Excitation energy-dependent nature of Raman scattering spectrum in GaInNAs/GaAs quantum well structures
© Erol et al.; licensee Springer. 2012
Received: 19 July 2012
Accepted: 9 November 2012
Published: 28 November 2012
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The excitation energy-dependent nature of Raman scattering spectrum, vibration, electronic or both, has been studied using different excitation sources on as-grown and annealed n- and p-type modulation-doped Ga1 − xIn x N y As1 − y/GaAs quantum well structures. The samples were grown by molecular beam technique with different N concentrations (y = 0%, 0.9%, 1.2%, 1.7%) at the same In concentration of 32%. Micro-Raman measurements have been carried out using 532 and 758 nm lines of diode lasers, and the 1064 nm line of the Nd-YAG laser has been used for Fourier transform-Raman scattering measurements. Raman scattering measurements with different excitation sources have revealed that the excitation energy is the decisive mechanism on the nature of the Raman scattering spectrum. When the excitation energy is close to the electronic band gap energy of any constituent semiconductor materials in the sample, electronic transition dominates the spectrum, leading to a very broad peak. In the condition that the excitation energy is much higher than the band gap energy, only vibrational modes contribute to the Raman scattering spectrum of the samples. Line shapes of the Raman scattering spectrum with the 785 and 1064 nm lines of lasers have been observed to be very broad peaks, whose absolute peak energy values are in good agreement with the ones obtained from photoluminescence measurements. On the other hand, Raman scattering spectrum with the 532 nm line has exhibited only vibrational modes. As a complementary tool of Raman scattering measurements with the excitation source of 532 nm, which shows weak vibrational transitions, attenuated total reflectance infrared spectroscopy has been also carried out. The results exhibited that the nature of the Raman scattering spectrum is strongly excitation energy-dependent, and with suitable excitation energy, electronic and/or vibrational transitions can be investigated.
KeywordsGaInNAs Photoluminescence Raman FT-Raman FT-IR Local modes 71.55.Eq; 63.22.+m
Raman spectroscopy has been a useful instrumental tool for characterization of semiconductors in terms of crystal quality, strain-induced effects, impurity modes and phonon energies[1, 2]. Recently, it has been shown that Raman spectroscopy is also a powerful method to determine carrier effective mass and carrier concentration of doped semiconductors by analysing the line shape of LO-plasmon coupled modes. Raman scattering is based on the inelastic scattering process of monochromatic light and mainly gives valuable information about vibrational normal modes. The energy of excitation source in conventional Raman spectroscopy is much higher than the phonon energies; therefore, the process does not only involve electron–phonon interaction, but also creates electron–hole pairs via absorption and then annihilation of electron–hole pairs via recombination. The radiative recombination process originating from transitions between electronic states can dominate the spectra and makes it impossible to resolve vibrational modes. Therefore, in Raman spectroscopy, selection of the excitation source is a crucial issue.
Raman and infrared absorption spectroscopies have also been widely used to probe the bond configuration of dilute nitride semiconductors. The presence of N in a host III-V material restructures the conduction band of the host material, and this modification has been well explained using the interaction between the localized N level and the extended conduction band state of the host material in terms of the band anti-crossing model. As a result of the interaction, the conduction band of Ga(In)As splits into two sub-bands, E − and E + . The E − band constitutes the fundamental band edge of the Ga1−xIn x N y As1−y alloy. Even a small percentage of N causes a large redshift of the band gap; therefore, incorporation of N into the III-V lattice brings more flexibility to tailor the band gap of the material. However, the optical quality of dilute nitrides is drastically affected by the presence of N. Post- or in situ thermal annealing has been used as an effective method to improve optical and crystal qualities, but this process is responsible for a significant blueshift of the band gap energy[6, 7]. The reason of the blueshift has been theoretically explained with the considerations of re-arrangement of the nearest neighbour configuration of the N environment and re-shaping of quantum well (QW) from a square to a parabolic-like shape due to Ga-In interdiffusion. Raman and infrared (IR) absorption spectroscopies have been used as experimental tools to confirm the theory.
In this work, we present the Raman scattering spectroscopy carried out with different laser lines (532, 785 and 1064 nm) in order to reveal the importance of the excitation source energy on the nature of the Raman scattering line shape as electronic, vibrational or both. Photoluminescence (PL) measurements were used to determine the electronic band gap energy of as-grown and annealed n- and p-type modulation-doped Ga1 − xIn x N y As1 − y/GaAs single QW structures with y = 0%, 0.9%, 1.2% and 1.7%. The results obtained with the 785 and 1064 nm excitation sources showed that when the energy of the excitation source is close to the electronic band gap energy of any constituent semiconductor material in the sample, a broad peak, which was supposed to stem from the electronic transitions, dominated the spectrum, making it impossible to resolve vibrational modes of respective semiconductors. A comparison between the results of Raman and PL spectroscopies supported our interpretation of Raman scattering spectroscopy. Both techniques followed the same trend under different N concentrations and thermal annealing process. On the other hand, using Micro-Raman scattering spectroscopy with the 532-nm line, even when the excitation energy is much higher than the band gap of the GaAs or Ga1 − xIn x N y As1 − y, only vibrational modes were observed. However, the intensity of the vibration modes has been observed to be very weak due to the multi-layered structure of the samples. In order to analyse the effect of the N amount and thermal annealing on vibrational modes, attenuated total reflectance (ATR) IR absorption method is preferred as a complement to the micro-Raman scattering results.
Descriptions and the codes of the samples
Micro-Raman spectra (100 to 3200 cm−1) of the samples were recorded using a Jasco NRS 3100 micro-Raman spectrometer (Jasco Corporation, Tokyo, Japan), equipped with 532 nm (green) and 785 nm (red) diode lasers, whereas Fourier transform (FT)-Raman scattering measurements were carried out using a Bruker MultiRam FT-Raman spectrometer (Bruker Optik GmbH, Ettlingen, Germany), equipped with a 1064 nm Nd-YAG laser. All Raman scattering measurements were done at back-scattering geometry at room temperature. The IR spectra of the samples were recorded on a Bruker Tensor-27 FT-IR spectrometer using a diamond ATR attachment in the 4,000 to 200 cm−1 range with a 1 cm−1 resolution.
On the other hand, PL spectra were not taken with a commercial spectrometer but with a special home-designed set-up, equipped with an Ar-ion laser (514 nm) as excitation source, thermoelectric cooled GaInAs photodetector and 0.5 m monochromator. The power of the laser was kept at 70 mW.
Results and discussions
PL peak energies and FT-Raman absolute peak energies
PL peak energy (eV)
FT-Raman absolute peak energy (eV)
As can be seen in Table2, there is a good match between FT-Raman scattering (using the absolute value of the wavenumber) and PL results. Therefore, it is obvious that the broad peaks observed in the Raman shift spectra originate from the recombination of electron and hole emitting a photon whose energy corresponds to the effective band gap of the Ga x In1−xN y As1−y semiconductor in the sample. Because the luminescence is so strong, it suppresses the possible vibrational modes related to the presence of the N atom in the host lattice which are expected to be observed between 400 and 600 cm−1.
LVM analysis of Ga1 − xIn x N y As1 − y alloys has been studied by many authors[9, 11–17] to investigate the local environment of N. In one of these studies, the LVM of N-implanted In y Ga1 − yAs grown by MBE method has been reported, and it was shown that with increasing In content in the epitaxial layer, the formation of In-rich environments was more pronounced than is expected for a random distribution of the constituents. The authors have observed two N-related LVMs at 447 and 510 cm−1 in a sample with an In content of more than 20% (In0.26Ga0.74As). They proposed N-GaIn3 configuration for these bands with C3v symmetry. As can be seen in Figure7, we also observed the same peaks at ca. 447 and 509 cm−1.
When N concentration is increased, the peak at ca. 420 cm−1 shifts down to 417 cm−1, and the relative intensity of the peak at approximately 410 cm−1 decreases. Peaks around 409 and 426 cm−1 have been reported before as related to N dimers[12, 13], but in this study, the peak at 410 cm−1 also appear in Raman spectrum for the reference sample (y = 0%). It is probably either In-related mode or Si-related mode since the GaAs barriers used are Si-doped, and the Si mode of Si-doped GaAs is known to be at approximately 399 cm−1. The peak is further affected by annealing process (see Figure9).
It is also worth mentioning that a peak at approximately 430 cm−1 is slightly forming during the annealing process (see Figure8). A peak at 434 cm−1 in the Raman spectrum of the GaInNAs quantum well has been observed after annealing, and it was proposed to be related to an In and NNAs dimer complex as can be the case in our sample. Also, the annealing procedure reveals the well-known 471 cm−1 Ga-N peak slightly (see Figure9).
We report here the raw data obtained from ATR IR and Raman spectra on n-type modulation-doped Ga0.68In0.32NyAs1−y. To assign each LVM mode correctly, further analysis of the spectra is needed like subtracting the reference spectra and band component analysis and/or second derivative analysis of the corresponding spectra. Also, the LVM analysis of p-type samples is left for a future study.
We have investigated the excitation energy-oriented nature of the Raman scattering spectrum using FT-Raman and micro-Raman techniques with different excitation sources on as-grown and annealed n- and p-type Ga1 − xIn x N y As1 − y/GaAs QW samples. ATR IR absorption and PL measurements were used to complement the Raman scattering results. FT-Raman scattering results exhibited a broad peak and two sharp peaks. A comparison between PL and FT-Raman absolute values revealed that the broad peak corresponds to the electronic transition in the Ga1 − xIn x N y As1 − y/GaAs QW and gives the well-known effect of N and thermal annealing on the band structure of the host material, i.e. In x Ga1 − xAs. On the other hand, micro-Raman with the 532 nm line of excitation source, whose energy is much higher than the electronic band gap energy of both GaAs and Ga1 − xIn x N y As1 − y, exhibited only vibrational modes. The results indicate that Raman spectroscopy can provide useful information for electronic and/or vibrational modes depending on the energy of excitation source. The effect of N and thermal annealing on chemical bond configuration is investigated using micro-Raman (with 532 nm excitation) and ATR IR absorption. We have proposed that the N environment in the samples changed as post-growth annealing was applied, and to clearly understand this new environment, further analysis of the experimental data should be made.
Attenuated total reflectance
Local vibrational modes
Molecular beam epitaxy
This work was supported by the Scientific Research Projects Coordination Unit of Istanbul University (project numbers: IRP9571, 20932 and 3875) and the Scientific and Technical Research Council of Turkey, TUBITAK (project number: 110T874). We also would like to thank COST action for enabling the collaboration possibilities.
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