Spectroscopy of Hybrid Inorganic/Organic Interfaces Vibrational Spectroscopy Dietrich RT Zahn.

Slides:



Advertisements
Similar presentations
Spectroscopy of Hybrid Inorganic/Organic Interfaces Electron Spectroscopy Dietrich RT Zahn.
Advertisements

On the Differences between SERS and Infrared Reflection Absorption Spectra of CO 2 on Cold-deposited Copper M.Lust, A.Pucci,Universität Heidelberg A.Otto,
Raman Spectroscopy A) Introduction IR Raman
FTIR Spectroscopy of Small Titanium-Carbides A Survey and Preliminary Results Robin Kinzer TCU Molecular Physics Laboratory 31 October 2005.
Raman Spectroscopy 1923 – Inelastic light scattering is predicted by A. Smekel 1928 – Landsberg and Mandelstam see unexpected frequency shifts in scattering.
Raman Spectroscopy Laser 4880 Å. Raman Spectroscopy.
RAMAN SPECTROSCOPY Scattering mechanisms
Surface-Enhanced Raman Scattering (SERS)
Surface Enhanced Infrared Absorption (SEIRA) Spectroscopy
Raman Spectroscopy 1923 – Inelastic light scattering is predicted by A. Smekel 1928 – Landsberg and Mandelstam see unexpected frequency shifts in scattering.
Raman Spectroscopy Laser 4880 Å. Raman Spectroscopy.
Raman Spectroscopy and Thin Films Alexander Couzis ChE5535.
Raman Spectroscopy 1923 – Inelastic light scattering is predicted by A. Smekel 1928 – Landsberg and Mandelstam see unexpected frequency shifts in scattering.
Lecture 3 INFRARED SPECTROMETRY
Mustafa KUMRU Fatih University, Faculty of Arts and Sciences, Physics Department, Büyükçekmece, Istanbul.
Raman Spectroscopy: Introductory Tutorial
Time out—states and transitions Spectroscopy—transitions between energy states of a molecule excited by absorption or emission of a photon h =  E = E.
STRUCTURAL CHANGES STUDIES OF a-Si:H FILMS DEPOSITED BY PECVD UNDER DIFFERENT HYDROGEN DILUTIONS USING VARIOUS EXPERIMENTAL TECHNIQUES Veronika Vavruňková.
Surface Enhanced Raman Spectroscopy (SERS) Jeanne Bonner PHYS 275 November 26, 2007.
Observation of magnetic domains in LSMO thin films by XMCD-PEEM M. Oshima A, T. Taniuchi A, H. Kumigashira A, H. Yokoya B, T. Wakita C, H. Akinaga D, M.
 PART Requirements for Spectroscopic Techniques for Polymers 1. High resolution 2. High sensitivity (>1%) 3. High selectivity between molecular.
High resolution studies of the 3 band of methyl fluoride in solid para-H 2 using a quantum cascade laser A.R.W. McKellar *, Asao Mizoguchi, Hideto Kanamori.
Raman scattering of a single freestanding rolled up SiGe/Si tube R. Songmuang and O. G. Schmidt Max-Planck-Institut für Festkörperforschung Stuttgart,
Optical Characterization of GaN-based Nanowires : From Nanometric Scale to Light Emitting Devices A-L. Bavencove*, E. Pougeoise, J. Garcia, P. Gilet, F.
Gilad Haran Chemical Physics Department Weizmann Institute of Science Charge-transfer effects in Raman Scattering of Individual Molecules FRISNO, EIN-BOKEK,
Spectroscopy of Hybrid Inorganic/Organic Interfaces Transport Properties Dietrich RT Zahn.
FTIR Spectroscopy of the n4 bands of 14NO3 and 15NO3
Photoacoustic Spectroscopy of Surface Defects States of Semiconductor Samples 1) M.Maliński, 2) J.Zakrzewski, 2) F.Firszt 1) Department of Electronics.
Atomic Scale Understanding of the Surface Intermixing during Thin Metal Film Growth 김상필 1,2, 이승철 1, 정용재 2, 이규환 1, 이광렬 1 1 한국과학기술연구원, 계산과학센터 2 한양대학교, 재료공학부.
Advanced Analytical Chemistry – CHM 6157® Y. CAIFlorida International University Updated on 9/18/2008Chapter 5Raman Spectrometry Chapter 5 Raman Spectrometry.
States and transitions
Andrew Durgan Department of Chemistry & Biochemistry Gonzaga University September 24, 2009.
日 期: 指導老師:林克默、黃文勇 學 生:陳 立 偉 1. Outline 1.Introduction 2.Experimental 3.Result and Discussion 4.Conclusion 2.
W I S S E N T E C H N I K L E I D E N S C H A F T  Januar 13 Name und OE, Eingabe über > Kopf- und Fußzeile.
Resonant SFG Line Shapes on Single Crystal Surfaces Scott K. Shaw, A. Laguchev, D. Dlott, A. Gewirth Department of Chemistry University of Illinois at.
Raman Spectroscopy A) Introduction IR Raman
LASER PHOTODISSOCIATION SPECTRA OF THE ANILINE-ARGON CATIONIC CLUSTER IN THE NEAR INFRARED T. PINO, S. DOUIN, Ph. BRECHIGNAC Laboratoire de Photophysique.
Infrared Spectra of Chloride- Fluorobenzene Complexes in the Gas Phase: Electrostatics versus Hydrogen Bonding Holger Schneider OSU International Symposium.
Application of optical techniques for in situ surface analysis of carbon based materials T. Tanabe, Kyushu University Necessity of development of (1) in-situ.
70th ISMS Vibration-Rotation Analysis of the 13 CO 2 Asymmetric Stretch Fundamental Band in Ambient Air for the Physical Chemistry Teaching Laboratory.
György Tarczay, Gábor Magyarfalvi
Ion Beam Analysis of the Composition and Structure of Thin Films
Ch 10 Pages ; Lecture 24 – Introduction to Spectroscopy.
Mineral Spectroscopy Visible Infrared Raman Mössbauer NMR.
EXAMPLE THE SPECTRUM OF HCl SHOWS A VERY INTENSE ABSORPTION BAND AT 2886 cm -1 AND A WEAKER BAND AT 5668 cm -1. CALCULATE x e, ṽ o, THE FORCE CONSTANT.
Hydrogen-bond between the oppositely charged hydrogen atoms It was suggested by crystal structure analysis. A small number of spectroscopic studies have.
Main Title Manori Perera 1 and Ricardo Metz University of Massachusetts Amherst 64 th International Symposium on Molecular Spectroscopy June 25th, 2009.
Tao Peng and Robert J. Le Roy
Electron-phonon coupling in alpha-hexathiophene single crystals
Infrared Spectra of Anionic Coinage Metal-Water Complexes J. Mathias Weber JILA and Department of Chemistry and Biochemistry University of Colorado at.
1 The r 0 Structural Parameters of Equatorial Bromocyclobutane, Conformational Stability from Temperature Dependent Infrared Spectra of Xenon Solutions,
O. PIRALI, J. OOMENS, N. POLFER FOM Rijnhuizen, 3439MN Nieuwegein, The Netherlands Y. UENO, R. MABOUDIAN Department of Chemical Engineering, U.C. Berkeley,
A. Nishiyama a, K. Nakashima b, A. Matsuba b, and M. Misono b a The University of Electro-Communications b Fukuoka University High Resolution Spectroscopy.
Thermal annealing effect of tetrahedral amorphous carbon films deposited by filtered vacuum arc Youngkwang Lee *†,Tae-Young Kim*†, Kyu Hwan Oh†, Kwang-Ryeol.
Raman spectroscopy.
1 Scattering of Light: Raman Spectroscopy Deanna O’Donnell Informal P-Chem Review June 4 th, 2009.
Surface-Enhanced Raman Scattering (SERS)
기계적 변형이 가능한 능동 플라즈모닉 기반 표면증강라만분광 기판 Optical Society of Korea Winter Annual Meting 강민희, 김재준, 오영재, 정기훈 바이오및뇌공학과, KAIST Stretchable Active-Plasmonic.
Intramolecular charge transfer (ICT) in two phenylpyrrol derivatives: PP and PBN Two similar molecules but a different behavior Danielle Schweke Baumgertan.
Strong infrared electroluminescence from black silicon
FORMATION OF CO-CRYSTAL AND CHARACTRIZATION OF ASPIRIN WITH CITRIC ACID AND PERCHLORIC ACID C.Muthuselvi.M.Sc.,M.Phil., Assistant.
Advertisement.
Optical band gaps from tetrahedral cation vacancy and variation of cation ordering in NCO films Weiwei Zhao.
Molecular Mechanism of Hydrogen-Formation in Fe-Only Hydrogenases
Raman Spectroscopy A) Introduction IR Raman
Lecture 8: Volume Interactions
Charge-transfer effects in Raman Scattering of Individual Molecules
Instrumental Analysis
Computation of Harmonic and Anharmonic Vibrational Spectra
Raman Spectroscopy A) Introduction IR Raman
Presentation transcript:

Spectroscopy of Hybrid Inorganic/Organic Interfaces Vibrational Spectroscopy Dietrich RT Zahn

The Application of Raman Spectroscopy in the DIODE Project The Overall Device Performance (iv) The Interface between the Organic Molecules and the Metal GaAs(100) Organic Interlayer Metal V I (iii) The Organic Molecular Film (ii) The Interface between GaAs Substrate and Organic Molecules (i) The GaAs Substrate Surface

Molecular Vibrational Properties DiMe-PTCDI: 3,4,9,10- Perylenetetracarboxylic diImide PTCDA: 3,4,9,10- Perylenetetracarboxylic diAnhydride C24H8O6 C26H14O4N2 Symmetry D2h Raman active: 19Ag+18B1g+10B2g+7B3g IR active: +10B1u+18B2u+18B3u Silent: + 8Au 108 internal vibrations C2h 44Ag+22Bg +23Au+43Bu + 8Au 132 internal vibrations Monoclinic crystallographic system in thin films: PTCDA: - and -phases: S. R. Forrest, Chem. Rev. 97 (1997), 1793. DiMe-PTCDI: Cambridge Structural Database.

Raman-active vibrations of PTCDA (C24H8O6): Effect of crystal formation 2-fold Davydov Splitting internal molecular modes: external molecular modes (phonons): C- C- O Bg C-H C-C Symmetry: D2h C2h (monoclinic) 6 rotational vibrations: 3Ag+3Bg 19Ag+18B1g+10B2g+7B3g Ag

Vibration modes of PTCDA molecule C-O Bg C-H C-C 19 Ag breathing modes very good agreement between experimental and calculated frequencies !

Raman Spectra of a PTCDA Crystal x0.1 assignment of modes and their relative atomic contribution using Gaussian `98 (B3LYP, 3-21G)

Ag Raman Modes of PTCDA with In x0.1

Raman Spectra of a PTCDA Crystal x0.5 C=O ring C-H and a DiMe-PTCDI x0.1 assignment of modes and their relative atomic contribution using Gaussian `98 (B3LYP:3-21G).

Raman Spectra of a PTCDA Crystal and a DiMe-PTCDI assignment of modes and their relative atomic contribution using Gaussian `98 (B3LYP:3-21G). Raman shift /cm-1

Raman-active vibrations of PTCDA: Effect of crystal formation external molecular modes (phonons): 6 rotational vibrations: 3Ag+3Bg Symmetry: C2h (monoclinic) Bg Ag Bg

Infrared Modes in Films on S-GaAs C-H+ C-N-C Reflection, s-polarized light. C=O C-O+ C-C ring C-O-C C-H (oop) Assignment of modes using Gaussian `98 (B3LYP, 3-21G).

Sample Preparation Epi-ready GaAs (100) Degreasing Acetone, Ethanol, Di-Water OMBD deposition: PTCDA, DiMe-PTCDI Thickness: 0.1 nm ÷15 nm Wet Chemical Treatment S2Cl2:CCl4=1:3 (10 sec) Rinsing (CCl4, Acetone, Ethanol, Di-Water) Metal deposition: Ag, In Thickness: 0.1 nm ÷260 nm Annealing at 620 K, 30 min S-GaAs(100):2x1

Ex Situ (Micro-) and In Situ (Macro- Configuration) Raman Spectroscopy Ar+ line Dilor XY 800 Spectrometer Monochromatic light source: Ar+ Laser (2.54eV), Detector: CCD resonance condition with the absorption band of the organic crystalline material. resolution: 1.2 cm-1 to 3.5 cm-1.

Monitoring of PTCDA Film Growth on S-GaAs E = 2.54 eV M. Ramsteiner et al., Appl. Opt. 28 (18) (1989), 4017. The relative intensity of internal modes does not change upon deposition. weak interaction of the molecules with the S-passivated substrate. Phonons are well resolved as soon as 20 nm of PTCDA are deposited.

Chemistry at Organic/S-GaAs(100):2x1 Vibrational Properties: PTCDA Annealing at 623 K for 30 min: Molecules remaining at the surface: NPTCDA(0.04nm)~1013 cm-2 NdSi ~ 1012 cm-2 Spectrum of annealed film similar to that of an annealed PTCDA film on Si(100). The strongest interaction: between the PTCDA molecules and defects due to Si at the GaAs surface. 0.45 nm (x 0.6) 0.18 nm ann. x 4.4 40 nm x 0.01

Calculated Vibrational Properties: PTCDA

Calculated Vibrational Properties: PTCDA Molecular charging with one elementary charge: significant spectral changes predicted for the C=C modes around 1600 cm-1 fractional charge transfer between the PTCDA and the defects at the GaAs surface.

In Situ Raman: Monitoring of Indium Deposition onto PTCDA (15 nm) /28 /10 /58 /13 /33 /5 /0.7 /1.5

Influence of Indium on Vibrational Spectra of PTCDA

Influence of Indium on Vibrational Spectra of PTCDA organic films grown on S-GaAs(100):2x1 reflection measurements at 20° incidence. all PTCDA modes are preserved in the spectrum of In/PTCDA. observation of C=O modes (around 1730-1770cm-1) In does not react with the O of PTCDA !

Indium/PTCDA: Separation of Chemical and Structural Properties In: 0 100 nm In: 1 nm/min PTCDA ~0.4 nm (~1 ML) S-GaAs(100) ~15 nm (~50ML)

Comparison of Indium and Silver Deposition on PTCDA and DiMe-PTCDI In: 1 nm/min Ag:1.6 ÷ 5.5 nm/min

Comparison of Indium and Silver Deposition on PTCDA and DiMe-PTCDI the PTCDA external modes: are preserved broadened after 0.3 nm Ag deposition. disappear after 0.4 nm In. the DiMe-PTCDI external modes: less affected compared to PTCDA. probably due to less compact crystalline structure.

Mg, In, Ag on PTCDA

Mg, In, Ag on DiMe-PTCDI +Mg

Indium and Silver Deposition: Enhancement Factors PTCDA (15 mn) DiMe-PTCDI (15 nm)

Determination of Molecular Orientation: DiMe-PTCDI  =0°: x II [011]GaAs =90°: x II [0-11] phonons phonons Azimuthal rotation of a 120 nm thick film; normal incidence. Periodic variation of signal in crossed and parallel polarization. M. Friedrich, G. Salvan, D. Zahn et al., J. Phys. Cond. Mater. submitted.

Determination of Molecular Orientation: DiMe-PTCDI Breathing mode at 221 cm-1 Good agreement with IR and NEXAFS results

Molecular Orientation with respect to GaAs substrate: PTCDA:  ~ 9° 

 [-110]  DiMe-PTCDI:  ~ 6°  ~ 60°

Raman Characterization of Organic Thin Films: Achievements and Outlook Interface reactions Internal Modes: Shifts, Intensities Film thickness Intensity modulations Crystalline Order Growth Mode Crystallinity Occurrence of Phonon-like Modes, FWHM Crystal modifications Phonons, Davydov Splitting of Internal Modes Orientation Further investigations

Raman Spectroscopy Team: