Supporting Information. A biofunctionalizable ink platform composed of catechol-modified. chitosan and reduced graphene oxide/platinum nanocomposite

Similar documents
NMRis the most valuable spectroscopic technique for organic chemists because it maps the carbon-hydrogen framework of a molecule.

Spectroscopy. Empirical Formula: Chemical Formula: Index of Hydrogen Deficiency (IHD)

Band-like transport in highly crystalline graphene films from

Exam (6 pts) Show which starting materials are used to produce the following Diels-Alder products:

Synthesis and Characterization of Graphene by Raman Spectroscopy

Technical Note. Introduction

CHEM Chapter 13. Nuclear Magnetic Spectroscopy (Homework) W

For more information, please contact: or +1 (302)

Synthesis and Characterization of Exfoliated Graphite (EG) and to Use it as a Reinforcement in Zn-based Metal Matrix Composites

Electronic Supplementary Information

Organic Chemistry II (CHE ) Examination I February 11, Name (Print legibly): Key. Student ID#:

OAT Organic Chemistry - Problem Drill 19: NMR Spectroscopy and Mass Spectrometry

Cu 2 O/g-C 3 N 4 nanocomposites: An insight into the band structure tuning and catalytic efficiencies

Graphene is a single, two-dimensional nanosheet of aromatic sp 2 hybridized carbons that

Experiment 11: NUCLEAR MAGNETIC RESONANCE SPECTROSCOPY

Supporting Information: A comparative Electron Paramagnetic Resonance study of expanded graphites and graphene

Chapter 9. Nuclear Magnetic Resonance. Ch. 9-1

Answers to Assignment #5

Calculate a rate given a species concentration change.

Spectroscopy in Organic Chemistry. Types of Spectroscopy in Organic

Metal hydroxides as conversion electrode for lithium-ion battery: A case study with Cu(OH) 2 nanoflower array

Structure Determination. How to determine what compound that you have? One way to determine compound is to get an elemental analysis

CH 3. mirror plane. CH c d

(b) How many hydrogen atoms are in the molecular formula of compound A? [Consider the 1 H NMR]

FMM, 15 th Feb Simon Zihlmann

PAPER No.12 :Organic Spectroscopy MODULE No.29: Combined problem on UV, IR, 1 H NMR, 13 C NMR and Mass - Part I

4. NMR spectra. Interpreting NMR spectra. Low-resolution NMR spectra. There are two kinds: Low-resolution NMR spectra. High-resolution NMR spectra

Chem 213 Final 2012 Detailed Solution Key for Structures A H

Chapter 14 Spectroscopy

Chemistry 605 (Reich)

Basic Concepts of NMR: Identification of the Isomers of C 4 O 2. by 1 H NMR Spectroscopy

11. Proton NMR (text , 12.11, 12.12)

Organic Chemistry II KEY March 25, a) I only b) II only c) II & III d) III & IV e) I, II, III & IV

REDUCTION OF FREESTANDING GRAPHENE OXIDE FILMS USING CONTINUOUS WAVE LASER

Principles of Molecular Spectroscopy: Electromagnetic Radiation and Molecular structure. Nuclear Magnetic Resonance (NMR)

- 1/2. = kb o = hνν + 1/2. B o increasing magnetic field strength. degenerate at B o = 0

ERRATA. p. 2 In the second line from the bottom, the expression should be , not

Chemistry 416 Spectroscopy Fall Semester 1997 Dr. Rainer Glaser

Magnetite decorated graphite nanoplatelets as cost effective CO 2 adsorbent

Paper 12: Organic Spectroscopy

18.1 Intro to Aromatic Compounds

Magnetic Nuclei other than 1 H

CHEM 344 Fall 2016 Spectroscopy and WebMO Exam (75 pts)

NUCLEAR MAGNETIC RESONANCE AND INTRODUCTION TO MASS SPECTROMETRY

ERRATA. Chapter 1 p. 2 In the second line from the bottom, the expression should be , not

Atomic and Molecular Dimensions

The Use of NMR Spectroscopy

NMR parameters intensity chemical shift coupling constants 1D 1 H spectra of nucleic acids and proteins

Direct Observation of Inner and Outer G Band Double-resonance Raman Scattering in Free Standing Graphene

Experiment 1. Lab Safety & IR Spectroscopy

Chapter 13 Structure t Determination: Nuclear Magnetic Resonance Spectroscopy

Hour Examination # 4

Organic Chemistry 321 Workshop: Spectroscopy NMR-IR Problem Set

4) protons experience a net magnetic field strength that is smaller than the applied magnetic field.

Chem Homework = cm -1, HF; cm -1, H 35 Cl; cm -1, H 81 Br; cm -1, H 127 I

The Raman Spectroscopy of Graphene and the Determination of Layer Thickness

Please do not adjust margins. Graphene oxide based moisture-responsive biomimetic film actuators with nacrelike layered structures

Characterization of partially reduced graphene oxide as room

Tautomerism in 1-hydroxy-2-naphthaldehyde Schiff bases: Calculation of tautomeric isomers using carbon-13 NMR

Supporting Information

Objective 4. Determine (characterize) the structure of a compound using IR, NMR, MS.

NMR = Nuclear Magnetic Resonance

Structure solving based on IR, UV-Vis, MS, 1 H and 13 C NMR spectroscopic data. Problem solving session

Understanding Aqueous Dispersibility of Graphene Oxide and Reduced Graphene Oxide through pka Measurements

Chapter 13: Nuclear Magnetic Resonance (NMR) Spectroscopy direct observation of the H s and C s of a molecules

Chapter 20: Identification of Compounds

William H. Brown & Christopher S. Foote

NMR study of complexes between low molecular mass inhibitors and the West Nile virus NS2B-NS3 protease

One-Step Combustion Synthesis of Carbon-Coated Nanoparticles using Multiple-Diffusion Flames

CHEMISTRY 332 FALL 08 EXAM II October 22-23, 2008

CM Chemical Spectroscopy and Applications. Final Examination Solution Manual AY2013/2014

Electronic Supplementary Information (ESI)

Experiment 2 - NMR Spectroscopy

4) protons experience a net magnetic field strength that is smaller than the applied magnetic field.

Smart Functional Nanoenergetic Materials

4) protons experience a net magnetic field strength that is smaller than the applied magnetic field.

Chapter 13 Nuclear Magnetic Resonance Spectroscopy

Module 13: Chemical Shift and Its Measurement

Chapter 13 Spectroscopy

Analysis of NMR Spectra Part 2

Spectroscopy in Inorganic Chemistry. Vibration and Rotation Spectroscopy

Nuclear Magnetic Resonance Spectroscopy: Tools for Structure Determination

Molecular Interactions between Graphene and Biological Molecules

The Final Learning Experience

School of Physical Science and Technology, ShanghaiTech University, Shanghai

In a solution, there are thousands of atoms generating magnetic fields, all in random directions.

PAPER No. 12: ORGANIC SPECTROSCOPY. Module 19: NMR Spectroscopy of N, P and F-atoms

for Brønsted Base-Mediated Aziridination of 2- Alkyl Substituted-1,3-Dicarbonyl Compounds and 2-Acyl-1,4-Dicarbonyl Compounds by Iminoiodanes

Synthesis of condensed polynuclear aromatic resin from furfural extract oil of reduced-pressure route II

22 and Applications of 13 C NMR

Chapter 24. Amines. Based on McMurry s Organic Chemistry, 7 th edition

Raman spectroscopy at the edges of multilayer graphene

Structure Determination: Nuclear Magnetic Resonance Spectroscopy

Chemistry 618B. Spring Midterm Exam I. Prof. Willson T-Th 12:30 2:00. Name (Print as it appears on the Class Roster) Social Security Number

Supporting Information

A Novel Electroless Method for the Deposition of Single-Crystalline Platinum Nanoparticle Films On

CHEMISTRY 213 XMAS 04 1 ANSWER ON THE GREEN COMPUTER ANSWER SHEET PROVIDED USING A PENCIL CHOICES MAY BE USED MORE THAN ONCE

Using NMR and IR Spectroscopy to Determine Structures Dr. Carl Hoeger, UCSD

CSIRO Land & Water, Black Mountain Science and Innovation Park, Acton, ACT 2601, Australia

Polarised Nucleon Targets for Europe, 2nd meeting, Bochum 2005

Transcription:

Supporting Information for A biofunctionalizable ink platform composed of catechol-modified chitosan and reduced graphene oxide/platinum nanocomposite Peter Sobolewski*,1, Agata Goszczyńska 1, Małgorzata Aleksandrzak 2, Karolina Urbaś 2, Joanna Derkowska,3, Agnieszka Bartoszewska 3, Jacek Podolski 3, Ewa Mijowska 2 and Mirosława El Fray 1 Address: 1 Division of Biomaterials and Microbiological Technologies, Faculty of Chemical Technology and Engineering, West Pomeranian University of Technology, Szczecin, 45 Piastów Ave., 70-311 Szczecin, Poland; 2 Nanomaterials Physicochemistry Department, Faculty of Chemical Technology and Engineering, West Pomeranian University of Technology, Szczecin, 45 Piastów Ave., 70-311 Szczecin, Poland and 3 NZOZ Meditest. Diagnostyka Medyczna, Bronisławy 14 D, 71-533, Szczecin, Poland Email: Peter Sobolewski* - psobolewski@zut.edu.pl * Corresponding author Present address: Clinic of Rheumatology, Internal Medicine, and Geriatrics, SPSK Nr. 1, Pomeranian Medical University, Unii Lubelskiej 1, 71-252 Szczecin, Poland Additional experimental data S1

Characterization of the rgo Pt material Figure S1 presents Raman spectra of graphite, graphene oxide (GO), and reduced graphene oxide (rgo) functionalized with Pt nanoparticles (rgo Pt). Three peaks are observed in the spectrum of graphite. The D band at 1311 cm 1, the G band at 1577 cm 1 and the 2D band at 2643 cm 1. The first band is a breathing mode of A 1g symmetry involving phonons near the K zone boundary [1]. The G mode originates from the in-plane vibration of sp 2 -hybridized carbon atoms and is a doubly degenerate phonon mode (E 2g symmetry) at the Brillouin zone center [2]. The 2D band comes from a two-phonon double resonance Raman process [3]. After oxidation treatment the G, D and 2D bands undergo significant changes. The G band becomes broader and up-shifts, as compared to that of graphite (1600 cm 1 ), which may be associated with isolated double bonds resonating at higher frequencies. The higher intensity of the D band in GO Raman spectrum is related with the presence of certain fraction of sp 3 -hybridized carbon atoms because of amorphization of graphite during oxidation process [4]. The 2D band of graphene oxide shifts to 2613 cm 1 and significant decrease in its intensity is observed as a result of oxidation of graphite and formation of material with lower number of graphene layers. It is reported in the literature that after reduction of graphene oxide, the G band shifts back near to the position of the G band in graphite, which is explained as graphitic self-healing [5]. However, in case of the rgo Pt nanocomposite, the G band is apparent at 1596 cm 1, a result of the functionalization with Pt nanoparticles. The high intensity of the D band in the spectrum of rgo Pt corresponds to formation of defects during thermal reduction of graphene oxide and functionalization with Pt nanoparticles. The position, intensity and shape of the 2D band did not change compared to graphene oxide, indicating that number of graphene layers did not change during functionalization process. S2

Figure S1: Raman spectra of graphite, graphene oxide (GO) and rgo Pt nanocomposite. Figure S2 depicts XRD patterns obtained from GO and rgo Pt. The spectrum of GO contains the intense and sharp peak at 2θ = 11.47, corresponding to d-spacing of 0.77 nm (002). The small diffraction peaks at 2θ = 26.7 and 42.7 indicate a short-range order in stacked graphene layers. The pattern for rgo Pt shows a strong reduction of the 11.47 peak intensity, associated with the removal of oxygen-containing functional groups. In addition, few new peaks appeared at around 39.7, 46.3, 67.6, and 81.5, which can be indexed to (111), (200), (220), and (311) reflections of pure Pt with face-centered-cubic (fcc) phase [6]. (111) GO Pt-rGO Counts (002) (200) (220) (311) 10 20 30 40 50 60 70 80 90 2 Theta [degree] Figure S2: XRD patterns of graphene oxide (GO) and rgo-pt nanocomposite. S3

NMR spectroscopy of catechol-modified chitosan 1 H NMR measurements were performed on a TM Bruker DPX 400 spectrometer, operating at 400 MHz, in deuterium oxide (D 2 O) solution at a temperature of 25 C. 1 H NMR (400 MHz, D 2 O) δ 6.75 6.56 (br m, 3H, Ar), 4.05 3.33 (br m, H-3, H-4, H-5, H-6 of GlcN and H-2, H-3, H-4, H-5, H-6 GlcNAc), 3.02 (br s, 1H, H-2 of GlcN), 2.65 (t, J = 7.7 Hz, 2H, -CH 2 CH 2 Ar), 2.48 (t, J = 7.6 Hz, 2H, -CH 2 CH 2 Ar), 1.94 (s, 3H, CH 3 of NHAc). The spectrum (Figure S3) shows the characteristic signal of the protons in the N-acetyl group (GlcNAc) at δ 1.94. The resonances of the ring protons H-3 to H-6 of GlcN and H-2 to H-6 of GlcNAc are present in the middle of the spectrum (δ = 4.05 3.33), forming a group of broad, overlapping signals. The remaining H-2 ring protons of GlcN units are shifted to lower values (δ 3.02). Finally, three hydrogens attached to an aromatic ring of the catechol group appear as a complex multiplet in the region between 6.75 ppm and 6.56 ppm. Additional signals appearing in the region of the spectrum δ = 1.33 0.95 are likely resonances of methyl groups of residual lactate from the starting chitosan oligosaccharide lactate substrate (and/or conjugates). S4

Figure S3: 1 H NMR spectrum of catechol-modified chitosan. The degree of HCA conjugation, defined as the mol % of the chitosan repeating units carrying HCA was calculated from the 1 H NMR spectrum by comparing the relative peak area of the CS-HCA catechol group (3H, aromatic ring proton, δ 6.75 6.56 ppm) and chitosan acetyl group (3H, NHCOOCH 3, δ 1.94 ppm) on a chitosan backbone, taking into account the degree of deacetylation (90%). Oligonucleotide probe design Primer and probe sequences were designed to target a region of the cfb gene of Streptococcus agalactiae, encoding group-b streptococcal CAMP factor. Probe design and specificity were assessed using the BLASTN tool (National Center for Biotechnology Information). Oligonucleotide synthesis was performed by Genomed S. A., with 6-carbon spacer and terminal amine group (C6-NH2). Primers were also prepared for a region of human HBE1 gene, to serve as a negative control. S5

DNA isolation and amplification DNA was extracted from S. agalactiae positive (GBS+) clinical isolates using automated extraction platform, DNA/RNA easymag (Biomerieux). Amplification was conducted using RT-PCR with Cy3- labeled reverse primer for cfb (GBS+ samples) and FastStart Essential mix (Roche). As a negative control, RT-PCR amplification was carried out using Cy3-labeled reverse primer for HBE1, yielding similar amounts of amplicon. Thermal cycle conditions (95 C 15 min; 50 cycles, 60 C 1 min, 72 C 2 sec; 95 C 30 sec, 40 C) and primer concentration were chosen following manufacturer instructions. References 1. Ferrari, A. C.; Robertson, J. Phys. Rev. B 2000, 61, 14095. doi:10.1103/physrevb.61.14095 2. Ni, Z.; Wang, Y.; Yu, T.; Shen, Z. Nano Res. 2008, 1, 273 291. doi:10.1007/s12274-008-8036-1 3. Narula, R.; Reich, S. Phys. Rev. B 2008, 78, 165422. doi:10.1103/physrevb.78.165422 4. Kudin, K. N.; Ozbas, B.; Schniepp, H. C.; Prud homme, R. K.; Aksay, I. A.; Car, R. Nano Lett. 2008, 8, 36 41. doi:10.1021/nl071822y 5. Naebe, M.; Wang, J.; Amini, A.; Khayyam, H.; Hameed, N.; Li, L. H.; Chen, Y.; Fox, B. Sci. Rep. 2014, 4, 4375. doi:10.1038/srep04375 6. Hyde, T. Platinum Met. Rev. 2008, 52, 129 130. doi:10.1595/147106708x299547 S6