Nonlinear dielectric polymers for high-power density capacitors generally possess a high dielectric constant (εr), a large breakdown electric field (Eb), but a large dielectric loss (tan δ) due to the relaxation of high polar dipoles. To address the inherent trade-off between dielectric response and loss, we propose a low polarity polystyrene-4-vinylpyridine (P(S-r-4VP)) multipolymer by incorporating a 4-vinylpyridine (4VP) into polystyrene (PS) using conventional emulsion polymerization. Interestingly, compared to pure PS, the π-electron density of P(S-r-4VP) is significantly improved for the addition of functional 4VP unit, thereby promoting the strong electronic polarization response under an electrical field. As such, εr and Eb of the P(S-r-4VP) films increase with molar content of 4VP, and reach to 3.7 at 100 Hz and ∼550 MV/m, respectively. Notably, the P(S-r-4VP) copolymer exhibits a considerable discharged energy density (Ue) of 3.43 J/cm3 under an electrical field of 500 MV/m. Thus, this work offers valuable insights for the application of polystyrene-based polymers in dielectric energy storage areas.
{"title":"A Polystyrene-4-vinylpyridine Copolymer with High Dielectric and Energy Storage Properties","authors":"Yinghui Wang, , , Weimin Xia*, , , Biao Guan, , , Jing Li, , , Chengmin Hou, , and , Xiaofang Zhang, ","doi":"10.1021/acsaelm.6c00039","DOIUrl":"https://doi.org/10.1021/acsaelm.6c00039","url":null,"abstract":"<p >Nonlinear dielectric polymers for high-power density capacitors generally possess a high dielectric constant (ε<sub>r</sub>), a large breakdown electric field (<i>E</i><sub>b</sub>), but a large dielectric loss (tan δ) due to the relaxation of high polar dipoles. To address the inherent trade-off between dielectric response and loss, we propose a low polarity polystyrene-4-vinylpyridine (P(S-<i>r</i>-4VP)) multipolymer by incorporating a 4-vinylpyridine (4VP) into polystyrene (PS) using conventional emulsion polymerization. Interestingly, compared to pure PS, the π-electron density of P(S-<i>r</i>-4VP) is significantly improved for the addition of functional 4VP unit, thereby promoting the strong electronic polarization response under an electrical field. As such, ε<sub>r</sub> and <i>E</i><sub>b</sub> of the P(S-<i>r</i>-4VP) films increase with molar content of 4VP, and reach to 3.7 at 100 Hz and ∼550 MV/m, respectively. Notably, the P(S-<i>r</i>-4VP) copolymer exhibits a considerable discharged energy density (<i>U</i><sub>e</sub>) of 3.43 J/cm<sup>3</sup> under an electrical field of 500 MV/m. Thus, this work offers valuable insights for the application of polystyrene-based polymers in dielectric energy storage areas.</p>","PeriodicalId":3,"journal":{"name":"ACS Applied Electronic Materials","volume":"8 5","pages":"2166–2173"},"PeriodicalIF":4.7,"publicationDate":"2026-02-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147382508","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pinku Roy*, , , Di Zhang, , , Nicholas Cucciniello, , , Sundar Kunwar, , , Aiping Chen*, , and , Quanxi Jia*,
The Hall effect in ferromagnetic (FM) materials is typically linked to magnetization, yet its manifestation in complex heterostructures remains poorly understood. Here, we demonstrate that antiferromagnetic (AFM) NiO can modulate the ferromagnetic state of epitaxial SrRuO3 (SRO). We systematically investigate the structural, magnetic, and transport properties of SRO/NiO, NiO/SRO, and single-layer SRO films. Remarkably, only the SRO/NiO bilayer exhibits a pronounced unconventional hump-dip feature in the Hall hysteresis, which is absent in NiO/SRO and pure SRO. Microstructural analysis reveals the presence of nanosized globular NiO in the SRO/NiO bilayer, which increases the interfacial area and promotes spin misalignment and modifies magnetic anisotropy of SRO. This spin disorder and modified anisotropy strongly alter the magnetic and transport responses in the SRO/NiO heterostructure. We attribute the irregular Hall feature to a temperature-dependent interplay of the anomalous Hall effect (AHE), planar Hall effect (PHE), and magnetoresistance in the SRO/NiO heterostructure. These findings highlight the critical role of the AFM/FM interfacial microstructure in tailoring Hall transport phenomena.
{"title":"Coupling of Anomalous Hall and Planar Hall Effects in Ferromagnet/Antiferromagnet Bilayers","authors":"Pinku Roy*, , , Di Zhang, , , Nicholas Cucciniello, , , Sundar Kunwar, , , Aiping Chen*, , and , Quanxi Jia*, ","doi":"10.1021/acsaelm.5c02399","DOIUrl":"https://doi.org/10.1021/acsaelm.5c02399","url":null,"abstract":"<p >The Hall effect in ferromagnetic (FM) materials is typically linked to magnetization, yet its manifestation in complex heterostructures remains poorly understood. Here, we demonstrate that antiferromagnetic (AFM) NiO can modulate the ferromagnetic state of epitaxial SrRuO<sub>3</sub> (SRO). We systematically investigate the structural, magnetic, and transport properties of SRO/NiO, NiO/SRO, and single-layer SRO films. Remarkably, only the SRO/NiO bilayer exhibits a pronounced unconventional hump-dip feature in the Hall hysteresis, which is absent in NiO/SRO and pure SRO. Microstructural analysis reveals the presence of nanosized globular NiO in the SRO/NiO bilayer, which increases the interfacial area and promotes spin misalignment and modifies magnetic anisotropy of SRO. This spin disorder and modified anisotropy strongly alter the magnetic and transport responses in the SRO/NiO heterostructure. We attribute the irregular Hall feature to a temperature-dependent interplay of the anomalous Hall effect (AHE), planar Hall effect (PHE), and magnetoresistance in the SRO/NiO heterostructure. These findings highlight the critical role of the AFM/FM interfacial microstructure in tailoring Hall transport phenomena.</p>","PeriodicalId":3,"journal":{"name":"ACS Applied Electronic Materials","volume":"8 5","pages":"2045–2054"},"PeriodicalIF":4.7,"publicationDate":"2026-02-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147384293","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
This work investigates charge exchange dynamics in MoS2 field-effect transistors (FETs) induced by organic molecule adsorption through both experimental and theoretical studies. Adsorption of various π-conjugated molecules such as copper phthalocyanine (CuPc), cobalt phthalocyanine (CoPc), phthalocyanine (H2Pc), and methylene blue (MB) on the MoS2 channel significantly modulates its electrical characteristics, resulting in distinctive changes in transfer curves (Id–Vg) and threshold voltages (Vth). These variations are consistent with the direction of charge transfer, as controlled by the relative energy levels of the molecular HOMO–LUMO gaps and band edges of MoS2. Electronic calculations based on density functional theory (DFT) confirm that electron-rich molecules act as electron acceptors, which display p-type behavior, and donor-type molecules allow n-type behavior. Theoretical calculation of bandgap and density of states analyses involving pristine and molecule-adsorbed MoS2 further supports interfacial interactions resulting in Fermi level tuning. These findings explain the molecular-level mechanisms governing charge modulation in MoS2-FETs, offering valuable insights for molecular sensing and nanoelectronic applications.
{"title":"Organic Molecule-Induced Charge Exchange in MoS2 FETs: Experimental and Theoretical Insights","authors":"Md Iftekharul Alam*, , , Tsuyoshi Takaoka, , , Tadahiro Komeda, , and , Akinobu Teramoto*, ","doi":"10.1021/acsaelm.5c02571","DOIUrl":"https://doi.org/10.1021/acsaelm.5c02571","url":null,"abstract":"<p >This work investigates charge exchange dynamics in MoS<sub>2</sub> field-effect transistors (FETs) induced by organic molecule adsorption through both experimental and theoretical studies. Adsorption of various π-conjugated molecules such as copper phthalocyanine (CuPc), cobalt phthalocyanine (CoPc), phthalocyanine (H<sub>2</sub>Pc), and methylene blue (MB) on the MoS<sub>2</sub> channel significantly modulates its electrical characteristics, resulting in distinctive changes in transfer curves (<i>I</i><sub><i>d</i></sub><i>–V</i><sub><i>g</i></sub>) and threshold voltages (<i>V</i><sub><i>th</i></sub>). These variations are consistent with the direction of charge transfer, as controlled by the relative energy levels of the molecular HOMO–LUMO gaps and band edges of MoS<sub>2</sub>. Electronic calculations based on density functional theory (DFT) confirm that electron-rich molecules act as electron acceptors, which display <i>p</i>-type behavior, and donor-type molecules allow <i>n</i>-type behavior. Theoretical calculation of bandgap and density of states analyses involving pristine and molecule-adsorbed MoS<sub>2</sub> further supports interfacial interactions resulting in Fermi level tuning. These findings explain the molecular-level mechanisms governing charge modulation in MoS<sub>2</sub>-FETs, offering valuable insights for molecular sensing and nanoelectronic applications.</p>","PeriodicalId":3,"journal":{"name":"ACS Applied Electronic Materials","volume":"8 5","pages":"2108–2115"},"PeriodicalIF":4.7,"publicationDate":"2026-02-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147382476","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
This study investigates Al-doped TiO2/Y2O3/ZrO2 trilayer capacitors grown by atomic layer deposition as a feasible material to scale high-k dielectric films for dynamic random-access memory (DRAM) capacitors. An ultrathin Y2O3 insertion layer (<0.5 nm) at the TiO2/ZrO2 interface facilitated the formation of a high-k tetragonal/cubic–like ZrO2 phase at ultrathin thicknesses, as verified by equivalent oxide thickness (EOT)–physical oxide thickness (POT) analysis, grazing-incidence X-ray diffraction, and transmission electron microscopy analysis. Such an enhanced crystallization enabled achieving a higher bulk k at a smaller POT and improved leakage properties. Postmetallization annealing (PMA) conditions were optimized for back-end-of-line compatibility, with PMA at 400 °C for 30 s in N2 providing adequate interfacial curing, minimal EOT increase, and a lower leakage current. In contrast, PMA at 400 °C for 30 min resulted in EOT growth driven by intermixing, and PMA at 600 °C for 30 s enhanced crystallinity but increased leakage due to grain-boundary-assisted conduction. Temperature-dependent transport revealed that the dominant mechanism is bulk-limited Poole–Frenkel emission in the ZrO2 layer for both bias polarities, while the leakage magnitude is modulated by asymmetric injection conditions at the Ru/Al-doped TiO2 and ZrO2/TiN interfaces. Poole–Frenkel analysis yielded a consistent trap depth of ∼1.1 eV and physically reasonable optical dielectric constants for ZrO2-based dielectrics. With Y2O3 insertion and short-time PMA at 400 °C, the Al-doped TiO2/Y2O3/ZrO2 film achieved a minimum EOT of ∼0.63 nm at a POT of ∼6.0 nm, outperforming other ZrO2-based stacks at comparable thickness while maintaining acceptable leakage. Overall, interfacial Y2O3 insertion combined with optimized PMA provided a practical pathway to achieve a lower POT at a given EOT in rutile TiO2-based next-generation DRAM capacitors.
{"title":"Al-Doped Rutile TiO2 with Y2O3–ZrO2 Stacks Achieving Thin Thickness and Low Leakage for Dynamic Random-Access Memory Capacitors","authors":"Tae Kyun Kim, , , Heewon Paik, , , Jonghoon Shin, , , Haewon Song, , , Dae Seon Kwon, , and , Cheol Seong Hwang*, ","doi":"10.1021/acsaelm.6c00060","DOIUrl":"https://doi.org/10.1021/acsaelm.6c00060","url":null,"abstract":"<p >This study investigates Al-doped TiO<sub>2</sub>/Y<sub>2</sub>O<sub>3</sub>/ZrO<sub>2</sub> trilayer capacitors grown by atomic layer deposition as a feasible material to scale high-<i>k</i> dielectric films for dynamic random-access memory (DRAM) capacitors. An ultrathin Y<sub>2</sub>O<sub>3</sub> insertion layer (<0.5 nm) at the TiO<sub>2</sub>/ZrO<sub>2</sub> interface facilitated the formation of a high-<i>k</i> tetragonal/cubic–like ZrO<sub>2</sub> phase at ultrathin thicknesses, as verified by equivalent oxide thickness (EOT)–physical oxide thickness (POT) analysis, grazing-incidence X-ray diffraction, and transmission electron microscopy analysis. Such an enhanced crystallization enabled achieving a higher bulk <i>k</i> at a smaller POT and improved leakage properties. Postmetallization annealing (PMA) conditions were optimized for back-end-of-line compatibility, with PMA at 400 °C for 30 s in N<sub>2</sub> providing adequate interfacial curing, minimal EOT increase, and a lower leakage current. In contrast, PMA at 400 °C for 30 min resulted in EOT growth driven by intermixing, and PMA at 600 °C for 30 s enhanced crystallinity but increased leakage due to grain-boundary-assisted conduction. Temperature-dependent transport revealed that the dominant mechanism is bulk-limited Poole–Frenkel emission in the ZrO<sub>2</sub> layer for both bias polarities, while the leakage magnitude is modulated by asymmetric injection conditions at the Ru/Al-doped TiO<sub>2</sub> and ZrO<sub>2</sub>/TiN interfaces. Poole–Frenkel analysis yielded a consistent trap depth of ∼1.1 eV and physically reasonable optical dielectric constants for ZrO<sub>2</sub>-based dielectrics. With Y<sub>2</sub>O<sub>3</sub> insertion and short-time PMA at 400 °C, the Al-doped TiO<sub>2</sub>/Y<sub>2</sub>O<sub>3</sub>/ZrO<sub>2</sub> film achieved a minimum EOT of ∼0.63 nm at a POT of ∼6.0 nm, outperforming other ZrO<sub>2</sub>-based stacks at comparable thickness while maintaining acceptable leakage. Overall, interfacial Y<sub>2</sub>O<sub>3</sub> insertion combined with optimized PMA provided a practical pathway to achieve a lower POT at a given EOT in rutile TiO<sub>2</sub>-based next-generation DRAM capacitors.</p>","PeriodicalId":3,"journal":{"name":"ACS Applied Electronic Materials","volume":"8 5","pages":"2174–2186"},"PeriodicalIF":4.7,"publicationDate":"2026-02-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://pubs.acs.org/doi/pdf/10.1021/acsaelm.6c00060","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147384244","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Two-dimensional (2D) semiconductors with atomic thickness hold promise as next-generation channel materials for transistors in the post-Moore era. However, the experimental mobility of most 2D semiconductors remains one order of magnitude lower than that of silicon. Strain engineering is widely recognized as an established strategy for modulating charge transport properties, particularly carrier mobility, in 2D semiconductors. Nevertheless, constrained by the multiscale challenge spanning from atomic-scale strain to micrometer-scale devices, achieving continuous modulation and enhancement of carrier mobility in 2D semiconductor transistors still poses a significant challenge. Here, we systematically investigated the influence of engineered strain on the electronic properties of atomically-thin molybdenum disulfide (MoS2). We transferred trilayer MoS2 onto SiNx/Si substrates with controlled roughness to induce precise and tunable lattice distortion. Such lattice distortion can effectively suppress electron–phonon scattering within the MoS2 channel, thereby modulating the band structure and electronic properties. We further fabricated back-gated MoS2 field-effect transistors (FETs) on the crested rough SiNx/Si substrates, which exhibited a continuously enhanced carrier mobility. Specifically, as the strain increased to 0.8%, the room-temperature mobility of the strained MoS2 FET was significantly enhanced to 326.9 cm2 V–1 s–1, representing a nearly 10-fold improvement over that of the non-strained MoS2 FET (30.6 cm2 V–1 s–1). Correspondingly, the maximum on-state current density of the strained MoS2 transistor increased by approximately 36 times compared to that of the non-strained device. Our work demonstrates that strain engineering can dramatically enhance the carrier mobility of 2D semiconductors, while being highly compatible with Si-based technology.
原子厚度的二维(2D)半导体有望成为后摩尔时代晶体管的下一代通道材料。然而,大多数二维半导体的实验迁移率仍然比硅低一个数量级。应变工程被广泛认为是调制二维半导体中电荷输运特性,特别是载流子迁移率的一种成熟策略。然而,受限于从原子尺度应变到微米尺度器件的多尺度挑战,在二维半导体晶体管中实现连续调制和增强载流子迁移率仍然是一个重大挑战。本文系统地研究了工程应变对原子薄二硫化钼(MoS2)电子性能的影响。我们通过控制粗糙度将三层MoS2转移到SiNx/Si衬底上,以诱导精确和可调的晶格畸变。这种晶格畸变可以有效抑制MoS2通道内的电子-声子散射,从而调制带结构和电子性质。我们进一步在粗糙的SiNx/Si衬底上制备了背控MoS2场效应晶体管(fet),其载流子迁移率不断提高。具体来说,当应变增加到0.8%时,应变MoS2 FET的室温迁移率显著提高到326.9 cm2 V-1 s-1,比未应变MoS2 FET (30.6 cm2 V-1 s-1)提高了近10倍。相应地,应变MoS2晶体管的最大导通电流密度比非应变器件增加了约36倍。我们的工作表明,应变工程可以显著提高二维半导体的载流子迁移率,同时与硅基技术高度兼容。
{"title":"Continuous Enhancement of Carrier Mobility in Strained Two-Dimensional Semiconductor Transistors","authors":"Yinuo Zhao, , , Siyu Zhou, , , Zhenlai Wang, , , Qiang Liu, , , Biyuan Zheng*, , and , Mengjian Zhu*, ","doi":"10.1021/acsaelm.5c02602","DOIUrl":"https://doi.org/10.1021/acsaelm.5c02602","url":null,"abstract":"<p >Two-dimensional (2D) semiconductors with atomic thickness hold promise as next-generation channel materials for transistors in the post-Moore era. However, the experimental mobility of most 2D semiconductors remains one order of magnitude lower than that of silicon. Strain engineering is widely recognized as an established strategy for modulating charge transport properties, particularly carrier mobility, in 2D semiconductors. Nevertheless, constrained by the multiscale challenge spanning from atomic-scale strain to micrometer-scale devices, achieving continuous modulation and enhancement of carrier mobility in 2D semiconductor transistors still poses a significant challenge. Here, we systematically investigated the influence of engineered strain on the electronic properties of atomically-thin molybdenum disulfide (MoS<sub>2</sub>). We transferred trilayer MoS<sub>2</sub> onto SiN<sub><i>x</i></sub>/Si substrates with controlled roughness to induce precise and tunable lattice distortion. Such lattice distortion can effectively suppress electron–phonon scattering within the MoS<sub>2</sub> channel, thereby modulating the band structure and electronic properties. We further fabricated back-gated MoS<sub>2</sub> field-effect transistors (FETs) on the crested rough SiN<sub><i>x</i></sub>/Si substrates, which exhibited a continuously enhanced carrier mobility. Specifically, as the strain increased to 0.8%, the room-temperature mobility of the strained MoS<sub>2</sub> FET was significantly enhanced to 326.9 cm<sup>2</sup> V<sup>–1</sup> s<sup>–1</sup>, representing a nearly 10-fold improvement over that of the non-strained MoS<sub>2</sub> FET (30.6 cm<sup>2</sup> V<sup>–1</sup> s<sup>–1</sup>). Correspondingly, the maximum on-state current density of the strained MoS<sub>2</sub> transistor increased by approximately 36 times compared to that of the non-strained device. Our work demonstrates that strain engineering can dramatically enhance the carrier mobility of 2D semiconductors, while being highly compatible with Si-based technology.</p>","PeriodicalId":3,"journal":{"name":"ACS Applied Electronic Materials","volume":"8 5","pages":"2116–2123"},"PeriodicalIF":4.7,"publicationDate":"2026-02-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147384273","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Imteaz Rahaman*, , , Botong Li, , , Hunter D. Ellis, , , Kathy Anderson, , , Feng Liu, , , Michael A. Scarpulla, , and , Kai Fu*,
Rutile germanium dioxide (r-GeO2) is an ultrawide bandgap semiconductor with potential for ambipolar doping, making it a promising candidate for next-generation power electronics and optoelectronics. Growth of phase-pure r-GeO2 films by vapor phase techniques like metalorganic chemical vapor deposition (MOCVD) is challenging because of polymorphic competition from amorphous and quartz GeO2. Here, we introduce seed-driven stepwise crystallization (SDSC) as a segmented growth strategy for obtaining r-GeO2 films on r-TiO2 (001) substrate. SDSC divides the growth into repeated cycles of film deposition and cooling–heating ramps, which suppress the nonrutile phases. We demonstrate continuous, phase-pure, partially epitaxial r-GeO2 (001) films of thickness ∼2 μm exhibiting X-ray rocking curves with a full-width at half-maximum of ∼597 arcsec. We discuss the underlying mechanisms of phase selection during SDSC growth. SDSC-based growth provides a generalizable pathway for selective vapor-phase growth of metastable or unstable phases, offering opportunities for phase-selective thin-film engineering.
{"title":"Phase Competition and Rutile Phase Stabilization of Growing GeO2 Films by MOCVD","authors":"Imteaz Rahaman*, , , Botong Li, , , Hunter D. Ellis, , , Kathy Anderson, , , Feng Liu, , , Michael A. Scarpulla, , and , Kai Fu*, ","doi":"10.1021/acsaelm.5c02249","DOIUrl":"https://doi.org/10.1021/acsaelm.5c02249","url":null,"abstract":"<p >Rutile germanium dioxide (r-GeO<sub>2</sub>) is an ultrawide bandgap semiconductor with potential for ambipolar doping, making it a promising candidate for next-generation power electronics and optoelectronics. Growth of phase-pure r-GeO<sub>2</sub> films by vapor phase techniques like metalorganic chemical vapor deposition (MOCVD) is challenging because of polymorphic competition from amorphous and quartz GeO<sub>2</sub>. Here, we introduce seed-driven stepwise crystallization (SDSC) as a segmented growth strategy for obtaining r-GeO<sub>2</sub> films on r-TiO<sub>2</sub> (001) substrate. SDSC divides the growth into repeated cycles of film deposition and cooling–heating ramps, which suppress the nonrutile phases. We demonstrate continuous, phase-pure, partially epitaxial r-GeO<sub>2</sub> (001) films of thickness ∼2 μm exhibiting X-ray rocking curves with a full-width at half-maximum of ∼597 arcsec. We discuss the underlying mechanisms of phase selection during SDSC growth. SDSC-based growth provides a generalizable pathway for selective vapor-phase growth of metastable or unstable phases, offering opportunities for phase-selective thin-film engineering.</p>","PeriodicalId":3,"journal":{"name":"ACS Applied Electronic Materials","volume":"8 5","pages":"2015–2023"},"PeriodicalIF":4.7,"publicationDate":"2026-02-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147382505","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The demand for advanced microwave dielectric ceramics for 5G base station filters drives the need for materials combining moderate permittivity, high quality factor (Q × f), and near-zero temperature stability (τf). This work investigates Ga2O3-doped SrTiO3–NdAlO3 (ST-NA) ceramics. The optimal base composition (0.5ST-0.5NA) achieves εr = 40.2, Q × f = 12,729 GHz, τf = 5.89 ppm/°C. To further enhance the microwave dielectric performance, Ga2O3 doping was introduced into the ST-NA ceramics. The substitution of Ga3+ for Ti4+ not only induces associated oxygen vacancy formation but also effectively suppressed the reduction of Ti4+ to Ti3+ during sintering, thereby reducing conduction loss, while the dielectric constant remained relatively stable. Consequently, 1.5% Ga2O3-doped ST-NA ceramic exhibited excellent overall microwave dielectric properties, with εr = 40.7, Q × f = 21,441 GHz, τf = 1.78 ppm/°C. These results demonstrate that Ga2O3-doped ST-NA ceramics are promising candidates for temperature-stable, low-loss microwave components in 5G and other high-frequency communication systems.
{"title":"Structure and Microwave Dielectric Properties of Ga2O3-Doped SrTiO3–NdAlO3 Ceramics","authors":"Qinghu Guo, , , Ting Wang, , , Mengchen Yao, , , Shangshu Li, , , Yiren Liu, , , Weiping Gong, , and , Hua Hao*, ","doi":"10.1021/acsaelm.5c02357","DOIUrl":"https://doi.org/10.1021/acsaelm.5c02357","url":null,"abstract":"<p >The demand for advanced microwave dielectric ceramics for 5G base station filters drives the need for materials combining moderate permittivity, high quality factor (<i>Q × f</i>), and near-zero temperature stability (τ<sub><i>f</i></sub>). This work investigates Ga<sub>2</sub>O<sub>3</sub>-doped SrTiO<sub>3</sub>–NdAlO<sub>3</sub> (ST-NA) ceramics. The optimal base composition (0.5ST-0.5NA) achieves ε<sub>r</sub> = 40.2, <i>Q</i> × <i>f</i> = 12,729 GHz, τ<sub><i>f</i></sub> = 5.89 ppm/°C. To further enhance the microwave dielectric performance, Ga<sub>2</sub>O<sub>3</sub> doping was introduced into the ST-NA ceramics. The substitution of Ga<sup>3+</sup> for Ti<sup>4+</sup> not only induces associated oxygen vacancy formation but also effectively suppressed the reduction of Ti<sup>4+</sup> to Ti<sup>3+</sup> during sintering, thereby reducing conduction loss, while the dielectric constant remained relatively stable. Consequently, 1.5% Ga<sub>2</sub>O<sub>3</sub>-doped ST-NA ceramic exhibited excellent overall microwave dielectric properties, with ε<sub>r</sub> = 40.7, <i>Q</i> × <i>f</i> = 21,441 GHz, τ<sub><i>f</i></sub> = 1.78 ppm/°C. These results demonstrate that Ga<sub>2</sub>O<sub>3</sub>-doped ST-NA ceramics are promising candidates for temperature-stable, low-loss microwave components in 5G and other high-frequency communication systems.</p>","PeriodicalId":3,"journal":{"name":"ACS Applied Electronic Materials","volume":"8 5","pages":"2024–2032"},"PeriodicalIF":4.7,"publicationDate":"2026-02-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147384214","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Abhinav Raina, , , Maurizio Sanfilippo, , , Chang-Ki Moon, , , Manuel Neubauer, , , Klaus Meerholz, , , Malte C. Gather, , and , Klas Lindfors*,
We present a graphene photodetector coupled to a layer of aggregated organic semiconductor. A graphene phototransistor is covered with a thin film of merocyanine molecules. The aggregation of the molecular layer can be controlled by the deposition parameters and postdeposition annealing to obtain films ranging from amorphous to a highly aggregated state. The molecular layer has a uniaxial structure with excitonic transitions, whose transition dipole moments are well-defined. The presence of the molecular layer results in an enormous increase in the response of the phototransistor. We further demonstrate that the signal enhancement is due to photodoping of graphene. The spectroscopic photoresponse hints that photodoping via monomers and molecular aggregates may take place differently. Our photodetector is a platform to study the influence of molecular aggregation and order on charge transport processes between aggregated organic semiconductors and two-dimensional materials.
{"title":"Tunable Photogating in a Molecular Aggregate Coupled Graphene Phototransistor","authors":"Abhinav Raina, , , Maurizio Sanfilippo, , , Chang-Ki Moon, , , Manuel Neubauer, , , Klaus Meerholz, , , Malte C. Gather, , and , Klas Lindfors*, ","doi":"10.1021/acsaelm.5c02433","DOIUrl":"https://doi.org/10.1021/acsaelm.5c02433","url":null,"abstract":"<p >We present a graphene photodetector coupled to a layer of aggregated organic semiconductor. A graphene phototransistor is covered with a thin film of merocyanine molecules. The aggregation of the molecular layer can be controlled by the deposition parameters and postdeposition annealing to obtain films ranging from amorphous to a highly aggregated state. The molecular layer has a uniaxial structure with excitonic transitions, whose transition dipole moments are well-defined. The presence of the molecular layer results in an enormous increase in the response of the phototransistor. We further demonstrate that the signal enhancement is due to photodoping of graphene. The spectroscopic photoresponse hints that photodoping via monomers and molecular aggregates may take place differently. Our photodetector is a platform to study the influence of molecular aggregation and order on charge transport processes between aggregated organic semiconductors and two-dimensional materials.</p>","PeriodicalId":3,"journal":{"name":"ACS Applied Electronic Materials","volume":"8 5","pages":"2068–2077"},"PeriodicalIF":4.7,"publicationDate":"2026-02-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://pubs.acs.org/doi/pdf/10.1021/acsaelm.5c02433","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147384215","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
In this work, a lead-free piezoelectric composite material comprising sodium potassium niobate (KNN) sol in an organic piezoelectric polymer (PVDF-TrFE) has been developed. The composite material can be deposited at low temperatures and is compatible with polymeric substrates. The piezoelectric coefficient has a maximum d33 value of 110 pm/V. This is superior to the piezoelectric coefficient for PVDF d33 = 28 pm/V, and most known lead-free piezocomposites that utilize PVDF. The controlled deposition of a thick (>1 μm) layer using spin coating can be easily achieved. The films are crack- and pinhole-free and require low-temperature processing. The introduction of the KNN sol in PVDF-TrFE improved the remnant polarization, dielectric constant, and piezoelectric coefficient of the resulting composite. Additionally, a tape-lift-off method for easily patterning these composite films has been developed, enabling the material to be utilized in micron-level devices. We demonstrate the piezoelectric properties of this composite by fabricating a flexible energy harvesting device that generates (Voc = 2.2 V) when compared to a PVDF-TrFE-based device (Voc = 0.05 V) for the same stimulation.
{"title":"Study of Electrical and Mechanical Properties of PVDF-TrFE/KNN Composite Film with Flexible Energy Harvesting Application","authors":"Nitika Batra*, , , Rajinder Singh Deol, , , Maninder Kaur, , , Henam Sylvia Devi, , , Madhusudan Singh, , and , Bhaskar Mitra, ","doi":"10.1021/acsaelm.5c01728","DOIUrl":"https://doi.org/10.1021/acsaelm.5c01728","url":null,"abstract":"<p >In this work, a lead-free piezoelectric composite material comprising sodium potassium niobate (KNN) sol in an organic piezoelectric polymer (PVDF-TrFE) has been developed. The composite material can be deposited at low temperatures and is compatible with polymeric substrates. The piezoelectric coefficient has a maximum <i>d</i><sub>33</sub> value of 110 pm/V. This is superior to the piezoelectric coefficient for PVDF <i>d</i><sub>33</sub> = 28 pm/V, and most known lead-free piezocomposites that utilize PVDF. The controlled deposition of a thick (>1 μm) layer using spin coating can be easily achieved. The films are crack- and pinhole-free and require low-temperature processing. The introduction of the KNN sol in PVDF-TrFE improved the remnant polarization, dielectric constant, and piezoelectric coefficient of the resulting composite. Additionally, a tape-lift-off method for easily patterning these composite films has been developed, enabling the material to be utilized in micron-level devices. We demonstrate the piezoelectric properties of this composite by fabricating a flexible energy harvesting device that generates (<i>V</i><sub>oc</sub> = 2.2 V) when compared to a PVDF-TrFE-based device (<i>V</i><sub>oc</sub> = 0.05 V) for the same stimulation.</p>","PeriodicalId":3,"journal":{"name":"ACS Applied Electronic Materials","volume":"8 5","pages":"1990–2000"},"PeriodicalIF":4.7,"publicationDate":"2026-02-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147382373","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Sein Lee, , , Jeong-Min Park, , , Wooho Ham, , , Junseo Lee, , , Gyeong-Hun Hwang, , , Seok Daniel Namgung, , , Min-Kyu Song, , and , Jang-Yeon Kwon*,
Conventional digital computing follows the von Neumann architecture, where memory and processing units are physically separated, resulting in limited throughput caused by data transfer bottlenecks, and high power consumption. In contrast, the human brain integrates computation and memory at synapses, enabling highly parallel and energy-efficient processing with only ∼20 W. Neuromorphic computing aims to replicate this efficiency by merging storage and computation within hardware. Oxide semiconductors (OSs) have emerged as promising candidates for synaptic transistors due to their favorable electrical, optical, and structural characteristics, as well as compatibility with low-temperature and large-area processing. This review outlines the fundamental principles of biological synapses and synaptic plasticity metrics, examines recent developments in OS-based synaptic transistors, and discusses prospects and challenges in implementing OS synaptic devices for neuromorphic hardware and artificial intelligence applications.
{"title":"Recent Progress of Oxide Semiconductor-Based Artificial Synaptic Transistors","authors":"Sein Lee, , , Jeong-Min Park, , , Wooho Ham, , , Junseo Lee, , , Gyeong-Hun Hwang, , , Seok Daniel Namgung, , , Min-Kyu Song, , and , Jang-Yeon Kwon*, ","doi":"10.1021/acsaelm.5c01798","DOIUrl":"https://doi.org/10.1021/acsaelm.5c01798","url":null,"abstract":"<p >Conventional digital computing follows the von Neumann architecture, where memory and processing units are physically separated, resulting in limited throughput caused by data transfer bottlenecks, and high power consumption. In contrast, the human brain integrates computation and memory at synapses, enabling highly parallel and energy-efficient processing with only ∼20 W. Neuromorphic computing aims to replicate this efficiency by merging storage and computation within hardware. Oxide semiconductors (OSs) have emerged as promising candidates for synaptic transistors due to their favorable electrical, optical, and structural characteristics, as well as compatibility with low-temperature and large-area processing. This review outlines the fundamental principles of biological synapses and synaptic plasticity metrics, examines recent developments in OS-based synaptic transistors, and discusses prospects and challenges in implementing OS synaptic devices for neuromorphic hardware and artificial intelligence applications.</p>","PeriodicalId":3,"journal":{"name":"ACS Applied Electronic Materials","volume":"8 5","pages":"1952–1972"},"PeriodicalIF":4.7,"publicationDate":"2026-02-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://pubs.acs.org/doi/pdf/10.1021/acsaelm.5c01798","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147384213","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}