Semiconductor Spin-Lasers

Igor Žutić; Rafał Oszwałdowski; Jeongsu Lee; Christian Gøthgen

doi:10.1201/b11086-42

Semiconductor Spin-Lasers

Igor Žutić
, Rafał Oszwałdowski
, Jeongsu Lee
, Christian Gøthgen

Physics

SUNY Buffalo

Research output: Chapter in Book/Report/Conference proceeding › Chapter › peer-review

Abstract

Both conventional lasers and spin-lasers share three main elements: the active (gain) region, the resonant cavity (resonator), and the pump, which injects (optically or electrically) energy/carriers. A typical vertical geometry, for so-called vertical cavity surface emitting lasers (VCSELs) [10] used in spin-lasers is illustrated in Figure 38.3. It is similar to the Faraday geometry of spin light emitting diodes (spin-LEDs) [7], which leads to well-defined 38.1 Introduction 731 38.2 Conventional Semiconductor Lasers 732.

Original language	English
Title of host publication	Handbook of Spin Transport and Magnetism
Publisher	CRC Press
Pages	731-745
Number of pages	15
ISBN (Electronic)	9781439803783
ISBN (Print)	9781439803776
DOIs	https://doi.org/10.1201/b11086-42
State	Published - Jan 1 2016

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AU - Oszwałdowski, Rafał

AU - Lee, Jeongsu

AU - Gøthgen, Christian

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AB - Both conventional lasers and spin-lasers share three main elements: the active (gain) region, the resonant cavity (resonator), and the pump, which injects (optically or electrically) energy/carriers. A typical vertical geometry, for so-called vertical cavity surface emitting lasers (VCSELs) [10] used in spin-lasers is illustrated in Figure 38.3. It is similar to the Faraday geometry of spin light emitting diodes (spin-LEDs) [7], which leads to well-defined 38.1 Introduction 731 38.2 Conventional Semiconductor Lasers 732.

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Semiconductor Spin-Lasers

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