Carbyne with finite length: The one-dimensional sp carbon

Slides:



Advertisements
Similar presentations
UV / visible Spectroscopy
Advertisements

Ultraviolet (UV) region 4 x m to m Region of greatest interest to organic chemists from 2 x m to 4 x meters 10.9 Ultraviolet Spectroscopy.
R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.
10-1 Application of IR Raman Spectroscopy 3 IR regions Structure and Functional Group Absorption IR Reflection IR Photoacoustic IR IR Emission Micro.
1 Miyasaka Laboratory Yusuke Satoh David W. McCamant et al, Science, 2005, 310, Structural observation of the primary isomerization in vision.
Molecular Nanostuctures 1. Introduction. Carbon hybridization and allotropes Alexey A. Popov, IFW Dresden
Infrared Spectroscopy
Characterization of Nanomaterials 1- Scanning Electron Microscopy (SEM) It is one of the most widely used techniques in the characterization of the morphology,
The many forms of carbon Carbon is not only the basis of life, it also provides an enormous variety of structures for nanotechnology. This versatility.
An introduction to Spectrometric Methods. Spectroscopy Definition Spectroscopy is a general term for the science that deal with the interactions of various.
Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. Photographs of exposed femoral bone surfaces and surrounding tissue prepared for.
1 Instrumental Analysis Tutorial 2. 2 Objectives By the end of this session the student should be able to: 1.Describe the grating principle of work. 2.Describe.
Date of download: 7/11/2016 Copyright © 2016 SPIE. All rights reserved. Typical temperature increase inside (solid line) and on the surface (dashed line)
Solids and Liquids Chapter 13.
Diguet, A. et al. Eelkema, R. et al.
Volume 3, Issue 4, Pages (October 2017)
Quan Pang, Xiao Liang, Abhinandan Shyamsunder, Linda F. Nazar  Joule 
The Protonation State of the Glu-71/Asp-80 Residues in the KcsA Potassium Channel: A First-Principles QM/MM Molecular Dynamics Study  Denis Bucher, Leonardo.
Can Non-Mechanical Proteins Withstand Force
Thermal Photonics and Energy Applications
Volume 83, Issue 3, Pages (September 2002)
Volume 5, Issue 3, Pages (March 2019)
by Jungwon Park, Hans Elmlund, Peter Ercius, Jong Min Yuk, David T
Chapter 13.3 The Nature of Solids.
Volume 104, Issue 1, Pages (January 2013)
Absence of Ion-Binding Affinity in the Putatively Inactivated Low-[K+] Structure of the KcsA Potassium Channel  Céline Boiteux, Simon Bernèche  Structure 
Volume 86, Issue 4, Pages (April 2004)
Kristen E. Norman, Hugh Nymeyer  Biophysical Journal 
The Role of Higher CO-Multipole Moments in Understanding the Dynamics of Photodissociated Carbonmonoxide in Myoglobin  Nuria Plattner, Markus Meuwly 
Volume 3, Issue 4, Pages (October 2017)
Reactivity-Guided Interface Design in Na Metal Solid-State Batteries
Organic Chemistry Molecules and Colour.
Volume 84, Issue 3, Pages (March 2003)
Fig. 1 Characterization of the device structure.
Fig. 3 Evolution of absorber with annealing.
Fig. 2 Characterization of fs-laser–induced degradation.
Fig. 1 Bands and hybridization in graphene-encapsulated WSe2 measured by μ-ARPES. Bands and hybridization in graphene-encapsulated WSe2 measured by μ-ARPES.
Fig. 3 Mechanism and result of the super-resolution RLP.
Volume 106, Issue 5, Pages (March 2014)
Fig. 2 Materials and designs for bioresorbable PC microcavity-based pressure and temperature sensors. Materials and designs for bioresorbable PC microcavity-based.
Fig. 1 Schematic illustration of in situ TEM imaging of Pt nanocrystals freely rotating in a graphene liquid cell (GLC) and 3D EM density maps calculated.
Mechano-thermo-chromic device with supersaturated salt hydrate crystal phase change by Hyunmin Cho, Jinhyeong Kwon, Inho Ha, Jinwook Jung, Yoonsoo Rho,
Fig. 4 The results of HRTEM and high-angle annular dark-field scanning TEM investigations. The results of HRTEM and high-angle annular dark-field scanning.
Fig. 3 Extension of our proposed programmable synthesis to the selective synthesis of a wide variety of liposome/metal hybrids. Extension of our proposed.
Molecular engineered conjugated polymer with high thermal conductivity
Ultrahigh mobility and efficient charge injection in monolayer organic thin-film transistors on boron nitride by Daowei He, Jingsi Qiao, Linglong Zhang,
Fig. 2 Raman characterization of CVD-grown graphene.
Ultratransparent and stretchable graphene electrodes
Fig. 1 Optical and STEM characterization of vdW heterostructures.
Fig. 4 Giant optical chirality.
High-density array of ferroelectric nanodots with robust and reversibly switchable topological domain states by Zhongwen Li, Yujia Wang, Guo Tian, Peilian.
Energy penetration into arrays of aligned nanowires irradiated with relativistic intensities: Scaling to terabar pressures by Clayton Bargsten, Reed Hollinger,
Triplet Sensitization by Lead Halide Perovskite Thin Films for Efficient Solid-State Photon Upconversion at Subsolar Fluxes  Sarah Wieghold, Alexander.
Large spin-orbit torque efficiency enhanced by magnetic structure of collinear antiferromagnet IrMn by Jing Zhou, Xiao Wang, Yaohua Liu, Jihang Yu, Huixia.
by Alan She, Shuyan Zhang, Samuel Shian, David R
Dipole-like electrostatic asymmetry of gold nanorods
Atomic structure of sensitive battery materials and interfaces revealed by cryo–electron microscopy by Yuzhang Li, Yanbin Li, Allen Pei, Kai Yan, Yongming.
Quasi-freestanding epitaxial silicene on Ag(111) by oxygen intercalation by Yi Du, Jincheng Zhuang, Jiaou Wang, Zhi Li, Hongsheng Liu, Jijun Zhao, Xun.
Fig. 2 Construction of a mimetic biomineralization frontier for epitaxial crystal growth by using CPICs. Construction of a mimetic biomineralization frontier.
Observation of twist-induced geometric phases and inhibition of optical tunneling via Aharonov-Bohm effects by Midya Parto, Helena Lopez-Aviles, Jose E.
by Mark T. Edmonds, James L
Fig. 1 MIR photovoltaic detector based on b-AsP.
Van der Waals engineering of ferromagnetic semiconductor heterostructures for spin and valleytronics by Ding Zhong, Kyle L. Seyler, Xiayu Linpeng, Ran.
Evidence of Cholesterol Accumulated in High Curvature Regions: Implication to the Curvature Elastic Energy for Lipid Mixtures  Wangchen Wang, Lin Yang,
Fig. 1 Sketch and schematic diagram of photobleaching reaction in a strongly coupled system. Sketch and schematic diagram of photobleaching reaction in.
Fig. 2 Characterization of metal-chalcogenide thin films.
Fig. 2 The possible interaction mechanism between IR-783 and albumin is critical to guide efficient nanocomplex synthesis and fluorescence enhancement.
Fig. 3 Supraballs and films assembled from binary 219/217nm SPs/SMPs.
Fig. 1 XRD and sp2/sp3 component of compressed GCs (Com
SEM and TEM images and photoluminescence properties of composites
Presentation transcript:

Carbyne with finite length: The one-dimensional sp carbon by Bitao Pan, Jun Xiao, Jiling Li, Pu Liu, Chengxin Wang, and Guowei Yang Science Volume 1(9):e1500857 October 30, 2015 Copyright © 2015, The Authors

Fig. 1 Schematic illustration of the three kinds of hybridization of carbon. Schematic illustration of the three kinds of hybridization of carbon. Diamond represents sp3 hybridization, and its derivatives are lonsdaleite and C8. The most familiar carbon material, graphite, shows sp2 hybridization, and its derivatives are fullerene, carbon nanotube, and graphene. Carbyne is the one-dimensional allotrope of carbon composed of sp-hybridized carbon atoms. However, definitive evidence for carbyne remains elusive. Therefore, the existence of carbyne derivatives remains unknown. Bitao Pan et al. Sci Adv 2015;1:e1500857 Copyright © 2015, The Authors

Fig. 2 Spectroscopic analysis of carbyne. Spectroscopic analysis of carbyne. (A) Raman spectrum. The peaks at 1050 and 2175 cm−1 belong to carbon-carbon single bonds and triple bonds, respectively. (B) FTIR spectrum. The signal at 2157 cm−1 is ascribed to the stretching vibration of carbon-carbon triple bonds. Bitao Pan et al. Sci Adv 2015;1:e1500857 Copyright © 2015, The Authors

Fig. 3 UV-Vis and fluorescence spectra of carbyne. UV-Vis and fluorescence spectra of carbyne. (A) UV-Vis absorption spectrum of the sample obtained at 2.3 min through HPLC (CH3OH/H2O; 97:3, v/v) and the corresponding optical graph of a colorless transparent solution. (B) Fluorescence emission of carbyne. Three fluorescence peaks (at 410, 435, and 465 nm) remain the same as excitation wavelength varies. Inset: The purple-blue fluorescence graph excited with a 370-nm light. (C) The lifetime of the sample is measured to be 1.3 ns. Inset: No photobleaching was observed with a 450-W xenon lamp across 1.5 hours. (D) Schematic illustration of three kinds of fluorescence behavior derived from different lengths of carbyne chains. (E) Dependence of energy gaps (ΔE) on the number of carbon atoms in carbyne. It is clear that the gaps between the highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular orbital (LUMO) of carbyne monotonically decrease with increasing number of carbon atoms. For the 4- and 100-carbon carbynes, the HOMO-LUMO gap is 4.061 and 0.487 eV, respectively, implying the tuning of energy gaps (from broad to narrow) accompanying the increase in carbon atoms in carbyne. (F) For comparison, the relative energy in vertical coordinates represents the absolute value of relative binding energy. Negative binding energy corresponds to a stable configuration. The greater is the absolute value, the higher is the stability of carbyne chains. The relative absolute value of binding energy decreases with increasing number of carbon atoms in carbyne, but the decreasing speed gradually becomes slower and ultimately reaches a specific value. Dotted horizontal curve, trend reaching a specific value; circle, turning point in the curve. Bitao Pan et al. Sci Adv 2015;1:e1500857 Copyright © 2015, The Authors

Fig. 4 Morphology and structural characterization of carbyne crystals. Morphology and structural characterization of carbyne crystals. (A) XRD pattern of the sample. The peaks are shaped and strong, showing the good crystallinity of carbyne. There is an obviously preferred orientation along the c axis. Inset: White carbyne powder coating on the glass substrate. Rectangular glass substrate with white crystal powder (left) compared with bare glass (right). (B) SEM image of carbyne crystals. They are in the shape of flakes stacked together. EDS showing that the sample contains C, O, and Au. O and Au originate from the surface adsorption of oxygen molecules and gold nanocrystals. (C) TEM image of carbyne crystals. Carbyne exhibits a rod shape (10 to 30 nm in width and 50 to >100 nm in length). The tiny spherical particles on the surface of nanorods are gold nanocrystals. (D to I) SAED patterns and HRTEM images are divided into three categories based on the direction of the incident electron beam ([1-20], [012], and [001], respectively). The former two are rectangular lattices, whereas the last one is a hexagonal lattice. Scale bars, 5 nm (E), 3 nm (G), and 3 nm (H). (J) EDS shows that the sample is almost completely composed of carbon and that the Cu signal originated from the Cu grid. Bitao Pan et al. Sci Adv 2015;1:e1500857 Copyright © 2015, The Authors

Fig. 5 Carbyne crystal structure. Carbyne crystal structure. (A) The proposed hexagonal structure frame (a = 5.78 Å, b = 5.78 Å, c = 9.92 Å, α = 90°, β = 90°, γ = 120°); the distance between neighboring carbon atoms is 3.34 Å. The corner at the kinks is conjugated by two carbon atoms forming a C–C single bond, and the kinked angle (the angle between the vertical direction and the kinked bond) is 30°. (B) The equilibrium configuration of the constructed carbyne crystal based on first-principles calculations. (Left) The unit cell observed from the top (top panel) and side (bottom panel). (Right) The 4 × 4 × 2 supercell observed from the cross-profile perpendicular to the c axis (top panel) and side (bottom panel). Bitao Pan et al. Sci Adv 2015;1:e1500857 Copyright © 2015, The Authors

Fig. 6 Mechanism of carbyne formation. Mechanism of carbyne formation. (A) Schematic illustration of four chemical reactions involved in LAL. Carbyne formation is probably involved in the second kind of chemical reaction occurring inside laser-induced plasma (T+ + L+) and in the chemical reactions occurring at the interface between the laser-induced plasma and liquid (T+ + L). T+, laser-induced target plasma; L+, excited liquid molecules. (B) The pathway from alcohol molecules to the carbon-carbon triple bond, in which alcohol dehydrogenated by Au ions plays a key role. [Au], Au ion; :Nu, nucleophile. (C) The emission spectra of different solvents during LAL; the peak of alcohol (558.1 and 563.3 nm) in the emission spectrum corresponding to the C2 swan band for Δv = −1. The spectra of nonalcohol solvent greatly differ from those of alcohol, and no C2 signal can be detected. (D) Similar fluorescence peaks using nanosecond (ns) and femtosecond (fs) lasers. (E) The thermodynamic phase diagram of carbyne adopted by Whittaker (33). Green region, the preferred thermodynamic region for carbyne formation. (F) Individual carbyne nanorod with gold nanocrystals adheres to its surface; the cartoon depicts how this structure forms. Scale bar, 10 nm. Bitao Pan et al. Sci Adv 2015;1:e1500857 Copyright © 2015, The Authors