It was done with one single dish,
...in Ku-band (16.7 GHz) and ... currently equipped with a high target resolution.
The Fraunhofer Institute for High Frequency Physics and Radar Techniques (FHR)'s March 21, 2018 press release - the original source of the picture in the question - links to an introductory description of their Space observation radar TIRA (Tracking and Imaging RAdar) facility, where it says:
The "ball" accommodates an antenna with a diameter of 34 meters. It can be turned 360° in azimuth (horizontal) and 90° in elevation (vertical). The movable part weighs 240 tons and can be turned at a speed of 24° per second (in azimuth), i.e. a full rotation takes 15 seconds.
As the name implies, the TIRA system comprises a tracking radar and an imaging radar. The narrowband, fully coherent, high power tracking radar has a transmission frequency in L-band (1,333 GHz) and the wideband imaging radar has a transmission frequency in Ku-band (16.7 GHz) and is currently equipped with a high target resolution.
I suspect that there'll be something more detailed about the technologies used in the Publications section of the FHR site, but couldn't find anything on the quick, and I lack the time right now to go through the complete lists for each year.
There is an animation showing 3D rotation of the radar image in this Fraunhofer FHR tweet and a video of the dish in motion as well. Note the #radarlove hash tag.
More on the TIRA System.
(The FHR is one of several dozen application-oriented research institutes in the umbrella Fraunhofer Gesellschaft, a.k.a. FGAN.)
Source Aerial view of the space observation radar TIRA © Fraunhofer FHR
The key principle is Inverse Synthetic Aperture Radar (ISAR). From an FHR publication FGAN contribution to the MIR deorbiting campaign 2001 by L.Leushacke (p68, courtesy the SAO/NASA Astrophysics Data System (ADS)):
...the cross range resolution is provided by Doppler frequency analysis and is mainly determined by the processed synthetic aperture, i.e. the target aspect angle changes during the processing interval. For a square resolution cell of 25 x 25cm the necessary aperture angle is about 2.7°.
(In: Proceedings of the international workshop "MIR deorbit", 14 May 2001, ESOC, Darmstadt, Germany. Eds.: Walter Flury & Huguette Sawaya-Lacoste. ESA SP-498, Noordwijk, Netherlands: ESA Publications Division, ISBN 92-9092-808-5, 2002, p. 67 - 72.)
In other words, the idea is that when you have a radar (as opposed to a passive radio observatory) capable of generating carefully controlled pulses, and when your receiver has sufficient bandwidth and sufficient spectral resolution, and when the target is moving across the line of sight, then you don't need a huge antenna baseline to attain high image resolution: The motion of the target is what provides the baseline. (Whence Inverse SAR).