MECSELs with direct emission in the 760 nm to 810 nm spectral range: A single- and double-side pumping comparison and high-power continuous-wave operation
“…As a conclusion, the values of the temperature increase generally do not differ much from each other. This is for example in accordance with the experimental comparison of SSP and DSP for a 577 nm thin gain membrane [28]. For membranes thicker than 1 µm, the curve saturates at ∼ 5.77 W/K.…”
Section: Single-side and Double-side Pumpingsupporting
confidence: 90%
“…Here, the main motivation behind DSP is the more symmetric temperature as well as charge carrier distribution that is created across the gain membrane when compared to SSP. While for a gain membrane with a small thickness of less than 1 µm the benefit is rather small [28], gain membranes with higher thicknesses can benefit more from DSP. This aspect has been recently simulated for a = 1.77 µm gain membrane, which is about 2 µm thick, using a one-dimensional thermal model [5].…”
Section: Single-side and Double-side Pumpingmentioning
confidence: 99%
“…The quantum defect differs by 1.7 percentage points only and the higher thermal conductivity of AlGaAs of ∼ 12 W/m•K can make a slight difference to the heat situation within the gain membrane [29]. On the other hand, the thermal resistances of the = 760 nm AlGaAs, sapphire-cooled MECSEL [28], the = 1.5 µm InAs/InP QD SiC-cooled MECSEL [6], and the = 1.77 µm InGaAlAs/InP diamond-cooled MECSEL [5] are in good agreement with the simulations. Although the thermal conductivities of the MECSELs included in Fig.…”
Section: Study Of Pumping Approaches Enabling Power Scalingmentioning
“…As a conclusion, the values of the temperature increase generally do not differ much from each other. This is for example in accordance with the experimental comparison of SSP and DSP for a 577 nm thin gain membrane [28]. For membranes thicker than 1 µm, the curve saturates at ∼ 5.77 W/K.…”
Section: Single-side and Double-side Pumpingsupporting
confidence: 90%
“…Here, the main motivation behind DSP is the more symmetric temperature as well as charge carrier distribution that is created across the gain membrane when compared to SSP. While for a gain membrane with a small thickness of less than 1 µm the benefit is rather small [28], gain membranes with higher thicknesses can benefit more from DSP. This aspect has been recently simulated for a = 1.77 µm gain membrane, which is about 2 µm thick, using a one-dimensional thermal model [5].…”
Section: Single-side and Double-side Pumpingmentioning
confidence: 99%
“…The quantum defect differs by 1.7 percentage points only and the higher thermal conductivity of AlGaAs of ∼ 12 W/m•K can make a slight difference to the heat situation within the gain membrane [29]. On the other hand, the thermal resistances of the = 760 nm AlGaAs, sapphire-cooled MECSEL [28], the = 1.5 µm InAs/InP QD SiC-cooled MECSEL [6], and the = 1.77 µm InGaAlAs/InP diamond-cooled MECSEL [5] are in good agreement with the simulations. Although the thermal conductivities of the MECSELs included in Fig.…”
Section: Study Of Pumping Approaches Enabling Power Scalingmentioning
“…In our case the host substrate is a silicon carbide or oxidised silicon (Boron doped) substrate, the fabrication steps are the same regardless of the substrate. The fabrication steps follow the same recipe as in MECSELs used in [16,17] and the contact bond is good enough to withstand 10s of Watts of pump power when silicon carbide or sapphire is used as a supporting substrate [17,22].…”
Section: Sample Description Imaging System and Calibrationmentioning
Coherent laser arrays compatible with silicon photonics are demonstrated in a waveguide geometry in epitaxially grown semiconductor membrane quantum well lasers transferred on substrates of silicon carbide and oxidised silicon; we record lasing thresholds as low as 60 mW of pump power. We study the emission of single lasers and arrays of lasers in the sub-mm range. We are able to create waveguide laser arrays with modal widths of approximately 5-10 µm separated by 10-20 µm, using real and reciprocal space imaging we study their emission characteristics and find that they maintain their mutual coherence while operating on either single or multiple longitudinal modes per lasing cavity.
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