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3.3-4.3 μm high brightness LEDs
 
B. A. Matveev, N. V. Zotova, N.D.Il’inskaya, S. A. Karandashev, M. A. Remennyi, N. M. Stus’ and V.V.Shustov
Ioffe Physical-Technical Institute, Polytechnicheskaya 26, 194021, St.Petersburg, Russia.
FAX: (812) 297 7446, e-mail: bmat@iropt3.ioffe.rssi.ru, http://www.mirdog.spb.ru
 
Recent years have seen extensive research of the mid-IR (2-5 um) diodes and resonant cavity LEDs [1] as well as conventional LEDs including those with immersion lenses have already broken the 1 mW output power barrier that is necessary for most practical applications. However, curtain applications, such as spectroscopic measurements with gratings and detector system calibration, call for high brightness/apparent temperature rather than high power devices and thus the latter should be free of lenses that magnify the image dimensions. LEDs with flat out-coupling surface emitting at 3.3-3.6 um at room temperature have already shown the ability to simulate the black body heated up to 593 K (positive contrast dt = 300 K in the 3-5 um range ) [2, 3]. In spite of high output power values that could be found in the literature for the flat uncoated LEDs it is clear that there is still a room for chip design and device performance improvements.
 Deep mesa that narrows the internal radiation diagram due to the reflections from the inclined mesa sidewalls contribute to the out-coupling enhancement and is thus a useful feature of the high brightness sources. The effect of the above geometrical factor is well known for the InSb (6 um) negative luminescent devices [1] and efficient NIR and visible LEDs. However, to the best of our knowledge there have been no attempts so far to investigate the impact of the mesa dimensions/shape on the output power in a Mid-IR LED with wavelengths shorter than 6 um.
 We report on double heterostructure (DH) LEDs grown onto heavily doped n+-InAs or undoped n-InAs substrates with 2-7 um thick active layers formed from n-InAs (3.3 um) or n-InGaAsSb (3.7 um) or n-InAsSb (4.3 um) and p-InAsSbP claddings (for all LED types). DHs were treated by two stage wet photolithography process that enable us to achieve 10-40 um high sidewalls in a 250 um wide mesas with a 50-210 um wide circular Au-anode in a flip-chip device.
Common features of the fabricated LEDs were superluminescence and blue shift of the emission spectrum at 77 K due to dynamic Moss-Burstein effect, current/emission crowding above the anode contact at 300 K and superiority of the negative luminescence power conversion efficiency over the forward one at elevated temperatures (say, at 480 K) due to suppression of the Auger recombination in a depleted active layer.
The report will focus on the discussion of experimentally observed impact of several geometrical factors (active layer thickness, mesa and contact diameter and side wall height) on near and far field patterns, emission spectrum and output power including the best achieved light extraction enhancement factor of 2 for the InAsSb LEDs and apparent temperature contrast of dt=400 K (I=1 A) in the 3-5 um band for the InAs LEDs.
References
[1]          A.M.Green et al , Physica E: Low-dimensional Systems and Nanostructures, Vol. 20(3-4), pp. 531-535 (2004)
[2]          Naresh C. Das et al, Proc. of SPIE Vol. 5408, pp.136-143 (2004)
[3]          V. Malyutenko et al , MIOMD –VI digest , pp.77-78,  St.Petersburg, Russia, 28 June–2 July 2004
[4]          G.R.Nash et al , Physica E: Low-dimensional Systems and Nanostructures, Vol. 20(3-4), pp. 540-547 (2004)