関連する実験動画
Updated: Jun 13, 2026

08:51
Monitoring Protein Adsorption with Solid-state Nanopores
Published on: December 2, 2011
13.6K
固体ナノ孔による誤折りたたまれたタンパク質オリゴマーの複合デジタル特性
Sarah E Sandler1, Robert I Horne2, Sara Rocchetti1
1Cavendish Laboratory, Maxwell Centre, Department of Physics, University of Cambridge, Cambridge CB3 0HE, U.K.
Journal of the American Chemical Society
|November 16, 2023
まとめ
この研究では,ナノ孔とDNAバーコードを使用して,誤った折りたたまれたタンパク質オリゴーマーを検出し,定量化するための新しい単分子法が導入されています. この技術はパーキンソン病のような 神経退行性疾患の診断と治療法を 開発するのに役立ちます
科学分野:
- 生物化学
- ナノテクノロジー
- 神経科学
背景:
- アルツハイマー病やパーキンソン病の 鍵となるものです
- これらのオリゴマーの検出と定量化のための現在の方法は,正確さと高通量能力が欠けている.
- 神経退行性疾患の 診断と治療に先端的なツールが不可欠です
研究 の 目的:
- タンパク質オリゴマーの検出と定量化のための新しい単分子アプローチを開発する.
- アルファシヌクレイン集積阻害剤の研究における方法の適用性を実証する.
- パーキンソン病の診断と治療の戦略を進めるために
主な方法:
- 固体ナノポールを単分子分析に使用した.
- オリゴマーの同時識別と特徴づけのために多重化DNAバーコードを使用した.
- アルファ・シヌクレイン・オリゴマーと小分子集積阻害剤との相互作用を研究した.
主要な成果:
- 単一分子レベルでアルファ-シヌクレインのオリゴーマーを検出し,定量化しました.
- DNAバーコードを用いて複数のサンプルを同時に分析する能力を示した.
- 潜在的治療薬のスクリーニングのための 敏感なプラットフォームを提供した.
結論:
- 提示された単一分子ナノポアとDNAバーコーディング方法は,オリゴマーの検出と定量化のための強力なツールを提供します.
- このアプローチはパーキンソン病の診断と治療の発展を加速させる大きな可能性を秘めています
- この方法は,他の誤折れタンパク質オリゴーマー関連疾患の研究に適応できます.
関連する概念動画
¹H NMR: Complex Splitting
A proton M that is coupled to a proton X results in doublet signals for M. However, NMR-active nuclei can be simultaneously coupled to more than one nonequivalent nucleus. When M is coupled to a second proton A, such as in styrene oxide, each peak in the doublet is split into another doublet.
Splitting diagrams or splitting tree diagrams are routinely used to depict such complex couplings. While drawing splitting diagrams, the splitting with the larger coupling constant is usually applied first.
Splitting diagrams or splitting tree diagrams are routinely used to depict such complex couplings. While drawing splitting diagrams, the splitting with the larger coupling constant is usually applied first.
¹H NMR: Interpreting Distorted and Overlapping Signals
Spin systems where the difference in chemical shifts of the coupled nuclei is greater than ten times J are called first-order spin systems. These nuclei are weakly coupled, and their chemical shifts and coupling constant can generally be estimated from the well-separated signals in the spectrum.
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are slanted or...
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are slanted or...
¹³C NMR: Distortionless Enhancement by Polarization Transfer (DEPT)
When proton-coupled carbon-13 spectra are simplified by a broadband proton decoupling technique, structural information about the coupled protons is lost. Distortionless enhancement by polarization transfer (DEPT) is a technique that provides information on the number of hydrogens attached to each carbon in a molecule. While the DEPT experiment utilizes complex pulse sequences, the pulse delay and flip angle are specifically manipulated. The resulting signals have different phases depending on...
NMR Spectrometers: Resolution and Error Correction
When magnetic nuclei in a sample achieve resonance and undergo relaxation, the signal detected in NMR is an approximately exponential free induction decay. Fourier transform of an exponential decay yields a Lorentzian peak in the frequency domain. Lorentzian peaks in an NMR spectrum are defined by their amplitude, full width at half maximum, and position, where the peak width is governed by the spin-spin relaxation time alone. In real experiments, however, the applied magnetic field is rendered...
¹H NMR Signal Multiplicity: Splitting Patterns
When protons A and X are coupled, their nuclear spin energy levels are slightly modified. This is because the energy required to excite proton A to a spin state parallel to proton X is slightly different from the energy required for it to become anti-parallel to spin X. Consequently, there are two possible excitation frequencies for A (A1 and A2), depending on the spin state of X, and vice versa. The mutual nature of coupling implies that the difference between frequencies A1 and A2, indicated...

