2.
Appl. Phys. Lett., Vol. 82, No. 17, 28 April 2003 ` Pages et al. 2809the surrounding medium, not by the local composition. Thetwo effects are opposite. Nonrandom N substitution should facilitate the forma-tion of hard clusters, so we expect clear (Ga–N) h activationeven at the present N-dilute limit. More precisely we expectthat the Nr rate in nonrandom GaAsN is larger than the Berrate in the random Be-based alloys. No Ga–N multimode was reported in GaAsN; additionalIn incorporation is believed to be needed to split the Ga–Nmode.5,10 However, we have shown that the reference(Be–VI) h mode is screened to the advantage of the FIG. 1. Geometry ͑1͒ ͑LO͒ Raman spectra of GaAs1Ϫx Nx obtained by off-(Be–VI) s mode in LO symmetry.7,8 Therefore actual Ga–N resonant 514.5 nm excitation. Open squares refer to LO modeling via thesplitting may exist in GaAsN, but barely in LO symmetry. In spatial correlation model. The L values derived are indicated. The two LO- modes calculated by taking C GaNϭϪ1.5 at xϭ0.03 are also shown ͑thincontrast the (Be–VI) h mode appears strongly in TO symme- line͒. Polarized spectra at xϭ0.03 are shown in the inset. I R and aretry. Accordingly, for (Ga–N) h -mode detection we use non- notations for the Raman intensity and wave number.standard backscattering analysis along the ͓110͔-edge layeraxis, corresponding to TO allowed only modes. This requires produce a minor signal at ϳ475 cmϪ1 between second-orderϳ1 m thick layers and high spatial resolution of the Raman GaAs-like modes, 2ϫGa–As,3 i.e., at much higher frequencymicroprobe. On a Be basis, ͑i͒ the (Ga–N) h mode should be than the dominant Ga–As signal, close to the GaAs opticalTO–LO degenerate, noted as Oh , and frequency stable when band, i.e., 268 –292 cmϪ1 . The poor structural quality due tox varies (xрx c ). Moreover ͑ii͒ it should emerge below the dӷd c is seen by the emergence of the polarization-usual GaAs:N local mode (xϳ0) at ϳ470 cmϪ1 . insensitive disorder-activated TOGa–As ͑DATO͒ mode, which The study is supported by a quantitative treatment based is theoretically forbidden ͑inset of Fig. 1͒. Further degrada-on our extension of the Hon and Faust dielectric formalism tion occurs with an increase of x. In the present DATO re-to the equations of motion and polarization given by the gime the build up of clear asymmetry on the low-frequencymodiﬁed random-element-isodisplacement model.11 The lat- side of LOGa–As mode is an indication of degradation. Basi-ter is the usual description for the two-mode A–B and A–C cally, structural defects limit the distance L, the so-calledqϭ0 oscillators in AB1Ϫx Cx alloys. Further three-mode ex- phonon correlation length, over which the phonons propa-tension is derived by adding one oscillator in the mechanical gate freely. This leads to the contribution of q 0 phonons toequations. We use the two- and three-mode Raman cross the Raman line shape. In GaAs the LO dispersion curve hassections to model the LO and TO line shapes, respectively. a negative slope near qϭ0, which accounts for the observed GaAs1Ϫx Nx layers are grown by molecular beam epitaxy asymmetry. L values between 15.5 and 11.5 are derived from͑MBE͒ on ͑001͒ GaAs substrates. Relatively large x of LOGa–As-contour modeling via the usual spatial correlation3%– 4% is considered because of potentially large Nr do- model with Gaussian distribution ͑see Fig. 1͒.11 A decrease inmains. x is measured within an accuracy of 0.25% by double L of ϳ25% is a lot for so small a variation in composition asx-ray diffraction. The layer thickness dϳ1 m required is far 1%, and indicates nonstandard structural degradation. As aabove the threshold, d c ϳ105 nm, for full relaxation at comparison the relaxed ZnBeTe layers have LOZn–Te lineNϳ3%,12 and gives rather poor crystalline quality. Raman shapes which ideally superimpose for Be variation of 2%–analysis is ﬁrst performed with the usual ͑LO-allowed, TO- 3%. Above all they exhibit a ZnTe-like strength ratio be-forbidden͒ backscattering geometry along the ͓001͔-growth tween the DATO mode at ϳ176 cmϪ1 and the allowed LO ataxis ͑1͒ to provide an overview of the Ga–As and Ga–N ϳ205 cmϪ1 below 10Ϫ2 ͑inset of Fig. 3͒, even at larger ¯two-phonon system. The LO-activated z(x,y)z and LO- substitution of 14%.8 At this stage it is feared that the requi- ¯extinct z(x,x)z polarized setups are considered, according to sed condition of dӷd c for Raman analysis of GaAsN in TOthe usual notations. The nonstandard ͑TO-allowed, LO- symmetry generates such poor crystalline quality that theforbidden͒ backscattering geometry along the ͓110͔-edge intrinsic Nr rate is altered. This is ruled out below.axis ͑2͒ is also used, with unpolarized excitation, for Possible (Ga–N) h -mode activation is investigated using(Ga–N) h -mode detection. This is optimized by taking the geometry ͑2͒, corresponding to TO data. The Ga–N range isnear-resonant 623.8 nm HeNe excitation. In geometry ͑1͒ the shown in detail in Fig. 2. The LO data at xϭ0.04 are added514.5 nm Arϩ line is preferred in order to avoid activation of for comparison. From the usual Ga–N mode at ϳ475 cmϪ1 ,the resonance of the parasitic TOGa–As mode.13 The penetra- which blueshifts when x increases, there is clear evidence oftion depth of ϳ100 nm is small with respect to d, so no an extra mode. This emerges at ﬁxed frequency, i.e., ϳ428signal comes from the substrate. Reference fully relaxed ϳ1 cmϪ1 , and appears to be TO–LO degenerate ͑see the upperm thick ͑001͒ Zn1Ϫx Bex Te layers with xϭ4% and 14% are spectra in Fig. 2͒. In the sample with xϭ0.035 the LO-likegrown by MBE on a GaInAs buffer lattice matched to InP. component of the extra mode is large enough for reliableRaman analysis is performed in geometries ͑1͒ and ͑2͒ with analysis of the symmetry ͑inset in Fig. 2͒. The usual LOGa–Nnonresonant 647.1 nm Arϩ excitation, which is relevant at mode and the extra mode undergo similar extinction withlow x. 8 respect to the polarization-insensitive 2ϫGa-As bands3 when The spectra in geometry ͑1͒ obtained with GaAs1Ϫx Nx changing from the z(x,y)z LO-activated ͑labeled 1͒ to the ¯are shown in Fig. 1. Due to small x, and to the small mass of z(x,x)z¯ LO-extinct ͑labeled 1͒ polarized setups. The sameN in comparison with As, in a ratio of 1:5, Ga–N bonds holds true for the Be reference.7,8 This establishes that the Downloaded 21 Apr 2003 to 128.118.112.221. Redistribution subject to AIP license or copyright, see http://ojps.aip.org/aplo/aplcr.jsp
3.
2810 Appl. Phys. Lett., Vol. 82, No. 17, 28 April 2003 ` Pages et al. FIG. 3. Geometry ͑1͒ ͑LO, inset͒ and ͑2͒ ͑TO͒ Raman spectra ofFIG. 2. Geometry ͑1͒ ͑LO͒ and ͑2͒ ͑TO͒ Raman spectra of GaAs1Ϫx Nx Zn1Ϫx Bex Te obtained by off-resonant 647.1 nm excitation. The calculatedobtained by resonant 623.8 nm excitation. The calculated TO multimodes BeTe-like TO multimodes are shown by thin lines. The Ber values derivedare shown by thin lines. The Nr values derived are indicated. The z(x,y)z ¯ are indicated. The two LO modes calculated at xϭ0.04 by takingLO-activated ͑1͒ and z(x,x)z LO-extinct ͑1Ј͒ polarized spectra at xϭ0.035 ¯ C Be–TeϭϪ0.2 are shown in the inset. I R and are notations for the Ramanare shown in the inset. I R and are notations for the Raman intensity and intensity and wave number.wave number. reference, for example. The TO spectra in the Be–Te rangeextra mode observed in geometry ͑1͒ can be safely regarded for xϭ4% and 14% are shown in Fig. 3. The h and s modesas a true LO mode with regard to the symmetry, which ex- appear at ϳ386 and ϳ415 cmϪ1 , respectively. The opticalcludes activation by structural disorder. Incidentally this band of BeTe is 461–503 cmϪ1 , 8 which gives R. C Be–Te ishelps to decide about point ͑i͒. In summary, the extra mode estimated to be Ϫ0.2 via the same procedure as that above,at ϳ428 cmϪ1 depicts an intrinsic feature, which satisﬁes S i.e., from the strength of the LOZn–Te /LOBe–Te ratio at xϭ4%,points ͑i͒ and ͑ii͒ in the h-mode picture above. ͑inset in Fig. 3͒. The Ber rates derived from contour model- The number of Ga–N bonds in the H domains, i.e., the ing of the TO multimodes at xϭ4% and 14% are 0.04 andNr rate, is directly derived from the amount of sharing of 0.15, respectively. Identical values are found for ZnBeSe.GaN-like oscillator strength (R) and Faust–Henry coefﬁ- Even the latter value is much smaller than the GaAsN onecient (C) between the two kinds of Ga–N bonds in the TO although it corresponds to a much larger substitution, as ex-multimode cross section. R is ﬁxed by the optical band in pected.cubic GaN, i.e., ϳ555–740 cmϪ1 . The most recent estimate We have shown by using a nonstandard TO-like Ramanof C of Ϫ3.8 refers to hexagonal GaN.14 This might differ setup that the percolation picture used for basic understand-from the value used with the present Ga–N bonds dispersed ing of atypical Raman multimodes in Be-chalcogenide al-in a GaAs-like zinc blende lattice. Therefore C is derived loys, with contrast in the shear modulus, basically applies tofrom the balance of strength between the LOGa–As and GaN–GaAs mixed crystals, with contrast in the bulk modu- SLOGa–N modes at xϭ0.03, corresponding to quasisymmetric lus. This allows one to discriminate between the signals frombroadening of the Ga–As mode and still signiﬁcant Ga–N N-poor and N-rich regions in GaAsN ͑Nϳ3%– 4%͒. Thesignal. Fair contour modeling is obtained by taking CϳϪ1.5 number of N atoms in the latter domains is derived from the͑solid line in Fig. 1͒. Slight misestimation due to possible balance of strength via curve ﬁtting of the TO multimodes. sdisorder activation of the theoretically forbidden TOGa–N We ﬁnd a value of ϳ30% which is much larger than themode close to the allowed-LO mode has basically no inﬂu- corresponding Be rate of ϳ4% in random Be-based alloys.ence on the ﬁnal Nr value ͑see below͒. Finally R and C areinjected in the TO multimode cross section, and Nr is ad- J. Neugebauer and C. G. Van De Walle, Phys. Rev. B 51, 10568 ͑1995͒. 1 2justed so as to mirror the balance of strength between the h- D. J. Friedman, J. F. Geisz, S. R. Kurtz, and J. M. Olson, J. Cryst. Growthand s-like Ga–N modes. The best ﬁts are shown in Fig. 2. A 195, 409 ͑1998͒. 3 A. M. Mintairov, P. A. Blagnov, V. G. Melehin, N. N. Faleev, J. L. Merz,typical Nr rate is ϳ30% at xϳ3%– 4%. We want to mention Y. Qiu, S. A. Nikishin, and H. Temkin, Phys. Rev. B 56, 15836 ͑1997͒.that Nr varies less than 5% when C assumes a value of Ϫ3.8. 4 T. Prokoﬁeva, T. Sauncy, M. Seon, M. Holtz, Y. Qiu, S. Nikishin, and H.Also, we have checked that the balance of strength between Temkin, Appl. Phys. Lett. 73, 1409 ͑1998͒. 5the h and s modes is stable with resonant ͑632.8 nm͒ and ¨ J. Wagner, T. Geppert, K. Kohler, P. Ganser, and N. Herres, J. Appl. Phys. 90, 5027 ͑2001͒.off-resonant ͑514.5 nm͒ excitations; only the signal-to-noise 6 M. J. Seong, M. C. Hanna, and A. Mascarenhas, Appl. Phys. Lett. 79,ratio varies. Therefore Nr misestimation due to possible 3974 ͑2001͒. 7 ¨parasitical resonance-induced Frohlich scattering by LO ` ´ O. Pages, M. Ajjoun, D. Bormann, C. Chauvet, E. Tournie, and J. P.modes from the ͑110͒ side face is excluded. The key point is 5 Faurie, Phys. Rev. B 65, 35213 ͑2002͒. 8 ` O. Pages, T. Tite, D. Bormann, O. Maksimov, and M. C. Tamargo, Appl.that while the structural quality degrades with an increase of Phys. Lett. 80, 3081 ͑2002͒.x ͑refer to L values in Fig. 1͒, Nr remains quasistable. Our 9 L. Bellaiche, S.-H. Wei, and A. Zunger, Phys. Rev. B 54, 17568 ͑1996͒. 10Nr estimate can therefore be taken as chieﬂy representative S. Kurtz, J. Webb, L. Gedvilas, D. Friedman, J. Geisz, J. Olson, R. King, D. Joslin, and N. Karam, Appl. Phys. Lett. 78, 748 ͑2001͒.of intrinsic nonrandom N substitution, in spite of the poor 11 ` ´ O. Pages, M. Ajjoun, D. Bormann, C. Chauvet, E. Tournie, J. P. Faurie,structural quality. and O. Gorochov, J. Appl. Phys. 91, 43211 ͑2002͒. Let us compare with the corresponding Ber rate in 12 R. Srnanek, A. Vincze, J. Kovac, I. Gregora, D. S. Mc Phail, and V.Zn–Be chalcogenides. Here the atomic substitution is truly Gottschalch, Mater. Sci. Eng., B 91, 87 ͑2002͒. 13 H. M. Cheong, Y. Zhang, A. Mascarenhas, and J. F. Geisz, Phys. Rev. Brandom since the x c value detected with good accuracy from 61, 13687 ͑2000͒.vibrational singularities7,8 coincides with the theoretical one 14 F. Demangeot, J. Frandon, M. A. Renucci, N. Grandjean, B. Beaumont, J.calculated on a random basis.9 Let us take Zn1Ϫx Bex Te as a Massies, and P. Gibart, Solid State Commun. 106, 491 ͑1998͒. Downloaded 21 Apr 2003 to 128.118.112.221. Redistribution subject to AIP license or copyright, see http://ojps.aip.org/aplo/aplcr.jsp
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