(4.3)

with the metric on $$L|_{{\mathscr {U}}}$$ such that $$|e|=1$$, cf. [4, Remark 8.2]. It follows that local statements that hold for must hold for as well. In particular, if $$\eta$$ defines the maximal ideal at $$x\in {\mathbb {P}}^M$$, then, in view of (2.15),

(4.4)

By (2.12) and (4.3), in $${{\mathscr {U}}}$$ we have the regularization

(4.5)

In particular, is effective if $$\mu$$ is; indeed is a positive (1, 1)-form.

We have the Fubini–Study norm $$|\xi |=\Vert \xi \Vert /\Vert x\Vert$$ on $$L={\mathscr {O}}(1)$$, where denotes the Euclidean norm on $${{\mathbb {C}}}^{M+1}_x$$.

Proposition 4.3

With the norm above is the value at $$\lambda =0$$ of the current valued function

(4.6)

a priori defined when $$\mathrm{Re\, }\lambda \gg 0$$.

Proof

The statement follows directly from Proposition 2.6 in a set where we have a local frame for L if we replace each occurrence of $$|\eta |$$ in (4.6) by . However one can verify, cf. [3, Proof of Lemma 2.1], that the value at $$\lambda =0$$ is independent of the choice of norm on L, and thus the proposition follows.$$\square$$

Notice that the Fubini–Study form represents the first Chern class $$\omega =c_1(L)$$. We have van Gastel’s formulas for generalized cycles [4, Theorem 9.7],

(4.7)

and

(4.8)

From [4, Proposition 9.12] we get, cf. (1.3),

Proposition 4.4

Assume that $$\mu \in {\mathscr {GZ}}_d(X)$$. We have the mass formula

(4.9)

If $$m\hbox {\,\char 054\,}d$$, then the last term in (4.9) vanishes since outside Z.

For future reference we also point out the following invariance result. Assume that $$i:{\mathbb {P}}^M\!\rightarrow {\mathbb {P}}^{M'}$$ is a linear embedding of $${\mathbb {P}}^M$$ in $${\mathbb {P}}^{M'}$$. Let $$p:{\mathbb {P}}^{M'} \!\dashrightarrow {\mathbb {P}}^M$$ be a projective (generically defined) projection, i.e., induced by an affine projection $${{\mathbb {C}}}^{M'+1}\!\rightarrow {{\mathbb {C}}}^{M+1}$$, so that is the identity on $${\mathbb {P}}^M$$. Then $$p^*\eta _{j}$$ are well-defined linear forms on $${\mathbb {P}}^{M'}$$. Let $$\eta '$$ be some additional linear forms on $${\mathbb {P}}^{M'}$$ that vanish on $$i({\mathbb {P}}^{M})$$.

Proposition 4.5

If $$\mu \in {\mathscr {GZ}}({\mathbb {P}}^M)$$, then

Proof

Since $$\eta '=0$$ on the Zariski support of $$i_*\mu$$,

Now the proposition follows from (2.1) and Proposition 4.3, or (4.5), since $$\eta =i^*\!p^*\eta$$.$$\square$$

5 $$\varvec{{{\mathscr {B}}}}$$-Intersection products on manifolds

Assume that $$\mu _1, \ldots , \mu _r$$ are cycles on a complex manifold Y of dimension n as in the introduction. It is well-known that if they intersect properly, then, see, e.g., [9, Chapter 12], one can define the wedge product by means of appropriate regularizations, see, e.g., [10, Chapter III.3], and this current coincides with (the Lelong current of) the proper intersection cycle , see, e.g., [9, p. 212]. It is easy to see that the cycle and the diagonal $$\Delta$$ in intersect properly, and one can prove that if we identify $$\Delta$$ and Y, then the proper intersection coincides with . If the $$\mu _{j}$$ do not intersect properly the basic idea is to consider the intersection of $$\Delta$$ and , cf. Sect. 3. The advantage then is that one of the factors is a regular embedding.

We now recall the classical nonproper intersection product. If $$\iota :Z_{{\mathscr {J}}}\rightarrow Y$$ is a regular embedding of codimension $$\kappa$$ and $$\mu \in {{\mathscr {A}}}_k(Y)$$, then we have, cf. (2.16), the product

see, e.g., [12, Chapter 6.1] for background and motivation. Let

\begin{aligned} i:Y\hookrightarrow Y^r\!, \quad x\mapsto (x,\ldots , x), \end{aligned}
(5.1)

be the diagonal $$\Delta$$; notice that this is a regular embedding. Given arbitrary cycles $$\mu _1,\ldots , \mu _r$$, we define the intersection product

see, e.g., [12, Chapter 8.1]. After identification of Y and $$\Delta$$ we have . In case $$\mu _1=Z_{{\mathscr {J}}}$$ is a regular embedding and $$\mu _2$$ is an arbitrary cycle, then , see [12, Corollary 8.1.1].

We will define analogues for $${{\mathscr {B}}}(Y)$$, cf. Definition 2.4, Lemma 2.1, and (2.11).

Definition 5.1

Assume that $$\iota :Z_{{\mathscr {J}}}\rightarrow Y$$ is a regular embedding. For $$\mu \in {{\mathscr {B}}}(Y)$$ we define, cf. (2.17), the product

Notice that if $$Z_{{\mathscr {J}}}$$ has codimension $$\kappa$$ and $$\mu \in {{\mathscr {B}}}_k(Y)$$, then ; recall that Z is the zero set of $${{\mathscr {J}}}$$. Moreover, the Zariski support of is contained in and so we can identify with an element in $${{\mathscr {B}}}_{k-\kappa }(Z\,{\cap }\,|\mu |)$$.

Remark 5.2

If $${{\mathscr {J}}}$$ is the radical ideal of a submanifold or a reduced locally complete intersection $$i:Z\hookrightarrow Y$$ of codimension $$\kappa$$ and $$\mu$$ is a k-cycle in Y intersecting Z properly, then is the proper intersection . In fact, in view of Definition 2.4 and Proposition 2.10,

Thus, by (2.17),

Definition 5.3

If $$\mu _1,\ldots ,\mu _r$$ are elements in $${{\mathscr {B}}}(Y)$$, we define

As above, notice that after identification of Y and $$\Delta$$ we have .

Remark 5.4

Let $$p:Y^r\rightarrow Y$$ be the projection on one of the factors. Then , hence $$p_* i_*=\mathrm{id}$$ and thus .

Assume that $$\mu _1$$ is a regular embedding. Contrary to the classical intersection product case it is not true in general that and coincide. Example 8.14 below shows that the $${{\mathscr {B}}}$$-self-intersection of the cusp $$\mu =\{x_1^3-x_0x_2^2=0\}\subset {\mathbb {P}}^2$$ is different from . This example also shows that the $${{\mathscr {B}}}$$-analogue of the classical self-intersection formula does not hold in general. However, it is true for smooth cycles.

Proposition 5.5

(Self-intersection formula) Let $$V\hookrightarrow Y$$ be a smooth subvariety of Y of codimension m. Then

(5.2)

Proof

Notice that the diagonal $$\Delta _Y$$ is smooth in and that . If is the product embedding, then $$j^*{{\mathscr {J}}}_{\Delta _Y}={{\mathscr {J}}}_{\Delta _{V}}$$. Therefore is the component of dimension $$n-2m$$ of

where the last equality follows from Proposition 2.10 and, since V is smooth, that . Via the natural isomorphisms $$Y\simeq {\Delta _Y}$$ and $$V\simeq \Delta _V$$ thus is the component of dimension $$n-2m$$ of

\begin{aligned} c(TY)|_V{\wedge }s(TV){\wedge }[V]&=c(TY)|_V{\wedge }\frac{1}{c(TV)}{\wedge }[V]\\&= c(TY/TV)|_V{\wedge }[V]= c(N_V Y){\wedge }[V], \end{aligned}

cf. (2.4). Thus we get (5.2).$$\square$$

Example 5.6

Let E be the exceptional divisor of the blow-up $$Y=\mathrm{Bl}_a{\mathbb {P}}^2\rightarrow {\mathbb {P}}^2$$ at a point $$a\in {\mathbb {P}}^2$$. Let $$L_E\rightarrow Y$$ be the line bundle with a section that defines E. It follows from (5.2) that . Since $$-c_1(L_E)$$ is positive is negative, which is expected in view of the classical self-intersection of E.

We have always coincidence of the various intersection products on cohomology level; recall the mappings (2.19) and (2.20).

Proposition 5.7

Assume that $$\mu _1, \ldots , \mu _r$$ are cycles in Y and let $$V=|\mu _1|\cap \cdots \cap |\mu _r|$$. Then

(5.3)

in $${\widehat{H}}(V)$$. Moreover, if $$r=2$$ and $$\mu _1$$ is a regular embedding, then

(5.4)

Proof

The equality (5.3) follows directly from the definitions and Proposition 2.16. Since the two possible definitions of coincide when $$\mu _1$$ is a regular embedding, (5.4) follows by another application of Proposition 2.16.$$\square$$

Proposition 5.8

1. (i)

If $$\mu _1, \ldots , \mu _r$$ are cycles in Y that intersect properly, then

(5.5)
2. (ii)

If h is a holomorphic section of $$L\rightarrow Y$$ such that $$\mathrm{div}\,h$$ intersects $$\mu \in {{\mathscr {B}}}(Y)$$ properly, then

(5.6)

Proof

Assume that the have dimensions , respectively. The assumption about proper intersection means that the set-theoretic intersection $$V=|\mu _1|\cap \cdots \cap |\mu _r|$$ has the expected dimension and that and are elements in $${{\mathscr {A}}}_k(V)$$ and $${{\mathscr {B}}}_k(V)$$, respectively. Now (5.5) follows from (5.3) and Example 2.15.

Let us now consider part (ii). We may assume that $$\mu =\tau _*\alpha$$, where $$\tau :W\rightarrow Y$$ is proper holomorphic and $$\alpha$$ is a product of components of Chern or Segre forms, cf. (2.6). The assumption of proper intersection implies that h is not identically zero on $$|\mu |=\tau (W)$$ so that . Let $$\iota$$ be the regular embedding given by the ideal sheaf $${{\mathscr {J}}}_h$$ generated by h. We have $$N_{{{\mathscr {J}}}_h}Y=L|_{h=0}$$, cf. Sect. 2.7. Thus

for the last equality, cf. [4, Equation (8.4)].

We now consider the last equality in (5.6). Consider the commutative diagram

(5.7)

where p is the projection on the first factor. By definition, cf. Remark 5.4, is $$p_*$$ of

(5.8)

Recall that if $${\sigma }$$ is a section that defines . Now so if we have, cf. (2.14) and (2.13),

Notice that g defines the graph G of $$\tau$$ in . Since $$\mathrm{div}\,h$$ and $$\mu$$ intersect properly, $$\tau ^*h$$ is generically nonvanishing on W and so is generically nonvanishing on G. Thus, G and intersect properly. The Zariski support of is , which thus has dimension $$\dim W-1$$. Since has dimension $$\dim W +n-\ell -1$$ it follows from the dimension principle that for $$\ell <n$$. Thus, for $$\ell <n$$ and from (5.8) we get

(5.9)

To compute , notice that g defines a regular embedding in of codimension n and that, since , the restriction of g to defines a regular embedding in of codimension n. Thus, by [4, Corollary 7.5],

(5.10)

where $${{\mathscr {J}}}_g$$ is the ideal sheaf generated by g. Since (5.7) is commutative, (5.9) and (5.10) give

(5.11)

cf. (2.18). Since , by (5.11) we get, cf. (2.1) and (2.18),

which finishes the proof. $$\square$$

6 The $$\bullet$$-product on $$\pmb {\mathbb {P}}^{\,n}$$

In this section we define the product (1.4) of generalized cycles on $${\mathbb {P}}^{\,n}$$ and prove Theorem 1.1. The first step is to define the join of two generalized cycles. For simplicity we first assume that $$r=2$$. The mapping

(6.1)

is well-defined outside the union of the two disjoint n-dimensional planes $$x=0$$ and $$y=0$$, and it has surjective differential. If $$\mu _1,\mu _2\in {\mathscr {GZ}}({\mathbb {P}}^{\,n})$$, therefore is a well-defined current outside the indeterminacy set of $${{\mathfrak {p}}}$$. We will see that extends in a natural way to a generalized cycle on $${\mathbb {P}}^{2n+1}_{x,y}$$.

Let $$\pi :\mathrm{Bl}\,{\mathbb {P}}^{2n+1}_{x,y}\!\rightarrow \mathbb P^{2n+1}_{x,y}$$ be the blow-up of $${\mathbb {P}}^{2n+1}_{x,y}$$ along $$\{x=0\}$$ and $$\{y=0\}$$. Then we have

(6.2)

where has surjective differential and hence is smooth, i.e., maps smooth forms onto smooth forms.

Lemma 6.1

1. (i)

If , then $$p^*\!\mu \in {\mathscr {GZ}}(Y)$$.

2. (ii)

$$\pi _*p^*\!\mu$$ is in $${\mathscr {GZ}}({\mathbb {P}}^{2n+1})$$ and coincides with $${{\mathfrak {p}}}^*\mu$$ where it is defined.

3. (iii)

If $$\mu =0$$ in , then $$\pi _*p^*\!\mu =0$$ in $${{\mathscr {B}}}({\mathbb {P}}^{2n+1})$$.

Proof

Note that (ii) is a direct consequence of (i).

Let and $$X'\!=\mathrm{Bl}\,{\mathbb {P}}^{2n+1}_{x,y}$$. We may assume that $$\mu =\tau _*\alpha$$, where $$\tau :W\rightarrow X$$ is proper and $$\alpha$$ is a product of components of Chern forms. Consider the fibre square

(6.3)

Since p is smooth it follows that the fibre product is smooth, cf. (6.5) below. The pullback $${\widetilde{\pi }}{}^*\alpha$$ is a product of Chern forms on $$W'$$ and thus $$\rho _*{\widetilde{\pi }}{}^*\alpha$$ is a generalized cycle on $$X'$$. We claim that

\begin{aligned} \rho _*{\widetilde{\pi }}{}^*\gamma =p^* \tau _*\gamma \end{aligned}
(6.4)

for any smooth form $$\gamma$$. Taking (6.4) for granted we conclude that $$p^*\!\mu =p^* \tau _*\alpha$$ is a generalized cycle, which proves (i). It is enough to prove (6.4) for all smooth forms $$\gamma$$ with small support. Notice that locally in X, say in a small open set $${{\mathscr {U}}}$$, $$X'|_{{\mathscr {U}}}$$ is biholomorphic to . Let us assume that $$\tau _*\gamma$$ has support in an open set $${{\mathscr {U}}}\subset X$$, where . Letting $${{\widetilde{W}}}=\tau ^{-1}({{\mathscr {U}}})$$, by the definition of fiber product,

(6.5)

and $$\rho (w,t)=(\tau (w),t)$$. Now (6.4) is obvious.

To see (iii), note that if $$\mu =\tau _*(\beta {\wedge }\alpha )$$, where $$\beta$$ is a component of a B-form, then it follows from (6.4) that and hence 0 in $${{\mathscr {B}}}({\mathbb {P}}^{2n+1})$$ since $${\widetilde{\pi }}^*\beta$$ is a component of a B-form.$$\square$$

If $$\mu _1,\mu _2\in {\mathscr {GZ}}({\mathbb {P}}^{\,n})$$, then by Lemma 2.1, and by virtue of Lemma 6.1 we can make the following definition.

Definition 6.2

For $$\mu _1,\mu _2\in {\mathscr {GZ}}({\mathbb {P}}^{\,n})$$ we define the join product by

It follows from the same lemmas that and, moreover, that if $$\mu _1$$ or $$\mu _2$$ is 0 in $${{\mathscr {B}}}({\mathbb {P}}^{\,n})$$. Hence, is well-defined for $$\mu _{j}\in {{\mathscr {B}}}({\mathbb {P}}^{\,n})$$.

Example 6.3

(Relation to the classical join) Assume that $$X_1,X_2\subset {\mathbb {P}}^{\,n}$$ are (irreducible) analytic sets. Let and be the natural maps. Notice that is homogeneous in $${{\mathbb {C}}}^{2n+2}$$ and $${\widetilde{\pi }}({{\widetilde{X}}})$$ is the classical join of $$X_1$$ and $$X_2$$. We claim that

(6.6)

Since on the common set of definition it follows that (6.6) holds outside the union $$V\subset {\mathbb {P}}^{2n+1}$$ of planes where $${\mathfrak {p}}$$ is not defined. To prove (6.6) it is thus enough to show that vanishes. In view of (2.2), if , which may be checked locally in $$\mathrm{Bl}\,\mathbb P^{2n+1}$$. We may therefore consider a subset of $$\mathrm{Bl}\,\mathbb P^{2n+1}$$, where is open, cf. the proof of Lemma 6.1. Note that, in , $$\pi ^{-1}V$$ is of the form and that . Thus, by the dimension principle, .

Example 6.4

Let $$\mu _1,\mu _2\in {{\mathscr {B}}}({\mathbb {P}}^{\,n})$$ and assume that $$\Lambda :{\mathbb {P}}^{\,n}\!\rightarrow {\mathbb {P}}^{\,n'}$$ is a linear embedding, i.e., $$\Lambda$$ is induced by an injective linear map $${\widetilde{\Lambda }}:{{\mathbb {C}}}^{n+1}\!\rightarrow {{\mathbb {C}}}^{n'+1}$$. Then is an injective linear map $${{\mathbb {C}}}^{2n+2}\!\rightarrow {{\mathbb {C}}}^{2n'+2}$$ and we get a linear embedding $${\varvec{\Lambda }} :\mathbb P^{2n+1}\!\rightarrow {\mathbb {P}}^{2n'+1}$$. Let $$\pi '$$ and $$p'$$ be defined in the same way as $$\pi$$ and p in (6.2) with n replaced by $$n'$$. Similarly to the proof of Lemma 6.1 one shows that as operations on currents in . It follows that

In a similar way as above we have the mapping

(6.7)

Let now $$\pi :\mathrm{Bl}\,{\mathbb {P}}^{\,r(n+1)-1}_{x^1\!,\ldots , x^r}\!\rightarrow {\mathbb {P}}^{\,r(n+1)-1}_{x^1\!,\ldots , x^r}$$ be the blow-up of $${\mathbb {P}}^{\,r(n+1)-1}_{x^1,\ldots , x^r}$$ along the codimension n-planes $$\{x^1\!=0\}, \ldots , \{x^r\!=0\}$$ and set . We get a diagram analogous to (6.2). As above, given $$\mu _1,\ldots , \mu _r$$ in $${\mathscr {GZ}}({\mathbb {P}}^{\,n})$$ or in $${{\mathscr {B}}}({\mathbb {P}}^{\,n})$$, we define in $${\mathscr {GZ}}({\mathbb {P}}^{\,r(n+1)-1})$$ or in $${{\mathscr {B}}}({\mathbb {P}}^{\,r(n+1)-1})$$, respectively, as .

Proposition 6.5

If $$\mu _1,\ldots , \mu _r\in {\mathscr {GZ}}({\mathbb {P}}^{\,n})$$, then

Proof

We may assume that the have pure dimension. There are currents in $${\mathbb {P}}^{\,n}$$ such that if , where $${\widehat{\omega }}$$ is the Fubini–Study form on $${\mathbb {P}}^{\,n}$$. It follows that there is a current A on such that

cf. Lemma 2.1. Applying $$\pi _*p^*$$, it is enough to show that ; but this is obvious if we just notice that $$\pi _*p^*$$ of a hyperplane in induced by a hyperplane in one of the factors $${\mathbb {P}}^{\,n}_{x^j}$$ is a hyperplane in $${\mathbb {P}}^{\,r(n+1)-1}_{x^1,\ldots , x^r}$$ and replace each by the intersection of generic hyperplanes.$$\square$$

For the last argument one can also observe that is a well-defined locally integrable function on $${\mathbb {P}}^{\,r(n+1)-1}_{x^1\!,\dots ,x^r}$$ and that

Let

\begin{aligned} j:{\mathbb {P}}^{\,n} \hookrightarrow {\mathbb {P}}^{\,r(n+1)-1}\!, \quad [x]\mapsto [x,\ldots ,x], \end{aligned}
(6.8)

be the parametrization of the join diagonal $$\Delta _J$$ in $$\mathbb P^{\,r(n+1)-1}$$ and let $${{\mathscr {J}}}_J$$ be the associated sheaf. Notice that $${{\mathscr {J}}}_J$$ is generated by the $$(r-1)(n+1)$$ linear forms, i.e., sections of $$L={\mathscr {O}}(1)$$,

\begin{aligned} \eta =\bigl (x_0^2-x_0^1,x_0^3-x_0^2,\ldots ,x_0^r-x_0^{r-1}, \ldots , x_n^2-x_n^1,x_n^3-x_n^2,\ldots ,x_n^r-x_n^{r-1}\bigr ).\qquad \quad \end{aligned}
(6.9)

Since

\begin{aligned} \mathrm{codim\,}\Delta _J=r(n+1)-1-n=(r-1)(n+1), \end{aligned}

we see that $$\eta$$ is a minimal generating set.

Definition 6.6

Given $$\mu _1,\ldots , \mu _r\in {{\mathscr {B}}}({\mathbb {P}}^{\,n})$$, $$\mu _1\bullet \cdots \bullet \mu _r$$ is the unique class in $${{\mathscr {B}}}({\mathbb {P}}^{\,n})$$ such that

(6.10)

Since (2.11) is injective, is well-defined. It is clear that is commutative, multilinear, and that its Zariski support is contained in $$|\mu _1|\cap \cdots \cap |\mu _r|$$.

If $$\mu _1,\ldots , \mu _r\in {\mathscr {GZ}}({\mathbb {P}}^{\,n})$$ denote representatives of the corresponding classes in $${{\mathscr {B}}}(\mathbb P^{\,n})$$, then the right-hand side of (6.10) is represented by

(6.11)

for any choice of $$\eta$$ generating $${{\mathscr {J}}}_J$$. If the $$\mu _{j}$$ have pure dimensions, then

(6.12)

and thus is represented by .

The $$\bullet$$-product is invariant in the following sense.

Proposition 6.7

Assume that $$\mu _{j}\in {{\mathscr {B}}}({\mathbb {P}}^{\,n})$$ and let $$\Lambda :{\mathbb {P}}^{\,n}\hookrightarrow {\mathbb {P}}^{\,n'}$$ be a linear embedding. Then .

In particular, if T is a linear automorphism of $${\mathbb {P}}^{\,n}$$, then

(6.13)

Proof

As in Example 6.4, $$\Lambda$$ induces a linear embedding $${\varvec{\Lambda }}:{\mathbb {P}}^{\,r(n+1)-1}\!\rightarrow \mathbb P^{\,r(n'+1)-1}$$ and , where j denotes the join diagonal in both $${\mathbb {P}}^{\,r(n+1)-1}$$ and $$\mathbb P^{\,r(n'+1)-1}$$. Therefore, since $$j_*$$ is injective, to show the proposition it is enough to check that , i.e., that

(6.14)

In the special case that $$\Lambda$$ is a linear automorphism of $${\mathbb {P}}^{\,n}$$, (6.14) follows by noticing that $${\varvec{\Lambda }}^*$$ in this case maps sections of L to sections of L, preserves $${{\mathscr {J}}}_J$$, and, in view of a simple extension of Example 6.4, that .

For the general case we may now assume that $$\Lambda :\mathbb P^{\,n}_x\rightarrow {\mathbb {P}}^{\,n'}_{x,y}$$ is the map $$[x]\mapsto [x\,{:}\,0]$$. Then $${\varvec{\Lambda }}[x^1\,{:}\,\ldots \,{:}\,x^r]=[x^1\,{:}\,0\,{:}\,\ldots \,{:}\,x^r\,{:}\,0]$$. Let $$\eta$$ be as in (6.9) and let $$\eta '$$ be the tuple of $$(r-1)(n'-n)$$ linear forms $$(y^{j+1}_k\!-y^j_k)$$, $$j=1,\ldots ,r-1$$, $$k=1,\ldots ,n'-n$$. Then $$\eta$$ and $$(\eta ,\eta ')$$ define $${{\mathscr {J}}}_J$$ in $${\mathbb {P}}^{\,r(n+1)-1}$$ and $${\mathbb {P}}^{\,r(n'+1)-1}$$, respectively. By Proposition 4.5 we get

which implies (6.14) in view of Example 6.4.$$\square$$

Proposition 6.8

If $$\mu _1, \ldots ,\mu _r\in {{\mathscr {B}}}({\mathbb {P}}^{\,n})$$ have pure dimensions, then

(6.15)

where d is given by (6.12).

Proof

First notice that $$j^*{\widehat{\omega }}_{\mathbb P^{\,r(n+1)-1}}={\widehat{\omega }}_{{\mathbb {P}}^{\,n}}$$, where j is defined in (6.8) and $${\widehat{\omega }}_{{\mathbb {P}}^M}$$ denote the Fubini–Study form on $${\mathbb {P}}^M$$. Therefore, for $$\mu \in {\mathscr {GZ}}_k({\mathbb {P}}^{\,n})$$,

In particular, . Now, by Proposition 4.4,

and thus (6.15) follows in view of Proposition 6.5.$$\square$$

The Bézout formula (1.7) holds if and only if the last term in (6.15) vanishes. This happens if $$(r+1)(n-1)\hbox {\,\char 054\,}d$$ which is the same as (1.6), cf. the remark after Proposition 4.4, (6.9), and (6.12).

However, as mentioned in the introduction, the condition (1.6) is not necessary for (1.7) to hold. For instance, by Proposition 6.7, the $$\bullet$$-product is not affected if we perform the multiplication in a larger $$\mathbb P^{\,n'}$$. Thus, as mentioned already in the introduction, the self-intersection of a k-plane is the k-plane itself, in particular, the self-intersection of a point is the point itself. On the other hand, clearly the product of two distinct points vanishes. In this case the last term in (6.15) carries the “missing mass” in the Bézout formula.

We are now in position to prove Theorem 1.1.

Proof of Theorem 1.1

The first statements, about multlilinearity, commutativity and the support, are already discussed after Definition 6.6.

Since local intersections numbers (multiplicities) are locally defined we can work in an affinization and use the results from [6, Sections 9 and 10] to prove (1.5). However, we omit the details since it is also a direct consequence of the global Proposition 7.1 below, cf. (3.2) and (7.1).

In the discussion after the proof of Proposition 6.8 is noticed that (1.7) holds if (1.6) is fulfilled. If are effective, then so is , and it follows that (6.11), and hence , are effective, cf. (4.5). Moreover are positive and the last term in (6.15) is nonpositive so we get (1.8).

If $$\mu _1,\ldots , \mu _r$$ are cycles that intersect properly, by the dimension principle only the component of of dimension $$\rho$$ is nonzero, where $$\rho$$ is as in (1.6), and this is a cycle. In this case the local intersections numbers $$\epsilon _\ell (\mu _1, \ldots , \mu _r,x)$$ coincide with the multiplicites of the proper intersection cycle , cf. [6, Example 10.2], and thus (1.9) follows. $$\square$$

We will now look at more explicit representations of the $$\bullet$$-product. Recall that we have a natural Hermitian metric on $${\mathscr {O}}(1)$$, cf. Sect. 4, and thus, cf. (6.9),

\begin{aligned} |\eta |^2=\sum _{i=1}^{r-1} \sum _{k=0}^n\,|x_k^{i+1}\!-x_k^i|^2\!. \end{aligned}

From (4.6) we see that if $$\mu _i$$ have pure dimension, then is given by the value at $$\lambda =0$$ of

where Notice that

so that term corresponding to $$k=0$$ in (4.6) is irrelevant here; indeed and so $$\ell \hbox {\,\char 054\,}\sum \dim \mu _{j}$$.

In an affinization we can also obtain the $$\bullet$$-product, cf. (4.5), as a limit of smooth forms times by the formula

When computing it can be convenient to compute the SV-cycle for generic hyperplanes , $$a_{j}\in {\mathbb {P}}^{\,n}$$, and then form the mean value, cf. Sect. 4. See Sect. 8 for examples.

Remark 6.9

Assume that $$r=2$$. Given the standard coordinates on $${{\mathbb {C}}}^{n+1}$$ there is a canonical choice of $$\eta$$ defining $$\Delta _J$$, namely , $$j=0,\ldots ,n$$, cf. (6.9). Thus, given representatives of , there are canonical representatives (6.11) of , and since (2.8) is injective we can define the $$\bullet$$-product on the level of generalized cycles. Indeed, given $$\mu _1,\mu _2\in {\mathscr {GZ}}({\mathbb {P}}^{\,n})$$, we define as the unique current in $${\mathscr {GZ}}({\mathbb {P}}^{\,n})$$ such that

Let T be a linear automorphism of $${\mathbb {P}}^{\,n}$$ induced by a unitary mapping $${{\widetilde{T}}}$$ on $${{\mathbb {C}}}^{n+1}$$, let , and let $${\mathbf {T}}$$ be the induced linear automorphism of $${\mathbb {P}}^{2n+1}$$; cf. Example 6.4 and the proof of Proposition 6.7. Then, considering $$\eta$$ as a tuple of linear forms on $${{\mathbb {C}}}^{2n+2}$$, $$|\widetilde{{\mathbf {T}}}^*\eta |^2_{{{\mathbb {C}}}^{2n+2}}=|\eta |^2_{{{\mathbb {C}}}^{2n+2}}$$. Moreover, $$dd^c\log |\eta |^2_{{{\mathbb {C}}}^{2n+2}} = dd^c\log |\eta |^2_{\circ }$$, where we on the right-hand side consider $$\eta$$ as a tuple of sections of $$L\rightarrow {\mathbb {P}}^{2n+1}$$. Hence, $$dd^c\log |{\mathbf {T}}^*\eta |^2_{\circ } = dd^c\log |\eta |^2_{\circ }$$, and so

It follows that as generalized cycles.

Remark 6.10

Consider (6.7) and the corresponding diagram (6.2). By abuse of notation, let $$\Delta _J$$ denote the preimage under $$\pi$$ of the join diagonal, let $${{\mathscr {J}}}_J$$ denote the sheaf in $$\mathrm{Bl}\,{\mathbb {P}}^{\,r(n+1)-1}$$ corresponding to $$\Delta _J$$, and let j denote the embedding of $${\mathbb {P}}^{\,n}$$ in $$\mathrm{Bl}\,{\mathbb {P}}^{\,r(n+1)-1}$$ as $$\Delta _J$$ induced by (6.8). Since (6.11) has support on $$\Delta _J$$ and $$\mathrm{Bl}\,{\mathbb {P}}^{\,r(n+1)-1}$$ and $${\mathbb {P}}^{\,r(n+1)-1}$$ coincide in a neighborhood of $$\Delta _J$$ we can alternatively think of (6.11) as a generalized cycle on Y.

Remark 6.11

(Green currents and the $$*$$-product) Recall that a $$(p-1,p-1)$$-current g is a Green current of a closed subvariety Z of codimension p of a complex manifold Y if $$dd^c g+[Z]=\omega$$, where $$\omega$$ is a smooth form. If g is locally integrable and smooth outside Z it is called a Green form. The calculus of Green forms, based on the $$*$$-product, is an important tool in the study of height in arithmetic intersection theory, see, e.g., [8, 15]. In the case $$p=1$$, if s is a section of a Hermitian line bundle that defines Z, then $$g=-\log |s|^2$$ is a Green form in virtue of the Poincaré–Lelong formula, cf., e.g., Proposition 2.12. The existence of Green forms of so-called logarithmic type for $$p>1$$ is a more delicate matter, see [8]. If g and $$g'$$ are Green forms of logarithmic type of Z and $$Z'$$, respectively, then one can form the product

If Z and $$Z'$$ intersect properly, then is a Green current for the proper intersection . In general, is the Green current of a kind of product $$\mu$$ of Z and $$Z'$$. However $$\mu$$ it is not comparable to our product (assuming $$Y=\mathbb P^{\,n}$$) since for degree reasons, $$\mu$$ has pure dimension $$\dim Z+\dim Z'\!-n$$. Also compare [4, Remark 5.10].

7 Relation to the $$\cdot _{\pmb {{{\mathscr {B}}}}(\pmb {\mathbb {P}}^{\,n})}$$ product

In this section we prove Theorem 1.2. For simplicity let us restrict from now on to the case $$r=2$$; the general case is handled in a similar way.

Consider the mapping

where i is given by (5.1). Notice that is the component of dimension $$\rho$$ of , where $$\rho$$ is given by (1.6), i.e., $$\rho =\dim \mu _1+\dim \mu _2-n$$.

Next, consider the mapping

where we are using the notation from Sect. 6 and where j is given by (6.8).

Proposition 7.1

The mappings $$i^{!!}$$ and $$j^\flat$$ coincide.

Let $$\eta$$ be the section (6.9) of $$L={\mathscr {O}}(1)$$ equipped with the Fubini–Study metric, and let $${\widehat{\omega }}$$ be the first Chern form. Then $${\widehat{c}}(N_{{{\mathscr {J}}}_J} \mathbb P^{2n+1})=(1+{\widehat{\omega }})^{n+1}$$ and thus, by (4.8), $$j^\flat$$ is represented by

Now assume that and let $$d=\dim \pi _* p^* \!\mu = \dim \mu _1+\dim \mu _2 +1$$, cf. (6.12). Note that $$\rho =d-(n+1)$$. It follows that

By Definition 6.6, is represented by and therefore

(7.1)

and thus Theorem 1.2 follows from Proposition 7.1.

Remark 7.2

There are classical mappings analogous to $$i^!$$ and $$j^\flat$$. If $$\mu _1$$ and $$\mu _2$$ are cycles and , then, see [12, Example 8.4.5], the analogue of Proposition 7.1 holds for the component of dimension $$\rho$$, which is the component of main interest also for us. However, the argument given in [12] cannot be transferred to the $${{\mathscr {B}}}$$-setting.

Proof of Proposition 7.1

Let $$\mathrm{Bl}\,{\mathbb {P}}^{2n+1}_{x,y}$$ be as in Sect. 6. Since $$\mathrm{Bl}\,{\mathbb {P}}^{2n+1}_{x,y}$$ coincides with $${\mathbb {P}}^{2n+1}$$ in a neighborhood of $$\Delta _J$$, the restrictions of $$c(N_{{{\mathscr {J}}}_J}{\mathrm{Bl}\,{\mathbb {P}}^{2n+1}_{x,y}})$$ and $$c(N_{{{\mathscr {J}}}_J}{{\mathbb {P}}^{2n+1}})$$ to $$\Delta _J$$ coincide, and moreover, $$\pi _* p^*\!\mu$$ and $$p^*\!\mu$$ coincide on $$\Delta _J$$, cf. Remark 6.10. Therefore $$j^\flat$$ coincides with the mapping

(7.2)

where we are identifying $$\Delta _J\subset \mathrm{Bl}\,\mathbb P^{2n+1}_{x,y}$$ with $${\mathbb {P}}^{\,n}$$. Hence it suffices to prove that $$i^!$$ coincides with (7.2).

Let $$M={\mathbb {P}}^{\,n}$$ so that $$\Delta =i(M)$$ and $$\Delta _J=j(M)$$ and let and $$Y=\mathrm{Bl}\,{\mathbb {P}}^{2n+1}_{x,y}$$. Then

commutes. Note that j(M) is a divisor in $$p^{-1}i(M)$$. Let $$E\rightarrow Y$$ and $$F\rightarrow X$$ be Hermitian vector bundles with holomorphic sections $$\phi$$ and $${\sigma }$$ that define $${{\mathscr {J}}}_{j(M)}$$ and $${{\mathscr {J}}}_{i(M)}$$, respectively. Fix Hermitian metrics on $$N_{j(M)}Y$$ and $$N_{i(M)}X$$ and let $${\widehat{c}}(N_{j(M)}Y)$$ and $${\widehat{c}}(N_{i(M)}X)$$ be the associated Chern forms. Moreover, let denote also a fixed representative of . $$\square$$

Lemma 7.3

Let $${{\mathscr {L}}}\rightarrow p^{-1} i(M)$$ be the line bundle associated with the divisor $$j(M)\subset p^{-1} i(M)$$. Then

(7.3)

and for any Hermitian metric on $${{\mathscr {L}}}$$,

(7.4)

Taking this lemma for granted we can conclude the proof of Proposition 7.1. We have to prove that if $$\mu _1$$ and $$\mu _2$$ are the unique elements in $${\mathscr {GZ}}(M)$$ such that

and

then $$\mu _1\sim \mu _2$$ in $${\mathscr {GZ}}(M)$$.

In view of (7.3) and (2.10) we have

in $${\mathscr {GZ}}(Y)$$. Therefore, cf. (2.5),

(7.5)

From (7.4) and (7.5) we get

which means that $$p_*j_*\mu _2\sim i_*\mu _1$$ on X. Since $$p_*j_*=i_*$$ and (2.11) is injective, we conclude that $$\mu _1\sim \mu _2$$ on M. Thus Proposition 7.1 is proved.$$\square$$

Proof of Lemma 7.3

Let us use the notation $$N_{\sigma }X$$ for $$N_{i(M)}X$$ etc. We first consider (7.3). Notice that, with the notation from [4, Section 7], for any columns of minimal sets of generators $$s,s'$$ of $${{\mathscr {J}}}_{i(M)}={{\mathscr {J}}}_{\sigma }$$ at points on $$iM\subset X$$ there is an invertible matrix g such that $$s'=gs$$. A section $$\xi$$ of the normal bundle $$N_{\sigma }X$$ can be defined as a set of holomorphic tuples $$\xi (s)$$ such that $$g\xi (s)=\xi (gs)$$ in i(M), i.e, the restriction to i(M) of such matrices are transition matrices for $$N_{\sigma }X$$. Let t and $$t'$$ be holomorphic functions in a neighborhood of a point on $$p^{-1}i(M)$$ such that both $$t|_{p^{-1}i(M)}$$ and $$t'|_{p^{-1}i(M)}$$ generate the sheaf associated with the divisor j(M) in $$p^{-1}i(M)$$. Then $$t'\!=ht$$ for a holomorphic function h, which is nonvanishing on $$p^{-1}i(M)$$, and $$h|_{p^{-1}i(M)}$$ is a transition function for $${\mathscr {L}}$$. Moreover, $$(p^*s,t)$$ and $$(p^*s'\!,t')$$ are minimal sets of generators for $${{\mathscr {J}}}_{j(M)}={{\mathscr {J}}}_\phi$$. It follows that for given such minimal sets of generators at a point on j(M) we have

\begin{aligned} \left[ \begin{array}{c} p^*s' \\ t' \end{array} \right] = \left[ \begin{array}{cc} p^*g &{}\quad 0 \\ 0 &{}\quad h \end{array} \right] \left[ \begin{array}{c} p^*s \\ t \end{array} \right] . \end{aligned}

Thus the restriction to j(M) of the matrices

\begin{aligned} G= \left[ {\begin{array}{cc} p^*g &{}\quad 0 \\ 0 &{}\quad h \\ \end{array} } \right] \end{aligned}

are transition matrices for $$N_{j(M)}Y$$; it is then clear that (7.3) holds. For future use let $$\eta$$ be the section of $${{\mathscr {L}}}\rightarrow p^{-1}i(M)$$ that defines j(M).

To prove (7.4) we must return to the definition of $$p^*$$, so let us assume that $$\mu =\tau _*\alpha$$ and recall the fiber square (6.3). We may also assume that W is chosen so that $$\tau ^*{\sigma }$$ is principal and hence $$\rho ^*\phi$$ is a regular embedding of codimension 2 in $$W'$$. We claim that

(7.6)

In fact, notice that $${\widetilde{\pi }}^*\tau ^*{\sigma }$$ combined with the section $$\rho ^*\eta$$ generate the same sheaf as $$\rho ^*\phi$$. Arguing precisely as above for (7.3) we then get (7.6).

We now claim that

\begin{aligned}{}[Z_{\tau ^*{\sigma }}]={\widetilde{\pi }}_*[Z_{\rho ^*\phi }], \end{aligned}
(7.7)

where $$Z_{\tau ^*\sigma }$$ is the fundamental cycle of the ideal sheaf generated by $$\tau ^*\sigma$$ etc. Since it is an equality of currents it is a local statement. By the dimension principle it is then enough to check it in an open set $${{\mathscr {U}}}\subset W$$ where $$Z_{\tau ^*{\sigma }}$$ is smooth and in suitable coordinates (xt) so that $${\widetilde{\pi }}$$ is $$(x,t)\mapsto x$$, cf. the proof of Lemma 6.1. Thus, we may assume that the ideal generated by $$\tau ^*{\sigma }$$ is generated by $$x_1^\ell$$ in $${{\mathscr {U}}}$$. Then $$\rho ^*\phi$$ is generated by $$(x_1^\ell ,t)$$ and (7.7) is reduced to the equality .

Next we claim that

\begin{aligned} M^{\tau ^*{\sigma }}\!\sim {\widetilde{\pi }}_*\bigl ( {\widehat{c}}(\rho ^*{{\mathscr {L}}}){\wedge }M^{\rho ^*\phi }\bigr ) \end{aligned}
(7.8)

on W. In fact, from [4, Proposition 1.5] we have

\begin{aligned} M^{\rho ^*\phi }\!={\widehat{s}}(N_{\rho ^*\phi }{W'}){\wedge }[Z_{\rho ^*\phi }]. \end{aligned}

By (7.6), noting that (2.10) holds for Segre forms as well in view of (2.4), we have that

\begin{aligned} {\widehat{c}}(\rho ^*{{\mathscr {L}}}){\wedge }M^{\rho ^*\phi }&\sim {\widehat{c}}(\rho ^*{{\mathscr {L}}}){\wedge }{\widehat{s}}({\widetilde{\pi }}^*N_{\tau ^*{\sigma }}{W}){\wedge }\widehat{s}(\rho ^*{{\mathscr {L}}}){\wedge }[Z_{\rho ^*\phi }] \\ {}&= {\widehat{s}}({\widetilde{\pi }}^*N_{\tau ^*{\sigma }}{W}){\wedge }[Z_{\rho ^*\phi }]. \end{aligned}

By (2.1) and (2.5) for Segre forms, thus

\begin{aligned} {\widetilde{\pi }}_*\bigl ( {\widehat{c}}(\rho ^*{{\mathscr {L}}}){\wedge }M^{\rho ^*\phi }\bigr ) \sim {\widehat{s}}(N_{\tau ^*{\sigma }}{W}){\wedge }{\widetilde{\pi }}_*[Z_{\rho ^*\phi }]. \end{aligned}

In view of (7.7) and [4, Proposition 1.5], now (7.8) follows.

We can now conclude (7.4). Since $$\alpha$$ is smooth, from (7.8) we have, cf. (2.1), that

and hence, by (2.14) and the commutivity of (6.3),

Now, by (2.5) and (2.14),

so

and since $$\rho _*{\widetilde{\pi }}^*\alpha =p^*\!\mu$$, cf. (6.4), therefore (7.4) follows.$$\square$$

8 Examples

We shall now present some further results on our products and various examples. We first consider an embedding $$i:\mathbb P^M\!\rightarrow {\mathbb {P}}^{M+1}$$ as a linear hyperplane defined by the linear form $$\xi$$. Let $$a\in {\mathbb {P}}^{M+1}$$ be a point outside this hyperplane and let $${{\mathfrak {p}}}:{\mathbb {P}}^{M+1}\dashrightarrow \mathbb P^M$$ be the induced projection. If Y is the blow-up of $$\mathbb P^{M+1}$$ at a we have the diagram

As in Sect. 6 we see that given $$\mu \in {\mathscr {GZ}}(\mathbb P^M)$$, the current $${{\mathfrak {p}}}^*\mu$$ has a well-defined extension to an element $$\pi _*p^*\!\mu$$ in $${\mathscr {GZ}}({\mathbb {P}}^{M+1})$$, cf. Lemma 6.1.

Proposition 8.1

Let $$\eta$$ be a tuple of linear forms on $${\mathbb {P}}^M$$. With the notation above we have

(8.1)

and

(8.2)

Proof

Since the support of $$i_*\mu$$ is contained in the hyperplane $$i({\mathbb {P}}^M)$$ and Y and $${\mathbb {P}}^{M+1}$$ coincide in a neighborhood of $$i({\mathbb {P}}^M)$$, the right-hand side of (8.1) is well-defined. Now (8.1) follows from (2.14) and (4.3) since so that $$i^*{{\mathfrak {p}}}^*\eta =\eta$$.

For the second equality first notice that both sides of (8.2) have support on $$i({\mathbb {P}}^M)$$ and that Y and $${\mathbb {P}}^{M+1}$$ coincide in a neighborhood of $$i({\mathbb {P}}^M)$$. For the rest of this proof let i denote also the inclusion of $${\mathbb {P}}^M$$ in Y. Since $$\eta$$ defines a regular embedding, it follows from [4, Example 7.8] that

if $$\mu$$ is a smooth form; here we use the standard metric on L. It follows in general, by assuming that $$\mu =\tau _*\alpha$$, $$\tau :W\rightarrow {\mathbb {P}}^M$$, and pulling back to W and $$W'$$ according to the fibre square

cf. the proofs of Lemmas 6.1 and 7.3 above. Since $${\widehat{c}}(\pi ^*L)=1+\pi ^*{\widehat{\omega }}$$ we get

Thus, in view of (4.7),

where we for the last equality have used that so that we may let the sum start from $$j=0$$; indeed, since $$\xi$$ is generically nonvanishing on the Zariski support of $$p^*\!\mu$$. Thus, (8.2) follows by applying $$\pi _*$$.$$\square$$

We will now deduce a formula for when A is a linear subspace.

Proposition 8.2

Assume that A is a linear subspace of $${\mathbb {P}}^{\,n}$$ of dimension m, defined by $$n-m$$ linear forms $${\sigma }_1,\ldots ,{\sigma }_{n-m}$$. If $$\mu \in {\mathscr {GZ}}_d({\mathbb {P}}^{\,n})$$, then

(8.3)

in $${{\mathscr {B}}}({\mathbb {P}}^{\,n})$$.

Proof

Let us use the notation from Sect. 6. By (6.13) the $$\bullet$$-product is not affected by a linear change of coordinates on $${{\mathbb {C}}}^{n+1}_x$$ and therefore we can assume that $$x=(x'\!,x'')$$ and $${\sigma }=x''$$. Then we need to prove that

in $${{\mathscr {B}}}({\mathbb {P}}^{\,n})$$. Recall that $$\eta =x-y$$. By definition we have, cf. (2.14) and (4.3),

(8.4)

Recall the diagram (6.2) associated with the mapping (6.1) and, as in the proof of Proposition 7.1, let $$Y=\mathrm{Bl}\,{\mathbb {P}}^{2n+1}_{x,y}$$. Consider the mapping , $$[x,y]\mapsto ([x],[y'])$$, and let $$\pi ':Y'\!\rightarrow \mathbb P^{\,n+m+1}_{x,y'}$$ be the blow-up of $${\mathbb {P}}^{\,n+m+1}_{x,y'}$$ along $$\{x=0\}$$ and $$\{y'\!=0\}$$. Similarly to (6.2) we then have

Let $$\iota :{\mathbb {P}}^{\,n+m+1}\!\hookrightarrow \mathbb P^{2n+1}$$, $$[x,y'] \mapsto [x,y'\!,0]$$. Then $$\iota$$ extends to a mapping $${\widetilde{\iota }}:Y'\!\rightarrow Y$$. Also, let , $$([x],[y']) \mapsto ([x],[y'\!,0])$$. Consider the fibre square

cf. (6.3). Notice that . By the same arguments as in the proof of Lemma 6.1, we get

(8.5)

cf. (6.4). It is straightforward to check that and so, by applying $$\pi _*$$ to (8.5), we get

(8.6)

Let be projection on the first factor and set . Then and . Thus, by (8.6),

(8.7)

By (8.4), (8.7), and repeated use of (8.1) we get

(8.8)

Let $$j':{\mathbb {P}}^{\,n}\!\rightarrow {\mathbb {P}}^{n+m+1}$$, $$[x]\mapsto [x,x']$$, and let $${\mathfrak {q}}:\mathbb P^{\,n+m+1}\!\dashrightarrow {\mathbb {P}}^{\,n}$$, $$[x,y']\mapsto [x]$$. Then we have the commutative diagram

By repeated use of (8.2), with , $$j=0,\ldots ,m$$, we get

and so, by (8.8),

Since $$j_*$$ is injective, to finish the proof it suffices to check that we may replace $$\iota _*j'_*$$ by $$j_*$$ in the right-hand side. Notice that is a generalized cycle with support $$\{x''\!=0\}$$ so that $$\nu =i_*\nu '$$ for some $$\nu '\!\in {\mathscr {GZ}}(\{x''\!=0\})$$, where $$i:\{x''\!=0\}\hookrightarrow {\mathbb {P}}^{\,n}$$ is the inclusion. Since we obtain

\begin{aligned} \iota _*j'_* \nu =\iota _*j'_*i_*\nu '=j_* i_*\nu '=j_*\nu . \end{aligned}

$$\square$$

Proposition 8.3

Assume that $$\mu \in {{\mathscr {B}}}({\mathbb {P}}^{\,n})$$. Then

(8.9)

If a is a point, then

(8.10)

Proof

From Proposition 8.2 we have that and so (8.9) follows. To see (8.10) let $$\xi$$ be linear forms that define a. By (8.3) and (4.4) we have .$$\square$$

Let $$\eta$$ be a fixed choice of a tuple of linear forms defining the join diagonal $$\Delta _J$$ in $${\mathbb {P}}^{\,r(n+1)-1}$$. Then, using the notation of Sect. 6, we can define a $$\bullet$$-product of $$\mu _1,\ldots ,\mu _r\in {\mathscr {GZ}}({\mathbb {P}}^{\,n})$$ by

(8.11)

cf. Definition 6.6. With this definition, for $$\mu \in {\mathscr {GZ}}({\mathbb {P}}^{\,n})$$, (8.9) and (8.10) hold in $${\mathscr {GZ}}({\mathbb {P}}^{\,n})$$.

Proposition 8.4

Let $$\eta$$ be a fixed choice as above. Assume that $$\mu _0,\mu _1,\ldots ,\mu _r\in {\mathscr {GZ}}({\mathbb {P}}^{\,n})$$ and that $$\mu _0=\gamma {\wedge }\mu _1$$ in an open set $${{\mathscr {U}}}\subset {\mathbb {P}}^{\,n}$$, and $$\gamma$$ is a smooth and closed form. Then

(8.12)

in $${{\mathscr {U}}}$$.

Combined with (8.9) we see that

(8.13)

in $${{\mathscr {U}}}$$ if $$\gamma \in {\mathscr {GZ}}({\mathbb {P}}^{\,n})$$ is a smooth form there.

Proof

In view of (2.14) and (4.3) we have

(8.14)

Now

in . Since is a smooth and closed form, it follows from (2.13) that the right-hand side of (8.14) equals

(8.15)

in . In a neighborhood of $$\Delta _J=\{\eta =0\}$$, $${\mathfrak {p}}$$ is defined and so

in a neighborhood of $$\{\pi ^*\eta =0\}$$ in . Thus, (8.15) equals

(8.16)

on $$j({{\mathscr {U}}})$$. Since in $${{\mathscr {U}}}$$, by (8.11) we see that (8.16) equals

on $$j({{\mathscr {U}}})$$. Using that $$j_*$$ is injective on currents we get (8.12).$$\square$$

Example 8.5

Let $${\widehat{\omega }}$$ be the Fubini–Study metric form on $${\mathbb {P}}^{\,n}$$. Then $${\widehat{\omega }}$$ is a generalized cycle of degree 1 and with multiplicity 0 at each point. Given any choice of $$\eta$$ as above, it follows from Proposition 8.4 that and, more generally, .

Example 8.6

Let $$a=[1,0,\ldots ,0]\in {\mathbb {P}}^{\,n}$$ and let $$\theta =dd^c\log (|x_1|^2+ \cdots + |x_n|^2)$$ in $$\mathbb P^{\,n}_{x_0,\ldots , x_n}$$. For each k, $$\theta ^k$$ is a well-defined positive closed current, see, e.g., [10, Chapter III]. It is an irreducible generalized cycle of dimension $$n-k$$ and degree 1, with $$\mathrm{mult}_a\theta ^k=1$$ and $$\mathrm{mult}_x\theta ^k=0$$ for $$x\ne a$$; for $$k<n$$, $$\theta ^k$$ has Zariski-support equal to $${\mathbb {P}}^{\,n}$$ whereas $$\theta ^n=[a]$$, see [4, Example 6.3] and cf. Example 2.9. One can think of $$\theta ^{k}$$ as an $$(n\,{-}\,k)$$-plane through a moving around a. We claim that

(8.17)

In fact, notice that both sides coincide outside a in virtue of Proposition 8.4. Thus they can only differ on a generalized cycle with Zariski support at a, that is, m[a] for some integer m. Since the degree of $$\theta$$ is 1, also the degree of $$\theta ^{k\bullet }$$ must be 1 by the Bézout formula (1.7); indeed note that $$\rho$$ in (1.6) in this case equals $$n-k\hbox {\,\char 062\,}0$$. Since the degree of the right-hand side is 1 it follows that $$m=0$$ and hence (8.17) holds.

Example 8.7

Let $$n=2$$, let a and $$\theta$$ be as in the previous example, and let $$\ell$$ be a line through a. Then

(8.18)

In fact, in view of (8.13), outside a, , which vanishes since the pullback of $$\theta$$ to $$\ell$$ vanishes. By the same argument as in Example 8.6, using Bézout’s formula (1.7), we get (8.18).

Example 8.8

Let $$\mu _1, \ldots , \mu _r$$, $$r\hbox {\,\char 062\,}2$$, be different lines through $$a\in {\mathbb {P}}^{\,n}$$. We claim that . In fact, since the set-theoretic intersection is a, the product must be m[a] for some integer m. Since the are effective it follows from (1.8) that m is 1 or 0. By (1.5) it is enough to determine the local intersection number $$\epsilon _0(\mu _1,\ldots , \mu _r, a)$$, and thus we can assume that the are lines through $$a=0$$ in $${{\mathbb {C}}}^n$$. In view of (3.1) and (4.3) this equals the multiplicity of , where $$\eta$$ is a tuple of linear forms defining the diagonal in . This, in turn, can be computed by intersecting by r generic hyperplanes , see Sect. 4. Doing this, we get [0] with multiplicity 1, which proves the claim.

Example 8.9

Let G be the graph in $${{\mathbb {C}}}^6_{x,y}={{\mathbb {C}}}^6_{x_1,x_2,x_3,y_1,y_2,y_3}$$ of the function

\begin{aligned} {{\mathbb {C}}}^3_x\rightarrow {{\mathbb {C}}}^3_y, \quad (x_1,x_2,x_3)\mapsto (x_1x_3, x_2x_3, x_3^2), \end{aligned}

and let Z be the closure in $${\mathbb {P}}^6_{x_0,x,y}$$. Clearly Z is irreducible of dimension 3. We want to compute , where $$A=\{y=0\}$$. By (8.3),

In view of Sect. 4 we can compute the right-hand side by successively intersecting [Z] by hyperplanes , where , and for generic $$\alpha , \beta , \gamma \in {\mathbb {P}}^2$$, and then taking averages.

The map $${\mathbb {P}}^3\!\dashrightarrow {\mathbb {P}}^6$$, $$[t_0,t_1,t_2,t_3]\mapsto [t_0^2,t_0t_1, t_0t_2, t_0t_3, t_3t_1, t_3t_2, t_3^2]$$, lifts to an injective holomorphic map from the blow-up $$Y=\mathrm{Bl}_{t_0=t_3=0}{\mathbb {P}}^3$$ to $${\mathbb {P}}^6$$ with image Z. Then Z can be parametrized by two copies of ,

identified by $$s=uv$$, $$s\sigma =u$$. Let $$Z_1$$ and $$Z_2$$ be the image of the first and second map, respectively. Since $$Z_2\cap A=\varnothing$$, the SV-cycle we are to compute is contained in $$Z_1$$.

Expressed in the $$([s, t_1, t_2], \sigma )$$-coordinates, $$A=\{\sigma t_1=\sigma t_2=\sigma ^2s=0\}=\{\sigma =0\}$$ and so, clearly, , cf. (4.1). Moreover, $$\mathrm{div}\,h_1$$ is given by

\begin{aligned} \sigma (\alpha _1t_1 + \alpha _2t_2 + \alpha _3s\sigma ) =0. \end{aligned}

Hence $$\mathrm{div}\,h_1$$ has two irreducible components; the component $$\sigma =0$$ is contained in A and thus contributes to whereas the component $$\alpha _1t_1 + \alpha _2t_2 + \alpha _3s\sigma =0$$ is not contained in A. Intersecting the latter component by $$\mathrm{div}\,h_2$$ gives

\begin{aligned} \alpha _1t_1 + \alpha _2t_2 + \alpha _3s\sigma = \sigma (\beta _1t_1 + \beta _2t_2 + \beta _3s\sigma ) =0. \end{aligned}

Again we get two irreducible components. The component $$\{\sigma =\alpha _1t_1+\alpha _2t_2=0\}$$ is contained in A and contributes to while the component $$\{\alpha _1t_1 + \alpha _2t_2 + \alpha _3s\sigma =\beta _1t_1 + \beta _2t_2 + \beta _3s\sigma =0\}$$ is not contained in A. Intersecting the latter one by $$\mathrm{div}\,h_3$$ gives

\begin{aligned} \alpha _1t_1 + \alpha _2t_2 + \alpha _3s\sigma =\beta _1t_1 + \beta _2t_2 + \beta _3s\sigma = \sigma (\gamma _1t_1 + \gamma _2t_2 + \gamma _3s\sigma )=0. \end{aligned}

The case $$\sigma \ne 0$$ forces $$t_1=t_2=s=0$$, which is impossible. The other case gives 2 times the point $$\{\sigma =t_1=t_2=0\}$$ as contribution to .

We thus get the SV-cycle

(8.19)

where $$P=\{x_3=y=0\}$$, $$L_\alpha =\{x_3=y=\alpha _1x_1+\alpha _2x_2=0\}$$, and $$a=[1,0,0,0,0,0,0]$$ expressed in the original $$x_0,x,y$$-coordinates. Taking the average of (8.19) over $$(\alpha , \beta , \gamma ) \in ({\mathbb {P}}^2)^3$$ we get

where $$\mu$$ is the generalized cycle obtained as the average of $$L_\alpha$$.

Note that the degree of is 4 since each term has degree 1 except for the double point 2[a]. Thus, in view of (1.7), $$\deg Z=4$$; indeed $$\rho$$ in (1.6) is 0 in this case. Moreover, by (1.5), the local intersection numbers at a are $$\epsilon _0(A, Z, a)=\mathrm{mult}_a 2[a]=2$$, $$\epsilon _1(A, Z,a)=\mathrm{mult}_a\mu =1$$, and $$\epsilon _2(A, Z, a)=\mathrm{mult}_a P =1$$. Here we have used that $$\mu$$ has multiplicity 1 at a since it is a mean value of lines through a in the 4-plane $$\{x_3=y=0\}$$, cf. Example 8.6.

We now give an example that shows that the $$\bullet$$-product is not associative.

Example 8.10

Consider the hypersurface $$Z=\{x_2x_1^m-x_3^2x_0^{m-1}=0\}$$ in $${\mathbb {P}}^3$$, let $$H_2=\{x_2=0\}$$ and $$H_3=\{x_3=0\}$$. Since $$H_2$$ and Z intersect properly,

cf. (1.9). Let $$A= \{x_2=x_3=0\}$$. It follows from Proposition 6.7 and (8.9) that ; this can also be verified by a symmetry argument and the Bézout formula (1.7). Moreover, $$\{x_3=0\}$$ and $$\{x_0=x_2=0\}$$ intersect properly and the intersection is $$b=[0,1,0,0]$$. Thus

(8.20)

Next note that . It is showed in [6, Example 11.5] that the local intersection number for A and Z in dimension 0 is m at $$a=[1,0,0,0]$$, and 1 in dimension 1 at all points $$x\in A$$. It follows that A and m[a] are components of . Moreover, since A and Z are effective, by Theorem 1.1, is effective and of degree at most . Hence

(8.21)

It follows that neither $$\cdot _{{{\mathscr {B}}}({\mathbb {P}}^N)}$$ is associative in $${{\mathscr {B}}}({\mathbb {P}}^{\,n})$$. In fact, it follows from (8.20), (8.21), and Theorem 1.2, that

whereas

and these right-hand sides are not equal in $${{\mathscr {B}}}({\mathbb {P}}^{\,n})$$.

Example 8.11

Let $$\gamma$$ be a smooth curve in $${\mathbb {P}}^2$$ of degree d. It is well-known, see, e.g., [6], that local intersection numbers are biholomorphic invariants. Therefore, since the $$\bullet$$-self-intersection of a line is the line itself, cf. the discussion after Proposition 6.8, it follows from (1.5) that at each $$x\in \gamma$$, and . Thus, since , in view of the dimension principle, where $$\mu$$ has dimension 0 and Zariski support equal to $$\gamma$$. By the Bézout formula (1.7) the degree of $$\mu$$ must be $$d^2-d$$. We can think of $$\mu$$ as $$d^2-d$$ points moving around on $$\gamma$$.

Example 8.12

We want to compute the $$\bullet$$-self-intersection of a curve Z in $${\mathbb {P}}^2$$. Assume that $$Z=\{F=0\}$$ where F is a section of $${\mathscr {O}}(d)$$ with differential generically nonvanishing on Z. Let , $$j=0,1,2$$, on . Then $$\eta$$ defines the join diagonal $$\Delta _J$$. Following Sect. 4 we can compute by successively intersecting by hyperplanes , where for generic $$\alpha ^j\in {\mathbb {P}}^2$$, and then averaging over $$\alpha =(\alpha ^1\!,\alpha ^2\!,\alpha ^2)\in ({\mathbb {P}}^2)^3$$. Note that we can write

\begin{aligned} F(y)-F(x)=\eta _0 A_0+\eta _1 A_1+\eta _2 A_2 \end{aligned}

for suitable homogeneous forms , and thus

cf. Example 6.3. It turns out that

for some $$\beta , \gamma \in {\mathbb {P}}^2$$. The second equation gives rise to two components. The component corresponding to $$\eta _2=0$$ is contained in $$\Delta _J$$ and equals

where j is the parametrization (6.8) of $$\Delta _J$$. Next, since on $$\Delta _J$$ we get that

(8.22)

The curve defined by $$\beta _0 F_0+\beta _1 F_1+\beta _2 F_2$$ is a so-called polar curve to Z; it is clear that it passes through all singular points $$a_1\ldots , a_r$$ of Z, since the gradient must vanish there. More precisely, in view of the Bézout formula (1.7), for generic $$\beta$$,

where are the multiplicities of and $$r_\beta$$ are $$d^2-d-(m_1+\cdots + m_r)$$ points on Z depending on $$\beta$$, cf. Example 8.11. Thus, taking averages over $$\alpha \in ({\mathbb {P}}^2)^3$$, we get that

(8.23)

where $$j_*\mu$$ is the average of the $$r_\beta$$. In particular, $$\mu$$ has dimension 0, Zariski-support equal to Z, and degree $$d^2-d-(m_1+\cdots + m_r)$$. Moreover, in view of Example 8.11, $$\mu$$ has multiplicity 0 at each point.

Let us now consider a simple cusp.

Example 8.13

Let us consider the situation of the previous example and let $$F=x_1^3-x_0x_2^2$$ so that $$Z\subset {\mathbb {P}}^2$$ is a cusp with a singularity only at the point $$a=[1,0,0]$$. Now

for some $$\beta \in {\mathbb {P}}^2$$, see (8.22). For generic choices of $$\alpha \in ({\mathbb {P}}^2)^3$$, $$\beta _2\ne 0$$ and we can identify this with the set of points

\begin{aligned} \varrho _\beta = \bigl \{x_1^3-x_0x_2^2=0, \ \beta _0 x_2^2+\beta _1 x_1^2+x_0x_2=0\bigr \}\subset {\mathbb {P}}^2\!. \end{aligned}

To compute the order of the zero at a, we can use affine coordinates and thus let $$x_0=1$$. Then $$\varrho _\beta =\bigl \{x_1^3-x_2^2=0, \ \beta _0 x_2^2+\beta _1 x_1^2 + x_2=0\bigr \}.$$ If we choose new coordinates $$z_1=x_1$$, $$z_2=x_2+\beta _0x_2^2+\beta _1x_1^2$$, then $$x_2=z_2+{\mathscr {O}}(z^2)$$, and thus $$\varrho _\beta$$ is defined by the equations

\begin{aligned} z_1^3- (z_2+{\mathscr {O}}(z^2) )^2=0,\quad z_2=0. \end{aligned}

Hence the zero at $$a=(0,0)$$ has order 3. In fact, for a complete intersection, as here, the order of the zero coincides with the degree of the associated mapping. From (8.23) we conclude that

(8.24)

where $$\mu$$ has dimension 0, Zariski-support equal to Z, multiplicity 0 at each point, and degree 3.

Example 8.14

Let $$Z\subset {\mathbb {P}}^2$$ be the cusp as in the previous example. In view of Theorem 1.2 and (8.24) we get

(8.25)

Since Z is a regular embedding in $${\mathbb {P}}^2$$ we can also form the product . Let $${{\mathscr {J}}}\rightarrow {\mathbb {P}}^2$$ be the sheaf defining Z. If $$i:Z\hookrightarrow {\mathbb {P}}^2$$, then $$i^*{{\mathscr {J}}}_Z=0$$ so that $$S({{\mathscr {J}}}_Z,Z)=S(0,Z)=[Z]$$, cf. Sect. 2.5. Moreover, $$N_Z{\mathbb {P}}^2\!={\mathscr {O}}(3)|_Z$$, so that $$c_1(N_Z{\mathbb {P}}^2)=3\omega$$. Thus

(8.26)

cf. Definition 5.1. Notice that (8.25) and (8.26) do not coincide in $${{\mathscr {B}}}({\mathbb {P}}^2)$$. For instance, the first one has multiplicity 3 at a, whereas the second one has multiplicity 0 at a.

However, in view of Proposition 5.7 their images in $${\widehat{H}}^{2,2}(Z)$$ coincide. Clearly the image of is represented by the restriction to Z of the form $$3\omega$$. It is easy to see that 3a is cohomologous with $$\omega$$ on Z as

It is somewhat less obvious that $$\mu$$ is cohomologous with $$\omega$$ on Z.

Example 8.14 also shows that the self-intersection formula, Proposition 5.5, does not generalize to nonsmooth Z.