Xunan
Jing
a,
Tianhui
Liu
a,
Daquan
Wang
a,
Jing
Liu
a and
Lingjie
Meng
*ab
aSchool of Science, State Key Laboratory for Mechanical Behavior of Materials and MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, Xi'an Jiaotong University, Xi'an 710049, China. E-mail: menglingjie@mail.xjtu.edu.cn
bInstrumental Analysis Center of Xi'an Jiaotong University, Xi'an 710049, China
First published on 18th January 2023
Correction for ‘Controlled synthesis of water-dispersible and superparamagnetic Fe3O4 nanomaterials by a microwave-assisted solvothermal method: from nanocrystals to nanoclusters’ by Xunan Jing et al., CrystEngComm, 2017, 19, 5089–5099, https://doi.org/10.1039/C7CE01191A.
Fig. 2 TEM images of (a–c) SPION crystals and (e–g) SPION clusters with different amounts of reactants (NaAc·3H2O): (a and e) 2 g, (b and f) 4 g, and (c and g) 6 g, while simultaneously maintaining other experimental parameters constant (FeCl3·6H2OSPION crystal = 0.8115 g, temperatureSPION crystal = 240 °C, Na3Cit = 0.4 g, time = 3 h; and FeCl3·6H2OSPION cluster = 1.3525 g, temperatureSPION cluster = 200 °C, Na3Cit = 0.4 g, time = 2 h). The scale bars of the TEM images in (a–c) and (e–g) represent 100 nm. The corresponding size statistics of (d) SPION crystals and (h) SPION clusters.
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