Skip to content
Licensed Unlicensed Requires Authentication Published by De Gruyter January 4, 2022

A speed preserving Hilbert gradient flow for generalized integral Menger curvature

  • Jan Knappmann , Henrik Schumacher , Daniel Steenebrügge ORCID logo EMAIL logo and Heiko von der Mosel

Abstract

We establish long-time existence for a projected Sobolev gradient flow of generalized integral Menger curvature in the Hilbert case and provide C 1 , 1 -bounds in time for the solution that only depend on the initial curve. The self-avoidance property of integral Menger curvature guarantees that the knot class of the initial curve is preserved under the flow, and the projection ensures that each curve along the flow is parametrized with the same speed as the initial configuration. Finally, we describe how to simulate this flow numerically with substantially higher efficiency than in the corresponding numerical L 2 gradient descent or other optimization methods.

MSC 2010: 53C44; 35S10; 49Q10; 57M25

Award Identifier / Grant number: 320021702/GRK2326

Award Identifier / Grant number: 282535003

Funding statement: D. Steenebrügge is partially supported by the Graduiertenkolleg Energy, Entropy, and Dissipative Dynamics (EDDy) of the Deutsche Forschungsgemeinschaft (DFG) – project no. 320021702/GRK2326. H. Schumacher and H. von der Mosel gratefully acknowledge support from DFG project 282535003: Geometric curvature functionals: energy landscape and discrete methods. This work is also partially funded by the Excellence Initiative of the German federal and state governments.

A Periodic Sobolev–Slobodeckiǐ spaces

For fixed > 0 , s ( 0 , 1 ) and ϱ [ 1 , ) , define the seminorm

(A.1) [ f ] s , ϱ := ( R / Z - 2 2 | f ( u + w ) - f ( u ) | ϱ | w | 1 + s ϱ d w d u ) 1 ϱ

for ℓ-periodic functions f : R R n that are locally 𝜚-integrable on ℝ, i.e., for f L ϱ ( R / Z , R n ) .

Definition A.1

For k N { 0 } , the function space

W k + s , ϱ ( R / Z , R n ) := { f W k , ϱ ( R / Z , R n ) f W k + s , ϱ < } ,

where f W k + s , ϱ ( R / Z , R n ) := ( f W k , ϱ ( ( 0 , ) , R n ) ϱ + [ f ( k ) ] ϱ ) 1 ϱ , is called the periodic Sobolev–Slobodeckiǐ space with fractional differentiability of order k + s and integrability 𝜚. Here, W k , ϱ ( R / Z , R n ) W loc k , ϱ ( R , R n ) denotes the usual Sobolev space of ℓ-periodic functions whose weak derivatives f ( i ) of order i { 0 , , k } are locally 𝜚-integrable, where we have set f ( 0 ) := f .

Since the restriction of any ℓ-periodic Sobolev function f W k , ϱ ( R / Z , R n ) to its fundamental domain ( 0 , ) R is contained in the Sobolev space W k , ϱ ( ( 0 , ) , R n ) , it suffices to compare the seminorm (A.1) to the standard Gagliardo seminorm (which we denote by ) used in the literature on (non-periodic) Sobolev–Slobodeckiǐ spaces in order to transfer known results to the periodic setting. Indeed, for w ( - 2 , 2 ) , the absolute value | w | in the integrand of (A.1) equals the ℓ-periodic distance | w | R / Z = min k Z | w + k | so that we rewrite the seminorm (A.1) by substituting v ( w ) := u + w and estimate, for f L ϱ ( R / Z , R n ) ,

(A.2) [ f ] s , ϱ ϱ = R / Z - 2 2 | f ( u + w ) - f ( u ) | ϱ | w | 1 + s ϱ d w d u = R / Z - 2 2 | f ( u + w ) - f ( u ) | ϱ | w | R / Z 1 + s ϱ d w d u = R / Z u - 2 u + 2 | f ( v ) - f ( u ) | ϱ | v - u | R / Z 1 + s ϱ d v d u = 0 0 | f ( v ) - f ( u ) | ϱ | v - u | R / Z 1 + s ϱ d v d u 0 0 | f ( v ) - f ( u ) | ϱ | v - u | 1 + s ϱ d v d u = f s , ϱ ϱ ,

where we used the ℓ-periodicity of the integrand to shift the domain of the inner integration by - u + 2 .

As a first application of inequality (A.2), we show that the well-known Morrey embedding into classical Hölder spaces transfers to the periodic setting. To be more precise, the periodic Hölder seminorm for an ℓ-periodic function f : R R n and α ( 0 , 1 ] is defined as (cf. [18, Definition 3.2.5])

(A.3) Höl R / Z , α ( f ) := sup x , y [ 0 , ] x y | f ( x ) - f ( y ) | | x - y | R / Z α = sup x [ 0 , ] sup 0 < | w | 2 | f ( x + w ) - f ( x ) | | w | α ,

and the periodic Hölder space C k , α ( R / Z , R n ) for k N { 0 } consists of those functions f C k ( R / Z , R n ) whose Hölder norm satisfies f C k , α ( R / Z , R n ) := f C k ( R / Z , R n ) + Höl R / Z , α ( f ( k ) ) < . Notice that the second equality in (A.3) follows from the ℓ-periodicity of 𝑓 since, for any distinct x , y [ 0 , ] with, say, x < y , we find 0 w [ - 2 , 2 ] such that x + w = y , or x + = y + w , namely, w := y - x if | y - x | 2 , or w := - ( y - x ) if 2 < | y - x | .

Theorem A.2

Theorem A.2 (Morrey embedding)

Let k N { 0 } and ( 0 , ) . If ϱ ( 1 , ) and s ( 1 ϱ , 1 ) , then there is a positive constant C E = C E ( n , k , s , ϱ , ) such that

(A.4) f C k , s - 1 ϱ ( R / Z , R n ) C E f W k + s , ϱ ( R / Z , R n ) for all  f W k + s , ϱ ( R / Z , R n ) .

Proof

It suffices to treat the case k = 0 ; the full statement follows by induction. Moreover,

f C 0 ( R / Z , R n ) = f C 0 ( [ 0 , ] , R n )

for any ℓ-periodic function f : R R n so that we can focus on the periodic Hölder seminorm. Rewrite the numerator in (A.3) as | f τ x - 2 ( w + 2 ) - f τ x - 2 ( 2 ) | , where we used the shift τ a ( x ) := x + a for some fixed a R . Hence the right-hand side of (A.3) for α := s - 1 ϱ ( 0 , 1 ) may be rephrased by setting z := w + 2 and estimated from above as

sup x [ 0 , ] sup z [ 0 , ] z 2 | f τ x - 2 ( z ) - f τ x - 2 ( 2 ) | | z - 2 | s - 1 ϱ sup x [ 0 , ] Höl [ 0 , ] , s - 1 ϱ ( f τ x - 2 ) .

By virtue of the non-periodic Morrey embedding [15, Theorem 8.2] and (A.2), the right-hand side may be bounded from above by the expression sup x [ 0 , ] C f τ x - 2 W s , ϱ ( [ 0 , ] , R n ) sup x [ 0 , ] C f τ x - 2 W s , ϱ ( R / Z , R n ) for some constant C = C ( n , s , ϱ , ) . Changing variables via translations by x - 2 and using the ℓ-periodicity of the respective integrands in the W s , ϱ -norm, one can easily check that f τ x - 2 W s , ϱ ( R / Z , R n ) = f W s , ϱ ( R / Z , R n ) for each x R , which concludes the proof. ∎

We frequently make use of the following Poincaré inequality.

Proposition A.3

Proposition A.3 (Poincaré inequality)

For every ( 0 , ) , s ( 0 , 1 ) and ϱ [ 1 , ) , there is a constant C P = C P ( s , ϱ , ) such that

(A.5) f L ϱ ( R / Z , R n ) C P [ f ] s , ϱ for all f W s , ϱ ( R / Z , R n ) with R / Z f ( t ) d t = 0 .

Proof

By Jensen’s inequality, we have

R / Z | f ( u ) | ϱ d u = R / Z | f ( u ) - R / Z f ( t ) d t | ϱ d u R / Z R / Z | f ( u ) - f ( t ) | ϱ d t d u 1 | R / Z | ( 1 2 | R / Z | ) 1 + s ϱ R / Z R / Z | f ( u ) - f ( t ) | ϱ | u - t | R / Z 1 + s ϱ d t d u .

As a first application, we deal with the composition of Sobolev–Slobodeckiǐ functions.

Lemma A.4

Let L ( 0 , ) , ϱ ( 1 , ) , s ( 1 ϱ , 1 ) , g C 1 ( [ 0 , L ] ) with | g | > 0 on [ 0 , L ] , := g ( L ) - g ( 0 ) and f W 1 + s , ϱ ( R / Z , R n ) . Then 𝑔 can be extended to a function G C 1 ( R ) such that f G C 1 ( R / L Z , R n ) and G C 0 ( R / L Z ) , satisfying

(A.6) [ ( f G ) ] s , ϱ C ( [ G ] s , ϱ ϱ + v g - 1 G C 0 ( R / L Z ) ϱ ( 1 + s ) ) 1 ϱ [ f ] s , ϱ

for some constant C = C ( n , s , ϱ , ) , where v g := min [ 0 , L ] | g ( ) | > 0 .

Notice that both sides in (A.6) may be infinite as we do not assume that g W 1 + s , ϱ ( ( 0 , L ) ) . We should mention also that we have suppressed the respective domains [ 0 , L ] , or R / L Z , or R / Z , in our notation for the seminorms of 𝐺 and f G , or of 𝑓 in these inequalities.

Proof

In order to prove (A.6), we extend 𝑔 onto all of ℝ, first by setting G ( x ) := g ( x ) for x ( 0 , L ] and G ( x ) := g ( x - L ) + consecutively for x ( L , 2 L ] , ( 2 L , 3 L ] , , and then by G ( x ) := g ( x + L ) - consecutively for x ( - L , 0 ] , ( - 2 L , - L ] , ( - 3 L , - 2 L ] , , to find G ( x + L ) = G ( x ) + , G ( x + L ) = G ( x ) for all x R . We then bound the numerator in the integrand of the seminorm [ ( f G ) ] s , ϱ for x R and | w | L 2 from above as | ( f G ) ( x + w ) - ( f G ) ( x ) | ϱ 2 ϱ - 1 ( | G ( x + w ) | ϱ | f ( G ( x + w ) ) - f ( G ( x ) ) | ϱ | f ( G ( x ) ) | ϱ | G ( x + w ) - G ( x ) | ϱ ) , which leads to

(A.7) [ ( f G ) ] s , ϱ ϱ 2 ϱ - 1 R / L Z - L 2 L 2 | w | - α | G ( x + w ) | ϱ | f ( G ( x + w ) ) - f ( G ( x ) ) | ϱ d w d x + 2 ϱ - 1 f C 0 ( R / Z , R n ) ϱ [ G ] s , ϱ ϱ ,

where we have set α := 1 + ϱ s . Note that 𝑓 is of class C 1 ( R / Z , R n ) due to Theorem A.2. From now on, we may assume without loss of generality that the seminorm [ G ] s , ϱ is finite; otherwise, there is nothing to prove for (A.6). Substituting u ( w ) := x + w and using periodicity, we can rewrite the double integral as

(A.8) R / L Z - L 2 L 2 | u - x | R / L Z - α | G ( u ) | ϱ | f ( G ( u ) ) - f ( G ( x ) ) | ϱ d u d x .

With | G ( u ) - G ( x ) | R / Z | u - x | R / L Z G C 0 ( R / L Z ) , we obtain for the inverse function G - 1 : R R , for all x , u R ,

(A.9) | G - 1 ( G ( u ) ) - G - 1 ( G ( x ) ) | R / L Z = | u - x | R / L Z G C 0 ( R / L Z ) - 1 | G ( u ) - G ( x ) | R / Z .

Now we use the transformation Φ : ( R / L Z ) 2 ( R / Z ) 2 , ( u , x ) ( u ~ , x ~ ) := ( G ( u ) , G ( x ) ) with

| det ( D Φ ( u , x ) ) | = G ( u ) G ( x ) v g 2 > 0 for all x , u R

due to periodicity of G and G | [ 0 , L ] = g to rewrite and estimate (A.8) by means of (A.9) as

(A.10) ( R / Z ) 2 | G - 1 ( u ~ ) - G - 1 ( x ~ ) | R / L Z - α | G ( G - 1 ( u ~ ) ) | ϱ - 1 | G ( G - 1 ( x ~ ) ) | - 1 | f ( u ~ ) - f ( x ~ ) | ϱ d u ~ d x ~ ( A.9 ) v g - 1 G C 0 ( R / L Z ) ϱ - 1 + α [ f ] s , ϱ ϱ = v g - 1 G C 0 ( R / L Z ) ϱ ( 1 + s ) [ f ] s , ϱ ϱ .

The C 0 -norm of f in (A.7) may be bounded by C E C P [ f ] s , ϱ according to the Morrey embedding, Theorem A.2, and the Poincaré inequality, Proposition A.3, and combining this with (A.10) leads to (A.6) with the constant C := ( 2 ϱ - 1 ( ( C E C P ) ϱ + 1 ) ) 1 ϱ . ∎

The following result provides an estimate for the Sobolev–Slobodeckiǐ norms of products of functions of fractional Sobolev regularity.

Proposition A.5

Proposition A.5 (Bounds on inner product)

Let k N { 0 } , ( 0 , ) , ϱ ( 1 , ) and s ( 1 ϱ , 1 ) . Then there is a constant C = C ( n , k , s , ϱ , ) ( 0 , ) such that

f ( ) , g ( ) R n W k + s , ϱ ( R / Z ) C f W k + s , ϱ ( R / Z , R n ) g W k + s , ϱ ( R / Z , R n ) for all f , g W k + s , ϱ ( R / Z , R n ) .

Proof

For brevity, we write ξ , ζ := ξ , ζ R n for ξ , ζ R n , and then F , G := F ( ) , G ( ) for any two functions F , G : R R n . By virtue of the Morrey embedding, Theorem A.2, the functions f , g are both of class C k . Then, according to the Leibniz rule, we have, for every 0 i k ,

(A.11) f , g ( i ) = j = 0 i ( i j ) f ( j ) , g ( i - j ) ,

of which the L ϱ -norm can be estimated as

f , g ( i ) L ϱ ( R / Z ) ϱ = R / Z | j = 0 i ( i j ) f ( j ) ( x ) , g ( i - j ) ( x ) | ϱ d x 2 ( 2 ϱ - 1 ) i f W i , ϱ ( R / Z , R n ) ϱ g C i ( R / Z , R n ) ϱ for all 0 i k ,

which implies by means of the Morrey embedding (A.4) that the Sobolev norm f , g W k , ϱ ϱ may be bounded from above by

(A.12) C E ϱ ( k + 1 ) 2 ( 2 ϱ - 1 ) k f W k , ϱ ( R / Z , R n ) ϱ g W k + s , ϱ ( R / Z , R n ) ϱ .

The numerator of the integrand in the seminorm [ f , g ( k ) ] s , ϱ can be estimated from above by means of (A.11) similarly to before by

2 ( 2 ϱ - 1 ) k j = 0 k | f ( j ) , g ( k - j ) ( x + w ) - f ( j ) , g ( k - j ) ( x ) | ϱ 2 ( 2 ϱ - 1 ) ( k + 1 ) j = 0 k { | f ( j ) ( x + w ) , g ( k - j ) ( x + w ) - g ( k - j ) ( x ) | ϱ + | f ( j ) ( x + w ) - f ( j ) ( x ) , g ( k - j ) ( x ) | ϱ } for x R , | w | 2 ,

which may be bounded by

2 ( 2 ϱ - 1 ) ( k + 1 ) j = 0 k { f C k ( R / Z , R n ) ϱ | g ( j ) ( x + w ) - g ( j ) ( x ) | ϱ + g C k ( R / Z , R n ) ϱ | f ( j ) ( x + w ) - f ( j ) ( x ) | ϱ } for x R , | w | 2 .

Integrating this against | w | - ( 1 + s ϱ ) and using the Morrey embedding inequality (A.4), we find

[ f , g ( k ) ] s , ϱ ϱ 2 ( 2 ϱ - 1 ) ( k + 1 ) { f C k ( R / Z , R n ) ϱ j = 0 k [ g ( j ) ] s , ϱ ϱ + g C k ( R / Z , R n ) ϱ j = 0 k [ f ( j ) ] s , ϱ ϱ } ( A.4 ) 2 ( 2 ϱ - 1 ) ( k + 1 ) C E ϱ { f W k + s , ϱ ( R / Z , R n ) ϱ j = 0 k [ g ( j ) ] s , ϱ ϱ + g W k + s , ϱ ( R / Z , R n ) ϱ j = 0 k [ f ( j ) ] s , ϱ ϱ } .

For i < k , we observe that

[ g ( i ) ] s , ϱ ϱ = R / Z - 2 2 | g ( i ) ( u + w ) - g ( i ) ( u ) | ϱ | w | - ( 1 + s ϱ ) d w d u g ( i + 1 ) L ( R / Z , R n ) ϱ - 2 2 | w | ϱ - 1 - s ϱ d w = : g ( i + 1 ) L ( R / Z , R n ) ϱ c ( s , ϱ , ) ( A.4 ) C E ϱ g W k + s , ϱ ( R / Z , R n ) ϱ c ( s , ϱ , )

since ϱ - 1 - s ϱ > ϱ - 2 > - 1 and by Morrey’s embedding (A.4). Analogous estimates hold for the seminorms of f ( j ) , which combine with (A.12) to the inequality as claimed with constant

C ( n , k , s , ϱ , ) := 2 ( 2 ϱ - 1 ) ( k + 1 ) ϱ C E ( k + 1 ) 1 ϱ [ 1 + 2 c ( s , ϱ , ) C E ϱ ] 1 ϱ .

Notice that target dimension 𝑛 enters this constant through the Morrey embedding constant C E ; cf. Theorem A.2. ∎

We conclude this section with an estimate on the fractional Sobolev norm of the multiplicative inverse of a non-vanishing Sobolev–Slobodeckiǐ function.

Lemma A.6

Let ( 0 , ) , ϱ ( 1 , ) , s ( 1 ϱ , 1 ) , c > 0 and h W s , ϱ ( R / Z ) with | h ( x ) | c for almost all x R . Then the multiplicative inverse 1 h : R R , x 1 h ( x ) is in W s , ϱ ( R / Z ) , and we have

1 h W s , ϱ ( R / Z ) h W s , ϱ ( R / Z ) c 2 .

Proof

The estimate

1 h L ϱ ( R / Z ) ϱ 1 h L ( R / Z ) ϱ c ϱ

follows immediately from the pointwise lower bound on ℎ. The integrand of the seminorm [ 1 h ] s , ϱ may be estimated as | w | - 1 - s ϱ | h ( x + w ) | - ϱ | h ( x ) | - 1 ϱ | h ( x + w ) - h ( x ) | ϱ c - 2 ϱ | w | - 1 - s ϱ | h ( x + w ) - h ( x ) | ϱ , which implies [ 1 h ] s , ϱ ϱ c - 2 ϱ [ h ] s , ϱ ϱ , and together with h L ϱ ( R / Z ) ϱ c ϱ , we obtain the desired estimate for 1 h W s , ϱ ( R / Z ) . ∎

B Arc length and bilipschitz constants

Whenever we speak about the arc length parametrization of a curve γ W 1 , 1 ( R / Z , R n ) with | γ | > 0 a.e. on ℝ and with length L := L ( γ ) ( 0 , ) , we refer to the mapping Γ := γ L ( γ , ) - 1 C 0 , 1 ( R / L Z , R n ) obtained from the inverse L ( γ , ) - 1 of the strictly increasing arc length function L ( γ , ) of class W loc 1 , 1 ( R ) defined as

(B.1) L ( γ , x ) := 0 x | γ ( y ) | d y for x R .

Notice that L ( γ , x + ) = L ( x ) + L , ( L ( γ , x + ) ) = ( L ( γ , x ) ) for all x R , as well as L ( γ , z + L ) - 1 = L ( γ , z ) - 1 + for all z R , and therefore, the composition Γ = γ L ( γ , ) - 1 is 𝐿-periodic and 1-Lipschitz because of

| d d s Γ ( s ) | = | γ ( L ( γ , s ) - 1 ) 1 | γ ( x ) | x = L ( γ , s ) - 1 | = 1 for a.e. s [ 0 , L ] .

Recall from the introduction the definition of the bilipschitz constant (1.15) and the notation W ir 1 , 1 ( R / Z , R n ) for the subset of all regular W 1 , 1 -curves such that their restriction to the fundamental interval [ 0 , ) is injective.

Lemma B.1

Let ( 0 , ) and γ W ir 1 , 1 ( R / Z , R n ) with length L := L ( γ ) ( 0 , ) and with arc length parametrization Γ W 1 , ( R / L Z , R n ) . Then the bilipschitz constants of 𝛾 and Γ are related by

(B.2) BiLip ( γ ) [ v γ BiLip ( Γ ) , v γ ] ,

where v γ = ess inf [ 0 , ] | γ ( ) | 0 .

Proof

The upper bound on BiLip ( γ ) in (B.2) follows immediately from the estimate

| γ ( x ) | = lim h 0 | h | R / Z - 1 | γ ( x + h ) - γ ( x ) | BiLip ( γ )

at points x R / Z where γ ( u ) exists. Taking the infimum over all such x R / Z establishes the upper bound in (B.2). For the proof of the lower bound in (B.2), assume without loss of generality that 0 y x < so that, by monotonicity, 0 L ( γ , y ) L ( γ , x ) < L . Then | γ ( x ) - γ ( y ) | can be written as and estimated from below by

(B.3) | Γ L ( γ , x ) - Γ L ( γ , y ) | BiLip ( Γ ) | L ( γ , x ) - L ( γ , y ) | R / L Z .

If | L ( γ , x ) - L ( γ , y ) | R / L Z = | L ( γ , x ) - L ( γ , y ) | = ( L ( γ , x ) - L ( γ , y ) ) , then the distance on the right-hand side of (B.3) equals y x | γ ( τ ) | d τ v γ ( x - y ) = v γ | x - y | v γ | x - y | R / Z , which proves the claim in this case. If, on the other hand, | L ( γ , x ) - L ( γ , y ) | R / L Z = L - | L ( γ , x ) - L ( γ , y ) | , the latter can be written as

L - ( L ( γ , x ) - L ( γ , y ) ) = L - y x | γ ( τ ) | d τ = 0 y | γ ( τ ) | d τ + x | γ ( τ ) | d τ ,

which can be bounded from below by v γ ( y + - x ) = v γ ( - | x - y | ) v γ | x - y | R / Z , and this again can be inserted into (B.3) to yield the desired inequality (B.2). ∎

Lemma B.2

Lemma B.2 (Seminorm of arc length)

Let s ( 0 , 1 ) , ϱ ( 1 , ) and γ W 1 , ϱ ( R / Z , R n ) . Then

[ ( L ( γ , ) ) ] s , ϱ [ γ ] s , ϱ .

Note that the right-hand side of this estimate might be infinite since we did not assume that 𝛾 is of class W 1 + s , ϱ ( R / Z , R n ) .

Proof

If the seminorm on the right-hand side is infinite, there is nothing to prove. If, on the other hand, γ W 1 + s , ϱ ( R / Z , R n ) , then we estimate

[ ( L ( γ , ) ) ] s , ϱ ϱ = R / Z - 2 2 | w | - 1 - s ϱ | | γ ( x + w ) | - | γ ( x ) | | ϱ d w d x R / Z - 2 2 | w | - 1 - s ϱ | γ ( x + w ) - γ ( x ) | ϱ d w d x = [ γ ] s , ϱ ϱ .

The bilipschitz constant BiLip ( γ ) , defined in (1.15), of a closed embedded, i.e., immersed and injective, C 1 -curve is strictly positive since, under this regularity assumption, the quotient in (1.15) converges to | γ ( u 2 ) | v γ = min [ 0 , ] | γ | > 0 as u 1 u 2 . This means that this positive quotient possesses a continuous extension onto all of R × R , which is bounded by a positive constant from below by periodicity and continuity. We now quantify a neighbourhood of such a curve 𝛾, in which the bilipschitz constant remains under control.

Lemma B.3

Let ( 0 , ) , and let γ C 1 ( R / Z , R n ) be injective on [ 0 , ) with | γ | > 0 on ℝ. Then

(B.4) BiLip ( η ) 1 2 BiLip ( γ ) > 0

for all η C 1 ( R / Z , R n ) with η - γ C 0 ( R / Z , R n ) 1 2 BiLip ( γ ) .

Proof

It suffices to prove the first inequality in (B.4), and for that, assume without loss of generality that 0 y x < . We have

(B.5) | η ( x ) - η ( y ) | | γ ( x ) - γ ( y ) | - | ( η - γ ) ( x ) - ( η - γ ) ( y ) | .

If | x - y | R / Z = | x - y | = ( x - y ) , then we can estimate the right-hand side from below by

BiLip ( γ ) | x - y | R / Z - y x | ( η - γ ) ( τ ) | d τ BiLip ( γ ) | x - y | R / Z - η - γ C 0 ( R / Z , R n ) | x - y | R / Z

which is bounded from below by 1 2 BiLip ( γ ) | x - y | R / Z . If, on the other hand,

| x - y | R / Z = - | x - y | = - ( x - y ) ,

then we use the ℓ-periodicity to replace the term ( η - γ ) ( y ) in (B.5) by ( η - γ ) ( + y ) to estimate the right-hand side of (B.5) from below by BiLip ( γ ) | x - y | R / Z - x + y | ( η - γ ) ( τ ) | d τ , which can be bounded from below by BiLip ( γ ) | x - y | R / Z - η - γ C 0 ( R / Z , R n ) | x - y | R / Z 1 2 BiLip ( γ ) | x - y | R / Z , which concludes the proof. ∎

The following corollary quantifies the fact that the set W ir 1 + s , ϱ ( R / Z , R n ) of all regular embedded Sobolev–Slobodeckiǐ loops is an open subset of that fractional Sobolev space if that space embeds into C 1 ( R / Z , R n ) .

Corollary B.4

Let ( 0 , ) , ϱ ( 1 , ) and s ( 1 ϱ , 1 ) , and suppose γ W ir 1 + s , ϱ ( R / Z , R n ) . Then BiLip ( γ ) > 0 , and one has, for the bilipschitz constant BiLip ( η ) and the minimal velocity v η := min [ 0 , ] | η | ,

(B.6) BiLip ( η ) 1 2 BiLip ( γ ) and v η v γ 2

for all η W 1 + s , ϱ ( R / Z , R n ) satisfying [ η - γ ] s , ϱ ( 2 C E C P ) - 1 BiLip ( γ ) , where C E = C E ( n , s , ϱ , ) denotes the constant in (A.4) of the Morrey embedding, Theorem A.2, and C P = C P ( n , s , ϱ , ) is the constant in the Poincaré inequality (A.5).

Notice that, neither in this corollary nor in the preceding Lemma B.3, anything is required about the C 0 -distance between the curves, so in principle, 𝛾 and 𝜂 could be very far apart in R n .

Proof

By the Morrey embedding, Theorem A.2, the curve 𝛾 is of class C 1 so that BiLip ( γ ) > 0 . Moreover, again by Theorem A.2, in combination with the Poincaré inequality, Proposition A.3, we estimate, using our assumption on 𝜂,

η - γ C 0 ( R / Z , R n ) ( A.4 ) C E η - γ W s , ϱ ( R / Z , R n ) ( A.5 ) C E C P [ η - γ ] s , ϱ 1 2 BiLip ( γ )

so that we can apply Lemma B.3 to finish the proof. Similarly, again by Morrey’s embedding (A.4) and Poincaré’s inequality (A.5), one finds

v η v γ - η - γ C 0 ( R / Z , R n ) v γ - C E C P [ η - γ ] 3 2 p - 3 , 2 > v γ - 1 2 BiLip ( γ ) v γ 2 > 0 .

Acknowledgements

Parts of Section 2 are contained in J. Knappmann’s Ph.D. thesis [23], and some of the content of Sections 36 will appear in D. Steenebrügge’s Ph.D. thesis [33].

  1. Communicated by: Frank Duzaar

References

[1] R. Abraham, J. E. Marsden and T. Ratiu, Manifolds, Tensor Analysis, and Applications, 2nd ed., Appl. Math. Sci. 75, Springer, New York, 1988. 10.1007/978-1-4612-1029-0Search in Google Scholar

[2] H. W. Alt, Linear Functional Analysis, Universitext, Springer, London, 2016. 10.1007/978-1-4471-7280-2Search in Google Scholar

[3] T. Ashton, J. Cantarella, M. Piatek and E. J. Rawdon, Knot tightening by constrained gradient descent, Exp. Math. 20 (2011), no. 1, 57–90. 10.1080/10586458.2011.544581Search in Google Scholar

[4] S. Bartels and P. Reiter, Stability of a simple scheme for the approximation of elastic knots and self-avoiding inextensible curves, Math. Comp. 90 (2021), no. 330, 1499–1526. 10.1090/mcom/3633Search in Google Scholar

[5] S. Bartels, P. Reiter and J. Riege, A simple scheme for the approximation of self-avoiding inextensible curves, IMA J. Numer. Anal. 38 (2018), no. 2, 543–565. 10.1093/imanum/drx021Search in Google Scholar

[6] S. Blatt, Note on continuously differentiable isotopies, Report no. 34, Institute for Mathematics, RWTH Aachen, 2009, http://www.instmath.rwth-aachen.de/Preprints/blatt20090825.pdf. Search in Google Scholar

[7] S. Blatt, The gradient flow of the Möbius energy near local minimizers, Calc. Var. Partial Differential Equations 43 (2012), no. 3–4, 403–439. 10.1007/s00526-011-0416-9Search in Google Scholar

[8] S. Blatt, A note on integral Menger curvature for curves, Math. Nachr. 286 (2013), no. 2–3, 149–159. 10.1002/mana.201100220Search in Google Scholar

[9] S. Blatt, The gradient flow of O’Hara’s knot energies, Math. Ann. 370 (2018), no. 3–4, 993–1061. 10.1007/s00208-017-1540-4Search in Google Scholar

[10] S. Blatt, The gradient flow of the Möbius energy: 𝜀-regularity and consequences, Anal. PDE 13 (2020), no. 3, 901–941. 10.2140/apde.2020.13.901Search in Google Scholar

[11] S. Blatt and P. Reiter, Towards a regularity theory for integral Menger curvature, Ann. Acad. Sci. Fenn. Math. 40 (2015), no. 1, 149–181. 10.5186/aasfm.2015.4006Search in Google Scholar

[12] H. Cartan, Differential Calculus, Hermann, Paris, 1971. Search in Google Scholar

[13] R. H. Crowell and R. H. Fox, Introduction to Knot Theory, Grad. Texts in Math. 57, Springer, New York, 1977. 10.1007/978-1-4612-9935-6Search in Google Scholar

[14] E. Denne and J. M. Sullivan, Convergence and isotopy type for graphs of finite total curvature, Discrete Differential Geometry, Oberwolfach Semin. 38, Birkhäuser, Basel (2008), 163–174. 10.1007/978-3-7643-8621-4_8Search in Google Scholar

[15] E. Di Nezza, G. Palatucci and E. Valdinoci, Hitchhiker’s guide to the fractional Sobolev spaces, Bull. Sci. Math. 136 (2012), no. 5, 521–573. 10.1016/j.bulsci.2011.12.004Search in Google Scholar

[16] P. Drábek and J. Milota, Methods of Nonlinear Analysis, 2nd ed., Birkhäuser Adv. Texts Basler Lehrbücher, Birkhäuser/Springer, Basel, 2013. Search in Google Scholar

[17] A. Gilsbach, On symmetric critical points of knot energies, PhD thesis, RWTH Aachen University, 2018, https://publications.rwth-aachen.de/record/726186/. Search in Google Scholar

[18] L. Grafakos, Classical Fourier Analysis, 2nd ed., Grad. Texts in Math. 249, Springer, New York, 2008. 10.1007/978-0-387-09432-8Search in Google Scholar

[19] M. Gromov, Filling Riemannian manifolds, J. Differential Geom. 18 (1983), no. 1, 1–147. 10.4310/jdg/1214509283Search in Google Scholar

[20] T. Hermes, Analysis of the first variation and a numerical gradient flow for integral Menger curvature, PhD thesis, RWTH Aachen University, 2012, https://publications.rwth-aachen.de/record/82904/. Search in Google Scholar

[21] K. Hoffman and R. Kunze, Linear Algebra, 2nd ed., Prentice-Hall, Englewood Cliffs, 1971. Search in Google Scholar

[22] J. F. P. Hudson and E. C. Zeeman, On combinatorial isotopy, Publ. Math. Inst. Hautes Études Sci. (1964), no. 19, 69–94. 10.1007/BF02684797Search in Google Scholar

[23] J. Knappmann, On the second variation of integral Menger curvature, PhD thesis, RWTH Aachen University, 2020, https://publications.rwth-aachen.de/record/802770/. Search in Google Scholar

[24] C.-C. Lin and H. R. Schwetlick, On a flow to untangle elastic knots, Calc. Var. Partial Differential Equations 39 (2010), no. 3–4, 621–647. 10.1007/s00526-010-0328-0Search in Google Scholar

[25] J. W. Neuberger, Sobolev Gradients and Differential Equations, Lecture Notes in Math. 1670, Springer, Berlin, 1997. 10.1007/BFb0092831Search in Google Scholar

[26] J. Nocedal and S. J. Wright, Numerical Optimization, 2nd ed., Springer Ser. Oper. Res. Financ. Eng., Springer, New York, 2006. Search in Google Scholar

[27] S. Redon, A. Kheddar and S. Coquillart, Fast continuous collision detection between rigid bodies, Comput. Graph. Forum 21 (2002), no. 3, 279–287. 10.1111/1467-8659.t01-1-00587Search in Google Scholar

[28] P. Reiter, All curves in a C 1 -neighbourhood of a given embedded curve are isotopic, Report no. 4, Institute for Mathematics, RWTH Aachen, 2005, https://www.instmath.rwth-aachen.de/Preprints/reiter20051017.pdf. Search in Google Scholar

[29] P. Reiter and H. Schumacher, Sobolev Gradients for the Möbius Energy, Arch. Ration. Mech. Anal. 242 (2021), no. 2, 701–746. 10.1007/s00205-021-01680-1Search in Google Scholar

[30] W. Rudin, Functional Analysis, McGraw-Hill Ser. High. Math., McGraw-Hill, New York, 1973. Search in Google Scholar

[31] R. Scharein, KnotPlot, 2017, Program for drawing, visualizing, manipulating, and energy minimizing knots, http://www.knotplot.com. Search in Google Scholar

[32] S. Scholtes, H. Schumacher and M. Wardetzky, Variational convergence of discrete elasticae, IMA J. Numer. Anal. (2020), 10.1093/imanum/draa084. 10.1093/imanum/draa084Search in Google Scholar

[33] D. Steenebrügge, Parametrization-controlling gradient flows and regularity of critical points for knot energies, PhD thesis, RWTH Aachen University, 2022. Search in Google Scholar

[34] P. Strzelecki, M. Szumańska and H. von der Mosel, Regularizing and self-avoidance effects of integral Menger curvature, Ann. Sc. Norm. Super. Pisa Cl. Sci. (5) 9 (2010), no. 1, 145–187. 10.2422/2036-2145.2010.1.06Search in Google Scholar

[35] P. Strzelecki and H. von der Mosel, Menger curvature as a knot energy, Phys. Rep. 530 (2013), no. 3, 257–290. 10.1016/j.physrep.2013.05.003Search in Google Scholar

[36] J. H. von Brecht and R. Blair, Dynamics of embedded curves by doubly-nonlocal reaction-diffusion systems, J. Phys. A 50 (2017), no. 47, Article ID 475203. 10.1088/1751-8121/aa9109Search in Google Scholar

[37] H. Whitney, Geometric Integration Theory, Princeton University, Princeton, 1957. 10.1515/9781400877577Search in Google Scholar

[38] C. Yu, C. Brakensiek, H. Schumacher and K. Crane, Repulsive surfaces, preprint (2021), https://arxiv.org/abs/2107.01664. Search in Google Scholar

[39] C. Yu, H. Schumacher and K. Crane, Repulsive curves, ACM Transactions on Graphics 40 (2021), no. 2, 1–21. 10.1145/3439429Search in Google Scholar

[40] E. Zeidler, Nonlinear Functional Analysis and its Applications. I: Fixed-Point Theorems, Springer, New York, 1993. Search in Google Scholar

Received: 2021-04-09
Revised: 2021-07-17
Accepted: 2021-10-08
Published Online: 2022-01-04
Published in Print: 2023-07-01

© 2022 Walter de Gruyter GmbH, Berlin/Boston

Downloaded on 1.12.2023 from https://www.degruyter.com/document/doi/10.1515/acv-2021-0037/html
Scroll to top button