Let ABC be a triangle.AA₁, BB₁, CC₁ are the angle bisectors of the triangle. ω is circumcircle of ABC. ω∩AA₁=A₂, ω∩BB₁=B₂, ω∩CC₁=C₂. Circumcircles of AB₁B₂, BC₁C₂, CA₁A₂ intersect with AB,BC and CA at D,E,F respectively. Prove that A₁D, B₁E, C₁F intersect at the same point. My try: After some angle chasing I have found out that C₂E=BC₂, A₂C=A₂F, B₂A=B₂D. And after considering 3 equal triangles. I found out that AB=AF, BD=BC, CA=CE. But after that I haven't managed to get anything. I am suspecting we might use Pascal's theorem since there are 6 points on circle ω.
Prove that A₁D, B₁E, C₁F intersect at the same point
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First of all, let us recall on the following picture what we have:
We have: $$ \begin{aligned} \widehat{DAB_2} &= 180^\circ - \widehat{BAB_2} = \widehat{BCB_2} \\ & =\widehat{BCA} + \widehat{ACB_2} =\widehat{BCA} + \widehat{ABB_2} =\widehat{BCA} + \widehat{B_2BC} \\ &=\widehat{BCB_1} + \widehat{B_1BC} =\widehat{AB_1B} \\ &=\widehat{ADB_2}\ . \end{aligned} $$ (At the last step we used $AB_1B_2D$ cyclic.)
Similarly, the other claimed equality of angles holds, so that the triangles $\Delta ADB_2$, $\Delta BEC_2$, and $\Delta CFA_2$ are isosceles.
Now from $BA_2=A_2C=A_2F$ we obtain the equality of the triangles $\Delta ABA_2$ and $\Delta AFA_2$, showing the claimed $AB=AF$ from the OP.
It remains to show the concurrence, and to start the answer.
For me, the simplest solution now is to use barycentric coordinates. A short introduction to barycentric coordinates is:
Max Schindler, Evan Chen, bary-short.pdf
(This is distroying the geometry, but it is the simplest solution.) We compute immediately the needed barycentric coordinates, and the equations of $A_1D$, $B_1E$, $C_1F$: $$ \begin{aligned} A_1 &=(0:b:c)\ ,\\ B_1 &=(a:0:c)\ ,\\ C_1 &=(a:b:0)\ ,\\[2mm] D &=(a:c-a:0)\ ,\\ E &=(0:b:a-b)\ ,\\ F &=(b-c:0:c)\ ,\\[2mm] & A_1D\ :& c(a-c) x +acy -abz &= 0\ ,\\ & B_1E\ :& -bc x +a(b-a)y +baz &= 0\ ,\\ & C_1F\ :& cb x -cay +b(a-b)z &= 0\ . \end{aligned} $$
I will say some words about this. Skip please, if already in a good shape using barycentric coordinates, and go straightforward to the determinant at the end.
A point $P$ has absolute barycentric coordinates $(x,y,z)$ w.r.t. the triangle $\Delta ABC$ with sides $a,b,c$ iff we can write $$P = xA+yB+zC\ ,\qquad x+y+z=1\ . $$ This has a formal sense, as written. To have a quick sense, either identify $A,B,C$ with their affixes in the complex plane and use operations from $\Bbb C$, or considered it "vectorially" with a missing (tacitly chosen) origin $O$, then fill in to the equality $OP=x\cdot OA+y\cdot OB+z\cdot OC$. (Vectorial computation, $OP$ is here the vector $OP$, not its length.)
Sometimes, $(x,y,z)$ is a specific expression with large denominator. It is simpler to ignore the denominator, so something like $(x:y:z)$ denotes $\left(\frac x{x+y+z},\frac y{x+y+z},\frac z{x+y+z}\right)$. (And $x+y+z\ne 0$.)
Now we compute the points above. I will do it formally, since i have to type. (Use complex numbers interpretation to have a sense of what follows.)
The angle bisector theorem gives $|A_1B|:|A_1C|=c:b$. We rewrite successively $b|A_1B|=c|A_1C|$, $b(B-A_1) = -c(C-A_1)$, $bB+cC=(b+c)A_1$, $A_1=\left(a,\frac b{b+c},\frac c{b+c}\right)=(0:b:c)$.
Corresponding formulas hold for $B_1$, $C_1$.
Let us compute also the barycentric coordinates for $D$. We start with $|BA|:|BD|=c:a$, and similarly we get $a|BA|=c|BD|$, $a(A-B)=c(D-B)$, $aA+(c-a)B=cD$, $D=(a:c-a:0)$.
The equation for the line $A_1D$ is obtained by taking the vector product of (the vectors built out of the coordinates of) $A_1$, $D$. Or we just verify the claimed equation with $A_1$ and $D$.
The concurrence of $A_1D$, $B_1E$, $C_1F$ is now equivalent to the vanishing of the following determinant, Lemma 18 in loc. cit.: $$ \begin{vmatrix} c(a-c) & ac & -ab\\ -bc & a(b-a) & ab\\ bc & -ca & b(c-b) \end{vmatrix} \overset{(!)}{=\!=} 0 \ . $$ This is an easy computation. In fact, we can also get the coordinates of the intersection point $X$, $$ X=(ab:bc:ca)=\left(\frac 1c:\frac 1b:\frac 1a\right)\ , $$ and there is some symmetry in the asymmetry of this formula. (Its shape shows that $X$ is a "complicated point".)
$\square$
(A solution using Ceva / Menalaus can also be given.)
Later edit: The Ceva / Menelaus solution is based on the above knowledge of the point $X$. We construct $A_3$ in the following picture by intersecting the parallel from $C_1$ to $AC$ with $BC$:
Similarly we construct $B_3$, and $C_3$. Then all six lines $AA_3$, $A_1D$; $BB_3$, $B_1E$; $CC_3$, $C_1F$ are concurrent in $X$. I will drop maybe an other solution based on this observation.
On
Here is an other answer, based on my already given answer using barycentric coordinates to get the location of the intersection point. Well, we already have an accepted answer, so i will make it short.
Let $a,b,c$ be the sides of the given triangle.
From the OP we know that $D$ is placed on $BA$ so that $\Delta BCD$ is isosceles, i.e. $BD=BC=a$. We construct $A_3$ on $BC$ so that $C_1A_3\| AC$. And similarly $B_3$, $C_3$. Let $U=BB_3\cap CD$. Picture so far:
As constructed, $AA_3$, $BB_3$, $CC_3$ are concurrent in a point $X$, reciprocal of the theorem of Ceva: $$ \frac{A_3B}{A_3C}\cdot \frac{B_3C}{B_3A}\cdot \frac{C_3A}{C_3B} = - \frac ab\cdot \frac bc\cdot \frac ca\cdot =-1\ . $$ Let us show that $DA_1$ is also passing through $X$.
Menelaus for $\Delta ADC$ w.r.t. the transverse line $BB_3U$ gives $$ 1 = \frac{BD}{BA}\cdot \frac{B_3A}{B_3C}\cdot \frac{UC}{UD} = - \frac{a}{c}\cdot \frac{c}{b}\cdot \frac{UC}{UD}\ . \qquad\text{ So } \frac{UC}{UD} = -\frac ba\ . $$ We need the position of $C_3$ on $BD$. From $\frac{C_3A}{C_3B}=\frac{B_1A}{B_1C}=\frac{BA}{BC}=\frac ca$ we have $C_3A=c^2/(a+c)$, $C_3B=ac/(a+c)$. This gives $C_3D=C_3A+AD=C_3A+(a-c)=a^2/(a+c)$.
We are now in position to apply the reciprocal of Ceva in $\Delta DBC$ for the points $A_1$, $U$, $C_3$, so we compute: $$ \frac{A_1B}{A_1C}\cdot \frac{UC}{UD}\cdot \frac{C_3D}{C_3B} = - \frac cb\cdot \frac ba\cdot \frac {a^2/(a+c)}{ac/(a+c)} =-1 \ . $$ So $A_1D$ passes through $BU\cap CC3=X$.
This shows the concurrence of the six lines $AA_3$, $BB_3$, $CC_3$; $A_1D$, $B_1E$, $C_1F$.
$\square$



Denote by $k$ the inscribed circle of triangles $ABC$ and let $I$ be its center. Let's focus on the quad $BEC_1C_2$. Then $$\angle\, C_1AC = \angle \, BAC = \alpha = \angle\, BC_2C = \angle \, BC_2C_1$$ Since $BEC_1C_2$ is cyclic, $$\angle \, C_1EC = \angle \, BC_2C_1 = \angle\, C_1AC = \alpha$$ However, $\angle \, ACC_1 = \angle \, BCC_1 = \angle \, ECC_1 = \frac{1}{2} \angle \, ACB$ which implies that triangles $ACC_1$ and $ECC_1$ are congruent and in fact mirror-symmetric with respect to the angle bisector $CC_1$. Since the incenter $I$ lies on the angle bisector $CC_1$, the mirror-symmetry with respect to $CC_1$ transforms the incircle $k$ to itself. However, line $AC_1 \equiv AB$ is tangent to $k$, so its image which is the line $EC_1$, is also tangent to the incircle $k$.
We can apply the same arguments to the other two angle bisectors $AA_1$ and $BB_1$ and the respective quads $CFA_1A_2$ and $ADB_1B_2$, and conclude that the pair of triangles $BAA_1$ and $FAA_1$ are mirror-symmetric with respect to angle bisector $AA_1$, and that the pair of triangles $CBB_1$ and $DBB_1$ are mirror-symmetric with respect to angle bisector $BB_1$. Consequently, the pair of mirror-symmetric lines $FA_1$ and $BA_1$ are tangent to the incircle $k$, as well as the pair of mirror-symmetric lines $DB_1$ and $CB_1$ are also tangent to the incircle $k$.
Therefore the hexagon $EA_1FB_1DC_1$ is superscribed around the incircle $k$ of the triangle $ABC$. By Brianchon's theorem the diagonals $$ A_1D, \,\, B_1E, \, \, C_1F$$ of the hexagon $EA_1FB_1DC_1$ must intersect in a common point.