2022
DOI: 10.1109/jstqe.2021.3095660
|View full text |Cite
|
Sign up to set email alerts
|

Experimental Studies Into the Beam Parameter Product of GaAs High-Power Diode Lasers

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

1
14
0

Year Published

2022
2022
2024
2024

Publication Types

Select...
6
2

Relationship

3
5

Authors

Journals

citations
Cited by 18 publications
(15 citation statements)
references
References 30 publications
1
14
0
Order By: Relevance
“…The change of the BPP lat with increasing ΔT is nearly identical, being slightly faster for the case of the ASLOC laser (S th = 0.36 vs. 0.33 mm.mrad/K). The reason for the lower BPP 0 for the ETAS laser requires further study: see [31]- [33]. Overall, the improvement in the BPP lat of the ETAS DBR lasers confirms the pattern observed in the FP BA lasers without DBRs in [21].…”
Section: Resultssupporting
confidence: 73%
See 1 more Smart Citation
“…The change of the BPP lat with increasing ΔT is nearly identical, being slightly faster for the case of the ASLOC laser (S th = 0.36 vs. 0.33 mm.mrad/K). The reason for the lower BPP 0 for the ETAS laser requires further study: see [31]- [33]. Overall, the improvement in the BPP lat of the ETAS DBR lasers confirms the pattern observed in the FP BA lasers without DBRs in [21].…”
Section: Resultssupporting
confidence: 73%
“…The measured data points are fitted with a linear empirical fit BPP lat = BPP 0 + S th ΔT, following [30], where ΔT is the increase of the average temperature in the active region over T HS (calculated by multiplying the dissipated power within the device by the thermal resistance). BPP 0 represents the non-thermal background of the BPP lat which include contributions from all the effects nearly unaffected with temperature change, e.g., process or packaging related waveguiding [31]. The second term in the fit equation describes the change of the BPP lat due to internal heating, with S th representing the rate.…”
Section: Resultsmentioning
confidence: 99%
“…As can be seen in Fig. 9(b)(top), the TM-polarized emission is enhanced at the stripe edges of the IG emitters which is associated with the mechanical stress fields originating from the trenches there [18]. The absence of such mechanical stresses in gain-guided ETAS bars improves their DOP by 1-3% up to I opt = 1.8 kA.…”
Section: Improvement Of Beam Quality By Lateral Waveguidingmentioning
confidence: 85%
“…Such kW-class bars contain an array of broad-area (BA) emitters arranged side-byside in lateral direction. Experimental studies show that a strong thermal lens evolves during laser operation and the lensing effect becomes stronger with increasing operating power [8,9]. The resulting stronger waveguiding allows more transverse modes to contribute to the laser emission deteriorating the beam quality (i.e.…”
Section: Introductionmentioning
confidence: 99%
“…A decrease in the thermal lensing in the emitters, by making the thermal profiles flatter, is an effective technique to improve the beam quality. For example, in [9], it has been shown that by bringing the emitters closer together in the bar the thermal interaction between the emitters can be enhanced which flattens the thermal profiles of the individual emitter and provides an overall lower θlat of the bar. Several other approaches have also been attempted, as recently reviewed in [9,10].…”
Section: Introductionmentioning
confidence: 99%