Perovskite Synthesis by Ultrasonication
The ultrasonic crystallization and precipitation of perovskite crystals is a highly effective and economical technique, which allows to produce perovskite nanocrystals on industrial scale for mass production.
Ultrasonic Synthesis of Perovskite Nanocrystals
Organic–inorganic lead halide perovskites exhibit exceptional optoelectronic properties such as high light absorption, very long long carrier lifetime, carrier diffusion length, and high carrier mobility, which makes the perovskite compounds a superior functional material for high-performance applications in solar panels, LEDs, photodetectors, lasers, etc.
Ultrasonication is one of the physical methods for accelerating various organic reactions. The crystallization process is influenced and controlled by the ultrasonic treatment, resulting in the controllable size properties of the single‐crystalline perovskite nanoparticles.
Case Studies of Ultrasonic Perovskite Synthesis
Research has conducted manifold types of ultrasonically assisted perovskite crystal growth. In general, perovskite crystals are prepared with the liquid growth method. In order to precipitate perovskite crystals, the solubility of the target samples is slowly and controlled reduced in a precursor solution. Ultrasonic precipitation of perovskite nano crystals is mainly based on an antisolvent quenching.
Ultrasonic Crystallization of Perovskite Nanocrystals
Jang et al. (2016) report the succesful ultrasonically assisted synthesis of lead halide perovskite nanocrystals. Using ultrasound, APbX3 perovskite nanocrystals with a wide range of compositions, where A = CH3NH3, Cs, or HN=CHNH3 (formamidinium), and X = Cl, Br, or I, were precipitated. Ultrasonication accelerates the dissolving process of the precursors (AX and PbX2) in toluene, and the dissolution rate determines the growth rate of the nanocrystals. Subsequently, the research team fabricated high-sensitivity photodetectors by homogenously spin coating the uniform size nanocrystals on large-area silicon oxide substrates.
Ultrasonic Asymetrical Crystallization of Perovskite
Peng et al. (2016) developed new growth method based on a cavitation-triggered asymmetrical crystallization (CTAC), which promotes heterogeneous nucleation by providing enough energy to overcome the nucleation barrier. Briefly, they introduced a very short ultrasonic pulses (≈ 1sec) to the solution when it reached a low supersaturation level with antisolvent vapor diffusion. The ultrasonic pulse is introduced at high supersaturation levels, where cavitation triggers excessive nucleation events and therefore the growth of a plethora of tiny crystals. Promisingly, MAPbBr3 monocrystalline films grew on the surface of various substrates within several hours of the cyclic ultrasonication treatment.
Ultrasonic Synthesis of Perovskite Quantum Dots
Chen et al. (2017) present in their research work a efficient method to prepare perovskite quantum dots (QDs) under ultrasonic irradiation. Ultrasonication is used as a mechanical method in order to accelerate the precipitation of perovskite quantum dots. The crystallization process of the perovskite quantum dots is intensified and controlled by the ultrasonic treatment, resulting in the precisely tailored size of the nanocrystals. The analysis of the structure, particle size and morphology of the perovskite quantum dots showed that the ultrasonic crystallization gives a smaller particle sizes and a more uniform particle size distribution. Using the ultrasonic (= sonochemical) synthesis, it was also possible to produce perovskite quantum dots with different chemical compositions. Those different compositions in the perovskite crystals allowed to unable emission peaks and adsorption edges of CH3NH3PbX3 (X = Cl, Br and I), which led to an extremely wide color gamut.
Ultrasonication of nano particle suspensions and inks is a reliable technique to disperse them homogeneously before applying the nano-suspension on substrates such as grids or electrodes. (cf. Belchi et al. 2019; Pichler et al. 2018)
Ultrasonic dispersion easily handles high solid concentrations (e.g. pastes) and distributes nano-particles into single-dispersed particles so that a uniform suspension is produced. This assures that in the subsequent application, when the substrate is coated, no clumping such as agglomerates impairs the performance of the coating.
Ultrasonic Processors for Perovskite Precipitation
Hielscher Ultrasonics designs and manufactures high-performance ultrasonic systems for the sonochemical synthesis of high-quality perovskite crystals. As market leader and with long-time experience in ultrasonic processing, Hielscher Ultrasonics assists its customers from first feasibility test to process optimization to the final installation of industrial ultrasonic processors for large scale production. Offering the full portfolio from lab and bench-top ultrasonicators up to industrial ultrasonic processors, Hielscher can recommend you the ideal device for your nanocrystal process.
All Hielscher ultrasonicators are precisely controllable and can be tuned from very low to very high amplitudes. The amplitude is one of the main factors that influences the impact and destructiveness of sonication processes. Hielscher Ultrasonics’ ultrasonic processors deliver a very wide spectrum of amplitudes covering the range of very mild and soft to very intense and destructive applications. Choosing the right amplitude setting, booster and sonotrode allows to set the required ultrasonic impact for your specific process. Hielscher’s special flow cell reactor insert MPC48 – MultiPhaseCavitator (see pic. left) – allows to inject the second phase via 48 cannulas as a thin strain into the cavitational hot-spot, where high performance ultrasound waves disperse the two phases into a homogeneous mixture. The MultiPhaseCavitator is ideal to initiate crystal seeding points and to control the precipitation reaction of perovskite nanocrystals.
Hielscher industrial ultrasonic processors can deliver extraordinarily high amplitudes. Amplitudes of up to 200µm can be easily continuously run in 24/7 operation. For even higher amplitudes, customized ultrasonic sonotrodes are available. The robustness of Hielscher’s ultrasonic equipment allows for 24/7 operation at heavy duty and in demanding environments.
Our customers are satisfied by the outstanding robustness and reliability of Hielscher Ultrasonic’s systems. The installation in fields of heavy-duty application, demanding environments and 24/7 operation ensure efficient and economical processing. Ultrasonic process intensification reduces processing time and achieves better results, i.e. higher quality, higher yields, innovative products.
The table below gives you an indication of the approximate processing capacity of our ultrasonicators:
|Batch Volume||Flow Rate||Recommended Devices|
|0.5 to 1.5mL||n.a.||VialTweeter|
|1 to 500mL||10 to 200mL/min||UP100H|
|10 to 2000mL||20 to 400mL/min||UP200Ht, UP400St|
|0.1 to 20L||0.2 to 4L/min||UIP2000hdT|
|10 to 100L||2 to 10L/min||UIP4000hdT|
|n.a.||10 to 100L/min||UIP16000|
|n.a.||larger||cluster of UIP16000|
Contact Us! / Ask Us!
- Raphaëlle Belchi; Aurélie Habert; Eddy Foy; Alexandre Gheno; Sylvain Vedraine; Rémi Antony; Bernard Ratier; Johann Bouclé; Nathalie Herlin-Boimecor (2019): One-Step Synthesis of TiO2/Graphene Nanocomposites by Laser Pyrolysis with Well-Controlled Properties and Application in Perovskite Solar Cells. ACS Omega. 2019 Jul 31; 4(7): 11906–11913.
- Dong Myung Jang, Duk Hwan Kim, Kidong Park, Jeunghee Park, Jong Woon Lee, Jae Kyu Song (2016): Ultrasound synthesis of lead halide perovskite nanocrystals. Journal of Materials Chemistry C. Issue 45, 2016.
- Lung-Chien Chen, Zong-Liang Tseng, Shih-You Chen, Shengyi Yang (2017): An ultrasonic synthesis method for high-luminance perovskite quantum dots. Cermaics international 43, 2017. 16032-16035.
- Birgit Pichler; Kurt Mayer; Prof. Viktor Hacker (2018): Long‐Term Operation of Perovskite‐Catalyzed Bifunctional Air Electrodes in Rechargeable Zinc‐Air Flow Batteries. Batteries & Supercaps Vol. 2, Issue 4, April 2019. 387-395.
- Wei Peng, Lingfei Wang, Banavoth Murali, Kang-Ting Ho, Ashok Bera, Namchul Cho, Chen-Fang Kang, Victor M. Burlakov, Jun Pan, Lutfan Sinatra, Chun Ma, Wei Xu, Dong Shi, Erkki Alarousu, Alain Goriely, Jr-Hau He, Omar F. Mohammed, Tom Wu, Osman M. Bakr (2016): Solution-Grown Monocrystalline Hybrid Perovskite Films for Hole-Transporter-Free Solar Cells. Advanced Materials 2016.
Facts Worth Knowing
Perovskite is a term that describes the mineral Perovskite (also known as calcium titanium oxide or calcium titanate, chemical formula CaTiO3) as well as a specific material structure. In accordance to the same name, the mineral Perovskite features the perovskite structure.
Perovskite compounds can occur in cubic, tetragonal or orthorhombic structure and have the chemical formula ABX3. A and B are cations, whilst X represents an anion, which bonds to both. In perovskite compounds, the A cation is significantly larger than the B cation. Other minerals with perovskite structure are Loparite and Bridgmanite.
Perovskites have a unique crystal structure and in this structure various chemical elements can be combined. Due to the special crystal structure, perovskite molecules can exhibit various valuable properties, such as superconductivity, very high magnetoresistance, and/or ferroelectricity, which make those compounds highly interesting for industrial applications . Furthermore, a large number of different elements can be combined together to form perovskite structures, which makes it possible to combine, modify and intensify certain material characteristics. Researchers, scientists and process developers use those options to selectively design and optimize perovskite physical, optical and electrical characteristics.
Their optoelectronic properties make hybrid perovskites ideal candidates for solar cell applications and perovskite solar cells are a promising technology, which might help to produce large amounts of clean, environmental-friendly energy.
Critical optoelectronic parameters of single‐crystalline perovskite reported in the literature:
τs = 28 ns τb = 300 ns PL
1.3–4.3 µm3 × 1010MAPbI31.51 eV 820 nm67.2 (SCLC)
τs = 18 ns τb = 570 ns PL
1.8–10.0 µm1.4 × 1010MAPbI3850 nm164 ± 25 Hole mobility (SCLC) 105 Hole mobility (Hall) 24 ± 6.8 electron SCLC
82 ± 5 µs TPV 95 ± 8 µs impedance spectroscopy (IS)9 × 109 p175 ± 25 µm3.6 × 1010 for hole 34.5 × 1010 for electronMAPbI31.53 eV 784 nm34 Hall
8.8 × 1011 p
1.8 × 109 for hole 4.8 × 1010 for electronMAPbBr31.53 eV 784 nm34 Hall
8.8 × 1011 p
1.8 × 109 for hole 4.8 × 1010 for electronMAPbBr32.24 eV 537 nm4.36 Hall
3.87 × 1012 p
2.6 × 1010 for hole 1.1 × 1011 for electronMAPbCl32.24 eV 537 nm4.36 Hall
3.87 × 1012 p
2.6 × 1010 for hole 1.1 × 1011 for electronMAPbCl32.97 eV 402 nm179 Hall
5.1 × 109 n
MAPbCl32.88 eV 440 nm42 ± 9 (SCLC)2.7 × 10-8τs = 83 ns τb = 662 ns PL4.0 × 109 p3.0–8.5 µm3.1 × 1010FAPbI31.49 eV 870 nm40 ± 5 Hole mobility SCLC1.8 × 10-8
2.8 × 109
1.34 × 1010
|Materials||Band gap or absorption onset||Mobility [cm2 V-1 s-1]||Conductance [Ω-1 cm-1]||Carrier lifetime and method||Carrier concentration and type [cm-3] (n or p)||Diffusion length||Trap density [cm-3]|
|MAPbBr3||2.21 eV 570 nm||115 (TOF) 20–60 (Hall) 38 (SCLC)||τs = 41 ns τb = 457 ns (PL)||5 × 109 to 5 × 1010 p||3–17 µm||5.8 × 109|