We demonstrate a Fourier domain mode locked (FDML) laser centered at 1190 nm with 2×410 kHz sweep repetition rate, a sweeping range of 100 nm and 2.5 mW output power. The laser is based on a quantum dot-semiconductor optical amplifier with small linewidth enhancement factor. The laser could be used as a probe laser in stimulated Raman scattering microscopy and it may be attractive for optical coherence tomography due to low water absorption and the spectral signature of lipids around 1200nm. Moreover, it is ideal to close the gap between FDML lasers at 1064 nm and 1300 nm. Combining these three lasers can enable ultrawideband sweeping to improve the axial OCT resolution down to 2 μm.
We present high average power femtosecond VECSELs based on both quantum dot (QD) and quantum well (QW) gain
with extremely low dispersion. 1.05 W in 784-fs pulses could be achieved from a QD-VECSEL modelocked by a QDSESAM
with fast recovery dynamics. A similar QW-gain structure modelocked by the same SESAM enabled stable
480-fs with an average output power of 300 mW at a repetition rate of 7 GHz. Furthermore, we investigated repetition
rate scaling by changing the cavity length. We demonstrated fundamentally modelocked pulses over a tuning range from
6.5 GHz to 11.3 GHz. Without any realignment of the cavity over the whole tuning range, the pulse duration remained
nearly constant around 625 fs (±3.5%) while the output power was 169 mW (±6%). The center wavelength changed
only about ±0.2 nm around 963.8 nm. A tunable repetition rate can be of interest for various metrology application such
as optical sampling by laser cavity tuning.
The latest achievements of quantum dot based semiconductor disk lasers are reviewed. Several lasers operating at 1040
nm - 1260 nm were studied. All the structures were grown with molecular beam epitaxy on GaAs substrates. The
number of quantum dot layers was varied and the gain was provided either by the ground or the excited state transition of
the quantum dots. Frequency doubling of the lasers was demonstrated and the dual-gain laser geometry was found to be
practical solution for intracavity frequency conversion. Intracavity heat spreader and thinned device heat management
approaches are studied and compared.
In this work the use of two identical QD SOAs to enhance the performance of swept laser system for OCT applications is
discussed, resulting in an increase in bandwidth up to 94nm. The combination of GaAs based QD SOAs and InP based
QW SOAs for realizing broad bandwidth sources for OCT system is described. For the swept laser source a 154nm
spectral bandwidth from 1193nm to 1347nm and an average power of 8mW is obtained and for the filtered ASE source a
225 nm bandwidth is demonstrated.
We describe a simple swept-laser design that characterizes the emission bandwidth, linewidth, spectral shape and output
noise. A short cavity Littmann configuration is used in which the semiconductor optical amplifier (SOA) lasing
wavelength is tuned by a galvanometer with an 830 grooves per mm diffraction grating. A 3dB coupler extracts light
from the cavity formed by the grating and end-mirror and the optical output uses to illuminate a balanced swept source
optical coherence tomography (SS-OCT) interferometer incorporating a circulator, 3dB coupler, dispersion compensator
and balanced detector. The SOA (SOA-1200-70-PM-20sB, Innolume GmbH) uses a novel III-V semiconductor
quantum-dot gain medium. ASE is emitted between 1150nm and 1300nm at a drive current of 700mA. When used in the
Littmann cavity laser a coherence length of about 10mm is produced, which is tunable over 60nm. The peak output
power is 12mW. The swept-laser has been incorporated into a fiber-based SS-OCT system and used to image biological
tissues. Axial resolution in air is 12 microns. Images of human palmar skin in-vivo are demonstrated, showing good
resolution and contrast, with the stratum corneum, epidermis, rete ridges and epidermal-dermal junction visualized.
Using quantum well gain materials, ultrafast VECSELs have achieved higher output powers (2.1 W) and shorter pulses (60 fs) than any other semiconductor laser. Quantum dot (QD) gain materials offer a larger inhomogeneously broadened bandwidth, potentially supporting shorter pulse durations. We demonstrate the first femtosecond QD-based VECSEL using a QD-SESAM for modelocking, obtaining 63 mW at 3.2 GHz in 780-fs pulses at 960 nm. In continuous wave operation we obtained 5.2 W using an intra-cavity diamond heat spreader, which has been the highest output power from a QD-VECSEL so far. Further power scaling is thus expected also for modelocked operation.
We demonstrate a frequency doubled dual-gain quantum dot semiconductor disk laser operating at 590 nm. The
reflective gain element, grown by molecular beam epitaxy, has active region composed of 39 layers of InGaAs Stranski-
Krastanov quantum dots. The gain mirrors produce individually 3 W and 4 W of output power while the laser with both
elements in a single cavity reveals 6 W at 1180 nm with beam quality factor of M2<1.2. The loss induced by the
nonlinear crystal is compensated by gain boosting in the dual-gain laser and 2.5 W of output power at 590 nm was
achieved after frequency conversion.
Quantum dot-based diode comb lasers can provide a single multi-channel-laser source for short-reach, high-speed WDM interconnects. In this paper, we review the technology and demonstrate for the first time a 15 channel, low RIN comb laser with 80 GHz channel spacing. We show that each of the Fabry-Perot (FP) modes can be externally modulated at 10 Gb/s or all modes directly modulated, at 3.2 Gb/s so far. The latter indicates that the comb laser may be an ideal broadband light source in WDM-PON applications. We further demonstrate that the whole comb laser spectrum can be amplified by a quantum dot SOA without increasing relative density noise (RIN) of the individual channels. The small signal amplification factor was measured up to 30dB and the saturated output power was as high as 15 dBm.
Quantum dot-based diode comb lasers enable a single multi-channel-laser source for short-reach, high-speed WDM
interconnects. In this paper, we demonstrate for the first time a 15 channel low RIN comb laser with 80 GHz channel
spacing. We show that all the FP modes can be simultaneously directly modulated simply by modulating the pump
current at 3.2 Gb/s, which indicates that the comb laser may be an ideal broadband light source in WDM-PON
applications.We demonstrate that the whole comb laser spectrum can be amplified by a quantum dot SOA without
increasing the relative intensity noise (RIN). Small signal amplification factor was measured as high as 30 dB and the
saturated output power was as high as 15 dBm.
980 nm VCSELs based on sub-monolayer growth show for 20 Gbit/s large signal modulation clearly open eyes without
adjustment of the driving conditions between 25 and 120 °C. To access the limiting mechanism for the modulation
bandwidth, a temperature dependent small signal analysis is carried out on these devices. Single mode devices are
limited by damping, whereas multimode devices are limited by thermal effects, preventing higher photon densities in the
cavity.
High-channel-count WDM will eventually be used for short reach optical interconnects since it maximizes link bandwidth and efficiency. An impediment to adoption is the fact that each WDM wavelength currently requires its own DFB laser. The alternative is a single, multi-wavelength laser, but noise, size and/or expense make existing options impractical. In contrast, a new low-noise, diode comb laser based on InAs/GaAs quantum dots provides a practical and timely alternative, albeit in the O-band. Samples are being evaluated in short reach WDM development systems. Tests show this type of Fabry-Perot laser permits >10 Gb/s error-free modulation of 10 to over 50 separate channels, as well as potential for 1.25 Gb/s direct modulation. The paper describes comb laser requirements, noise measurements for external and direct modulation, O-band issues, transmitter photonic circuitry and components, future CMP applications, and optical couplers that may help drive down packaging costs to below a dollar.
We report on edge-emitting InAs/GaAs quantum dot laser promising as multiple wavelength light source for dense
wavelength-division-multiplexing systems in future generation of silicon photonic integrated circuits. Broad and flat gain
spectrum of quantum dots as well as pronounced gain saturation effect facilitate simultaneous lasing via a very large
number of longitudinal modes with uniform intensity distribution (comb spectrum). A very broad lasing spectrum of
about 75 nm in the 1.2-1.28 μm wavelength range with a total output power of 750 mW in single lateral mode regime is
achieved by intentional inhomogeneous broadening of ground state transition peak and contribution of lasing via excited
state transitions. Average spectral power density exceeds 10 mW/nm. A bit error rate less than 10-13 is demonstrated for
ten spectrally filtered and externally modulated at 10 Gb/s Fabry-Perot modes owing to a low (<0.3% in the 0.001-10 GHz range) relatively intensity noise of each individual mode. This result shows aptitude of a multimode quantum dot
laser for high bandwidth wavelength-division-multiplexing systems.
A. Ramdane, A. Martinez, S. Azouigui, D.-Y. Cong, K. Merghem, A. Akrout, C. Gosset, G. Moreau, F. Lelarge, B. Dagens, J.-G. Provost, A. Accard, O. Le Gouezigou, I. Krestnikov, A. Kovsh, M. Fischer
This paper presents recent progress in the field of semiconductor lasers based on self-assembled quantum dots grown
either on GaAs or InP substrates.
Quantum dot (QD) based lasers are attracting a lot of interest owing to their remarkable optoelectronic properties that
result from the three dimensional carrier confinement. They are indeed expected to exhibit much improved performance
than that of quantum well devices. Extremely low threshold currents as well as high temperature stability have readily
been demonstrated in the InAs/GaAs material system.
The unique properties of quantum dot based active layers such as broad optical gain spectrum, high saturation output
power, ultrafast gain dynamics and low loss are also very attractive for the realization of mode-locked lasers.
Recent results in the field of directly modulated InAs/GaAs lasers emitting in the 1.3 μm window are discussed. We
report in particular on temperature independent linewidth enhancement factor (or Henry factor αH) up to 85°C. This is a
key parameter which determines many laser dynamic properties. Optical feedback insensitive operation of specifically
band-gap engineered devices, compatible with high bit rate isolator-less transmission is also reported at 1.55 μm.
Monolithic mode locked lasers based on InAs/InP quantum dashes have been investigated for 1.55 μm applications. Subpicosecond
pulse generation at very high repetition rates (> 100 GHz) is reported for self-pulsating one-section Fabry
Perot devices. Specific applications based on these compact pulse generators including high bit rate clock recovery are
discussed.
980 nm vertical-cavity surface-emitting laser based on sub-monolayer growth of quantum dots show at 25 and 85°C for 20 Gb/s without current adjustment clearly open eyes and error free operation with bit error rates better than 10-12. For these multimode lasers the small signal modulation bandwidth decreases only from 15 GHz at 25°C to 13 GHz at 85°C. Single mode devices demonstrate at 20°C a small signal modulation bandwidth of 16.6 GHz with 0.8 mW optical output power and a record high modulation current efficiency factor of 19 GHz/mA1/2.
Through absorber length optimisation, sub-picosecond pulse generation and low timing jitter are demonstrated in a 20GHz passively mode-locked quantum-dot laser diode. Pulse-widths as low as 800fs and timing jitter performance of 390fs (20kHz-50MHz) are achieved.
We have performed a systematic study of structural and optical properties of Quantum dot (QDs) lasers based on InAs/InGaAs quantum dots grown on GaAs substrates emitting in the 1.3 - 1.5 μm range. 1.3 μm range QD lasers are grown using GaAs as matrix material. It is shown that the lasers, grown with large number of QD stacks are metamorphic, with plastic relaxation occurring through the formation of misfit dislocations. Thus, 1.3 μm QD lasers with large number of stacks grown without strain compensation are metamorphic. Another type of defects is related to local dislocated clusters, which are the most dangerous. When proper optimization of the growth conditions is carried out, including a selective thermal etching off of statistically formed dislocated clusters through the defect-reduction technique (DRT), no significant impact of misfit dislocations on the degradation robustness is observed. In uncoated devices a high cw single mode power of ~700 mW is realized limited by thermal roll-over, which is not affected by 500 h ageing at room temperature. At elevated temperatures the main degradation mechanism revealed is catastrophic optical mirror damage (COMD). When the facet are passivated, the devices show the extrapolated operation lifetime in excess of 106 h at 40°C at ~100 mW cw single mode output power. Longer wavelength (1.4 - 1.5 μm) devices are grown on metamorphic (In,Ga,Al)As layers deposited on GaAs substrates. In this case, the plastic relaxation occurs through formation of both misfit and threading dislocations. The latter kill the device performance. Using DRT in this case enables blocking of threading dislocation with growth of QDs in defect-free upper layers. DRT is realized by selective capping of the defect-free areas and high-temperature etching of nano-holes at the non-capped regions near the dislocation. The procedure results in etching of holes and is followed by fast lateral overgrowth with merger of the growth fronts. If the defect does not propagate into the upper layer when the hole is capped, the upper layers become defect-free. Lasers based on this approach exhibited emission wavelength in the 1.4 -1.5 μm range with a differential quantum efficiency of about ~50%. The narrow-stripe lasers operate in a single transverse mode and withstand continuous current density above 20 kA cm-2 without degradation. A maximum continuous-wave output power of 220 mW limited by thermal roll-over is obtained. No beam filamentation was observed up to the highest pumping levels. Narrow stripe devices with as-cleaved facets are tested for 60°C (800 h) and 70°C (200 h) on-chip temperature. No noticeable degradation has been observed at 50 mW cw single mode output power. This shows the possibility of degradation-robust devices on foreign substrates. The technology opens a way for integration of various III-V materials and may target degradation-free lasers on silicon for further convergence of computing and communications.
The characteristics of p-doped 1.1 μm and 1.3 μm self-assembled In(Ga)As quantum dot lasers grown by molecular beam epitaxy have been studied. With optimum p-doping, we demonstrate quantum dot lasers with zero-temperature dependence of the threshold current (T0 = ∞) and the output slope efficiency. These characteristics are explained through a self-consistent model that includes temperature-dependent Auger recombination in the quantum dots. With tunnel injection, we measure greatly enhanced -3dB frequency response, 25 GHz and 11 GHz in 1.1 μm and 1.3 μm tunnel injection quantum dot lasers, respectively. These devices also exhibit near zero α-parameters and extremely small chirp (< 0.2 Å), in addition to temperature insensitive operation.
The Tilted Cavity (TC) concept has been proposed to combine advantages of edge- and surface-emitting lasers (detectors, amplifiers, switches, etc.). Tilted Cavity Lasers (TCL) enable wavelength-stabilized high-power edge and surface emitters (TCSEL) in low-cost single-epitaxial step design. The concept covers numerous applications including mode-locked TCL for light speed control, dispersion and linewidth engineering, GaN-based light-emitters, electrooptic wavelength tunable devices, and other applications. Presently, wavelength stabilized TC operation is realized between -200°C and 70°C in broad TCL diodes with cleaved facets based on quantum dots (QDs). The spectral width is below 0.6 nm in broad area 100 μm-wide-stipe devices. The far fields are: 4° (lateral) and 42° (vertical). Wavelength-stabilized 1.16 μm and 1.27 μm edge-emitting QD TCL lasers are demonstrated. Quantum well TCL demonstrate high-temperature operation up to 240°C with a low threshold, high temperature stability and improved wavelength stability. The tilted cavity approach can also be applied in wavelength-optimized photodetectors, switches, semiconductor optical amplifiers, including multi-channel devices, in optical fibers, in photodetectors, in light-emitting diodes and in many other applications. Moreover, microelectronic devices based on similar tilted angle resonance phenomena in quantum wells and superlattices can be realized in electron- or hole-wavefunction-engineered structures, thus, merging the fields of nanophotonics and nanoelectronics. The tilted cavity concept can be further complimented by lateral patterning and (or) processing of three-dimensional photonic crystal structures further extending horizons of modern optoelectronics.
Quantum dot (QDs) heterostructures structurally represent tiny 3D insertions of a narrow bandgap material, coherently embedded in a wide-bandgap single-crystalline matrix. The QDs are produced by conventional epitaxial techniques applying self-organized growth and behave electronically as artificial atoms. Strain-induced attraction of QDs in different rows enables vertically-coupled structures for polarization, lifetime and wavelength control. Overgrowth with ternary or quaternary alloy materials allows controllable increase in the QD volume via the island-activated alloy phase separation. Repulsive forces during overgrowth of QDs by a matrix material enable selective capping of coherent QDs, keeping the defect regions uncapped for their subsequent selective evaporation. Low-threshold injection lasing is achieved up to 1350 nm wavelength at 300K using InAs-GaAs QDs. 8 mW VCSELs at 1.3 μm with doped DBRs are realized. Edge-emitters demonstrate 10 GHz bandwidth up to 70°C without current adjustment. VCSELs show ~4 GHz relaxation oscillation frequency. QD lasers demonstrate above 3000 h of CW operation at 1.5 W at 45°C heat sink temperature without degradation. The defect reduction technique (DRT) applied to thick layers enables realization of defect-free structures on top of dislocated templates. Using of DRT metamorphic buffer layers allowed 7W GaAs-based QD lasers at 1500 nm.
Tilted Cavity Laser (TCL) is developed that combines advantages of a high power operation of an edge-emitting semiconductor diode laser and wavelength-stabilized operation of a surface emitting laser. A TCL emits laser light in a tilted optical mode that propagates effectively at a certain tilt angle to the p-n junction. Designed TCL comprises a high-finesse cavity into which an active region is placed and at least one multilayer interference reflector (MIR). The cavity and the MIR are designed such that the spectral position of the reflectivity dip of the cavity and the position of the stopband reflectivity maximum of the MIR coincides at one tilt angle of a tilted optical mode, and draw apart as the angle deviates from the optimum value. As a result, the leakage loss of the optical modes to the substrate is minimum at the optimum wavelength and increases dramatically as the wavelength deviates from the optimum one. This ensures the stabilization of the wavelength of the emitted laser light. Both quantum well (QW) and quantum dot (QD) TCLs have been fabricated on the basis of GaAs/GaAlAs waveguides. QW TCL using InGaAs QW as the active region and operating at 1000-1100 nm reveals the temperature shift of the lasing wavelength 0.2 nm/K. QW TCL operates up to and above 210°C with the differential efficiency 20%. QD TCL using InAs QD overgrown by InGaAs alloy as the active region and operating at 1100-1200 nm reveals the temperature shift of the lasing wavelength 0.165 nm/K. These shifts are significantly slower than the shift for a conventional edge-emitting semiconductor diode laser. The QD TCL shows an output power 2W in a pulsed mode. Characteristic temperature of the threshold current measured at and below room temperature (T0) is 150 K.
Access to the requested content is limited to institutions that have purchased or subscribe to SPIE eBooks.
You are receiving this notice because your organization may not have SPIE eBooks access.*
*Shibboleth/Open Athens users─please
sign in
to access your institution's subscriptions.
To obtain this item, you may purchase the complete book in print or electronic format on
SPIE.org.
INSTITUTIONAL Select your institution to access the SPIE Digital Library.
PERSONAL Sign in with your SPIE account to access your personal subscriptions or to use specific features such as save to my library, sign up for alerts, save searches, etc.