(Corrected answer):
I propose to use the superposition principle for finding - as the first step - the base potential Vb=Vb1+Vb2. The two voltage sources contributing to Vb are the supply voltage Vs (for Vb1) and the base-emitter voltage Vbe (for Vb2), which will be treated as a constant DC voltage source Vbe=0.65...0.7 volts.
- This method requires nothing else than to use twice the voltage divider principle.
1.) For Vb1 (simple voltage divider) we set Vbe=0 and find the voltage at the parallel connection of Rb2 and the reflected emitter resistor Re" (which must be transferred to the base side): Re"=(1+B*Re).
2.) For Vb2 we set the supply voltage Vs to zero and calculate the voltage at the base node - driven by Vbe (again, a simple voltage divider).
3.) Now we have Vb=Vb1+Vb2 and Ve=IeRe=Vb-Vbe.
4.) As the last step we can find Ie (via Ve) and Ic.
5.) Comment: As you can see, it was NOT necessary to find the base current Ib. This is not surprising because the current Ie is controlled by the voltage Vbe - and Ib is nothing else than an (unwanted) by-product. Of course, if you wish you can calculate Ib as the last step: Ib=Ic/β.