1991
DOI: 10.1049/el:19911389
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1W CW, 672 nm visible laser diodes

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Cited by 28 publications
(3 citation statements)
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“…Extrapolation to the infinite cavity length yielded J th = J ∞ = 150 A cm −2 . The obtained J th are still slightly larger than the values obtained for the visible emitters by other growth methods, as J th values around 300 A cm −2 are obtained for MOCVD-grown devices emitting near 680 nm [1,15]. However, the present values are among the best ones reported for SSMBE-grown material [8], and further reduction in J th is still to be expected.…”
Section: Resultscontrasting
confidence: 65%
“…Extrapolation to the infinite cavity length yielded J th = J ∞ = 150 A cm −2 . The obtained J th are still slightly larger than the values obtained for the visible emitters by other growth methods, as J th values around 300 A cm −2 are obtained for MOCVD-grown devices emitting near 680 nm [1,15]. However, the present values are among the best ones reported for SSMBE-grown material [8], and further reduction in J th is still to be expected.…”
Section: Resultscontrasting
confidence: 65%
“…Extrapolation to the infinite cavity length yielded J th = J ∞ = 150 A cm −2 . The obtained J th are still slightly larger than the values obtained for the visible emitters by other growth methods, as J th values around 300 A cm −2 are obtained for MOCVD-grown devices emitting near 680 nm [1,15]. However, the present values are among the best ones reported for SSMBE-grown material [8], and further reduction in J th is still to be expected.…”
Section: Methodscontrasting
confidence: 53%
“…The highest η D ≈ 37% per facet was attained for lasers with a 480 µm long cavity. Typically, η D of a singleelement red laser at 680 nm is more modest, around 30% per uncoated facet [15]. A decrease of less than 10% in η D was observed for a 1020 µm cavity length, when temperature was increased from 10 • C to 70 • C. In addition, the characteristic temperature (T 0 ) was rather high.…”
Section: Resultsmentioning
confidence: 99%