W. Dabrowski, Faculty of Physics and Nuclear Techniques, UMM, Cracow, Poland, F. Anghinolfi, CERN, Geneva, Switzerland, P. Jarron, CERN, Geneva, Switzerland, J. Kaplon, CERN, Geneva, Switzerland, C. Lacasta, CERN, Geneva, Switzerland, P. Weilhammer, CERN, Geneva, Switzerland, R. Szczygiel, Institute of Nuclear Physics, Cracow, Poland, A. Clark, University of Geneva, Switzerland, D. LaMarra, University of Geneva, Switzerland, D. Macina, University of Geneva, Switzerland, V. Cindro, Jozef Stefan Institute, Ljubljana, Slovenia, I. Mandic, Jozef Stefan Institute, Ljubljana, Slovenia, M. Mikuz, Jozef Stefan Institute, Ljubljana, Slovenia, T. Dubbs, Santa Cruz Institute for Particle Physics, UCSC Santa Cruz, CA, USA, A. Grillo, Santa Cruz Institute for Particle Physics, UCSC Santa Cruz, CA, USA, G. Meddeler, Lawrence Berkeley National Laboratory, Berkeley, CA, USA, H. Niggli, Lawrence Berkeley National Laboratory, Berkeley, CA, USA, !! The ABCD design is a single chip implementation of the binary readout architecture for silicon strip detectors in the ATLAS Semiconductor Tracker. The design follows the previously developed prototype, the SCT128B chip. Functionally it is fully compatible with another technological option being developed for the SCT and employing two separate chips: CAFE - a front-end chip realized in the MAXIM bipolar process, and ABC - a binary pipeline chip realized in the Honeywell bulk CMOS process. The DMILL technology, in which the ABCD chip has been fabricated, offers a possibility to implement the complete binary architecture, as required for the ATLAS SCT, in a single chip. The chip comprises all blocks of the binary readout architecture, the front-end circuitry, binary pipeline, derandomizing buffer, data compression logic and the readout control logic. The ABCD design has been manufactured successfully in an engineering run at the TEMIC foundry. The radiation hardness requirements of the ABCD chips are driven by the radiation levels expected in the SCT, which are 10 Mrad of ionizing dose and 2x10E14 of equivalent 1 MeV neutron fluence. The ABCD chips have been irradiated separately with X-ray, with a 50 MeV proton beam and with neutrons from a nuclear reactor in several steps up to the levels as mentioned above. The analog performance of the ABCD chip before and after irradiation was evaluated using a single chip test set-up. The extraction of basic parameters, i.e. gain, noise and offset spread was obtained from discriminator threshold scans for various input charges. The speed of the front-end was evaluated from a delay scan of the internal calibration signal. The measurements were performed for various bias condition of the front-end circuit, in particular for a wide range of the bias current in the input transistor. The main observed radiation effect in the front-end circuit is the increase of the parallel current noise due to degradation of the current gain factor beta in bipolar transistors, as expected and anticipated in the design. For detailed evaluation of the digital part of the ABCD design a general-purpose mixed signal tester at CERN was used. The tester allowed measuring the digital functionality at various clock frequencies and supply voltages. Based on a comprehensive evaluation of the digital performance of the chip some critical tests were identified for which we observed the speed limitations first. The results of these critical tests were monitored with increasing radiation dose. The tests were run in two modes: (a) at a constant supply voltage of 4 V and various (increasing) clock frequency and (b) at constant clock frequency of 40 MHz and decreasing supply voltage up to the points where the chips failed to respond correctly. A global radiation effect observed in the digital circuitry was slowing down by about 10-20%. In the paper the details of radiation effects regarding the analog and the digital performance of the ABCD chip will be presented. !! The ABCD design is a single chip implementation of the binary readout architecture for silicon strip detectors in the ATLAS Semiconductor Tracker. The radiation hardness requirements of the ABCD chips are driven by the radiation levels expected in the SCT, which are 10 Mrad of ionizing dose and 2x10E14 of equivalent 1 MeV neutron fluence. The ABCD chips have been irradiated separately with X-ray, with a 50 MeV proton beam and with neutrons from a nuclear reactor in several steps up to the levels as mentioned above. The details of the radiation effects regarding the analog and the digital performance of the chip will be presented and discussed. !!