advanced31 min studyLesson 469 in Mathematics

Morse functions and handle attachments

Read a nondegenerate Hessian as a local topological transition and state the compact-band hypotheses behind a global handle attachment.

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What you’ll understand

  • Compute a Morse critical point's index from its Hessian.
  • Identify the handle attached when a sublevel crosses one critical value.
  • Use alternating critical-point counts without confusing them with a complete manifold classification.

Imagine raising the allowed value of a smooth function and watching its sublevel set grow. Away from critical values the topology stays unchanged under suitable compactness conditions. Passing a nondegenerate critical point produces one controlled change: attachment of a handle whose index is the number of negative Hessian directions. Morse theory makes this relation precise. The local quadratic form explains the index, while compactness of the relevant band prevents unobserved changes at infinity from invalidating the global conclusion.

At a critical point the Hessian has an intrinsic signature

A critical point p satisfies dfₚ=0. At such a point the second derivative defines a symmetric bilinear form on the tangent space independently of the chosen coordinates: the extra coordinate-change terms involving first derivatives vanish. Nondegeneracy means this Hessian is invertible. Its index λ is the number of negative eigenvalues counted with multiplicity. A minimum has index zero, a maximum has index n, and intermediate indices describe saddle behavior. Eigenvalue magnitudes can change under coordinates, while the numbers of positive and negative directions do not.

A smooth function is Morse when every critical point is nondegenerate. The Morse lemma gives smooth coordinates in which the function is exactly a constant plus negative squares in λ directions and positive squares in the remaining directions, rather than merely having that quadratic Taylor approximation. This is a theorem about a neighborhood of one critical point. The gradient flow also depends on a chosen Riemannian metric, so these coordinates do not automatically make every global flow line a straight coordinate trajectory.

f(x)=f(p)−x12−⋯−xλ2+xλ+12+⋯+xn2f(x)=f(p)-x_1^2-\cdots-x_\lambda^2+x_{\lambda+1}^2+\cdots+x_n^2
This exact local normal form requires a smooth function at a nondegenerate critical point. The integer λ is the Hessian index, not the dimension of the ambient Euclidean drawing.↔ Scroll wide equations horizontally.

A compact regular band isolates one topological event

Let a<b be regular values and assume f⁻¹([a,b]) is compact, is contained in the source interior, and contains no critical points. A normalized gradient construction gives a product structure across that band and identifies the sublevels at its ends up to diffeomorphism. Compactness prevents a trajectory from escaping before it reaches the other level. On a closed manifold this protection is automatic; for a noncompact source it must be supplied, for example by a proper function and a bounded value interval.

If the compact band contains exactly one critical point of index λ, with critical value strictly between its regular endpoints, the upper sublevel is obtained from the lower by attaching an n-dimensional λ-handle and smoothing corners. The handle is D^λ×D^(n−λ), attached along S^(λ−1)×D^(n−λ). Up to homotopy this adds a λ-cell, so Euler characteristic changes by (−1)^λ. The local model does not eliminate the need for compactness, regular endpoints, or control of the rest of the band.

Hλ=Dλ×Dn−λ,attaching region Sλ−1×Dn−λ,Δχ=(−1)λH_\lambda=D^\lambda\times D^{n-\lambda},\qquad \text{attaching region }S^{\lambda-1}\times D^{n-\lambda},\qquad \Delta\chi=(-1)^\lambda
This is the change across one isolated nondegenerate critical point in a compact band with regular endpoints and no other critical points. For λ=0 the attaching region is empty.↔ Scroll wide equations horizontally.

Counts constrain topology but do not determine every attachment

On a closed manifold a Morse function has finitely many critical points, and its handle decomposition yields the Euler characteristic as the alternating sum of their index counts. The weak Morse inequalities say that each count is at least the corresponding homology rank over a field. Extra critical points can cancel algebraically or support attachments that do not create independent homology classes. An index count is therefore a constraint on topology, not a direct list of Betti numbers.

Attaching maps and framings can distinguish manifolds even when the numbers of handles agree. Morse functions themselves can be perturbed and compared, and genericity theorems establish their existence, but cancellation of a particular handle pair has further geometric conditions. Keep a computational workflow modest and precise: locate critical points, verify nondegeneracy, determine index and value, isolate compact regular bands, and only then infer the corresponding handle changes. A Hessian sign table alone is not a complete classification theorem.

Read a torus from a four-point Morse function

On T²=S¹×S¹ let f(θ,φ)=2cosθ+cosφ. Find its critical values and indices, then calculate the Euler characteristic from the handle counts.

  1. The first derivatives are −2sinθ and −sinφ, so each angle is 0 or π at a critical point. The four values are 3 at (0,0), 1 at (0,π), −1 at (π,0), and −3 at (π,π).

  2. The Hessian is diagonal with entries −2cosθ and −cosφ. At the respective points it has two, one, one, and zero negative eigenvalues. Every Hessian is invertible, so f is Morse with one index-0 point, two index-1 points, and one index-2 point.

  3. The compact torus allows regular levels between these distinct values. Sublevels attach handles of indices 0,1,1,2 in increasing-value order, giving alternating count 1−2+1=0.

The result

The Morse count recovers χ(T²)=0. The two saddles contribute negatively to the alternating sum; knowing their count alone does not specify all attaching data for a general surface or higher-dimensional manifold.

Explore the model

Interactive lab

Interactive lab · function

Compare positive and negative quadratic directions

Pause and Reset; set a=1,x=0 and predict a minimum with second derivative 2. For a fresh comparison Reset and set a=−1,x=0 and predict a maximum with second derivative −2. In this one-dimensional model the Morse indices are respectively 0 and 1. The instrument shows individual quadratic directions, not a multidimensional Hessian, a handle attachment, or the compactness of a global sublevel band.

Compare positive and negative quadratic directionsThis lab uses only y = ax². Playback traces the curve within the fixed integration interval from 0 to x; it does not estimate numerical error or change the chosen point. Current readings: y at chosen x: 0.608; Tangent slope · 2ax: 1.35; Signed area · ax³/3: 0.182. All parameters are adjustable with the labeled controls below.−2.4−1.201.22.4−9−4.504.59xy(x, ax²)
y = ax²TangentSigned integral
y at chosen x
0.608
Tangent slope · 2ax
1.35
Signed area · ax³/3
0.182
t = 0 s

This lab uses only y = ax². Playback traces the curve within the fixed integration interval from 0 to x; it does not estimate numerical error or change the chosen point. Parameter changes pause playback and recompute the model at the current elapsed time. Reset restores both parameters and returns time to zero. Playback starts paused. Adjust either parameter, then choose Play or Step.

Look forNegative Hessian directions determine Morse index, while global handle conclusions require additional band hypotheses.

Check your understanding

An isolated nondegenerate critical point on a 4-manifold has Hessian eigenvalues 2,4,−6,−8. Which handle index does it contribute in an otherwise regular compact band?

Try it yourself

Suppose f has local expression 5+x12+2x22−3x32−4x425+x_1^2+2x_2^2-3x_3^2-4x_4^2 at the only critical point of a compact regular sublevel band on a 4-manifold. Find its index, handle type, attaching region, and Euler-characteristic increment.

Take a moment to make a prediction or work it out on paper. Open a hint when you need one.

Give me a hint

Compute the Hessian signs first. The local indefinite polynomial alone does not assert that its entire Euclidean sublevel band is compact; compactness is an additional hypothesis here.

Compare with the solution

The Hessian is diag(2,4,−6,−8), so the critical point is nondegenerate with index 2. The handle is D²×D² and attaches along S¹×D². Its cell-level contribution changes Euler characteristic by (−1)²=+1. The stated compact band and regular endpoints justify the global attachment; one cannot infer that compactness from this local quadratic formula.

Take it with you

  • Morse index counts the negative directions of a nondegenerate Hessian.
  • One critical point in a controlled compact band attaches a handle of that index.
  • Alternating counts recover Euler characteristic, while attaching data carry more information.

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