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Interface-Mismatch-Induced High Thermoelectricity in MSe–TlSe Superlattices MSe-TlSe超晶格中界面失配诱导的高热电性
IF 4.126 3区 化学 Q2 CHEMISTRY, PHYSICAL Pub Date : 2026-03-20 DOI: 10.1021/acs.jpcc.5c07242
Shivani Vinod, Tanu Choudhary, Raju K. Biswas
Engineering superlattices with enhanced intrinsic in-plane transport and high thermoelectric performance involves exploring new quantum phenomena that emerge from their individual sublayers and corresponding interfaces, which play crucial roles in modern semiconductor technology. Herein, we report a first-principles formalism along with Boltzmann transport theory to study the structural, mechanical, electronic, and thermoelectric properties of MSe (M = Ga, In) layer stacked on TlSe, forming MSe–TlSe superlattices. Lattice dynamics confirm that TlSe layers exclusively dominate the low-frequency region, inducing flat acoustic modes that are absent in pristine GaSe and InSe but intrinsic to TlSe, thereby enhancing phonon scattering and lowering lattice thermal conductivity (κl). Electronic structure analysis exhibits TlSe sublayer-induced valley degeneracy and strong unconventional band convergence originating from MSe sublayer in the conduction band regime, which enhances the density of states near the Fermi level and promotes favorable Seebeck coefficients as well as improved thermoelectric performance. Bonding and charge density analyses indicate that the MSe sublayer combined with TlSe introduces a conductive network that enhances carrier transport relative to pristine bulk systems. To address the inconsistencies present in the conventional DPT formalism, we incorporate the Fröhlich interaction, allowing for a more comprehensive and accurate assessment of carrier mobility. Quantitatively, GaSe–TlSe behaves as an n-type material with ZT values of 1.09 (electrons) and 0.79 (holes) at 600 K, while InSe–TlSe is p-type with superior ZT values of 2.45 (holes) and 0.74 (electrons) at 600 K. Overall, these results demonstrate how the TlSe layer suppresses phonon transport, while the MSe layer establishes a conductive network for efficient electronic transport, offering a rational pathway toward next-generation thermoelectric quantum materials.
具有增强的内在面内输运和高热电性能的工程超晶格涉及探索从其单个子层和相应界面中出现的新量子现象,这些现象在现代半导体技术中起着至关重要的作用。本文采用第一性原理和玻尔兹曼输运理论研究了MSe (M = Ga, In)层叠加在TlSe上形成MSe - TlSe超晶格的结构、力学、电子和热电性质。晶格动力学证实,TlSe层独占低频区,诱导了原始GaSe和InSe中不存在但TlSe固有的平坦声模式,从而增强了声子散射并降低了晶格热导率(κl)。电子结构分析显示,在导带区,TlSe亚层诱导的谷简并和源自MSe亚层的强非常规带收敛,增强了费米能级附近的态密度,促进了有利的塞贝克系数和改善的热电性能。键合和电荷密度分析表明,与TlSe结合的MSe子层引入了一个导电网络,相对于原始体系统,它增强了载流子传输。为了解决传统DPT形式中存在的不一致性,我们结合了Fröhlich交互,允许对航母移动性进行更全面和准确的评估。定量上,在600 K时,se - tlse表现为n型材料,ZT值为1.09(电子)和0.79(空穴);而在600 K时,se - tlse表现为p型材料,ZT值为2.45(空穴)和0.74(电子)。总的来说,这些结果证明了TlSe层如何抑制声子输运,而MSe层建立了一个有效的电子输运的导电网络,为下一代热电量子材料提供了一条合理的途径。
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引用次数: 0
Mechanistic Insights into L-Glutamic Acid–Assisted CuCo2O4/Bi2O3 Hybrid Nanomaterial for Photodegradation of Fluoroquinolone Drug: Optimization of Operational Parameters and Byproducts Profiling 谷氨酸辅助CuCo2O4/Bi2O3杂化纳米材料光降解氟喹诺酮类药物的机理研究:操作参数优化和副产物分析
IF 4.126 3区 化学 Q2 CHEMISTRY, PHYSICAL Pub Date : 2026-03-19 DOI: 10.1021/acs.jpcc.6c00519
Sakthivel Sowndharya, Sankaran Meenakshi
To achieve superior photocatalytic activity, this research focused on incorporating a natural compound, such as an amino acid, into heterojunction photocatalysts. Amino-modified metal oxide compounds that achieve a high level of amino group coverage on their surfaces are utilized for various applications, including adsorption and chromatographic techniques. l-glutamic acid (L-GA) is an aliphatic branched-chain amino acid composed of a proton-acceptor amino group and a proton-donor carbonyl group that exists in a zwitterionic form. Refractory antibiotic pollutants pose a significant and hazardous threat to both the environment and human health. Ciprofloxacin (CIP) has one of the highest rates of antibiotic resistance and may have adverse environmental effects. This work describes the l-glutamic acid-assisted CuCO2O4/Bi2O3 (GCB) as a hybrid photocatalyst for CIP photodegradation. The photogenerated carriers are separated more quickly by the p–n junction, which also generates more active species to react with CIP. The optimum photocatalyst, GCB-0.5, exhibited excellent photocatalytic performance, achieving 97% degradation of CIP within 50 min under optimum conditions of an initial CIP concentration of 50 mg/L (pH 6) and a photocatalyst dosage of 50 mg. The reaction rate constant of GCB is 0.0666 min–1, which was 3.87, 2.86, and 2.4 times greater than the respective CuCo2O4, Bi2O3, and CuCo2O4/Bi2O3 photocatalysts.
为了获得优异的光催化活性,本研究的重点是将天然化合物(如氨基酸)掺入异质结光催化剂中。氨基修饰的金属氧化物化合物在其表面实现高水平的氨基覆盖,用于各种应用,包括吸附和色谱技术。l-谷氨酸(L-GA)是一种脂肪族支链氨基酸,由质子受体氨基和质子供体羰基以两性离子形式存在。难治性抗生素污染物对环境和人类健康都构成了重大的危险威胁。环丙沙星(CIP)具有最高的抗生素耐药率之一,并可能对环境产生不利影响。本研究描述了l-谷氨酸辅助CuCO2O4/Bi2O3 (GCB)作为CIP光降解的杂化光催化剂。光生成的载流子通过p-n结更快地分离,这也产生了更多的活性物质与CIP反应。最佳光催化剂GCB-0.5表现出优异的光催化性能,在初始CIP浓度为50 mg/L (pH 6)、光催化剂用量为50 mg的最佳条件下,在50 min内对CIP的降解率达到97%。GCB的反应速率常数为0.0666 min-1,分别是CuCo2O4、Bi2O3和CuCo2O4/Bi2O3光催化剂的3.87、2.86和2.4倍。
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引用次数: 0
Hydrogen Separation in Flexible Nanoporous Graphene under Steady-State Permeation: A Molecular Dynamics Study 稳态渗透下柔性纳米多孔石墨烯中的氢分离:分子动力学研究
IF 4.126 3区 化学 Q2 CHEMISTRY, PHYSICAL Pub Date : 2026-03-19 DOI: 10.1021/acs.jpcc.5c08540
Hiroki Nagashima, Shu Iha
Efficient separation of hydrogen from mixed gas feeds remains a key challenge in hydrogen production. Here, nanoporous graphene (NPG) is investigated as a hydrogen-selective membrane using nonequilibrium molecular dynamics simulations that enforce steady-state flux via a constant axial driving force while allowing spontaneous membrane deformation. This approach captures realistic operating conditions often overlooked in idealized fixed-membrane studies. Binary mixtures of H2 with CO2, CO, CH4, O2, H2O, N2, and NH3 were examined across three nanopore geometries. The results demonstrate that membrane flexibility significantly influences separation performance: while dynamic pore expansion (parallel deflection) enhances permeance, it reduces selectivity relative to rigid models. We demonstrate that the hydraulic diameter governs the energy barrier for permeance: increasing pore area while disproportionately enlarging the perimeter reduces the hydraulic diameter, thereby increasing steric hindrance. Under these realistic conditions, NPG exhibits much higher permeance than polymer membranes. These findings highlight the importance of accounting for the dynamic coupling between permeation flux and membrane deformation for accurate performance prediction and suggest that mechanical strain is a potential strategy to balance the permeance–selectivity trade-off.
从混合气体原料中有效分离氢气仍然是制氢的关键挑战。在这里,纳米多孔石墨烯(NPG)作为氢选择膜进行了研究,使用非平衡分子动力学模拟,通过恒定的轴向驱动力强制稳态通量,同时允许自发膜变形。这种方法捕捉了在理想化固定膜研究中经常被忽视的实际操作条件。H2与CO2、CO、CH4、O2、H2O、N2和NH3的二元混合物通过三种纳米孔几何形状进行了测试。结果表明,膜的柔韧性对分离性能有显著影响:相对于刚性模型,动态孔膨胀(平行偏转)增强了渗透,但降低了选择性。我们证明了水力直径控制着渗透的能量屏障:增加孔隙面积而不成比例地扩大周长会减少水力直径,从而增加空间位阻。在这些实际条件下,NPG表现出比聚合物膜更高的渗透率。这些发现强调了考虑渗透通量和膜变形之间的动态耦合对于准确预测性能的重要性,并表明机械应变是平衡渗透选择性权衡的潜在策略。
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引用次数: 0
Gate-Tunable Coherent and Incoherent Charge Transfer Pathways in Graphene/MoS2 Heterostructures Revealed by Terahertz Emission Spectroscopy 石墨烯/二硫化钼异质结构中门可调谐的相干和非相干电荷转移途径的太赫兹发射光谱研究
IF 4.126 3区 化学 Q2 CHEMISTRY, PHYSICAL Pub Date : 2026-03-19 DOI: 10.1021/acs.jpcc.6c00646
Chen Wang, Yidan Zhang, Shujie Wang, Xian Lin, Peng Suo, Guohong Ma
Understanding coherent ultrafast charge transfer in two-dimensional van der Waals heterostructures is essential for revealing nonequilibrium processes and advancing optoelectronic device engineering. Here, we employ terahertz emission spectroscopy to probe gate-tunable coherent charge transfer (CT) in graphene/MoS2 heterostructures. Our experimental and analytical results demonstrate that the gate voltage modulates coherent CT (i.e., direct CT) by tuning the heterostructure’s built-in electric field; a higher gate voltage diminishes this field, thereby suppressing the coherent CT component. In contrast, the incoherent CT (photothermionic emission) component exhibits the opposite trend. We attribute this to a gate-induced increase in hot carriers that can overcome the interfacial barrier, an effect that dominates the concurrent reduction in the built-in field. Our findings reveal the fundamental mechanisms of gate-controlled charge dynamics, providing deeper insight into carrier transport in van der Waals heterostructures and a guideline for device development.
了解二维范德华异质结构中的相干超快电荷转移对于揭示非平衡过程和推进光电器件工程至关重要。在这里,我们使用太赫兹发射光谱来探测石墨烯/MoS2异质结构中的门可调谐相干电荷转移(CT)。我们的实验和分析结果表明,栅极电压通过调节异质结构的内置电场来调制相干CT(即直接CT);较高的栅极电压会减弱该场,从而抑制相干CT分量。相反,非相干CT(光热离子发射)组件呈现相反的趋势。我们将此归因于栅极诱导的热载流子的增加,热载流子可以克服界面势垒,这种效应主导了内置场的并发减少。我们的发现揭示了门控电荷动力学的基本机制,为范德华异质结构中的载流子输运提供了更深入的见解,并为器件开发提供了指导。
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引用次数: 0
ZnO/MoSx Heterostructure as a Noble Metal-Free SERS Substrate for the Detection of MB in Lower Concentration Levels ZnO/MoSx异质结构作为无贵金属SERS底物用于低浓度MB检测
IF 4.126 3区 化学 Q2 CHEMISTRY, PHYSICAL Pub Date : 2026-03-19 DOI: 10.1021/acs.jpcc.5c08514
Samya Suvra Datta, Surojit Pande
Surface-enhanced Raman scattering (SERS) is a sensitive spectroscopic method for enhancing Raman signals on roughened metal surfaces or nanostructures. Transition metal-based chalcogenide semiconductors are effective SERS substrates due to their low cost and various tunable properties; however, their enhancement factor (EF) is rather modest. To address this issue, semiconductor heterostructures can be used as SERS substrates due to their large-scale electron–hole pair separation, high interlayer interaction, and efficient photo-induced charge transfer (PICT). In this study, a ZnO/MoSx heterostructure is synthesized and employed as a SERS substrate for the detection of methylene blue (MB). To develop a ZnO/MoSx heterostructure, ZnO is first synthesized using seed-mediated electrodeposition, followed by calcination, and then MoSx is fabricated on ZnO via electrodeposition. The heterostructure ZnO/MoSx is able to detect MB at a lower concentration of 10–10 M with an apparent enhancement factor of 1.2 × 106. The substrate is also extremely stable and robust in nature. The photoluminescence peak intensity of ZnO decreases when MoSx is decorated on it, showing less electron–hole pair recombination in the ZnO/MoSx heterostructure. Thus, the improved SERS performance of the ZnO/MoSx substrate is attributed to the efficient electron–hole pair separation at the heterostructure interface, resulting in facile PICT between the substrate and the Raman analyte.
表面增强拉曼散射(SERS)是一种用于增强粗糙金属表面或纳米结构上拉曼信号的灵敏光谱方法。过渡金属基硫族半导体由于其低成本和各种可调特性而成为有效的SERS衬底;然而,它们的增强因子(EF)相当有限。为了解决这一问题,半导体异质结构可以用作SERS衬底,因为它们具有大规模的电子-空穴对分离,高层间相互作用和高效的光诱导电荷转移(PICT)。在本研究中,合成了ZnO/MoSx异质结构,并将其用作检测亚甲基蓝(MB)的SERS底物。为了制备ZnO/MoSx异质结构,首先采用种子介导电沉积法合成ZnO,然后进行煅烧,然后通过电沉积在ZnO上制备MoSx。异质结构ZnO/MoSx能够在较低浓度(10-10 M)下检测MB,其表观增强因子为1.2 × 106。基材在本质上也是非常稳定和坚固的。ZnO的光致发光峰强度随着MoSx的修饰而降低,表明ZnO/MoSx异质结构中电子-空穴对复合较少。因此,ZnO/MoSx衬底SERS性能的提高归因于异质结构界面上有效的电子-空穴对分离,导致衬底和拉曼分析物之间容易发生PICT。
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引用次数: 0
Salts Induce Enhanced Disintegration of Natural Minerals in Charged Water Microdroplets 盐诱导带电水微滴中天然矿物质的加速分解
IF 4.126 3区 化学 Q2 CHEMISTRY, PHYSICAL Pub Date : 2026-03-19 DOI: 10.1021/acs.jpcc.6c00820
Jamshiya Sulthana, Anubhav Mahapatra, Mridula Bhan, Depanjan Sarkar, Thalappil Pradeep
Charged water microdroplets have been demonstrated to be microreactors capable of disintegrating hard minerals into nanoparticles (NPs) under ambient conditions. However, the high applied potentials required (∼4–4.5 kV) limit the energy efficiency and industrial applications of the phenomenon. Herein, we demonstrate that when aqueous solutions containing trace concentrations of salts (0.1 ppm) are electrosprayed, the threshold potential for quartz disintegration decreases by up to 85%, leading to the formation of 2–10 nm NPs at voltages as low as 1.5 kV. Systematic variation in salt concentration reveals that enhanced droplet conductivity, surface tension, interfacial charge polarization, and localized electric field amplification collectively facilitate efficient disintegration at lower voltages. The effect of ionic size was systematically investigated through different cations (H+ to Cs+) and anions (F to I), establishing that smaller ions promote stronger field localization and faster charge relaxation dynamics. COMSOL simulations elucidate how ionic additives modulate droplet deformation and cleavage of the mineral lattice. This salt-assisted electrospray route offers a green, energy-efficient, and scalable strategy for the ambient synthesis of mineral-derived nanomaterials.
带电水微滴已被证明是一种微反应器,能够在环境条件下将硬质矿物分解成纳米颗粒(NPs)。然而,所需的高应用电位(~ 4-4.5 kV)限制了该现象的能源效率和工业应用。在此,我们证明了当含有微量盐浓度(0.1 ppm)的水溶液被静电喷涂时,石英分解的阈值电位降低了85%,导致在低至1.5 kV的电压下形成2-10 nm的NPs。盐浓度的系统性变化表明,液滴电导率、表面张力、界面电荷极化和局域电场放大的增强共同促进了低电压下的有效分解。通过不同的阳离子(H+到Cs+)和阴离子(F -到I -)系统地研究了离子大小的影响,确定了较小的离子促进更强的场定位和更快的电荷弛豫动力学。COMSOL模拟阐明了离子添加剂如何调节液滴变形和矿物晶格的解理。这种盐辅助电喷雾路线为矿物衍生纳米材料的环境合成提供了一种绿色、节能和可扩展的策略。
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引用次数: 0
Hydrogen Bond Donor-Mediated Selectivity-to-Efficiency Trade-Off in Sustainable Recycling of Lithium-Ion Battery Cathodes 锂离子电池阴极可持续回收中氢键供体介导的选择性与效率权衡
IF 4.126 3区 化学 Q2 CHEMISTRY, PHYSICAL Pub Date : 2026-03-19 DOI: 10.1021/acs.jpcc.6c00085
Xuemin Jing, Pengli Zhang, Ziyi Sun, Liyuan Liu, Wenbin Su, Guangxian Liu, Yu Chen
Sustainable recycling of lithium-ion battery (LIB) cathodes is essential for mitigating resource depletion and environmental pollution. However, the inherent trade-off between selectivity and efficiency remains a critical barrier limiting the performance of current recycling technologies. Herein, we demonstrate that the selectivity and efficiency of metal leaching from LiCoO2 cathodes in spent LIBs can be effectively mediated by the hydrogen bond donor (HBD) in sustainable low-melting mixture solvents. Employing phosphorous acid as the HBD in a betaine:phosphorous acid-based solvent system yields ultrahigh Li/Co selectivity during leaching from the LCO cathode. In contrast, high overall recovery efficiencies for both Li and Co are achieved when phosphoric acid serves as the HBD in a betaine:phosphoric acid-based solvent system.
锂离子电池(LIB)阴极的可持续回收利用对于缓解资源枯竭和环境污染至关重要。然而,选择性和效率之间的内在权衡仍然是限制当前回收技术性能的关键障碍。在此,我们证明了在可持续低熔点混合溶剂中,氢键供体(HBD)可以有效地介导废lib中LiCoO2阴极金属浸出的选择性和效率。在甜菜碱:磷酸基溶剂体系中,采用磷酸作为HBD,在从LCO阴极浸出过程中产生了超高的Li/Co选择性。相比之下,当磷酸作为甜菜碱:磷酸基溶剂体系中的HBD时,锂和钴的总体回收率都很高。
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引用次数: 0
Unveiling Clusterization-Triggered Emission Mechanism Through a Small-Molecule Clusteroluminogen with Color Tunable and White-Light Emission 利用颜色可调、白光发射的小分子簇致发光原揭示簇化触发发光机制
IF 4.126 3区 化学 Q2 CHEMISTRY, PHYSICAL Pub Date : 2026-03-18 DOI: 10.1021/acs.jpcc.5c08523
Kawthar Abid, Sébastien Pillet, Amira Samet, Younes Abid
Clusterization-triggered emission (CTE) is a photophysical phenomenon where clusteroluminogens (CLgens) generate efficient luminescence through supramolecular self-assembly in the solid state. This phenomenon offers unique photophysical properties, distinguishing it from traditional chromophores. In the context of light-emitting devices, there is growing interest in single-component white-light (SCWL) emission, where a single material produces broad emission. However, SCWL emission based on CLgens has been rarely reported, particularly in single crystals, and fabricating SCWL emitters from small-molecule, nonconjugated luminogens remains a significant challenge. The underlying mechanism of CTE is still not fully understood, prompting investigations into small-molecule CLgens to explore their structure–property relationships. In this study, a novel organic salt, TET.Br4 (TET = N,N′-bis(2-aminoethyl)-1,3-propanediamine), is synthesized, consisting of saturated TET cations connected by a hydrogen-bonded network of bromine anions in the crystalline state. The photophysical properties of TET.Br4 are characterized through optical absorption, photoluminescence measurements, and density functional theory (DFT) calculations. The results demonstrate color-tunable CTE and near-white-light emission, highlighting the synergetic role of through-space conjugation, energy/charge transfer, and halogen atoms in the CTE mechanism. This study aims to unravel the mechanism of CTE in small-molecule CLgens and address the scarcity of reports on SCWL emission from nonconjugated luminogens, contributing to advancements in this field.
簇化触发发光(CTE)是一种光物理现象,簇发光原(CLgens)在固体状态下通过超分子自组装产生高效发光。这种现象提供了独特的光物理性质,将其与传统的发色团区分开来。在发光器件的背景下,人们对单组分白光(SCWL)发射越来越感兴趣,其中单一材料产生广泛的发射。然而,基于CLgens的SCWL发射很少有报道,特别是在单晶中,并且从小分子非共轭发光源制造SCWL发射器仍然是一个重大挑战。CTE的潜在机制尚不完全清楚,这促使人们对小分子CLgens进行研究,以探索它们的结构-性质关系。在这项研究中,一种新的有机盐,TET。合成了Br4 (TET = N,N ' -双(2-氨基乙基)-1,3-丙二胺),由饱和TET阳离子以结晶态的溴阴离子氢键网络连接而成。TET的光物理性质。Br4通过光学吸收、光致发光测量和密度泛函理论(DFT)计算来表征。结果表明CTE的颜色可调和近白光发射,突出了通过空间共轭、能量/电荷转移和卤素原子在CTE机制中的协同作用。本研究旨在揭示CTE在小分子CLgens中的作用机制,并解决非共轭发光源的SCWL发射报道不足的问题,为该领域的发展做出贡献。
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引用次数: 0
Challenges in Pulsed-Field Gradient Nuclear Magnetic Resonance on Magnetically Heterogeneous Interfaces: Sequence and Field-Dependent Apparent Diffusion Coefficients 磁非均质界面上脉冲场梯度核磁共振的挑战:序列和场相关表观扩散系数
IF 4.126 3区 化学 Q2 CHEMISTRY, PHYSICAL Pub Date : 2026-03-18 DOI: 10.1021/acs.jpcc.5c08558
Kee Sung Han, Pasquale F. Pulvio
It is well known that the internal gradient (<i>g</i><sub>i</sub>) that exists within pores haunts the diffusion coefficient (<i>D</i>) as measured by the pulsed-field gradient (PFG) nuclear magnetic resonance (NMR). Several PFG-NMR methods developed to determine accurate <i>D</i> were not successful. Then, the steady-state diffusion coefficient (<i>D</i><sub>app,∞</sub>) for the cation [C<sub>4</sub>mim]<sup>+</sup> of [C<sub>4</sub>mim][Tf<sub>2</sub>N] [1-butyl-3-methylimidazolium][bis(trifluoromethylsulfonyl)imde] ionic liquid confined in ordered mesoporous carbon (OMC) was determined by comparing <i>D</i><sub>app,∞</sub> obtained from <sup>1</sup>H PFG-NMR performed with three different stimulated echo sequences: STE, alternating pulsed-field gradient (APFG), and magic pulsed-field gradient (MPFG) under the two external magnetic field strengths, <i>B</i><sub>0</sub> = 9.4 and 14.1 T. The measured <i>D</i><sub>app</sub>,<sub>∞</sub>, which is an order of magnitude smaller than <i>D</i> of bulk [C<sub>4</sub>mim][Tf<sub>2</sub>N], is in good agreement between APFG and MPFG in both <i>B</i><sub>0</sub> = 9.4 and 14.1 T. However, the strong <i>g</i><sub>i</sub> artifact, which caused apparent diffusion coefficient (<i>D</i><sub>app</sub>), depending strongly and weakly on <i>B</i><sub>0</sub> and temperature, respectively, in diffusion time-dependent <i>D</i><sub>app</sub>, <i>D</i><sub>app</sub>(Δ), obtained from a sequence with monopolar gradients (STE), was suppressed by using sequences employing bipolar gradients (APFG and MPFG) in the region of steady-state diffusion. However, the incompletely suppressed <i>g</i><sub>i</sub> artifact resulting in the different behaviors of the early part of <i>D</i><sub>app</sub>(Δ) between the sequences leads to α ≈ 0.6 and 0.9 in MPFG and APFG, respectively, in the relationship between mean-squared displacement and diffusion time: ⟨<i>z</i>(<i>t</i>)<sup>2</sup>⟩ = 2<i>Dt</i><sup>α</sup>, where α = 0.5 and 1 for one-dimensional single-file diffusion and 3D bulk diffusion, respectively. The above observations clearly show that the diffusion behavior of ions/molecules within the pores and pore structure, such as the surface-to-volume ratio <i></i><math display="inline"><mo stretchy="true">(</mo><mrow><msub><mi>D</mi><mi>app</mi></msub><mo stretchy="false">(</mo><mi mathvariant="normal">Δ</mi><mo stretchy="false">)</mo><mo>=</mo><msub><mi>D</mi><mn>0</mn></msub><mrow><mo stretchy="true">[</mo><mrow><mn>1</mn><mo>−</mo><mfrac><mn>4</mn><mrow><mn>9</mn><msqrt><mi>π</mi></msqrt></mrow></mfrac><mfrac><mi>S</mi><mi>V</mi></mfrac><msqrt><mrow><msub><mi>D</mi><mn>0</mn></msub><mi mathvariant="normal">Δ</mi></mrow></msqrt></mrow><mo stretchy="true">]</mo></mrow></mrow><mo stretchy="true">)</mo></math> and tortuosity (<i>T</i> ≡ <i>D</i><sub>0</sub>/<i>D</i><sub>app,∞</sub>), is possible to be misunderstood, especially in systems with a non-negligible <i>g</i><sub>i</sub>. This work demonstrates that it may be necess
众所周知,通过脉冲场梯度(PFG)核磁共振(NMR)测量,孔隙内部梯度(gi)影响扩散系数(D)。几种PFG-NMR测定精确D的方法都不成功。然后,通过比较三种不同刺激回波序列1H PFG-NMR得到的Dapp,∞,确定了约束在有序介孔碳(OMC)中的[C4mim][Tf2N][1-丁基-3-甲基咪唑][双(三氟甲基磺酰基)酰亚胺]离子液体阳离子[C4mim]+的稳态扩散系数(Dapp,∞):在B0 = 9.4和14.1 t两种外部磁场强度下,STE、交变脉冲场梯度(APFG)和魔幻脉冲场梯度(MPFG)的测量值在B0 = 9.4和14.1 t下,APFG和MPFG的测量值∞比体[C4mim][Tf2N]的D值小一个数量级,两者吻合较好。在扩散依赖时间的Dapp中,Dapp(Δ)由单极梯度序列(STE)得到,在稳态扩散区域被双极梯度序列(APFG和MPFG)抑制。然而,不完全抑制的gi伪影导致序列之间Dapp(Δ)早期部分的不同行为,在均方位移和扩散时间之间的关系中,在MPFG和APFG中分别导致α≈0.6和0.9:⟨z(t)2⟩= 2Dtα,其中一维单文件扩散和3D体扩散的α = 0.5和1。上述观察清楚地表明,离子/分子在孔隙和孔隙结构中的扩散行为,如表面体积比(Dapp(Δ)=D0[1−49πSVD0Δ])和弯曲度(T≡D0/Dapp,∞),可能会被误解,特别是在具有不可忽略gi的系统中。这项工作表明,可能有必要在多个外部磁场下测试几个PFG序列,以正确确定离子或分子在具有较大内部梯度的孔隙中的扩散行为。
{"title":"Challenges in Pulsed-Field Gradient Nuclear Magnetic Resonance on Magnetically Heterogeneous Interfaces: Sequence and Field-Dependent Apparent Diffusion Coefficients","authors":"Kee Sung Han, Pasquale F. Pulvio","doi":"10.1021/acs.jpcc.5c08558","DOIUrl":"https://doi.org/10.1021/acs.jpcc.5c08558","url":null,"abstract":"It is well known that the internal gradient (&lt;i&gt;g&lt;/i&gt;&lt;sub&gt;i&lt;/sub&gt;) that exists within pores haunts the diffusion coefficient (&lt;i&gt;D&lt;/i&gt;) as measured by the pulsed-field gradient (PFG) nuclear magnetic resonance (NMR). Several PFG-NMR methods developed to determine accurate &lt;i&gt;D&lt;/i&gt; were not successful. Then, the steady-state diffusion coefficient (&lt;i&gt;D&lt;/i&gt;&lt;sub&gt;app,∞&lt;/sub&gt;) for the cation [C&lt;sub&gt;4&lt;/sub&gt;mim]&lt;sup&gt;+&lt;/sup&gt; of [C&lt;sub&gt;4&lt;/sub&gt;mim][Tf&lt;sub&gt;2&lt;/sub&gt;N] [1-butyl-3-methylimidazolium][bis(trifluoromethylsulfonyl)imde] ionic liquid confined in ordered mesoporous carbon (OMC) was determined by comparing &lt;i&gt;D&lt;/i&gt;&lt;sub&gt;app,∞&lt;/sub&gt; obtained from &lt;sup&gt;1&lt;/sup&gt;H PFG-NMR performed with three different stimulated echo sequences: STE, alternating pulsed-field gradient (APFG), and magic pulsed-field gradient (MPFG) under the two external magnetic field strengths, &lt;i&gt;B&lt;/i&gt;&lt;sub&gt;0&lt;/sub&gt; = 9.4 and 14.1 T. The measured &lt;i&gt;D&lt;/i&gt;&lt;sub&gt;app&lt;/sub&gt;,&lt;sub&gt;∞&lt;/sub&gt;, which is an order of magnitude smaller than &lt;i&gt;D&lt;/i&gt; of bulk [C&lt;sub&gt;4&lt;/sub&gt;mim][Tf&lt;sub&gt;2&lt;/sub&gt;N], is in good agreement between APFG and MPFG in both &lt;i&gt;B&lt;/i&gt;&lt;sub&gt;0&lt;/sub&gt; = 9.4 and 14.1 T. However, the strong &lt;i&gt;g&lt;/i&gt;&lt;sub&gt;i&lt;/sub&gt; artifact, which caused apparent diffusion coefficient (&lt;i&gt;D&lt;/i&gt;&lt;sub&gt;app&lt;/sub&gt;), depending strongly and weakly on &lt;i&gt;B&lt;/i&gt;&lt;sub&gt;0&lt;/sub&gt; and temperature, respectively, in diffusion time-dependent &lt;i&gt;D&lt;/i&gt;&lt;sub&gt;app&lt;/sub&gt;, &lt;i&gt;D&lt;/i&gt;&lt;sub&gt;app&lt;/sub&gt;(Δ), obtained from a sequence with monopolar gradients (STE), was suppressed by using sequences employing bipolar gradients (APFG and MPFG) in the region of steady-state diffusion. However, the incompletely suppressed &lt;i&gt;g&lt;/i&gt;&lt;sub&gt;i&lt;/sub&gt; artifact resulting in the different behaviors of the early part of &lt;i&gt;D&lt;/i&gt;&lt;sub&gt;app&lt;/sub&gt;(Δ) between the sequences leads to α ≈ 0.6 and 0.9 in MPFG and APFG, respectively, in the relationship between mean-squared displacement and diffusion time: ⟨&lt;i&gt;z&lt;/i&gt;(&lt;i&gt;t&lt;/i&gt;)&lt;sup&gt;2&lt;/sup&gt;⟩ = 2&lt;i&gt;Dt&lt;/i&gt;&lt;sup&gt;α&lt;/sup&gt;, where α = 0.5 and 1 for one-dimensional single-file diffusion and 3D bulk diffusion, respectively. The above observations clearly show that the diffusion behavior of ions/molecules within the pores and pore structure, such as the surface-to-volume ratio &lt;i&gt;&lt;/i&gt;&lt;math display=\"inline\"&gt;&lt;mo stretchy=\"true\"&gt;(&lt;/mo&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;mi&gt;app&lt;/mi&gt;&lt;/msub&gt;&lt;mo stretchy=\"false\"&gt;(&lt;/mo&gt;&lt;mi mathvariant=\"normal\"&gt;Δ&lt;/mi&gt;&lt;mo stretchy=\"false\"&gt;)&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/msub&gt;&lt;mrow&gt;&lt;mo stretchy=\"true\"&gt;[&lt;/mo&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mfrac&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;mrow&gt;&lt;mn&gt;9&lt;/mn&gt;&lt;msqrt&gt;&lt;mi&gt;π&lt;/mi&gt;&lt;/msqrt&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;mfrac&gt;&lt;mi&gt;S&lt;/mi&gt;&lt;mi&gt;V&lt;/mi&gt;&lt;/mfrac&gt;&lt;msqrt&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/msub&gt;&lt;mi mathvariant=\"normal\"&gt;Δ&lt;/mi&gt;&lt;/mrow&gt;&lt;/msqrt&gt;&lt;/mrow&gt;&lt;mo stretchy=\"true\"&gt;]&lt;/mo&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;mo stretchy=\"true\"&gt;)&lt;/mo&gt;&lt;/math&gt; and tortuosity (&lt;i&gt;T&lt;/i&gt; ≡ &lt;i&gt;D&lt;/i&gt;&lt;sub&gt;0&lt;/sub&gt;/&lt;i&gt;D&lt;/i&gt;&lt;sub&gt;app,∞&lt;/sub&gt;), is possible to be misunderstood, especially in systems with a non-negligible &lt;i&gt;g&lt;/i&gt;&lt;sub&gt;i&lt;/sub&gt;. This work demonstrates that it may be necess","PeriodicalId":61,"journal":{"name":"The Journal of Physical Chemistry C","volume":"17 1","pages":""},"PeriodicalIF":4.126,"publicationDate":"2026-03-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147478196","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Benchmarking a Computational Workflow Modeling Near-Infrared-Emitting Graphene Quantum Dots 近红外发射石墨烯量子点计算工作流的基准测试
IF 4.126 3区 化学 Q2 CHEMISTRY, PHYSICAL Pub Date : 2026-03-18 DOI: 10.1021/acs.jpcc.5c08269
Muhammad Hammad Ali, Benjamin G. Janesko, MD Masud Rana, Umar Saleem, Naga Mani Gajula
Graphene quantum dots (GQDs) are emerging nanocarbon materials with tunable electronic structures and strong NIR emission, making them promising for bioimaging and optoelectronic applications. The chromophores responsible for GQDs’ NIR emission are often poorly characterized, limiting rational design and clinical applications. Extended π-conjugation, charge-transfer excitations, the presence of diradicaloids, stacking of multiple GQD layers, and blocking of nonradiative decay (as seen in nonaromatic fluorescence) may all contribute to GQDs’ NIR emission. Computation may help disentangle these contributions and aid development of NIR-emitting GQD nanostructures. However, predictive modeling of candidate GQD structures’ stability and NIR emission remains challenging. In this work, we develop a benchmark set of 16 well-defined GQD nanostructures known to emit in the NIR-I window, and we benchmark computational workflows for predicting these structures’ thermodynamic stability and NIR emission. Our workflows combine fast “pre-screening” of thermodynamic stability with symmetry-broken and symmetry-restricted time-dependent density functional theory (TD-DFT) predictions of absorption and emission, selected according to the open- or closed-shell nature of each nanostructure. We find that B3LYP provides acceptable agreement with experimental absorption, while CAM-B3LYP shows good agreement with experimental emission, and that a “synthetic feasibility” descriptor provides reasonable initial screening. We believe that this workflow provides the foundation for high-throughput computational studies accelerating development of NIR-emitting GQDs.
石墨烯量子点(GQDs)是一种新兴的纳米碳材料,具有可调谐的电子结构和强的近红外发射,在生物成像和光电子领域具有广阔的应用前景。负责GQDs近红外发射的发色团通常特征不佳,限制了合理的设计和临床应用。扩展π共轭、电荷转移激发、二根碱的存在、多个GQD层的堆叠以及非辐射衰变的阻断(如非芳族荧光所示)都可能有助于GQD的近红外发射。计算可能有助于解开这些贡献,并有助于nir发射GQD纳米结构的发展。然而,候选GQD结构的稳定性和近红外发射的预测建模仍然具有挑战性。在这项工作中,我们开发了一个由16个已知在NIR- i窗口中发射的定义良好的GQD纳米结构组成的基准集,并对预测这些结构的热力学稳定性和近红外发射的计算工作流程进行了基准测试。我们的工作流程结合了热力学稳定性的快速“预筛选”与对称破缺和对称限制时依赖密度泛函理论(TD-DFT)的吸收和发射预测,根据每个纳米结构的开壳或闭壳性质进行选择。我们发现B3LYP与实验吸收具有良好的一致性,而CAM-B3LYP与实验发射具有良好的一致性,并且“合成可行性”描述符提供了合理的初始筛选。我们相信这一工作流程为高通量计算研究提供了基础,加速了nir发射GQDs的发展。
{"title":"Benchmarking a Computational Workflow Modeling Near-Infrared-Emitting Graphene Quantum Dots","authors":"Muhammad Hammad Ali, Benjamin G. Janesko, MD Masud Rana, Umar Saleem, Naga Mani Gajula","doi":"10.1021/acs.jpcc.5c08269","DOIUrl":"https://doi.org/10.1021/acs.jpcc.5c08269","url":null,"abstract":"Graphene quantum dots (GQDs) are emerging nanocarbon materials with tunable electronic structures and strong NIR emission, making them promising for bioimaging and optoelectronic applications. The chromophores responsible for GQDs’ NIR emission are often poorly characterized, limiting rational design and clinical applications. Extended π-conjugation, charge-transfer excitations, the presence of diradicaloids, stacking of multiple GQD layers, and blocking of nonradiative decay (as seen in nonaromatic fluorescence) may all contribute to GQDs’ NIR emission. Computation may help disentangle these contributions and aid development of NIR-emitting GQD nanostructures. However, predictive modeling of candidate GQD structures’ stability and NIR emission remains challenging. In this work, we develop a benchmark set of 16 well-defined GQD nanostructures known to emit in the NIR-I window, and we benchmark computational workflows for predicting these structures’ thermodynamic stability and NIR emission. Our workflows combine fast “pre-screening” of thermodynamic stability with symmetry-broken and symmetry-restricted time-dependent density functional theory (TD-DFT) predictions of absorption and emission, selected according to the open- or closed-shell nature of each nanostructure. We find that B3LYP provides acceptable agreement with experimental absorption, while CAM-B3LYP shows good agreement with experimental emission, and that a “synthetic feasibility” descriptor provides reasonable initial screening. We believe that this workflow provides the foundation for high-throughput computational studies accelerating development of NIR-emitting GQDs.","PeriodicalId":61,"journal":{"name":"The Journal of Physical Chemistry C","volume":"13 1 1","pages":""},"PeriodicalIF":4.126,"publicationDate":"2026-03-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"147478506","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
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The Journal of Physical Chemistry C
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