Abstract

We report the first room temperature CW operation of two dimensional single-mode edge-emitting photonic crystal Bragg lasers. Single-mode lasing with single-lobed, diffraction limited far-fields is obtained for 100microm wide and 550microm long on-chip devices. We also demonstrate the tuning of the lasing wavelength by changing the transverse lattice constant of the photonic crystal. This enables a fine wavelength tuning sensitivity (change of the lasing wavelength/change of the lattice constant) of 0.072. This dependence proves that the lasing mode is selected by the photonic crystal lattice.

Highlights

  • The idea of using two dimensional distributed feedback in lasers dates back to 1973 [1]

  • We report the first room temperature continuous wave (CW) operation of two dimensional distributed feedback, single-mode, edge-emitting semiconductor lasers

  • The far-field of the photonic crystal Bragg laser is single-lobed and possesses a small beam divergence angle of 1°, as shown in Fig. 4(b). (In the CCD far-field image, the fringes in the vertical direction are due to unwanted interferences in the measurement.) The emitting aperture of the laser is about 100μm, corresponding to a theoretical diffraction-limited far-field FWHM width of 0.99° [15]

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Summary

Introduction

The idea of using two dimensional distributed feedback in lasers dates back to 1973 [1]. Single-mode operation of large-area, edge-emitting semiconductor lasers using two dimensional distributed feedback has only been demonstrated either in room temperature pulsed condition [9, 10] or low temperature CW condition [11]. We report the first room temperature CW operation of two dimensional single-mode edge-emitting photonic crystal Bragg lasers. These lasers break the limit of the index guiding for designing edge-emitting, single-mode semiconductor lasers using distributed feedback structures. Despite the non-uniform intensity distribution in the near-field, the far-field is single-lobed and diffraction-limited This proves that the photonic crystal Bragg structure can prevent filamentation and ensure a single-mode operation. This dependence proves that the lasing mode is selected by the photonic crystal lattice

Design and fabrication of photonic crystal Bragg lasers
Experiment results and discussions
Conclusion
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