在半导体寡合体中锁定共价键可增强超明亮NIR-II发光效应,用于深度大脑神经学
Xiliang Li1, Haohong Gan2, Chi Zhang3
1College of Pharmaceutical Sciences, The Fourth Affiliated Hospital of Soochow University, Suzhou Medical College, Soochow University, Suzhou, P.R. China.
Angewandte Chemie (International ed. in English)
|February 27, 2026
概括
研究人员开发了一种共价键锁定策略,以创建明亮的近红外II (NIR-II) 光体,用于增强脑成像和质瘤治疗学. 这项创新改进了分子设计,用于有效的深层组织可视化和疾病治疗.
科学领域:
- 生物医学工程 生物医学工程
- 纳米技术纳米技术
- 有机化学 有机化学
背景情况:
- 近红外II (NIR-II) 光成像 (1000-1700nm) 对于深层组织可视化和脑疾病治疗学至关重要.
- NIR-II光体的有限的分子设计阻碍了为有效的脑神经治疗药物开发明亮的候选者.
研究的目的:
- 开发一种用于设计明亮的NIR-II光体的新策略.
- 为了设计一个纳米平台,用于增强脑质瘤神经学.
主要方法:
- 开发了一种共价键锁定 (CBL) 策略,以限制扭曲的分子内电荷转移状态.
- 合成了具有终端螺旋供体群的螺旋光素.
- 创建了CBL纳米粒子 (NP) 并用阿波利波蛋白E (ApoE) 修改它们.
主要成果:
- 通过CBL的策略,能够设计出具有高分子灭绝系数和量子产量的明亮NIR-II螺旋光体.
- 通过使用一光子和两光子光生物成像,CBL NPs实现了多尺度高分辨率NIR-II血管学.
- CBL@ApoE NPs在高级脑质瘤治疗中显示出增强的血脑屏障透性.
结论:
- 该CBL策略提供了一种可行的方法,用于设计高亮度NIR-II光光灯.
- CBL NPs提供了一个可靠的纳米平台,用于深度大脑治疗,能够跨越生物障碍以向脑瘤.
相关概念视频
Photoluminescence: Applications
1.2K
Photoluminescence offers a wide range of applications due to its inherent sensitivity and selectivity. This technique allows for both direct and indirect analyses of the analyte. Direct quantitative analysis is possible when the analyte exhibits a favorable quantum yield for fluorescence or phosphorescence. However, an indirect analysis may be feasible if the analyte is not fluorescent or phosphorescent, or if the quantum yield is unfavorable. Indirect methods include reacting the analyte with...
1.2K
Nuclear Overhauser Enhancement (NOE)
1.5K
Irradiation of a spin-active nucleus causes an increase or decrease in the signal intensity of neighboring nuclei that are not necessarily chemically bonded or involved in J-coupling. This phenomenon, called the nuclear Overhauser enhancement (NOE), results from through-space interactions between the nuclear spins. The NOE effect decreases with increasing internuclear distance and is generally not observed beyond 4 angstroms. In NOE, dipole-dipole interactions between neighboring spin-active...
1.5K
Covalent Bonds
166.1K
Overview
166.1K
Covalent Bonds
12.1K
Overview
When two atoms share electrons to complete their valence shells, they create a covalent bond. An atom's electronegativity—the force with which shared electrons are pulled towards an atom—determines how the electrons are shared. Molecules formed with covalent bonds can be either polar or nonpolar. Atoms with similar electronegativities form nonpolar covalent bonds; the electrons are shared equally. Atoms with different electronegativities share electrons unequally,...
When two atoms share electrons to complete their valence shells, they create a covalent bond. An atom's electronegativity—the force with which shared electrons are pulled towards an atom—determines how the electrons are shared. Molecules formed with covalent bonds can be either polar or nonpolar. Atoms with similar electronegativities form nonpolar covalent bonds; the electrons are shared equally. Atoms with different electronegativities share electrons unequally,...
12.1K
Insensitive Nuclei Enhanced by Polarization Transfer (INEPT)
1.1K
Insensitive Nuclei Enhanced by Polarization Transfer (INEPT) is an advanced Nuclear Magnetic Resonance (NMR) technique specifically designed to detect and enhance the signals of low-abundance nuclei, such as carbon-13 and nitrogen-15, in small molecules. The fundamental principle behind INEPT is the transfer of polarization from a more abundant and highly polarizable nucleus, typically hydrogen-1, to the low-abundance nucleus of interest. This process effectively boosts the NMR signal of the...
1.1K
Metal-Semiconductor Junctions
1.2K
The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
1.2K


