Composite resonator vertical cavity lasers enable several modulation methods that lead to high speed performance and can be conf igured to perform different functionalities for data communications. In particular, push/pull modulation can produce modulation of the light output without changing the total carrier and photon densities in the laser.The v ertical-cavity surface -emitting laser (VCSEL) is the dominant source for short -haul optical communication . VCSEL modulation at higher speeds is desired to satisfy the increasing demand for information bandwidth. Recently the VCSEL consisting of two optical cavities has demonstrated abili ties to achieve higher speed modulation [1 -3], as well as to provide additional functionalities for optical communications [4][5][6][7][8]. Specifically, the VCSEL with an optically coupled -cavity structure is known as the composite -resonator verticalcavity laser s (CRVCLs). We review the various approaches for laser modulation in these devices, as well as new functionality such as microwave mixing and the generation of 10 Gb/s three -or four -level pulse amplitude modulation (PAM) signaling. These unique functionalit ies make the CRVCL attractive for future optical systems and potentially can address low power data center applications. Fig. 1 illustrates the stru cture of the CRVCL which we have studied . The CRVCL is composed of a monolithic bottom p -type distributed Br agg reflector (DBR) with 35 periods, a middle n -type DBR with 12.5 periods, and an upper p -type DBR with 22 periods. The middle DBR mirror separate s two optical cavities, each of which contains five GaAs/Al 0.2 Ga 0.8 As quantum wells. An 8 8 implant and 5 5 oxide aperture are formed in the upper and bottom mesa, respectively. The g round-signal-signal-ground (GSSG) coplanar waveguide contacts are deposited to facilitate high -speed signaling into both cavities as shown in Fig.1 (b). Fig. 1: (a) Sketch and (b) scanning electron micrograph of a CRVCL with GSSG high -speed contacts on the planarized surface.The CRVCL can be modulated by: (i) varying current injection into the top or bottom cavity [1,5]; (ii) varying the reverse bias into one or the other cavity [2,3,6]; (iii) a combination of simultaneous current injection and reverse bias into the cavities. As a special case, the CRVCL cavities can be directly modulated by two out -ofphase electrical signals [8]. The amplitude ratio between the two direct mo dulation signals can be adjusted such that there is no net change in the carrier and photon densities inside the laser, and thus the RO frequency is suppressed . The laser output modulation occurs by varying the longitudinal mode profile in the cavities. The longitudinal optical mode is either 'pushed' toward the laser output facet produ cing higher output p ower, or is 'pulled' toward the substrate side producing lower output power. Fig. 2 (a) illustrates the input modulation signals into the CRVCL. The peak-to-peak input voltage is 1.55 V a nd 1.02 V, and the diff erential series resistance is 95 0 ohm...