MRS Meetings and Events

 

EQ06.07.03 2022 MRS Fall Meeting

Probing Charge Transfer of Aβ-Proteins Examined Using Two-Dimensional Materials as Raman Spectroscopic Platform

When and Where

Nov 30, 2022
2:15pm - 2:30pm

Sheraton, 2nd Floor, Back Bay B

Presenter

Co-Author(s)

Wujoon Cha1,2,Chaejeong Heo1,2,Sang Hyub Lee1,2,Seok Jun Yun3,Byeong Wook Cho1,2,Taewoo Ha1,2,Young Hee Lee1,2

Institute for Basic Science1,Sungkyunkwan University2,Oak Ridge National Laboratory3

Abstract

Wujoon Cha1,2,Chaejeong Heo1,2,Sang Hyub Lee1,2,Seok Jun Yun3,Byeong Wook Cho1,2,Taewoo Ha1,2,Young Hee Lee1,2

Institute for Basic Science1,Sungkyunkwan University2,Oak Ridge National Laboratory3
We report distinguished charge transfer of amyloid-<i>β</i> (A<i>β</i>) proteins at different aggregation stages with two-dimensional (2D) materials that can potentially be critical for understanding the fibrillization mechanism and developing an early-stage diagnostic method of Alzheimer’s disease. We previously identified notable variations in conductance of A<i>β</i> proteins in monomer, oligomer, and fibril forms measured by THz spectroscopy, suggesting significant changes in electronic structures as A<i>β</i> fibrillizes [1]. In this work, we show that A<i>β</i>s exhibit distinct charge-transfer behavior depending on their aggregated states when interacting with monolayer graphene and molybdenum disulfide (MoS<sub>2</sub>). In particular, we found that small and soluble A<i>β </i>monomers <i>p-</i>doped both graphene and MoS<sub>2</sub> sheets while large and insoluble A<i>β </i>fibrils <i>n-</i>doped them. These findings provide critical insights into the electronic properties of A<i>β</i>s that could be essential to identifying the onset of neurotoxic A<i>β</i> fibril formation and developing a rapid, label-free diagnosis based on two-dimensional materials.<br/><br/>In Alzheimer’s disease (AD), the accumulation of senile plaques, dominantly composed of fibrillized A<i>β</i>s in the cerebral cortex, has been identified as the primary indication of degeneracy. Therefore, early diagnosis of AD is strongly dependent on the ability to detect the emergence of toxic A<i>β</i> oligomers and fibrils. It has been suggested that charge transfer plays a key role in the formation and the interaction of proteins [2]. Although A<i>β</i> states can be identified based on ‘fingerprints’ of vibrational modes observed with optical spectroscopies, there is a gap in knowledge about the electronic properties of A<i>β </i>that varies significantly as A<i>β</i> fibrillizes. To address this gap, we used Raman spectroscopy to probe A<i>β</i> proteins interacting with two-dimensional materials that are sensitive to molecular charge transfer.<br/><br/>Graphene, an atomically thin semimetal, and monolayer MoS<sub>2</sub>, a semiconductor with a direct bandgap, react sensitively to charge-transfer-induced doping. The shifts in the carrier concentrations and in the Fermi levels can be distinguished from the characteristic Raman bands in graphene (G and 2D) and in MoS<sub>2</sub> (E<sub>2g</sub> and A<sub>1g</sub>) [3,4]. Here, we conducted Raman spectroscopy on monolayer graphene and MoS<sub>2</sub> added with A<i>β</i> proteins at different fibrillization stages - monomer, oligomer, and fibril. The graphene and MoS<sub>2</sub> sheets were prepared <i>via</i> chemical vapor deposition and transferred on a Si/SiO<sub>2</sub> 300-nm substrate separately. Then,10 <i>µ</i>M protein solutions were loaded and dried in air for subsequent Raman spectroscopy. A statistically significant (p-value &lt; 0.0001) distinction was shown for doping due to monomers and fibrils. Taking the effects of buffer media into account, we observed that, in both graphene and MoS<sub>2</sub>, monomer withdrew electrons and <i>p</i>-doped while fibril injected electrons and <i>n</i>-doped on average. This was evidenced by the upshift(downshift) of G and 2D band, sharpening(broadening) of G band, and decrease(increase) of 2D to G intensity ratio for graphene with monomer(fibril). Similarly, in MoS<sub>2</sub>, A<sub>1g</sub> frequency increased(decreased) and width stiffened(softened) by monomer(fibril). The changes in carrier concentrations were calculated based on the relative positions of the signature Raman bands. In turn, we estimated that the monomers and fibrils shifted the graphene Fermi level by approximately -1.0 eV and +1.9 eV, respectively. The contrary charge-transfer behavior suggests that the electronic states of A<i>β</i>, such as its highest occupied (HOMO) and lowest unoccupied (LUMO) molecular orbital levels, shift significantly as A<i>β</i> fibrillizes. The transition point from <i>p</i>-doping to <i>n</i>-doping can serve as a marker for the onset of toxic A<i>β </i>aggregates.<br/><br/>[1] Heo<i> et al.</i>, ACS Nano, <b>14</b>, 6548 (2020).<br/>[2] Cordes <i>et al.,</i> Chem. Soc. Rev., <b>38</b>, 892 (2009).<br/>[3] Das <i>et al.</i>, Nat. Nanotech., <b>3</b>, 210 (2008).<br/>[4] Zhong <i>et al</i>., Chem. Soc. Rev., <b>44</b>, 2757 (2015).

Keywords

2D materials | Raman spectroscopy

Symposium Organizers

Xu Zhang, Carnegie Mellon University
Monica Allen, University of California, San Diego
Ming-Yang Li, TSMC
Doron Naveh, Bar-Ilan Univ

Publishing Alliance

MRS publishes with Springer Nature