$AD, BE, CF$ are the three heights of $\Delta ABC$, and they concurrent at $H$. $P, Q, R$ are the incenters of $\Delta AQR, \Delta > BRP, \Delta CPQ$, respectively. $\odot (BPR)$ and $ \odot (CPQ) $ intersect with $ \odot (AQR)$ again at $K$ and $L$, respectively. $\odot (BPR)$ and $ \odot (CPQ) $ intersect with $ \odot (ABC)$ again at $S$ and $T$, respectively. $\odot(SKH)$ and $ \odot (LTH)$ intersect with each other again at $X$ Show that:
1) $K,S,T,L$ are cyclic
2) $P,H,X$ are colinear
What I thought: $P$ is the incenter of $\Delta AEF$, where $BE \perp AC$ at $E$, $CF \perp AB$ at $ F$. $Q$ and $R$ are defined analogously.

It is clear that the "composer" of the problem constructed a very special situation for (1), and did not want to tell us which are the "minimal requirements" for the points $A,B,C;P,Q,R$, so that the result in (1) is still holding. The solution of the problem goes then through the step of finding such a "minimal configuration" of points.
(Personally i do not consider is it a good idea to make out a clean geometry situation an overloaded situation by passing to very particular cases, so that it becomes a puzzle.)
So in order to solve the puzzle, i have to extract the following situation, with points having names obtained by applying an inversion $W\to W^*$ centered in $A$ starting from the given situation.
Proof: Let $Z$ be the intersection of $P^*Q^*$ and $B^*C^*$. We will denote by the small capital letter $x$ the lenghth of $ZX^*$, so for instance $b=ZB^*$. The using the powers of $Z$ w.r.t. the given circles we have $bs=kr$, $ct=ql$, and $bc=qr$. From the first two relations we get $$ bcst=qrkl\ ,$$ and dividing with the third one, $st=kl$, which means that the four constructed intersections are on a circle.
$\square$
Proof: The marked angles based in $A,B,C;D,E,F$ having measures $x,y,z$ are clear.
We show now the metric relation. First of all, the triangles $\Delta ABC$ and $\Delta AEF$ are similar (in this order of vertices), so the constructed distances from $A$ to the incenters are also respecting the same similarity factor, $$ \frac{AP}{AI}= \frac{AE}{AB}=\cos A=\cos (2x)\ . $$ This implies $$ IA\cdot IP=(1-\cos (2x))\cdot IA^2=2\sin ^2 x\cdot IA^2\ . $$ Similar relations for the other two products. The claimed relation follows now from the sine theorem applied for (two of) the triangles $\Delta IBC$, $\Delta ICA$, $\Delta IAB$. For instance, in the first triangle we have $$ \frac{IB}{\sin z}=\frac{IC}{\sin y}\ . $$ From the obtained metric relation, the following quadrilaterals are cyclic: $BCRQ$, $CAPR$, $ABQP$. This explains the distribution of the marked angles inside $\Delta PQR$.
$\square$
Proof of (1): We have shown above in the Result 1.2 that $B,C,Q,R$ are on a circle. Let us apply an inversion centered in $A$, denoted by $*$. Then the image points $B^*,C^*,Q^*,R^*$ are on a circle and we are in the position to apply the Result 1.1, showing that $K^*,S^*, T^*, L^*$ are on a circle. These points, constructed as in Result 1.1 are the images of the points $K,S,T,L$ from the OP, since by inversion, we have the following transformations:
And intersections correspond to intersections.
We apply the same inversion "back" to see that the circle $(K^*S^*T^* L^*)$ transforms in a circle $KSTL$.
$\square$
Now for the second part we also have to isolate a simple configuration first, this will be Result 2.1, then show that the hypotesis of this result is matched in the complicated figure we start with.
Proof: After an inversion, we can and do assume w.l.o.g. that the four starting points $S,K,T,L$ are on a line. We now apply a further inversion with center in $S$. It moves $S$ to an infinity point and the two circles $C,\Gamma$ through $S$ are mapped into lines. We assume w.l.o.g. that we have this situation, and do not introduce notations to show the difference. The picture is now as follows:
From the transfer of powers w.r.t. the two remained circles and the point $K$, using the intermediate power $KT\cdot KL$, $$ KP\cdot KY = KT\cdot KL =KH\cdot KX $$ we obtain immediately $P,Y,H,X$ on a circle.
$\square$
It is now clear, that we "only" have to show for (2) in the OP the following...
Proof: Here i am missing a synthetic idea, so in order to buy my freedom and submit a solution the proof will be an analytic one, using barycentric coordinates. Computations are straightforward.
Let $a,b,c$ be the (lengths of the) sides of $\Delta ABC$.
A point $W$ has (true) barycentric coordinates $x,y,z$ if $x+y+z=1$ and $W=xA+yB+zC$ (afix computation), i.e. iff for one or any reference point $O$ in the plane we have (vectorially) $OW=xOA+yOB+zOC$. Sometimes, rather often, we use the notation $(x:y:z)$ for the coordinates, in this case one has to divide by the sum $x+y+z\ne 0$, so $(x:y:z)$ is $\displaystyle \left( \frac x{x+y+z}, \frac y{x+y+z}, \frac z{x+y+z} \right) $.
Barycentric coordinates are collected for instance in the ETC (encyclopedia of triangle centers). Central triangles are also important in the context. (The triangle $PQR$ is one of them, i can not identify which on right now.)
The incenter $I=X(1)$ has (inhomogenous) barycentric coordinates $(a:b:c)$. The point $A$ has coordinates $(1:0:0)$. The point $P$ is on $IA$ and we have already computed $AP:AI=\cos A$, so $$ \begin{aligned} P &=\cos A\cdot I + (1-\cos A)\cdot A\\ &=\cos A\left(\ \frac a{a+b+c},\ \frac b{a+b+c},\ \frac c{a+b+c}\ \right) + (1-\cos A)(1,0,0) \\ &=\left(\ 1- \cos A\frac {b+c}{a+b+c},\ \cos A\frac b{a+b+c},\ \cos A\frac c{a+b+c}\ \right) \\ &=\left(\ \frac {a+b+c}{\cos A}-(b+c)\ :\ b\ :\ c\ \right) \\ &=(x_P:b:c)\ . \end{aligned} $$ The expression $x_P$ is defined by the last line.
Similar computations give $Q=(a:y_Q:c)$, and $R=(a:b:z_R)$ with similar expressions for $y_Q$, $z_R$.
(We can replace at any point $\cos A$ by the rational expression in $a,b,c$ extracted from $a^2=b^2+c^2-2bc\cos A$. The other cosine values for $B,C$, too.)
The general homogenous equation of a circle in barycentric coordinates $(x:y:z)$ is $$ 0=-a^2yz-b^2xz-c^2xy +(ux+vy+wz)(x+y+z)\ . $$ We need the specific equation for the circle $(CPQ)$ first, and denote by $u_1,v_1,w_1$ the matching coefficients. (I.e. the specific values for the unknowns $u,v,w$ that verify.) Since $C(0,0,1)$ verifies, we get for instance immediately $w_1=0$. The other values are not so simple, so i decided to get computer help, here sage. For the circle $(BPQ)$ we obtain coefficients $u_2,v_2,w_2$, as a matter of notation, and this time $v_2=0$ since $B(0,1,0)$ verifies the equation.
The following sage code checks in a simple manner, that the orthocenter $$ H=(\tan A:\tan B:\tan C) = \left( \frac a{\cos A}: \frac b{\cos B}: \frac c{\cos C} \right) $$ is on the line $(u_1-u_2)x+(v_1-v_2)y+(w_1-w_2)z=0$, which is the intersection of the two circles, obtained by formally subtracting there equations. (And dividing by $x+y+z\ne 0$.)
The above delivers a clean zero. This was the check.
$\square$
I am not proud of this solution, but somehow i have to part in peace with the whole ticket. The above is in my eyes a valid solution. It may be desirable in such situations to have a less analytic solution, best would be to provide a synthetic solution, so that esthetic criteria are not hurt, well, if i find a short one i will insert it next days.
Proof of (2):
We can now conclude using the two results above (if this is not already done). We apply Result 2.1 mot-a-mot for the letters from the OP, so the four points $P,Y;H,X$ are either on a line or on a circle. From Result 2.2 the points $P,H,Y$ are on a line, so the circle is a line. (And we have four points known on it.)
$\square$
A final comment. After the whole procession we have a result which is a dead end, so the whole effort is not really a decent reward. For (2), the points $S,T,K,L$ are so complicated that i cannot see a possibility to show (2) without introducing $Y$. The problem could do this for us and claim more, not doing so is part of a puzzle.