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In conventional laser devices, the diode forward current is used to create light amplification (forward) and the extrinsic current (for backward and optical power) is used to create optical power based on absorption. The efficiency of conventional laser devices (at least those having a gain medium) is generally higher than conventional LED devices. Conventional laser devices often have forward and backward diode currents that flow in opposite directions and are typically defined by a single control parameter, such as a threshold voltage or turn-on current for a diode. Conventional laser devices in which the diode forward and backward currents flow in opposite directions may be referred to as “diode-pumped” lasers or simply “diode-pumped lasers.” These conventional laser devices typically require simultaneous forward and backward diode currents for reliable operation. A conventional method of generating such simultaneous forward and backward diode currents in a diode-pumped laser is by switching or modulating the laser between a forward bias and a reverse bias, thereby alternately generating forward and backward optical power and driving the laser into a saturated state in which a flow of current is maintained despite variations in the diode current. Conventional diode-pumped lasers generally use a forward bias to facilitate lasing and a reverse bias to control the diode currents. As a result, diode-pumped lasers require relatively low forward bias current to initiate lasing, and a much higher reverse bias current to create the lasing characteristics. However, because of the relatively high reverse bias current required to create the lasing characteristics, a diode-pumped laser with a relatively high reverse bias current may be susceptible to electrical breakdown during operation. 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