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Band-Unknotting Number

Updated 14 December 2025
  • Band-unknotting number is defined as the minimum count of band surgeries required to transform a knot into the unknot, with variations for orientable and non-orientable bands.
  • It bridges classical knot invariants with 4-manifold topology by employing surface and homological techniques, such as Betti number evaluations, to derive bounds.
  • Computational methods and diagrammatic strategies, including broken surface diagrams and Floer-theoretic invariants, provide practical insights into estimating these invariant values.

The band-unknotting number and its generalizations quantify how knots in the 3-sphere can be simplified or transformed to the unknot using band surgeries, a class of local operations that generalize classical Reidemeister moves and crossing changes. These invariants, and their associated constructions, play a central role in knot theory, especially in the study of surfaces in 4-manifolds, double slicing, and the topological properties of knot complements.

1. Definitions and Basic Properties

Let KS3K \subset S^3 be a knot. Band surgery refers to the process of cutting KK at two points and reconnecting via a band—either orientable or non-orientable—yielding a new knot or link.

  • Band-unknotting number (ub(K)u_b(K)): The minimum number of (possibly orientable or unoriented) band surgeries needed to transform KK into the unknot. For oriented bands (oriented saddle moves), ub(K)u_b(K) is the minimal such count subject to producing a connected ribbon surface with a single disk as its 0-handle. This is equivalently the minimum number of bands in an oriented band-presentation of KK with a single disk (McDonald, 2019, Abe et al., 2011).

$u_b(K) = \min\{\text{number of oriented bands in a presentation of %%%%6%%%% with a single disk}\}$

  • Band number (b(K)b(K)): A generalization of ub(K)u_b(K) allowing ribbon surfaces in B4B^4 with multiple disks (0-handles) in their handle decomposition. It is the minimal number of ribbon bands in any handle decomposition whose boundary is KK (McDonald, 2019):

$b(K) = \min\{\,b\,|\,\exists\,\text{ribbon–surface for }K\text{ with %%%%11%%%% bands}\}$

Always b(K)ub(K)b(K) \le u_b(K), since ub(K)u_b(K) corresponds to the case with a single disk.

  • Non-orientable band-unknotting number (unb(K)u_{nb}(K)): The smallest number of non-orientable (half-twisted) band moves needed to unknot KK (Ghanbarian et al., 6 Dec 2025).
  • H(2)-unknotting number (u2(K)u_2(K)): The minimal number of twisted band moves (so-called H(2)-moves: special band surgeries that preserve the number of components) required to unknot KK (Bao, 2010, Abe et al., 2011).

For torus knots, the unoriented band-unknotting number coincides with the "pinch number," defined as the minimal number of Batson's pinch moves (special non-orientable band surgeries) needed to unknot the knot (Himeno, 20 Feb 2025).

2. Surface-Theoretic and Algebraic Characterizations

Band-unknotting numbers admit a surface-theoretic and homological interpretation. For any two knots J,KS3J, K \subset S^3, the band-Gordian distance db(J,K)d_b(J,K) is defined as the minimal number of band surgeries required to convert JJ to KK. The following characterization holds (Abe et al., 2011):

db(J,K)=min{b1(F)FS3,F=JK,F connected}1d_b(J, K) = \min\{\,b_1(F)\,|\, F \subset S^3,\, \partial F = J \cup K,\, F \text{ connected}\,\} - 1

Here, b1(F)b_1(F) denotes the first Betti number of the spanning surface FF. For the unknot UU,

ub(K)=min{b1(F)F=KU,F connected}1u_b(K) = \min\{\,b_1(F)\,|\, \partial F = K \cup U,\, F \text{ connected}\} - 1

There is a close relationship between band-unknotting numbers and 4-dimensional knot invariants. Specifically:

  • Every sequence of nn non-orientable band moves from KK to the unknot yields a non-orientable surface in B4B^4 bounding KK with Betti number n+1n+1 (Ghanbarian et al., 6 Dec 2025).
  • The band-unknotting number is always at least the maximum of the classical unknotting number u(K)u(K) and twice the genus 2g3(K)2g_3(K) of the minimal-genus Seifert surface for KK (McDonald, 2019). For non-orientable band moves:

μan(K)γ4,t(K)γ4,s(K)unb(K)\mu_{an}(K) \leq \gamma_{4,t}(K) \leq \gamma_{4,s}(K) \leq u_{nb}(K)

where μan(K)\mu_{an}(K) is the minimal number of generators of the anisotropic part of the linking form, and γ4,t\gamma_{4,t}, γ4,s\gamma_{4,s} are the minimal topological and smooth non-orientable genera in D4D^4 (Ghanbarian et al., 6 Dec 2025).

3. Relationships with Other Knot Invariants

Band-unknotting numbers are bounded above by and interact with various classical and 4-dimensional invariants:

Quantity Definition/Relation Source
ub(K)u_b(K) $\min\{\textrm{oriented bands to unknot$K$}\}$ (McDonald, 2019)
unb(K)u_{nb}(K) $\min\{\textrm{non-orientable bands to unknot$K$}\}$ (Ghanbarian et al., 6 Dec 2025)
b(K)b(K) Band number, allowing multiple disks (McDonald, 2019)
u(K)u(K) Classical unknotting number
g3(K)g_3(K) Minimal genus of orientable Seifert surface in S3S^3
gds(K)g_{ds}(K) Double slice genus: minimal genus of an unknotted closed surface in S4S^4 with cross-section KK (McDonald, 2019)
u2(K)u_2(K) Minimum H(2)–moves to unknot KK (Abe et al., 2011)
γ4(K)\gamma_4(K) Non-orientable 4-genus in B4B^4
μan(K)\mu_{an}(K) Minimal number of anisotropic generators in the linking form of Σ2(K)\Sigma_2(K) (Ghanbarian et al., 6 Dec 2025)

The following inequalities hold (selected):

  • ub(K)max{u(K),2g3(K)}u_b(K) \ge \max\{u(K), 2g_3(K)\}
  • gds(K)b(K)ub(K)g_{ds}(K) \le b(K) \le u_b(K)
  • ub(K)u_b(K) is either u2(K)u_2(K) or u2(K)1u_2(K) - 1, and ub(K)u_b(K) odd iff ub(K)=u2(K)u_b(K) = u_2(K) (Abe et al., 2011)
  • ub(K)u(K)u_b(K) \le u(K) if u(K)u(K) is even; u(K)+1\le u(K)+1 if u(K)u(K) is odd (Abe et al., 2011)
  • For every KK, gds(K)min{2g3(K),2u(K),ub(K),b(K)}g_{ds}(K) \le \min\{2g_3(K), 2u(K), u_b(K), b(K)\} (McDonald, 2019)
  • For torus knots, ub(T(p,q))=P(p,q)u_b(T(p,q)) = P(p,q), where P(p,q)P(p,q) is the pinch number derived from a special continued fraction expansion (Himeno, 20 Feb 2025)

4. Computational and Diagrammatic Aspects

Explicit computation of the band-unknotting number for specific knots involves both diagrammatic strategies and algebraic bounds:

  • Broken surface diagrams: Used extensively for analyzing surfaces in S4S^4 and verifying that double constructions or band-surgeries yield unknotted surfaces (i.e., those bounding handlebodies) (McDonald, 2019).
  • Use of covering spaces: Bounds from the homology of the double-branched cover Σ2(K)\Sigma_2(K)—particularly, minimal nn for an embedding in #nS2×S2\#_n S^2 \times S^2—are intimately related to gds(K)g_{ds}(K) and thus to the band number.
  • Link invariants: The Jones polynomial at special values, the QQ-polynomial, and linking forms furnish lower bounds for ub(K)u_b(K) and related quantities (Abe et al., 2011, Ghanbarian et al., 6 Dec 2025).
  • Floer-theoretic invariants: Torsion order of the unoriented knot Floer homology provides an exact computation of ub(T(p,q))u_b(T(p,q)) for torus knots (Himeno, 20 Feb 2025).

Remarkable phenomena, such as strict subadditivity (i.e., unb(K1#K2)<unb(K1)+unb(K2)u_{nb}(K_1 \# K_2) < u_{nb}(K_1) + u_{nb}(K_2)), have been established, notably for two-bridge knots and double-twist knots (Ghanbarian et al., 6 Dec 2025).

5. Explicit Examples and Formulas

Several instructive examples illustrate the invariants' values and bounds:

  • The unknot UU: ub(U)=b(U)=0u_b(U) = b(U) = 0, so gds(U)=0g_{ds}(U) = 0 (McDonald, 2019).
  • Stevedore knot 616_1: b(61)1b(6_1) \leq 1, gds(61)=1g_{ds}(6_1) = 1, with minimal-band ribbon surface using fewer bands than required for minimal-genus ribbon disk (McDonald, 2019).
  • Untwisted Whitehead double Wh(K)Wh(K) (for ribbon KK): ub(Wh(K))3u_b(Wh(K)) \leq 3, so gds(Wh(K))3g_{ds}(Wh(K)) \leq 3 (McDonald, 2019).
  • For torus knots T(p,q)T(p,q), once qp\frac{q}{p} is written in the specified continued-fraction expansion, the number of layers nn yields ub(T(p,q))=nu_b(T(p,q)) = n (Himeno, 20 Feb 2025).

6. Applications, Embeddings, and Open Problems

Band-unknotting numbers have meaningful consequences for 3- and 4-manifold topology and knot concordance:

  • Embeddings and slicing: gds(K)g_{ds}(K) bounds the minimal number nn so that Σ2(K)\Sigma_2(K) embeds in #nS2×S2\#_{n} S^2 \times S^2 (McDonald, 2019).
  • Ribbon fusion number: b(K)b(K) may be strictly less than the minimal-genus ribbon disk's band count. McDonald conjectures the existence of such knots, establishing the non-coincidence of band number and ribbon fusion number (McDonald, 2019).
  • Knots with isomorphic groups but differing unbu_{nb}: The knot group does not determine unbu_{nb}; for infinitely many alternating K1,K2K_1, K_2, one has π1(S3(K1#K2))π1(S3(K1#(K2ˉ)))\pi_1(S^3 \setminus (K_1 \# K_2)) \cong \pi_1(S^3 \setminus (K_1 \# (-\bar{K_2}))) but unb(K1#K2)unb(K1#(K2ˉ))u_{nb}(K_1\#K_2) \neq u_{nb}(K_1\#(-\bar{K_2})) (Ghanbarian et al., 6 Dec 2025).

Open questions remain regarding:

  • The possible strict decrease of unbu_{nb} under iterated connected sum,
  • Analogues for other band-type operations (e.g., nn-twisted band moves),
  • The construction of knots for which b(K)b(K) is strictly less than minimal genus ribbon disk band counts,
  • The realization of the theoretical bounds in infinite families.

7. Broader Significance and Research Directions

The study of band-unknotting numbers and generalizations provides profound connections between knot theory, 3-manifold topology, and 4-manifold theory. These invariants:

  • Bridge the combinatorial complexity of knot diagrams with the smooth and topological properties of surfaces in 3- and 4-manifolds.
  • Furnish new bounds and embedding theorems for branched covers, impacting the study of S4S^4, slice genus, and double slicing.
  • Reveal structural phenomena such as strict subadditivity and the independence of the band-unnoting number from group-theoretic knot invariants.
  • Motivate the development of new invariants (e.g., torsion order in Floer homology) and computational approaches for classical and satellite knots.

Continued research involves fine-tuning lower and upper bounds, exploring relationships with quantum invariants, and constructing explicit families illustrating extremal behavior and exceptional cases among these band-type unknotting invariants (McDonald, 2019, Ghanbarian et al., 6 Dec 2025, Himeno, 20 Feb 2025, Abe et al., 2011, Bao, 2010).

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