TITLE: Can the orbits of a semigroup touch without one being included in the other?
QUESTION [7 upvotes]: Question. Let $(S(t))_{t \ge 0}$ be a continuous semigroup of linear operators on some Banach space $X$. Might there exist $f, g\in X$ and $0<t_0<t_1$ such that 
  \begin{equation}S(t_0)f=S(t_1)g\end{equation}
  but \begin{equation} S(t_0-\varepsilon_0)f\ne S(t_1-\varepsilon_1)g \end{equation}
  for all $0<\varepsilon_0\le t_0$ and $0<\varepsilon_1\le t_1$ (in particular, $f\ne g$)? 

Pictorially, I am wondering if the following configuration is possible:

Of course we know that, when the evolution is given by a group, this is not possible: orbits either coincide or are disjoint. This is the case of autonomous ODE systems or of the Schrödinger equation. But here we have a semi group, such as the heat one, which only goes forward in time, not backwards. So the only obvious thing that we can say is that, as soon as they touch, orbits merge into one. But in principle I don't see why they should coincide in the past. 
Added: After some searches, I have found that for the special case of the heat equation, the answer is negative. This is commonly referred to as backward uniqueness property. Here is a simplified version, which takes into account classical solutions on bounded domains: 
Theorem (Taken from Evans's book on PDE, 2nd ed., pag.64) Let $U\subset \mathbb{R}^n$ be an open and bounded domain. Suppose $u, \bar{u}$ are classical solutions of 
\begin{equation}
\begin{cases} u_t=\Delta u & \text{in }U\times(0, T) \\  u=0 &\text{on }\partial U \times [0, T] \end{cases}
\end{equation}
If at time $T$ we have 
\begin{equation}
u(x, T)=\bar{u}(x, T),\quad \forall x\in U,
\end{equation} 
then $u\equiv \bar{u}$ on the whole parabolic cylinder $U\times (0, T]$. 
The property holds in much more general functional settings, as I read here (look for the keyword backward uniqueness). 
All of this leaves the general question open. Is the backward uniqueness property true for all continuous linear semigroups? I guess that the answer should be negative, otherwise this would not be regarded as a special feature of the heat equation. However, I cannot find an explicit example.

REPLY [2 votes]: I believe this is a counterexample:
Consider the semigroup on $L_2[0,\infty)$ given by
$$ S(t) f(x) = f(x+t)$$
Let $f = I_{[0,1)}$, and $g = 2I_{[0,2)}$.  Then $S(1)f = S(2)g = 0$, but $S(1-\epsilon_1)f \ne S(2-\epsilon_2)g$.