Antimicrobial Gold Nanoclusters: Recent Developments and ...
O PROPERTIES OF SILICON NANOCLUSTERS · oligosilanes and their optical properties and compared...
1
O PTICAL P ROPERTIES OF S ILICON N ANOCLUSTERS Olli Lehtonen and Dage Sundholm Department of Chemistry, University of Helsinki, Finland e-mail: [email protected], [email protected] Introduction Light emitting silicon nanoclusters (Si NCs) have been studied ex- tensively during recent years after ∼ 1 nm size Si NCs were discov- ered to be photoluminescent with intense blue emission [1]. This phenomenon is demonstrated in Figure 1a where directed light beams from number of crystallites are shown. Dependence of the luminescence wavelength on the NC size has also been demon- strated, as shown in Figure 1b [2]. (a) (b) F IG . 1. (a) Photoluminescence from ∼ 1 nm crystallites (20 μm × 20 μm) and (b) Si NCs in a colloid with diameter 1.0, 1.67, 2.15 and 2.9 nm. We have investigated number of different Si NCs and also short oligosilanes and their optical properties and compared different computational methods and experiments. We also suggest new kind of silane modified clusters which have strong optical re- sponse as possible light emitters. Computational methods Molecular structures of the silicon clusters were optimized us- ing density functional theory (DFT) and the BP functional. Time-dependent DFT (TDDFT) with local density approximation (SVWN), gradient corrected functionals (BP, BLYP and PBE) and hybrid functionals (B3LYP and PBE0) was employed to obtain ex- citation energies and the oscillator strengths. Resolution of the identity (RI) approximation, or density fitting, for the Coulomb term was used to speed up the computations. For largest clus- ters also multipole-accelerated RI (MARIJ) was used. Addition- ally, second-order approximate coupled cluster model with RI (RI- CC2) was used for short oligosilanes for benchmarking purposes. Computations have been done using T URBOMOLE program pack- age [3]. Results Surface dimer model Surface dimer model suggested by Allan et al. has been often used to explain the luminescence from Si NCs [4]. In this model the dimer has a double well potential in the excited state and the ob- served blue emission would take place from the outer well in the excited state. To study the validity of this model, potential energy surfaces (PESs) of a single dimer for the ground state and few low- est excited states were investigated. PESs are shown in Figure 2. However, no double well potential is observed. Therefore, to use this model to explain luminescence from Si NCs is questionable. (a) (b) F IG . 2. The potential energy curves for the surface dimer in (a) Si 29 H 24 and (b) Si 29 H 34 as a function of the dimer elongation are shown for the singlet ground state (GS), the lowest triplet state (T), and the five lowest excited states of each irreducible representation. T d symmetric nanoclusters The dependence of the emission wavelength and the cluster size is explained by using the quantum confinement model (QCM), which is also used to explain luminescence in porous silicon [5]. As the size of the NC decreases, the wave function becomes spa- tially more confined and the energy levels recede from each other. This trend is clearly visible in Figure 3, in which lowest excitation energies for 34 T d symmetric clusters (up to Si 329 H 196 ) were cal- culated using TDDFT at MARIJ-BP/def2-SV(P) level. In our pre- vious work excitation energies and oscillator strengths of various small NCs up to about 1 nm in size have been studied [6, 7, 8, 9]. In all Si NCs the oscillator strengths at the visible region are far too small as compared to the experimentally derived oscillator strength of the emission which is 0.92 [10]. F IG . 3. Optical gap (•) and oscillator strength (×) of different clusters at MARIJ-BP/def2-SV(P) level. Fitted curve (- -) based on experimental measurements is also shown. Oxygen modified nanoclusters Various Si NCs with siloxane and hydroxyl groups attached on the surface were also investigated. Si–O–Si, Si=O and Si–OH groups usually lower the optical gap to 2.0–3.0 eV but all the oscillator strengths in the visible region are still significantly lower than ex- periments suggest. (a) (b) (c) F IG . 4. Oxygen modified Si NCs (a) Si 29 (OH) 24 (OSiH 3 ) 12 (b) Si 29 (OH) 36 and (c) Si 29 @Si 58 O 96 H 76 . Silane modified nanoclusters For short silane chains oscillator strengths have been observed to increase with the chain length [11]. Therefore, the oscillator strengths of Si NCs could be affected by modifying the NCs sur- face by attaching silane chains on it. This approach was tried with three different types of clusters [12].These structures are shown in Figure 6. (a) (b) F IG . 5. Optical spectra of silane modified clusters with (a) BP/def2- TZVP and (b) PBE0/def2-TZVP (a) (b) (c) F IG . 6. Excited state density differences for lowest excited states in (a) C s , (b) T d and (c) bridged structures. Electron accumulation is indicated with red and depletion with blue. The hybrid functional PBE0 predicts larger oscillator strengths than the BP functional and also the computed excitation energies are somewhat higher with PBE0, as is seen from optical spectra presented in Figure 5. As the length of the silane chain increases, the oscillator strengths increase as well but the excitation energies are affected only little. Similar trend is observed with smaller clus- ter containing only 10 Si atoms. This supports the concept that the oscillator strength is determined by the chain length but the energy is determined by the cluster size. The density difference between the excited and ground state for the lowest excitation are shown in Figure 6. Oligosilanes Comparison of computational methods and experimental results was possible using oligosilanes (Si m H 2m+2 , m = 1,..., 7) for which accurate and well defined experimental results are avail- able. Both density functional methods and coupled cluster meth- ods were used to obtain optical excitation energies and oscillator strengths [11]. F IG . 7. Optical gap and oscillator strength of oligosilanes at RI- CC2/aug-cc-pVQZ level. Available experimental values are also shown. The most accurate RI-CC2 results are presented in Figure 7 with experimental values. Solvation effects lower the optical gap by 0.3–0.4 eV. Close to basis set limit (aug-cc-pVQZ) LDA/GGA func- tionals underestimate the optical gap by 0.7-1.0 eV and hybrid functionals by 0.3-0.4 eV. With smaller basis sets deviations are less, e.g. def2-SV(P) ±0.2 eV and def2-TZVP underestimate by 0.2-0.5 eV. These results can be used to estimate the accuracy of computations with larger Si NCs. Conclusions The computed excited state PESs do not support the surface dimer model which is often used to explain luminescence from Si NCs. The oscillator strengths for T d symmetric hydrogen terminated Si NCs are significantly lower than experimentally observed values derived from the luminescence spectrum. In silane capped and bridged NCs both the oscillator strengths and excitation thresh- olds are comparable to experimental values and these results sug- gest a possible mechanism for bright luminescence. For accu- rate optical gaps RI-CC2 method combined with large basis sets is needed but TDDFT with moderate basis sets can be also used due to cancellation of errors. Acknowledgements Financial support from the Academy of Finland on FinNano (OPNA) project and Centers of Excellence Programme 2006-2011 is acknowledged. CSC – the Finnish IT Center for Science is ac- knowledged for providing part of the computer resources. We thank Prof. R. Ahlrichs for a copy of T URBOMOLE program pack- age. References [1] M. H. Nayfeh, N. Barry, J. Therrien, O. Akcakir, E. Gratton and G. Belomoin. Appl. Phys. Lett. 78, 1131 (2001). [2] G. Belomoin, J. Therrien, A. Smith, S. Rao, R. Twesten, S. Chaieb, M. H. Nayfeh, L. Wagner and L. Mitas. Appl. Phys. Lett. 80, 841 (2002). [3] R. Ahlrichs, M. B ¨ ar, M. H¨ aser, H. Horn and C. K ¨ olmel. Chem. Phys. Lett. 162, 165 (1989). For current version see www.turbomole.com. [4] G. Allan, C. Delerue and M. Lannoo. Phys. Rev. Lett. 76, 2961 (1996). [5] L. Canham. Visible photoluminescence from porous silicon. In L. Canham (ed.), Properties of Porous Silicon, p. 249–255. Institution of Engineering and Technology, 1997. [6] D. Sundholm. Nano Lett. 3, 847 (2003). [7] D. Sundholm. Phys. Chem. Chem. Phys. 6, 2044 (2004). [8] O. Lehtonen and D. Sundholm. Phys. Rev. B 72, 085424 (2005). [9] O. Lehtonen and D. Sundholm. Phys. Rev. B 74, 045433 (2006). [10] A. Smith, Z. H. Yamani, N. Roberts, J. Turner, S. R. Habbal, S. Granick and M. H. Nayfeh. Phys. Rev. B 72, 205307 (2005). [11] O. Lehtonen and D. Sundholm. J. Chem. Phys. 125, 144314 (2006). [12] O. Lehtonen and D. Sundholm. Phys. Chem. Chem. Phys. 8, 4228 (2006).
Transcript of O PROPERTIES OF SILICON NANOCLUSTERS · oligosilanes and their optical properties and compared...
OPTICAL PROPERTIES OF SILICON NANOCLUSTERS
Olli Lehtonen and Dage SundholmDepartment of Chemistry, University of Helsinki, Finland
e-mail: [email protected], [email protected]
IntroductionLight emitting silicon nanoclusters (Si NCs) have been studied ex-tensively during recent years after∼ 1 nm size Si NCs were discov-ered to be photoluminescent with intense blue emission [1]. Thisphenomenon is demonstrated in Figure 1a where directed lightbeams from number of crystallites are shown. Dependence of theluminescence wavelength on the NC size has also been demon-strated, as shown in Figure 1b [2].
(a) (b)FIG. 1. (a) Photoluminescence from ∼ 1 nm crystallites (20 µm × 20µm) and (b) Si NCs in a colloid with diameter 1.0, 1.67, 2.15 and 2.9 nm.
We have investigated number of different Si NCs and also shortoligosilanes and their optical properties and compared differentcomputational methods and experiments. We also suggest newkind of silane modified clusters which have strong optical re-sponse as possible light emitters.
Computational methodsMolecular structures of the silicon clusters were optimized us-ing density functional theory (DFT) and the BP functional.Time-dependent DFT (TDDFT) with local density approximation(SVWN), gradient corrected functionals (BP, BLYP and PBE) andhybrid functionals (B3LYP and PBE0) was employed to obtain ex-citation energies and the oscillator strengths. Resolution of theidentity (RI) approximation, or density fitting, for the Coulombterm was used to speed up the computations. For largest clus-ters also multipole-accelerated RI (MARIJ) was used. Addition-ally, second-order approximate coupled cluster model with RI (RI-CC2) was used for short oligosilanes for benchmarking purposes.Computations have been done using TURBOMOLE program pack-age [3].
Results
Surface dimer model
Surface dimer model suggested by Allan et al. has been often usedto explain the luminescence from Si NCs [4]. In this model thedimer has a double well potential in the excited state and the ob-served blue emission would take place from the outer well in theexcited state. To study the validity of this model, potential energysurfaces (PESs) of a single dimer for the ground state and few low-est excited states were investigated. PESs are shown in Figure 2.However, no double well potential is observed. Therefore, to usethis model to explain luminescence from Si NCs is questionable.
(a) (b)
FIG. 2. The potential energy curves for the surface dimer in (a) Si29H24
and (b) Si29H34 as a function of the dimer elongation are shown for thesinglet ground state (GS), the lowest triplet state (T), and the five lowestexcited states of each irreducible representation.
Td symmetric nanoclusters
The dependence of the emission wavelength and the cluster sizeis explained by using the quantum confinement model (QCM),which is also used to explain luminescence in porous silicon [5].As the size of the NC decreases, the wave function becomes spa-tially more confined and the energy levels recede from each other.This trend is clearly visible in Figure 3, in which lowest excitationenergies for 34 Td symmetric clusters (up to Si329H196) were cal-culated using TDDFT at MARIJ-BP/def2-SV(P) level. In our pre-vious work excitation energies and oscillator strengths of varioussmall NCs up to about 1 nm in size have been studied [6, 7, 8, 9].In all Si NCs the oscillator strengths at the visible region are fartoo small as compared to the experimentally derived oscillatorstrength of the emission which is 0.92 [10].
FIG. 3. Optical gap (•) and oscillator strength (×) of different clustersat MARIJ-BP/def2-SV(P) level. Fitted curve (- -) based on experimentalmeasurements is also shown.
Oxygen modified nanoclusters
Various Si NCs with siloxane and hydroxyl groups attached on thesurface were also investigated. Si–O–Si, Si=O and Si–OH groupsusually lower the optical gap to 2.0–3.0 eV but all the oscillatorstrengths in the visible region are still significantly lower than ex-periments suggest.
(a) (b) (c)FIG. 4. Oxygen modified Si NCs (a) Si29(OH)24(OSiH3)12 (b) Si29(OH)36
and (c) Si29@Si58O96H76.
Silane modified nanoclusters
For short silane chains oscillator strengths have been observedto increase with the chain length [11]. Therefore, the oscillatorstrengths of Si NCs could be affected by modifying the NCs sur-face by attaching silane chains on it. This approach was tried withthree different types of clusters [12].These structures are shown inFigure 6.
(a) (b)FIG. 5. Optical spectra of silane modified clusters with (a) BP/def2-TZVP and (b) PBE0/def2-TZVP
(a) (b) (c)FIG. 6. Excited state density differences for lowest excited states in (a)Cs, (b) Td and (c) bridged structures. Electron accumulation is indicatedwith red and depletion with blue.
The hybrid functional PBE0 predicts larger oscillator strengthsthan the BP functional and also the computed excitation energiesare somewhat higher with PBE0, as is seen from optical spectrapresented in Figure 5. As the length of the silane chain increases,the oscillator strengths increase as well but the excitation energiesare affected only little. Similar trend is observed with smaller clus-ter containing only 10 Si atoms. This supports the concept thatthe oscillator strength is determined by the chain length but theenergy is determined by the cluster size. The density differencebetween the excited and ground state for the lowest excitation areshown in Figure 6.
Oligosilanes
Comparison of computational methods and experimental resultswas possible using oligosilanes (SimH2m+2, m = 1, . . . , 7) forwhich accurate and well defined experimental results are avail-able. Both density functional methods and coupled cluster meth-ods were used to obtain optical excitation energies and oscillatorstrengths [11].
FIG. 7. Optical gap and oscillator strength of oligosilanes at RI-CC2/aug-cc-pVQZ level. Available experimental values are alsoshown.
The most accurate RI-CC2 results are presented in Figure 7 withexperimental values. Solvation effects lower the optical gap by0.3–0.4 eV. Close to basis set limit (aug-cc-pVQZ) LDA/GGA func-tionals underestimate the optical gap by 0.7-1.0 eV and hybridfunctionals by 0.3-0.4 eV. With smaller basis sets deviations areless, e.g. def2-SV(P) ±0.2 eV and def2-TZVP underestimate by0.2-0.5 eV. These results can be used to estimate the accuracy ofcomputations with larger Si NCs.
ConclusionsThe computed excited state PESs do not support the surface dimermodel which is often used to explain luminescence from Si NCs.The oscillator strengths for Td symmetric hydrogen terminated SiNCs are significantly lower than experimentally observed valuesderived from the luminescence spectrum. In silane capped andbridged NCs both the oscillator strengths and excitation thresh-olds are comparable to experimental values and these results sug-gest a possible mechanism for bright luminescence. For accu-rate optical gaps RI-CC2 method combined with large basis setsis needed but TDDFT with moderate basis sets can be also useddue to cancellation of errors.
AcknowledgementsFinancial support from the Academy of Finland on FinNano(OPNA) project and Centers of Excellence Programme 2006-2011is acknowledged. CSC – the Finnish IT Center for Science is ac-knowledged for providing part of the computer resources. Wethank Prof. R. Ahlrichs for a copy of TURBOMOLE program pack-age.
References[1] M. H. Nayfeh, N. Barry, J. Therrien, O. Akcakir, E. Gratton and G. Belomoin. Appl. Phys.
Lett. 78, 1131 (2001).
[2] G. Belomoin, J. Therrien, A. Smith, S. Rao, R. Twesten, S. Chaieb, M. H. Nayfeh, L. Wagnerand L. Mitas. Appl. Phys. Lett. 80, 841 (2002).
[3] R. Ahlrichs, M. Bar, M. Haser, H. Horn and C. Kolmel. Chem. Phys. Lett. 162, 165 (1989). Forcurrent version see www.turbomole.com.
[4] G. Allan, C. Delerue and M. Lannoo. Phys. Rev. Lett. 76, 2961 (1996).
[5] L. Canham. Visible photoluminescence from porous silicon. In L. Canham (ed.), Propertiesof Porous Silicon, p. 249–255. Institution of Engineering and Technology, 1997.
[6] D. Sundholm. Nano Lett. 3, 847 (2003).
[7] D. Sundholm. Phys. Chem. Chem. Phys. 6, 2044 (2004).
[8] O. Lehtonen and D. Sundholm. Phys. Rev. B 72, 085424 (2005).
[9] O. Lehtonen and D. Sundholm. Phys. Rev. B 74, 045433 (2006).
[10] A. Smith, Z. H. Yamani, N. Roberts, J. Turner, S. R. Habbal, S. Granick and M. H. Nayfeh.Phys. Rev. B 72, 205307 (2005).
[11] O. Lehtonen and D. Sundholm. J. Chem. Phys. 125, 144314 (2006).
[12] O. Lehtonen and D. Sundholm. Phys. Chem. Chem. Phys. 8, 4228 (2006).
![Tuning of the optical and electrochemical properties of ... · properties of the P dimer [13–20]. The mutation abolishes the hydrogen bond interaction between the acetyl carbonyl](https://static.fdocuments.in/doc/165x107/5f724f69abb0ce56f779aa30/tuning-of-the-optical-and-electrochemical-properties-of-properties-of-the-p.jpg)
