Electrostatic solitary structures are generated by injection of a suprathermal electron beam parallel to the magnetic field in a laboratory plasma. Electric microprobes with tips smaller than the Debye length (位De) enabled the measurement of positive potential pulses with half-widths 4 to 25位De and velocities 1 to 3 times the background electron thermal speed. Nonlinear wave packets of similar velocities and scales are also observed, indicating that the two descend from the same mode which is consistent with the electrostatic whistler mode and result from an instability likely to be driven by field-aligned currents. [4,5]. Electron holes were also recently detected in a laboratory magnetic reconnection experiment [6]. Electron holes can be generated by energetic streaming electrons and are thought to play an important role in scattering these electrons. However, although these small-scale (one to tens of Debye lengths, 位 De ) solitary structures seem ubiquitous in key regions of space their exact origin often remains unclear. In the laboratory, experiments dedicated to electron holes were carried out in a strongly magnetized Q-machine [7]. These holes were generated by a voltage pulse and had sizes comparable to the plasma column radius, making comparison with holes observed in space difficult.This Letter reports measurements of electrostatic solitary waves generated by an electron beam injected into a magnetized low-尾 plasma column much larger than the structure scales (Fig. 1). The experiment was conducted at the upgraded Large Plasma Device (LAPD) [8] at the University of California, Los Angeles. The helium plasma column has a 60 cm diameter, is 17.1 m long and pulsed at 1 Hz with pulses lasting several milliseconds (Fig. 1a) An electron beam 0.4 to 1 cm in diameter is injected from a 3 mm diameter LaB6 crystal source for about 140 碌s along the axis of the column in the afterglow phase, between 50 and 150 ms after the end of the discharge pulse. The beam density 5 cm from the source is approximately 25% of the background electron density. The magnetic field strength, plasma density and beam voltage can be changed from experiment to experiment. The range of the main plasma parameters is summarized in