1. Introduction
Photoluminescence (PL) measurements on nominally undoped n-type GaN bulk and epitaxial layers grown by different techniques on different substrates usually show besides the near band edge emission a broad yellow band with maximum at 2.25 eV Reference Ogino and Aoki[1] Reference Hofmann, Kovalev, Steude, Meyer, Hoffmann, Eckey, Heitz, Detchprom, Amano and Akasaki[2] Reference Monteiro, Pereira, Correia, Xavier, Hofmann, Meyer, Fischer, Cremades and Piqueras[3] Reference Glaser, Kennedy, Doverspike, Rowland, Gaskill, Freitas, Khan, Olson, Kuznia and Wickenden[4] Reference Calleja, Sanchez, Basak, Sanchez-Garcia, Munoz, Izpura, Calle, Tijero, Sanchez- Rojas, Beaumont, Lorenzini and Gibart[5].
It is known that GaN and its alloys are important materials for light-emitting devices as blue-UV lasers and LEDs, short-wavelength optical detectors and high-temperature electronics. However, the presence of unwanted deep states in the band gap due to native or extrinsic defects reduces the efficiency of devices.
The yellow band has been attributed either to a shallow donor to a deep donor (acceptor) pair recombination Reference Ogino and Aoki[1] Reference Hofmann, Kovalev, Steude, Meyer, Hoffmann, Eckey, Heitz, Detchprom, Amano and Akasaki[2], to a deep double donor to a shallow acceptor Reference Glaser, Kennedy, Doverspike, Rowland, Gaskill, Freitas, Khan, Olson, Kuznia and Wickenden[4] or to a shallow donor and a deep state Reference Calleja, Sanchez, Basak, Sanchez-Garcia, Munoz, Izpura, Calle, Tijero, Sanchez- Rojas, Beaumont, Lorenzini and Gibart[5]. The first model accounts for a binding energy of the acceptor at EA ≈ 860 meV Reference Ogino and Aoki[1] and a binding energy of the donor of ED › 35 meV Reference Hofmann, Kovalev, Steude, Meyer, Hoffmann, Eckey, Heitz, Detchprom, Amano and Akasaki[2]. In the second one, the donor state is located 700 meV below the conduction band (CB) while the acceptor level is located 200 meV above the valence band (VB). The third model agrees with a deep state near 1eV above the VB Reference Calleja, Sanchez, Basak, Sanchez-Garcia, Munoz, Izpura, Calle, Tijero, Sanchez- Rojas, Beaumont, Lorenzini and Gibart[5] not far from the energy of the deep acceptor of previous work Reference Ogino and Aoki[1] Reference Hofmann, Kovalev, Steude, Meyer, Hoffmann, Eckey, Heitz, Detchprom, Amano and Akasaki[2]. Currently most of the experimental evidence favours the first model.
In order to clarify the recombination mechanisms involved in the yellow band emission different techniques as photoluminescence Reference Ogino and Aoki[1] Reference Hofmann, Kovalev, Steude, Meyer, Hoffmann, Eckey, Heitz, Detchprom, Amano and Akasaki[2] Reference Monteiro, Pereira, Correia, Xavier, Hofmann, Meyer, Fischer, Cremades and Piqueras[3] Reference Glaser, Kennedy, Doverspike, Rowland, Gaskill, Freitas, Khan, Olson, Kuznia and Wickenden[4] Reference Calleja, Sanchez, Basak, Sanchez-Garcia, Munoz, Izpura, Calle, Tijero, Sanchez- Rojas, Beaumont, Lorenzini and Gibart[5], optically detected magnetic resonance (ODMR) Reference Hofmann, Kovalev, Steude, Meyer, Hoffmann, Eckey, Heitz, Detchprom, Amano and Akasaki[2] Reference Glaser, Kennedy, Doverspike, Rowland, Gaskill, Freitas, Khan, Olson, Kuznia and Wickenden[4], time resolved ODMR Reference Koschnick, Spaeth, Glaser, Doverspike, Rowland, Gaskill and Wickenden[6], photocapacitance Reference Calleja, Sanchez, Basak, Sanchez-Garcia, Munoz, Izpura, Calle, Tijero, Sanchez- Rojas, Beaumont, Lorenzini and Gibart[5], deep level transient spectroscopy (DLTS) Reference Calleja, Sanchez, Basak, Sanchez-Garcia, Munoz, Izpura, Calle, Tijero, Sanchez- Rojas, Beaumont, Lorenzini and Gibart[5], cathodoluminescence Reference Piqueras, Xavier, Monteiro, Pereira, Fischer, Hofmann, Meyer and Cremades[7] Reference Li and Coleman[8] and PL under hydrostatic pressure Reference Suski, Perlin, Teisseyre, Leszczynski, Grzegory, Jun, Bockowski, Porowski and Moustakas[9] have been used. However its origin and the nature of shallow and deep levels still lacks explanation.
As this emission band is detected in different samples grown under different conditions native defects as VN and GaI are potential candidates involved in the recombination mechanism. The n-type conductivity of undoped GaN is commonly attributed to these point defects Reference Boguslawski, Briggs and Bernholc[10] Reference Jenkins and Dow[11]. Also, impurities as O Reference Zolper, Wilson, Pearton and Stall[12] and C Reference Ogino and Aoki[1] as well as complex defects like VGa-O Reference Neugebauer and Walle[13] have been considered to explain the yellow luminescence recombination. In the present work we identify a level 13.7 meV below the shallow donor responsible for an intensity increase with temperature of the yellow band luminescence and an underlying band of long lifetime in the high energy side of the yellow band.
2. Materials and Methods
The samples used in this work were undoped wurtzite GaN layers grown by metal organic vapour phase epitaxy (MOVPE) on (0001) sapphire substrates at a growth temperature of ~ 1050°C. TrimethylGallium was used as Ga metalorganic and NH3 as nitrogen precursor. The layer thickness was 500 nm and the carrier concentration 1017 to 1018 cm−3 at RT. Time resolved photoluminescence (TRPL) spectra and lifetime measurements were carried out with a 1934C Spex phosphorimeter using a pulsed Xe arc lamp with a pulse width of 3 μs (tail after 10 μs accounts for 1% of initial intensity) as light source. Steady state photoluminescence (SSPL) spectra were obtained after excitation above the band gap by using a Xe arc lamp as light source in combination with a monochromator. In both cases the luminescence was dispersed by a Spex 1704 monochromator and detected by a photomultiplier. The samples were held in a cold tip of a closed cycle Air-Products He cryostat in a temperature range between 10K and RT.
3. Experimental Results and Discussion
In figure 1 the steady state luminescence spectra of a non-intentionally doped MOVPE grown GaN sample are shown for different temperatures. There is a noticeable increase in luminescence intensity of the yellow band from 30K to ca. 100K (figure 1a), followed by a steady decrease. This feature is not found in all samples, as in most the luminescence stays fairly constant for lower temperatures and becomes thermally quenched above 120K Reference Hofmann, Kovalev, Steude, Meyer, Hoffmann, Eckey, Heitz, Detchprom, Amano and Akasaki[2]. The temperature dependence of the intensity of the yellow band is shown in figure 2.
Figure 1. Steady state luminescence spectra for different temperatures.
Figure 1a. Steady state luminescence spectra for different temperatures. Expanded yellow band region.
Figure 1b. Steady state luminescence spectra for different temperatures. High energy shift of the yellow band with temperature.
Figure 2. Temperature dependence of the yellow band intensity. Solid line: fit to equation 2.
When the spectra are taken in transient spectroscopy we can see that the yellow band does not change for delays after the light pulse from 80 μs to 1 ms. However, as illustrated in figure 3 for longer delays (above 10 ms) a broader band starts to appear in the high energy side of the emission (centred at 2.35eV). It has a decay of ca. 300 ms at 10K, and it is not as strongly temperature quenched as the yellow band centred at 2.25eV. This accounts for the shift towards higher energies with temperature as seen in the steady state spectra of figure 1b. As this emission is well separated from the yellow band in time resolved spectroscopy it does not interfere with the following analysis of the yellow band.
Figure 3. Time resolved spectra for different time delays (TD) and time windows (TW) at 10K.
The temperature dependence of the lifetimes of the yellow band is shown in figure 4. We can observe a dominant decay of 0.2 ms fairly temperature independent and a second component with a value of 3 ms at 10K, that between 50 and 100K is strongly reduced. The fast component is of the order of magnitude commonly found for the yellow band Reference Koschnick, Spaeth, Glaser, Doverspike, Rowland, Gaskill and Wickenden[6]. The change in value of the slower component (that is observed only in samples where the intensity increase occurs) is seen in the temperature region where the band presents the intensity increase.
Figure 4. Temperature dependence of lifetimes. Solid line: fit of the slow decay according to equation 1.
The temperature dependence of the slower component of the decay follows an exponential law (1), from which an activation energy (Ea) of 13.7 meV can be obtained:
With this value for the activation energy we can fit the temperature dependence of the intensity up to 100K with the equation 2. This is shown by the full line in figure 2.
From these results we can conclude that there is a level 13.7 meV below the shallow donor that can populate the levels responsible for the yellow emission. At present we cannot identify the nature of this level. Recent reports on ODMR have been presented showing that besides the shallow donor with g=1.952 , a second resonance appears with g=1.958, that might be associated with the level below the shallow donor Reference Gibart[14]. For samples which do not show the intensity increase of the yellow band with temperature, the relative intensity of the yellow band emission compared with the near band edge emission is higher. The fact that in samples with a relatively strong yellow band emission there is no noticeable increase in luminescence intensity with temperature might be attributed to the fact that the emission due to the indirect population of the excited states of the yellow band represents only a minor fraction of the total emission. This might be due to a low concentration of the defects that are responsible for the indirect population of the yellow band. Therefore, the process is only observed in samples where the total yellow band emission is relatively weak.
The long lived emission with maximum at 2.35eV is also found in other samples. It can be seen independently in samples where there is no increase in intensity of the yellow band, as for delays above 10 ms the 2.25eV band emission is relatively weak in these samples. This band is responsible for the broadening and shift to higher energies of the yellow band when the temperature increases, as it becomes less quenched than the yellow band centred at 2.25eV.
4. Conclusions
A trap 13.7 meV below the shallow donor is responsible for the intensity increase of the yellow band luminescence observed between 30 and ca.100K
Although the yellow band in GaN is a common feature of most samples, complex mechanisms are involved in this emission. An intensity increase with temperature is attributed to a level 13.7meV below the shallow donor from where the emission originates. Time resolved spectroscopy reveals the presence of another emission with maximum at 2.35eV and a decay time of ca. 300 ms at 10K. This band is responsible for the shift towards higher energies with temperature as it is less temperature quenched than the yellow band.
Acknowledgments
This work has been performed under the auspices of the Commission of the European Communities, under contract BRPR-CT96-034 (DG 12 - RSMT). Also financial support by JNICT, contract PRAXIS XXI PBIC/C/CTM/1925/95 is acknowledged.
