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Effect of Post Thermal Annealing on the Optical Properties of InP/ZnS Quantum Dot Films
Nanoscale Research Letters volume 13, Article number: 369 (2018)
The enhancement of optical properties via thermal annealing on InP/ZnS core/shell quantum dot (QD) film was investigated in this work. The increase of emission intensities of the QD films was observed after thermal annealing at 180 °C for 5 min. Through temperature dependence photoluminescence (TDPL) and power dependence photoluminescence (PL) measurement, the peak located at the low-energy shoulder was confirmed to be localized state emission and the high energy one comes from free-carrier emission. Moreover, from the TDPL spectra of the sample annealed at 180 °C for 5 min, the full width at half maximum (FWHM) of localization state emission was nearly the same before which is 250 K and then decreased with increasing temperature. However, the FWHM was decreased significantly when temperature increased in the untreated sample. We conclude that the escape of localization states with increasing temperature contributes to this anomaly phenomenon. Our studies have significance on the application of QDs in electroluminescence devices and down-conversion light-emitting devices.
Colloidal quantum dots (QDs) have various applications such as displays , spectrometers , sensing , light-emitting diodes , laser , photoelectrochemicals [6, 7], and biolabeling . InP-based QDs appear to be an ideal candidate for Cd-based QDs due to their similar band gap to CdSe, band gap tenability which covers the entire visible range, and the reduced toxicity . It is reported that the synthesized InP QDs always have a larger size distribution, and the full width at half maximum (FWHM) of the photoluminescence (PL) spectra of InP-based QDs usually lie in the range of 50–100 nm. This value is significantly larger than the Cd-based QDs, where the typical FWHM is around 20–30 nm. Considering the difficult synthesis and the larger size distribution of InP-based QDs, it still needs a lot of work to do for researchers.
At the same time, due to the surface traps, dangling bonds, stacking faults in the crystal, and a high activation barrier for the trapping centers, the PL quantum yield (QY) of InP QDs is relatively low (< 1%) . Strategies to enhance the emission include chemical modification the particle surface [11, 12], or epitaxial growth of a shell of larger band gap semiconductors [13,14,15]. These strategies aim to reduce non-radiative recombination centers by surface passivation. Beside the above treatments, researchers also use thermal annealing to improve the crystalline properties of materials. It is known that thermal treatment can remove the organic surfactants from the surface of QDs to reduce the distance and consequently increase the electronic coupling between the QDs [16, 17]. Post thermal treatment processes have significantly influenced the optical and electrical properties of the QDs and improved the performance of QD-based optoelectronic devices. And it is essential to understand the effect of thermal annealing on the carriers’ recombination processes inside core/shell QDs for better device performance.
Here we fabricated InP/ZnS core-shell QD films by spin coating. QDs were spun onto the Si substrate to form a solid film. The films were annealed at different temperatures. We measured the PL spectra for these samples at 300 K, and it is found that only the sample annealed at 180 °C shows enhanced light emission. Temperature- and power-dependent PL measurements were carried out, and the untreated sample was compared with the sample annealed at 180 °C. Based on the experimental results, the origin of the peak of QD films and the effect of annealing have been discussed in detail.
InP/ZnS nanocrystals are synthesized based on protocols published on other papers [8, 9]. Two hundred milligrams (0.45 mmol) of indium (III) chloride and 122 mg (2.2 mmol) of zinc (II) chloride are mixed in 5 mL of oleylamine which is a coordinating solvent. The reaction mixture is stirred and degassed at 100 °C for half an hour and then heated to 220 °C under inert atmosphere. Upon reaching 220 °C, a volume of 0.25 mL oftris(dimethylamino)phosphine is quickly injected in the above mixture. After the phosphorous precursor injection, the InP nanocrystal synthesis proceeded. The InP core reaction occurs during 3 min. At 3 min, slow injection of 0.6 mL of saturated TOP-S (2.2 M) was done. At 17 min, injection of 1 mL of stoichiometric TOP-S (2.2 M) was done. At 30 min, slow injection of 1 g of Zn(stearate)2 in 4 mL of octadecene was done. At 60 min, temperature is increased from 220 to 240 °C. At 65 min, injection of 0.7 mL of stoichiometric TOP-S (2.2 M) was done. At 90 min, injection of 1 g of Zn(stearate)2 in 4 mL of octadecene was done. At 95 min, temperature is increased from 240 to 260 °C. At 150 min, the reaction ended. At the end of the reaction, the temperature is cooled down. InP/ZnS nanocrystals are then precipitated in ethanol and suspended in chloroform. A 3.2 nm InP core with a 2 nm-thick ZnS shell was prepared. The QY was measured to be 47%.
Then the core/shell QD solutions with very low concentration were spun onto the Si substrate with a speed of 1500 rpm for 30 s. After drying, we measured their emission and find the intensity nearly the same, which avoids the influence of the QDs loading in the films. And then, three samples of them were treated by thermal annealing; the temperatures were set at 180, 200, and 220 °C, respectively with a treatment time of 5 min [18, 19]. The annealing procedure was carried out under a nitrogen atmosphere at ambient pressure using a commercially available RTA reactor (Accu Thermo AW410, Allwin 21 Corp.). For the PL measurement, the emissions of the samples were recorded using LAB-RAM Infinity system. During the measurement, a 488-nm Argon laser was used as the excitation source.
Results and Discussion
Figure 1a shows the PL spectra (red line) and absorption spectra (blue line) of colloidal InP/ZnS QDs in solution. The absorption and PL peaks are located at 2.215 eV (560 nm) and 1.914 eV (648 nm), respectively. The FWHM of the PL peak is 70 nm. The black line is the PL spectra of InP/ZnS QD films. Compared with the PL spectra of QDs in solution, a new peak appears at the low energy side. The reason for these differences may be due to the cluster of the QD in film state as reported before . The colloidal QDs in solution are well dispersed and have been protected by surface ligands. Therefore, the colloidal QDs in the solution are relatively stable. As for the QD film, surface ligands will be broken and QDs will be easier to get clusters, introducing a more local state. As shown in Fig. 1b, the PL spectra of InP/ZnS QD film could be well-fitted by three individual Gaussian peaks, namely, the low-energy tail, peak A, and peak B. The low-energy tail is probably due to shallow level defects as described in other articles [21, 22]. Peak A locates at 1.80 eV, with the FWHM of 0.140 eV, while peak B locates at 1.923 eV and the FWHM is 0.151 eV. The origin of peaks A and B will be analyzed through power-dependent PL and temperature dependence photoluminescence (TDPL) later.
Figure 2 shows the excitation power-dependent PL spectra of the QD film measured at room temperature. The insert is the integrated PL intensity of the peaks with excitation power. The excitation power-dependent PL intensity is widely used to determine the origin of emission. It has been pointed out that the PL intensity (I) can be expressed as the following equation [22, 23],
where I0 is the power of the excitation laser, η is the emission efficiency, and the exponent α represents the radiative recombination mechanism. For recombination of excitons, the value of α has been reported to be in the range 1 < α < 2. For band to band transition, α ≈ 2. For impurity- or defect-related emission, the value of α is less than 1, such as free-to-bound recombination and donor–acceptor transition [24,25,26]. According to the equation, the parameter α can be obtained to be 0.895 for peak A and 1.103 for peak B. Moreover, it can be seen that with the increase of excitation power, peak A shows a slight blueshift, which agrees well with the conclusion that peak A comes from the localization states . From the discussions shown above, it can be concluded that peak A is emission related to localized states, and peak B is due to the free-carrier transition.
The PL spectra of all the four samples at room temperature are displayed in Fig. 3a. After annealing at 180 °C, the absolute intensities of the PL spectra increased. The intensity of the emission contrarily decreases with the further increase of annealing temperature, which has been shown in the inset of Fig. 3a. Later, the untreated sample and the sample annealed at 180 °C for 5 min will be discussed intensively. For the sample annealed at 200 and 220 °C, the annealing process introduced other non-radiative recombination centers, suppressing the free carrier emission. Figure 3b, c displays the transmission electron microscopy (TEM) images of the untreated sample and sample annealed at 180 °C for 5 min, respectively. From these two images, the same QDs’ shape, size, and crystalline can be found. It can be seen from the TEM image that the lattice constant is 0.34 nm, which is consistent with the (111) crystal plane of the sphalerite structure InP, and the core size is about 3 nm.
The TDPL measurements of two samples have been conducted, as shown in Fig. 4a, b. Figure 4c, d shows the PL peak position as a function of temperature for the two samples. Solid lines are the fitting curves according to Varshni’s equation , which gives the temperature dependence of the band gap of bulk semiconductors and has also been used for quantum dots [21, 22, 29, 30],
where Eg(0) is the band gap at 0 K, α is the temperature coefficient, and the value of β is the Debye temperature. From the graph, it can be seen that peak B can be well fitted by Varshni’s equation, which suggests peak B emissions from the near band emission. The parameters obtained from the fitting are Eg(0) = 1.983 eV, α = 4.910 × 10−4 eV/K, and β = 320 K for the untreated sample and Eg(0) = 1.991 eV, α = 4.896 × 10−4 eV/K, and β = 320 K for the annealed sample. It can be seen that the values of α and β are nearly the same as those of bulk InP, which are α = 4.91 × 10−4 eV/K and β = 327 K . For Eg(0), it has an 8-meV blueshift after annealing. This is probably due to the inter-diffusion of atoms near the core-shell interface and leads to the decrease of InP core. For peak A, it can be fitted well from 95 to 200 K. After 200 K, it shows an increasing red shift according to Varshni’s equation. This phenomenon can be explained by the carrier’s localization. It is known that with the increase of temperature, the carriers from the shallow level defect states will gain enough energy to escape and become free carriers. From the experimental results, it can be seen that both samples show a carrier localization effect. However, after annealing, the depth of localization states increased. From the fitting curve, we can conclude that peak A originates from the localization states, and peak B emissions from the free carrier transition. This result is in accordance with the result from the excitation power-dependent PL spectra of the untreated sample.
From Fig. 5a, b, we can clearly see the increase of free carrier emission, which can be interpreted by the removal of some shallow localization states of QDs after annealing. Compared with the PL spectra of these two samples at 300 K, we found that, for the untreated sample, peak A and B emissions are located at 1.798 and 1.917 eV, respectively. For the sample annealed at 180 °C for 5 min, the A and B emissions are located at 1.794 and 1.922 eV, respectively. After annealing, the peak positions are nearly the same, but the FWHM of peak B broadens from 0.1508 to 0.1761 eV.
Figure 6a shows the FWHM variation with temperature of peak A for the untreated sample and sample annealed at 180 °C for 5 min. For the untreated sample, the FWHM of peak A decreases with increasing temperature. However, for the sample annealed at 180 °C for 5 min, the FWHM is nearly the same before 250 K and then narrows down with increasing temperature. In the usual cases, the FWHM of TDPL spectra will homogeneously broaden with increasing temperature because of the scattering of the exciton by acoustic and optical phonons . For better understanding, an energy band diagram after annealing is used to study the phenomenon and fitting curve of peak A in Fig. 4, as shown in Fig. 6b. There are a series of localization states in the samples to form peak A. When the temperature increases, the carriers at shallow localization states can escape, causing the red shift compared with Varshni’s equation and the narrowing down of FWHM. When the thermal annealing is performed, some shallow localization states are removed. So the FWHM were constant and then narrowed down.
In summary, we have reported the enhancement of optical properties of thermal annealing on InP/ZnS core/shell QD films. By combining temperature-dependent emission peak position and power dependence spectra, we find direct evidence that peak A emission is from localization states and peak B from free-carrier emission. Referring to the energy band structure revealed by TDPL spectrum, the change of temperature-dependent emission peak position is quantitatively described based on thermal activated redistribution of localized excitons. With the discussion of the effect of annealing on PL spectra, we find annealing significantly increases the emission of free carrier for the removal of some localization states. Our studies have significance on the application of QD devices in electroluminescence or down-conversion of light-emitting applications.
Full width at half maximum
Rapid thermal annealing
Temperature dependence photoluminescence
Transmission electron microscopy
Bourzac K (2013) Quantum dots go on display. Nature 493(7432):283
Bao J, Bawendi MG (2015) A colloidal quantum dot spectrometer. Nature 523(7558):67
Lorenzon M, Christodoulou S, Vaccaro G, Pedrini J, Meinardi F, Moreels I et al (2015) Reversed oxygen sensing using colloidal quantum wells towards highly emissive photoresponsive varnishes. Nat Commun 6:6434
Sun Q, Wang YA, Li LS, Wang D, Zhu T, Xu J et al (2007) Bright, multicoloured light-emitting diodes based on quantum dots. Nat Photonics 1(12):717–722
Klimov VI, Mikhailovsky AA, Xu S, Malko A, Hollingsworth JA, Leatherdale CA et al (2000) Optical gain and stimulated emission in nanocrystal quantum dots. Science 290(5490):314–317
Tong X, Zhou Y, Jin L et al (2017) Heavy metal-free, near-infrared colloidal quantum dots for efficient photoelectrochemical hydrogen generation. Nano Energy 31:441–449
Tong X, Kong X, Zhou Y et al (2018) Near-infrared, heavy metal-free colloidal “giant” core/shell quantum dots. Adv Energy Mater 8(2):1870010
Jr MB, Alivisatos AP (1998) Semiconductor nanocrystals as fluorescent biological labels. Science 281(5385):2013
Brunetti V, Chibli H, Fiammengo R, Galeone A, Malvindi MA, Vecchio G et al (2012) InP/ZnS as a safer alternative to CdSe/ZnS core/shell quantum dots: in vitro and in vivo toxicity assessment. Nanoscale 5(1):307
Guzelian AA, Katari JEB, Kadavanich AV, Banin U, Hamad K, Juban E et al (1996) Synthesis of size-selected, surface-passivated InP nanocrystals. J Phys Chem 100(17):7212–7219
Mićić OI, Cheong HM, Fu H, Zunger A, Sprague JR, Mascarenhas A et al (1997) Size-dependent spectroscopy of InP quantum dots. J Phys Chem B 101(25):4904–4912
Talapin DV, Gaponik N, Borchert H, Rogach AL, Markus Haase A, Weller H (2003) Etching of colloidal InP nanocrystals with fluorides: photochemical nature of the process resulting in high photoluminescence efficiency. ChemInform 34(9):12659–12663
Mićić OI, Smith BB, Nozik AJ (2000) Core−shell quantum dots of lattice-matched ZnCdSe2 shells on InP cores: experiment and theory. J Phys Chem B 104(51):12149–12156
Bharali DJ, Lucey DW, Jayakumar H, Pudavar HE, Prasad PN (2005) Folate-receptor-mediated delivery of InP quantum dots for bioimaging using confocal and two-photon microscopy. J Am Chem Soc 127(32):11364–11371
Haubold S, Haase M, Kornowski A, Weller H (2001) Strongly luminescent InP/ZnS core-shell nanoparticles. ChemPhysChem 2(5):331
Lee JS, Kovalenko MV, Huang J, Chung DS, Talapin DV (2011) Band-like transport, high electron mobility and high photoconductivity in all-inorganic nanocrystal arrays. Nat Nanotechnol 6(6):348
Mentzel TS, Porter VJ, Geyer S, Maclean K, Bawendi MG, Kastner MA (2008) Charge transport in arrays of PbSe nanocrystals. Phys Rev B 77:075316
Bangalore RB, Lin L, Perillo EP, Peng X, Yu WW, Dunn AK, Zheng Y (2017) High-Resolution Bubble Printing of Quantum Dots. ACS Appl Mater Interfaces 9:16725.
Dubowski JJ, Stanowski R, Dan D, Poole PJ (2018) Precision tuning of InAs quantum dot emission wavelength by iterative laser annealing. Opt Laser Technol 103:382–386.
Shao C, Meng X, Jing P, Sun M, Zhao J, Li H (2013) Enhancement of electron transfer from CdSe core/shell quantum dots to TiO2 films by thermal annealing. J Lumin 142(142):196–201
Biadala L, Siebers B, Beyazit Y, Tessier MD, Dupont D, Hens Z et al (2016) Band-edge exciton fine structure and recombination dynamics in InP/ZnS colloidal nanocrystals. ACS Nano 10(3):3356–3364
Narayanaswamy A, Feiner LF, Meijerink A, Van der Zaag PJ (2009) The effect of temperature and dot size on the spectral properties of colloidal InP/ZnS core-shell quantum dots. ACS Nano 3(9):2539–2546
Bergman L, Chen XB, Morrison JL, Huso J, Purdy AP (2004) Photoluminescence dynamics in ensembles of wide-band-gap nanocrystallites and powders. J Appl Phys 96(1):675–682
He H, Yu Q, Hui L, Jing L, Si J, Jin Y et al (2016) Exciton localization in solution-processed organolead trihalide perovskites. Nat Commun 7:10896
Cooper DE, Bajaj J, Newman PR (1988) Photoluminescence spectroscopy of excitons for evaluation of high-quality CdTe crystals. J Cryst Growth 86(1–4):544–551
Schmidt T, Lischka K, Zulehner W (1992) Excitation-power dependence of the near-band-edge photoluminescence of semiconductors. Phys Rev B Condens Matter 45(16):8989
Bao J, Bell DC, Capasso F, Wagner JB, Mårtensson T, Trägårdh J et al (2008) Optical properties of rotationally twinned InP nanowire heterostructures. Nano Lett 8(3):836–841
Varshni YP (1970) Temperature dependence of the elastic constants. Phys Rev B 2(10):3952–3958
Valerini D, Creti A, Lomascolo M, Manna L, Cingolani R, Anni M (2005) Temperature dependence of the photoluminescence properties of colloidal CdSe/ZnS core/shell quantum dots embedded in a polystyrene matrix. Phys Rev B 71(23):235409.
Bol AA, van Beek R, Ferwerda J, Meijerink A (2003) Temperature dependence of the luminescence of nanocrystalline CdS/Mn2+. J Phys Chem Solids 64(2):247–252
Varshni YP (1967) Temperature dependence of the energy gap in semiconductors. Physica 34(1):149–154
Rudin S, Reinecke TL, Segall B (1995) Erratum: temperature-dependent exciton linewidths in semiconductors. Phys Rev B 3(15):11517
This work is supported by the National Natural Science Foundation of China (61704011, 61574022, 61504012, 61674021, 11404219, 11404161, 11574130, 11674038), the Foundation of State Key Laboratory of High Power Semiconductor Lasers, the Developing Project of Science and Technology of Jilin Province (20160519007JH, 20160520117JH, 20160101255JC, 20160204074GX, 20170520117JH), and the Foundation of NANO X(18JG01). RC acknowledges the national 1000 plan for young talents and Shenzhen Science and Technology Innovation Committee (Projects Nos. JCYJ20150630162649956, JCYJ20150930160634263, and KQTD2015071710313656).
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Zhang, B., Wei, Z., Wang, X. et al. Effect of Post Thermal Annealing on the Optical Properties of InP/ZnS Quantum Dot Films. Nanoscale Res Lett 13, 369 (2018). https://doi.org/10.1186/s11671-018-2784-y
- InP/ZnS QD film
- Thermal annealing
- Optical properties