Inspired by this difficult Sangaku problem, I created the following Sangaku-style problem of my own.
In equilateral $\triangle ABC$, $D$ is on $AB$, $E$ is on $AC$, and the incircles of $\triangle ADE$, $\triangle DBE$ and $\triangle EBC$ have equal radii. Prove that $BD=DE$.
I have a solution that requires a computer. I am looking for a solution that does not require a computer.
My solution
Assume the side length of $\triangle ABC$ is $1$.
Let
$x=BD$
$y=DE$
$\theta=\angle BDE$
Use the sine rule and cosine rule to express $\theta$, $AE$ and $BE$ in terms of $x$ and $y$:
$\theta=\arcsin{\left(\frac{\sqrt3 (1-x)}{2y}\right)}+\frac{\pi}{3}$
$AE=\sqrt{(1-x)^2+y^2+2y(1-x)\cos{\theta}}$
$BE=\sqrt{x^2+y^2-2xy\cos{\theta}}$
The inradius of a triangle is $\frac{2\times \text{area}}{\text{perimeter}}$.
$r_1=$ inradius of $\triangle ADE=\dfrac{y(1-x)\sin{\theta}}{1-x+y+AE}$
$r_2=$ inradius of $\triangle DBE=\dfrac{xy\sin{\theta}}{x+y+BE}$
$r_3=$ inradius of $\triangle EBC=\dfrac{(1-AE)\frac{\sqrt3}{2}}{2-AE+BE}$
Setting $r_1=r_2$ and $r_1=r_3$ gives two equations in $x$ and $y$. Desmos shows they are satisfied only when $x=y$, both approximately $0.5502282106$.




Here is a solution from one of my coworkers.
Assume $AD=DE$ and $OF=KG=r$. We will prove that $HL=r$.
Define $\alpha=\angle{DAE}$. Simple angle chasing gives the other angles shown in the diagram.
$$AT=CO+OE+EK$$ $$\frac1r(OE+CO)=\frac1r(AT-EK)$$ $$\cot{(60^0-\alpha)}+\sqrt3=\cot{\left(30^0-\frac{\alpha}{2}\right)}-\cot{\left(30^0+\frac{\alpha}{2}\right)}$$ $$\frac{\cos{\alpha+\sqrt3 \sin{\alpha}}}{\sqrt3 \cos{\alpha}-\sin{\alpha}}+\sqrt3=\frac{\sin{(30^0+\alpha/2)\cos{(30^0-\alpha/2)-\cos{(30^0+\alpha/2)}\sin{(30^0-\alpha/2)}}}}{\sin{(30^0-\alpha/2)\sin{(30^0+\alpha/2)}}}$$ $$\frac{\cos{\alpha}+\sqrt3 \sin{\alpha}}{\sqrt3\cos{\alpha}-\sin{\alpha}}+\sqrt3=\frac{2\sin{\alpha}}{\cos{\alpha}-\cos{60^0}}$$ $$2\cos^2{\alpha}-\cos{\alpha}=\sqrt3 \sin{\alpha}\cos{\alpha}-\sin^2{\alpha}$$ $$\cos^2{\alpha}-\cos{\alpha}+1=\sqrt3\sin{\alpha}\cos{\alpha}$$ $$(\cos^2{\alpha}-\cos{\alpha}+1)^2=3(1-\cos^2{\alpha})\cos^2{\alpha}$$ $$(2\cos{\alpha}-1)(2\cos^3{\alpha}-1)=0$$ Obviously, $\cos{\alpha}\ne1/2$.
Let $m=2^{1/3}$.
$$\cos{\alpha}=\frac1m=\frac{1-\tan^2{(\alpha/2)}}{1+\tan^2{(\alpha/2)}}$$ $$\tan{\alpha}=\sqrt{m^2-1}$$ $$\tan{\frac{\alpha}{2}}=\sqrt{\frac{m-1}{m+1}}$$ $$\begin{align} HL&=DE\cos{\alpha}\tan{\frac{\alpha}{2}}\\ &=(DM+ME)\cos{\alpha}\tan{\frac{\alpha}{2}}\\ &=r(\cot{\alpha}+\cot{(60^0-\alpha)})\cos\alpha\tan{\frac{\alpha}{2}}\\ &=r\left(\frac{1}{\sqrt{m^2-1}}+\frac{1+\sqrt3\sqrt{m^2-1}}{\sqrt3-\sqrt{m^2-1}}\right)\frac1m\sqrt{\frac{m-1}{m+1}}\\ &=\frac{\sqrt3mr}{(m+1)(\sqrt3-\sqrt{m^2-1})}\\ &=\frac{\sqrt3mr}{\sqrt3m+\sqrt3-(m+1)\sqrt{m^2-1}}\\ &=\frac{\sqrt3mr}{\sqrt3m+\sqrt3-\sqrt{\color{red}{(m^2-1)(m+1)^2}}}\end{align}$$
$$\color{red}{(m^2-1)(m+1)^2}=(m+2)(m^3-2)+3=0+3=3$$
$$\therefore HL=r$$