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1.4.2 Single‐Mode and Multi‐Mode Behavior

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Semiconductor lasers oscillate in different modes (power radiation patterns) that depend on the dimensions of the optical resonator. Especially for VCSELs, the mode structure or pattern depends on the size and shape of the oxide aperture (mode) diameter used for current and optical confinement [53, 54]. Several kinds of modes appear in the emission spectra, namely longitudinal, transverse, single, and multi‐modes. In Figure 1.16 we show how the behavior of VCSEL in single longitudinal and multi‐transverse (and longitudinal) operation. More details on the VCSEL mode structure will be discussed in Chapter 2.

Table 1.2 Milestones of surface emitting laser research and development.

1977 Surface‐emitting laser concept proposed
1979 First device demonstrated (77 K, pulsed)
1988 First RT CW operation
1988 Semiconductor DBR
1989 QW VCSEL
1989 Micro‐post QW laser RT CW (Bell Labs)
1989 Periodic gain proposed (UCSB)
1990 AlGaAs hydro‐oxidization (UIUC)
1992 VCSEL mechanical tuning demonstrated
1995‐ Low threshold device competition Ith < 0.1 mA
1995 MEMS tunable VCSEL (USB)
1996 VCSEL commercialization (Honeywell)
1999 VCSEL LAN
2000 Oxide aperture device reliability
2001 VCSEL printer (Fuji, Xerox),
2001 Computer mouse (HP)
2002 10G Ethernet standard IEEE802.3ae
2003 4Gb/s VCSELs (Honeywell)
2006 High‐contrast grating for VCSEL (UC Berkeley)
2010 100G Ethernet standard IEEE802.3ba
2011‐ VCSEL photonics
2016 VCSEL arrays for sensing
2016 VCSEL SWDM in datacom
2017 VCSEL face ID 3D sensor (iPhone X from Apple)
2018 400G AOC (Finisar/II–VI)
2020 LiDAR scanner (iPhone 12 Pro, iPad Pro 11″/12″ from Apple)
2021‐ VCSEL Industry

Italic: From K. Iga’s group.

RT CW: Room‐temperature continuous wave

QW: Quantum well.


Figure 1.16 Origin of single‐mode and multi‐mode behavior in VCSELs.

Source: [55, 8]. Figure by K. Iga [copyright reserved by author].

The origin of multi‐mode operation in a VCSEL is not from longitudinal mode behavior but multiple transverse mode oscillation. When the lateral extent of the optical resonator diameter is extended to larger than several microns, multi‐transverse with multispectral‐mode operation is achieved. On the other hand, small diameters lead to single‐transverse and single spectral‐mode operation.

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