A high-intensity pulsed ion source of TEMP-type series, operating in bipolar mode, has been developed as a unique pulsed energy source to produce a high-intensity pulsed ion beam ͑HIPIB͒ for surface modification of materials. To generate the ion beam, a specially shaped bipolar pulse, consisting of a first negative pulse and a second delayed positive pulse both of nanosecond width, is formed by a double coaxial pulse-forming line ͑PFL͒ powered with a Marx generator and supplied to a magnetically insulated ion diode ͑MID͒ by a self-magnetic field. It is found that the efficient generation of a HIPIB is mainly dependent on the delay time of the bipolar pulse, adjusted by pressure ratio in the two gas switches of a PFL, and the anode-cathode ͑A-K͒ gap distance in the self-magnetic field MID. The delay time determines the effective area on the anode surface for plasma generation and the A-K gap distance ensures the stability of the process. A proper delay time and a proper A-K gap distance are obtained by a series of experimental investigations. Under delay time from 30 to 280 ns and several different A-K gap distances, the typical wave forms of the bipolar pulses at a dc charging voltage of 45 kV to Marx generator are illustrated to clarify the effects of delay time and A-K gap distance on the ion beam generation. The proper A-K gap distance is not uniform, varied from 6 to 8 mm, and the corresponding proper delay time is 250 ns. The most efficient plasma generation leads to a maximum output of HIPIB with a peak ion current density of 350 A cm Ϫ2 and a beam pulse width of 75 ns ͑full width at half maximum͒, at an accelerating pulse of 220 kV with a pulse width of 100 ns.