Nonsingular Varieties
A variety is nonsingular (or smooth) if it has a well-defined tangent space of the expected dimension at every point. Singularities โ nodes, cusps, and worse โ are the points where the geometry degenerates. Understanding where and how singularities arise is one of the central concerns of algebraic geometry.
Throughout, denotes an algebraically closed field and varieties are as in Hartshorne, Chapter I.
The Zariski tangent space
Let be a variety over and let be a point. Let be the maximal ideal of the local ring at . The Zariski tangent space of at is the -vector space
Equivalently, , the space of -derivations .
The Zariski tangent space is defined intrinsically from the local ring, without reference to an embedding. This is crucial: it means the tangent space is an invariant of the variety, not of a particular presentation by equations.
Let and . The local ring is where . Then
so . The tangent space at every point of is -dimensional, as expected.
Let and . For each , consider the differential
These are linear forms on . The Zariski tangent space is
In other words, where is the Jacobian matrix. We always have , with equality characterizing nonsingularity.
The Jacobian criterion
Let . The Jacobian matrix of at a point is the matrix
Let be a variety of dimension in , and write where (or any set of generators). A point is nonsingular if and only if
Equivalently, is nonsingular iff .
The rank condition does not depend on the choice of generators of . If we add redundant generators, the Jacobian gets more rows but the rank at a nonsingular point remains .
Let be an irreducible plane curve (). Here , , so the Jacobian criterion requires , i.e.,
A point is singular iff and both partial derivatives vanish at .
Let over with . The Jacobian is
At a point on : . This vanishes iff , but does not lie on (since ). So is nonsingular at every point.
Let . Here , , so we need . The Jacobian is
This has rank 0 only at the origin, which does not lie on . Hence is smooth (when ).
Singular vs. nonsingular points
Let be a variety of dimension . A point is nonsingular (or smooth) if . Otherwise (), is a singular point of .
A variety is nonsingular (or smooth) if every point is nonsingular.
Let . Set . The partial derivatives are
At the origin : , , . Both partial derivatives vanish, so the origin is a singular point (a node).
The tangent space is , which is -dimensional -- strictly larger than .
At a generic point, say : we check , so this point is not on . Try : and . So is a smooth point.
Let . Set .
At : , , . The origin is singular.
At : , . So is smooth. In fact, the origin is the only singular point.
The cusp is "worse" than the node: the local ring has two-dimensional (same as the node), but the tangent cone is different (see below).
Let . Set .
At : both vanish, so the origin is singular. The curve factors as , giving two smooth branches (the parabolas and ) that are tangent to each other at the origin. This is a tacnode: the two branches share the same tangent line (with contact of order 2).
Compare with the node , where the two branches have distinct tangent directions at the singular point.
Consider (over a field where ). Since where is a primitive cube root of unity, the curve is actually reducible -- three lines through the origin.
For a genuinely irreducible example, take . The origin need not be singular here. Instead, consider the curve germ at the origin. Set :
The origin is a singular point. The lowest-degree terms are , giving three distinct tangent lines. This is an ordinary triple point (or ordinary 3-fold point): a point of multiplicity 3 with 3 distinct tangent directions.
More generally, a singular point of multiplicity with distinct tangent directions is called an ordinary -fold point.
The singular locus
Let be a variety. The singular locus
is a proper closed subset of . In particular, the set of nonsingular points is a dense open subset.
For , we computed that is determined by
From the partials: and , so or . Check on : gives (singular); gives (not on ). Thus , a single point -- a proper closed subset of .
Let (the Whitney umbrella). Set :
The singular locus is , which gives , , and then is automatic. So , the entire -axis.
Here the singular locus is a line sitting inside a surface -- a closed subset of dimension 1 inside a variety of dimension 2.
Smooth varieties
A variety is smooth (or nonsingular) if , i.e., every point of is nonsingular.
is smooth: the local ring at every point is , which is a regular local ring of dimension , and .
is smooth: it is covered by affine charts , each of which is smooth. Smoothness is a local property, so is smooth.
Let (assuming ). In the affine chart , this is , i.e., . The Jacobian is , which vanishes only at the origin, but , so no singular point exists in this chart. By symmetry, the same holds in every chart. So is smooth.
More generally, a quadric in is smooth if and only if the associated symmetric matrix is nonsingular (i.e., has nonzero determinant).
The Fermat cubic surface (with ). In the chart :
requires , but then . By symmetry, all charts give the same conclusion: is smooth.
A classical result: every smooth cubic surface over contains exactly 27 lines. This is one of the most famous theorems in 19th-century algebraic geometry (Cayley-Salmon theorem, 1849).
Let where (the discriminant condition). Set :
A singular point requires (so ) and and . From , substitute into : one can show this system has a solution iff . So the condition is precisely what ensures smoothness.
For instance, (where , , discriminant ) is smooth. But (where , , discriminant ) has a cusp at the origin.
The Grassmannian is smooth. This can be seen from its local description: around any point , choose a complementary subspace of dimension . Then the open set is isomorphic to (the space of matrices, representing as the graph of a linear map ). Since is smooth and smoothness is local, is smooth.
The tangent cone
Let be a hypersurface and . Write where is the homogeneous component of degree (in the variables , centered at ) and . The tangent cone to at is
the zero set of the leading form . The integer is the multiplicity of at , denoted .
If is a smooth point (multiplicity 1), then is a nonzero linear form, and the tangent cone is a hyperplane -- this is the tangent space. For singular points, the tangent cone carries more refined information than the tangent space. The tangent space is always a linear subspace; the tangent cone is a (possibly reducible) cone.
For , the lowest-degree terms at the origin are . So
two distinct lines through the origin. The multiplicity is .
Geometrically, the two lines and are the two tangent directions of the two branches of the curve at the node.
For , the lowest-degree terms at the origin are (degree 2). So
a "double line" along the -axis. The multiplicity is .
Although the cusp and the node both have multiplicity 2, their tangent cones differ: the node has two distinct tangent lines, while the cusp has a single tangent line with multiplicity 2. The cusp is "more singular" in this sense.
For , the lowest-degree terms at the origin are (degree 2, since has degree 4). So
the same double line as the cusp. The multiplicity is 2. But the tacnode and the cusp are genuinely different singularities (the tacnode is analytically equivalent to two smooth branches tangent to each other; the cusp is an irreducible singular germ). Distinguishing them requires looking beyond the tangent cone, e.g., at higher-order jet spaces or the resolution.
Multiplicity of a point
Let be a variety and . The multiplicity is defined as follows. If is a hypersurface, it is the order of vanishing of at , i.e., the degree of the leading form in the Taylor expansion at .
More generally, if is the maximal ideal of and , the Hilbert-Samuel multiplicity is
where denotes the length. For a hypersurface, this agrees with the order of vanishing.
| Curve | Equation | | Tangent cone | |---|---|---|---| | Smooth point | (at origin: not on curve) | -- | -- | | Node | | 2 | : two lines | | Cusp | | 2 | : double line | | Tacnode | | 2 | : double line | | Triple point | | 3 | : three lines | | singularity | | 2 | : double line |
The multiplicity determines the "order" of the singularity, while the tangent cone captures the tangent geometry. Two singularities can have the same multiplicity and tangent cone (cusp vs. tacnode) but be analytically different.
Regular local rings
A Noetherian local ring is regular if
where is the Krull dimension. In general, (this is a consequence of the Krull principal ideal theorem). Equality is the condition of regularity.
Let be a variety and . The following are equivalent:
- is a nonsingular point of .
- .
- The local ring is a regular local ring.
- (For ) The Jacobian matrix has rank .
Moreover, every regular local ring is an integral domain, a UFD (Auslander-Buchsbaum theorem), and in particular is normal (integrally closed).
For and :
The maximal ideal satisfies (2-dimensional), but (since is a curve). Since , the local ring is not regular, confirming that the origin is a singular point.
Furthermore, is not a UFD: the element is irreducible but not prime (since , and ). It is also not integrally closed: is integral over but not in it.
For and :
The maximal ideal is , which is principal: (1-dimensional), and . Since , this is a regular local ring -- a discrete valuation ring (DVR). Every smooth curve has DVRs as its local rings.
Normalization and resolution of singularities
The normalization of a variety is the unique (up to isomorphism) normal variety with a finite birational morphism . For curves, normalization resolves all singularities:
- The normalization of the cuspidal cubic is , via .
- The normalization of the nodal cubic is , via .
In both cases, the normalization "unravels" the singularity by pulling apart branches (node) or "smoothing" the parametrization (cusp). For higher-dimensional varieties, normalization resolves singularities in codimension 1 but may leave higher-codimension singularities.
A resolution of singularities of a variety is a proper birational morphism where is smooth. Hironaka's celebrated theorem (1964) guarantees that resolutions exist for varieties over fields of characteristic zero.
Resolution is typically achieved by blowing up along the singular locus (or subvarieties thereof), repeatedly, until the result is smooth.
Blowing up singularities
Consider with a node at the origin. The blowup of at the origin replaces by a (the exceptional divisor ). In local coordinates:
Chart 1 (): Substituting into :
The factor corresponds to the exceptional divisor (with multiplicity 2). The strict transform is , a smooth curve. On (where ), the strict transform meets at , i.e., . These are two distinct points, corresponding to the two tangent directions of the node.
Chart 2 (): Substituting into :
The strict transform is , also smooth.
The blowup resolves the node in a single step: the strict transform is smooth, and is an isomorphism away from the origin. Above the origin, has two points (the two branches are separated).
Consider with a cusp at the origin.
First blowup (chart ): Substitute into :
The strict transform is smooth (it is a parabola in the -plane). On the exceptional divisor (): , so . The strict transform meets at a single point with multiplicity 2 (tangency).
But wait -- is actually smooth. The intersection with is transverse after a coordinate change: set , then , and via . The cusp is resolved after a single blowup.
However, note that the strict transform meets the exceptional divisor with contact order 2, not transversally. If we want normal crossings (for the purpose of embedded resolution), we would need a second blowup. For the abstract resolution of alone, one blowup suffices.
| Singularity | Blowups needed | Strict transform meets at | Behavior | |---|---|---|---| | Node | 1 | 2 distinct points | Two branches separated | | Cusp | 1 | 1 point (tangent to ) | Branch smoothed | | Tacnode | 2 | After 1st: cusp; after 2nd: smooth | Two tangent branches separated | | : | 2 | Successive blowups resolve | Higher-order contact resolved iteratively |
Nonsingularity in the projective setting
For a projective hypersurface with homogeneous of degree , the singular points are
By Euler's formula for homogeneous polynomials (), the condition is redundant when : it follows from the vanishing of all partials at a point of .
Concretely: the Klein quartic (over ) is smooth. Its partials are:
One can verify (e.g., by Grobner basis or direct computation) that the system has no solution in . The Klein quartic is a smooth curve of genus 3, and it has the largest automorphism group (168 elements) among genus-3 curves.
For "most" choices of coefficients, a degree- hypersurface in is smooth. More precisely, the locus of singular hypersurfaces in the parameter space (where ) is a proper closed subset -- the discriminant hypersurface .
For plane curves ():
- Degree 1 (lines): always smooth. .
- Degree 2 (conics): singular iff the matrix has . is a degree-3 hypersurface in .
- Degree 3 (cubics): the discriminant has degree 12.
This is a manifestation of Bertini's theorem: a "general" member of a linear system is smooth.
Summary: a taxonomy of plane curve singularities
| Name | Equation | Mult. | Tangent cone | -invariant | Blowups |
|---|---|---|---|---|---|
| (node) | 2 | Two distinct lines | 1 | 1 | |
| (cusp) | 2 | Double line | 1 | 1 | |
| (tacnode) | 2 | Double line | 2 | 2 | |
| 2 | Double line | 2 | 2 | ||
| (ordinary triple pt) | 3 | Three distinct lines | 3 | 1 | |
| 3 | Triple line | 3 | 3 |
The ADE classification of simple curve singularities (du Val singularities for surfaces) connects algebraic geometry to Lie theory, representation theory, and mathematical physics via the McKay correspondence.
Nonsingularity is preserved by many natural operations: smooth subvarieties of smooth varieties are smooth, products of smooth varieties are smooth, and a general hyperplane section of a smooth projective variety is smooth (Bertini's theorem). The theory of nonsingular varieties is the foundation for intersection theory, differential forms, sheaf cohomology, and the Riemann-Roch theorem in later chapters.
For a more general framework that handles singularities on equal footing -- including nilpotent elements, non-reduced structures, and arithmetic geometry -- one passes to the language of schemes and the notion of regular schemes.