FiniteEnergyPlane.windPi_eq_windInf_sub_card

Data and hypotheses. Exactly the same as in exists_hasWindPi_of_nondegenerate: $H:\mathbb{R}^4\to\mathbb{R}$ has a strictly star-shaped level; $J$ is a compatible $\xi$-structure for $H$; $\Gamma\subset\mathbb{C}$ is a finite set (possibly empty); $u:\mathbb{C}\to\mathbb{R}^4$ is a finite-energy curve on $\mathbb{C}\setminus\Gamma$; $P_\infty$ is a Reeb orbit with $\mathrm{NdEnd}(u, \mathrm{cyl}_\infty, P_\infty, +1)$; for every $z\in\Gamma$ some Reeb orbit $P_z$ satisfies $\mathrm{NdEnd}(u, \mathrm{cyl}_z, P_z, -1)$; and there is $z\notin\Gamma$ with $\Pi(z)\neq0$, where

$$\Pi(z) = \Xi_{w(z)}\big(\pi_\xi(w(z))\,\partial_s w(z)\big)\in\mathbb{C},\qquad w = \mathrm{pr}\circ u.$$

Conclusion. There exist integers $k_\infty$, $k_\pi$ and a function $k:\mathbb{C}\to\mathbb{Z}$ such that

1. $\mathrm{wind}_\infty(u, \mathrm{cyl}_\infty, +1) = k_\infty$;
2. for every $z\in\Gamma$: $\mathrm{wind}_\infty(u, \mathrm{cyl}_z, -1) = k(z)$;
3. $\mathrm{wind}_\pi(u,\Gamma) = k_\pi$;
4. the integer identity

$$k_\pi = k_\infty - \sum_{z\in\Gamma} k(z) - 2 + (\#\Gamma + 1)$$

holds (equivalently $k_\pi = k_\infty - \sum_{z\in\Gamma}k(z) + \#\Gamma - 1$), where $\#\Gamma$ is the number of points of $\Gamma$.

Here:

• "$\mathrm{wind}_\infty(u, e, \varepsilon) = k$" means: there is $s_0$ such that for every $s\ge s_0$ the loop

$$t\mapsto \Xi_{W_e(s,\varepsilon t)}\Big(\pi_\xi\big(W_e(s,\varepsilon t)\big)\,\partial_s W_e(s,\varepsilon t)\Big)$$

has $\mathrm{wind} = k$, where $\partial_s W_e(s,t')$ is the derivative of $(s,t)\mapsto W_e(s,t)$ at $(s,t')$ in the direction $(1,0)$. For $\varepsilon = -1$ the loop is traversed with $t$ reversed.

• "$z_0$ is a zero of $f$ of index $m$" means: $f(z_0)=0$, there is $r>0$ with $f(z)\neq0$ for $0<|z-z_0|\le r$, and for every $\rho\in(0,r)$ the loop $t\mapsto f(z_0+\rho e^{2\pi it})$ has $\mathrm{wind}=m$.
• "$\mathrm{wind}_\pi(u,\Gamma) = k$" means: there is a finite set $Z$ with $z\in Z\iff(z\notin\Gamma$ and $\Pi(z)=0)$, and a function $\mathrm{idx}:\mathbb{C}\to\mathbb{Z}$ such that each $z\in Z$ is a zero of $\Pi$ of index $\mathrm{idx}(z)$ and $\sum_{z\in Z}\mathrm{idx}(z) = k$.

The values $k(z)$ for $z\notin\Gamma$ are irrelevant. The orbits $P_\infty$, $P_z$ are not required to be prime or distinct.

Meaning of the notions used

Throughout, the ambient space is $\mathbb{R}^4$ with coordinates $(y_0,y_1,y_2,y_3)$ (the code's space of functions on a 4-element index set), and $\mathbb{C}$ is identified with $\mathbb{R}^2$ via $z = s + it$.

Linear algebra. $j_0(v) = (-v_1, v_0, -v_3, v_2)$ and

$$\omega_0(u,v) = u_0v_1 - u_1v_0 + u_2v_3 - u_3v_2, \qquad \lambda_x(v) = \tfrac12\,\omega_0(x,v).$$

Star-shaped level. "$H$ has a strictly star-shaped level" means: $H:\mathbb{R}^4\to\mathbb{R}$ is $C^\infty$; for every $u\neq 0$ there is exactly one $r>0$ with $H(ru)=1$; and $dH_x(x) > 0$ at every $x$ with $H(x)=1$. Write $S = \{H = 1\}$.

Reeb field and contact plane. $X_H(x) = j_0(\nabla H(x))$, and $R(x) = \lambda_x(X_H(x))^{-1} X_H(x)$ (with the convention $0^{-1} = 0$). The plane $\xi_x$ is $\{v : \lambda_x(v) = 0 \text{ and } dH_x(v) = 0\}$ (defined for every $x$, not only on $S$). The projection $\pi_\xi$ is $\pi_\xi(x)v = v - \lambda_x(v)\,R(x)$.

Compatible $J$. "$J$ is a compatible $\xi$-structure for $H$" means: $J:\mathbb{R}^4\to \mathrm{L}(\mathbb{R}^4,\mathbb{R}^4)$ is $C^\infty$, and for every $x\in S$ and all $v,w\in\xi_x$: $J(x)v\in\xi_x$, $J(x)^2 v = -v$, $\omega_0(v,J(x)v) > 0$ if $v\neq 0$, and $\omega_0(J(x)v,J(x)w) = \omega_0(v,w)$. Nothing is required of $J(x)$ off $\xi_x$ or off $S$.

Radial projection. For $y\in\mathbb{R}^4$ let $\sigma(y)$ be the unique $r>0$ with $H(ry)=1$ if such $r$ exists, and $\sigma(y)=1$ otherwise (in particular $\sigma(0)=1$). Then $\mathrm{pr}(y) = \sigma(y)\,y$ and $a(y) = -\tfrac12\log\sigma(y)$.

Almost complex structure $\tilde J$. For $y\in\mathbb{R}^4$ put $x = \mathrm{pr}(y)$, $r=\sigma(y)$, $\alpha(v) = \frac{r}{2\,dH_x(x)}\,dH_x(v)$, $\beta(v) = r\,\lambda_x(v)$, $w(v) = v - 2\alpha(v)\,y - \beta(v)\,r^{-1}R(x)$, and

$$\tilde J(y)v = \alpha(v)\,r^{-1}R(x) - 2\beta(v)\,y + J(x)\,w(v).$$

Finite-energy curve. For $U\subseteq\mathbb{C}$, "$u$ is a finite-energy curve on $U$" means: $u:\mathbb{C}\to\mathbb{R}^4$ is $C^\infty$ on $U$; $u(z)\neq 0$ for $z\in U$; at every $z\in U$, $u$ is (real-)differentiable and $\partial_s u(z) + \tilde J(u(z))\,\partial_t u(z) = 0$; and

$$E(u) = \sup_{\varphi}\int_U \max\Big(0,\ \varphi'(a)\big(\partial_s a\,\lambda_w(\partial_t w) - \partial_t a\,\lambda_w(\partial_s w)\big) + \varphi(a)\,\omega_0(\partial_s w,\partial_t w)\Big)\,dz < \infty,$$

where $a = a\circ u$, $w = \mathrm{pr}\circ u$, and $\varphi$ ranges over $C^\infty$ nondecreasing functions $\mathbb{R}\to[0,1]$. Values of $u$ outside $U$ are unconstrained. Derivatives here and below are Fréchet derivatives, with the convention that the derivative at a point of non-differentiability is $0$.

Reeb orbit. A Reeb orbit $P$ of $H$ is a pair $(x,T)$ with $T>0$ and $x:\mathbb{R}\to\mathbb{R}^4$ such that $H(x(\tau)) = 1$, $x'(\tau) = R(x(\tau))$ and $x(\tau+T) = x(\tau)$ for all $\tau$. $T$ is any positive period (not necessarily the minimal one).

End parametrizations. $\mathrm{cyl}_\infty(s,t) = e^{2\pi s}e^{2\pi i t}$ (large circles, counterclockwise in $t$), and for $z_0\in\mathbb{C}$, $\mathrm{cyl}_{z_0}(s,t) = z_0 + e^{-2\pi s}e^{-2\pi i t}$ (small circles around $z_0$, clockwise in $t$). For such a map $e$ write $W_e(s,t) = \mathrm{pr}(u(e(s,t)))$ and $A_e(s,t) = a(u(e(s,t)))$. Note that only large $s$ enters the conditions below; for small $s$ these maps may leave the region where $u$ is constrained.

"Nondegenerate end". For $\varepsilon\in\mathbb{R}$, $\mathrm{NdEnd}(u, e, P, \varepsilon)$ means: there are $d, c\in\mathbb{R}$ and $b>0$ such that, uniformly in $t\in\mathbb{R}$, as $s\to+\infty$,

$$A_e(s,t) - \varepsilon T s - d \to 0, \qquad e^{bs}\,\big|W_e(s,t) - x(\varepsilon T t + c)\big| \to 0.$$

(This is an exponential convergence condition on $u$ along the end; it contains no hypothesis on the linearized Reeb flow of $P$.)

$\xi$-coordinates. For $x, v\in\mathbb{R}^4$, with $|x|$ the Euclidean norm, define $Q_1x = (-x_2, x_3, x_0, -x_1)$, $Q_2x = (x_3, x_2, -x_1, -x_0)$,

$$e_i(x) = |x|^{-1}\Big(Q_ix - \frac{dH_x(Q_ix)}{dH_x(x)}\,x\Big)\quad(i=1,2),$$

(with $0^{-1}=0$ and division by $0$ giving $0$), and

$$\Xi_x(v) = \omega_0(v, e_2(x)) + i\,\omega_0(e_1(x), v)\ \in\mathbb{C}.$$

Winding of a loop. For $f:\mathbb{R}\to\mathbb{C}$ and $k\in\mathbb{Z}$, $\mathrm{wind}(f) = k$ means: $f$ is continuous, $1$-periodic, never $0$, and there is a continuous $\theta:\mathbb{R}\to\mathbb{R}$ with $f(t) = |f(t)|e^{i\theta(t)}$ for all $t$ and $\theta(1) - \theta(0) = 2\pi k$.