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   Wu, Wei; Morales-Acosta, Mayra Daniela; Wang, Yongqiang; Pettes, Michael Thompson (February 2019, Nano Letters)
2. Microwave Synthesis and Magnetocaloric Effect in AlFe ₂ B ₂

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   Mann, Dallas K.; Wang, YiXu; Marks, Jeanette D.; Strouse, Geoffrey F.; Shatruk, Michael (September 2020, Inorganic Chemistry)

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3. High Current Density SmTiO ₃ /SrTiO ₃ Field-Effect Transistors

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   Chandrasekar, Hareesh; Ahadi, Kaveh; Razzak, Towhidur; Stemmer, Susanne; Rajan, Siddharth (January 2020, ACS Applied Electronic Materials)

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4. Thermoelectric Effect of Ca₂Fe₂O₅ at Low Temperatures

   https://doi.org/10.4236/msce.2025.136001  

   Schultz, Ebony; Hona, Ram Krishna (January 2025, Journal of Materials Science and Chemical Engineering)

   This study investigates the thermoelectric properties of Ca2Fe2O5 over a temperature range of 7˚C to 50˚C. The experiment measured the voltage generated by temperature differences across two sides of the material, with a focus on the voltage response at temperatures both below and above room temperature. Results indicate that at lower temperatures (7˚C to 15˚C), the voltage generated by the temperature difference was higher, though not directly proportional to the magnitude of the temperature gradient. The highest voltage recorded for the smallest temperature difference in this range was 109 mV, observed between 14.6˚C and 17.6˚C (smallest temperature difference, 3˚C). Similarly, at temperatures above room temperature, the voltage generated was relatively lower, peaking at 125 mV between 9˚C and 44˚C (higher temperature difference). These results suggest complex behavior of Ca2Fe2O5’s thermoelectric response, with non-linear relationships between voltage and temperature differences at both low and high temperatures. 

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5. Optical Momentum Alignment Effect in WSe ₂ Phototransistor

   https://doi.org/10.1002/adom.202002243  

   Zhang, Yuchen; Xu, Ya‐Qiong (April 2021, Advanced Optical Materials)

   Abstract The optical momentum alignment effect is demonstrated in WSe₂phototransistors . When the photon energy is above the A exciton energy, the maximum photocurrent response occurs for the light polarization direction parallel to the metal electrode edge, suggesting that electrons in the valence band of WSe₂prefer to absorb photons with the polarization direction perpendicular to their momentum direction. Further studies indicate that the anisotropic distribution of photo‐excited carriers is likely due to the pseudospin‐induced optical transition selection rules. If the photon energy is below the A exciton energy, the photocurrent signals are maximized when the incident light is polarized in the direction perpendicular to the electrode edge, which is mainly attributed to the polarized absorption of the plasmonic gold electrodes. Moreover, the photocurrent peak can be controlled by an electric field via the quantum confined Stark effect. This resonance peak can also be shifted by adjusting environmental temperatures due to the temperature‐dependent nature of the WSe₂band gap. These experimental studies shed light on the knowledge of photocurrent generation mechanisms, opening the door for engineering future anisotropic optoelectronics. 

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