Optical Identification of Helical ss-DNA Wrapping on the Nanotube

Slides:



Advertisements
Similar presentations
Aim: How can we explain energy transitions in an atom? Do Now: What were the limitations of the Rutherford model of the atom and how did the Bohr model.
Advertisements

Raman Spectroscopy A) Introduction IR Raman
Apr 13, 2007PHYS General Physics II Applications of Quantum Mechanics.
3.8 Slopes of Parallel and Perpendicular Lines
3.3 Parallel and Perpendicular Lines To Relate Parallel and Perpendicular Lines.
Screening of Water Dipoles inside Finite-Length Carbon Nanotubes Yan Li, Deyu Lu,Slava Rotkin Klaus Schulten and Umberto Ravaioli Beckman Institute, UIUC.
RAMAN SPECTROSCOPY Scattering mechanisms
Molecular Luminescence Spectrometry Chap 15. Three Related Optical Methods Fluorescence Phosphorescence Chemiluminescence } From excitation through absorption.
Photons of Light The smallest unit of light is a photon A photon is often called a particle of light The Energy of an individual photon depends on its.
Advancing electronics and photonics through interdisciplinary research.
Rotational and Vibrational Spectra
Structural and electronic characterization
Advanced Higher Chemistry Unit 1 Spectroscopy. Spectroscopy  Spectroscopy is used to give information regarding the structure of atoms or molecules.
Satish Mohapatra, PhD VP, Engineering & Daniel Loikits President
Carbon Dioxide Clusters and Copper Complexes Formed in Argon Matrices Michael E. Goodrich & David T. Moore Chemistry Department, Lehigh University Bethlehem.
Quantum numbers n principal magnetic l angular momentum spin m1 ms
Christopher Devulder, Slava V. Rotkin 1 Christopher Devulder, Slava V. Rotkin 1 1 Department of Physics, Lehigh University, Bethlehem, PA INTRODUCTION.
Physics Education Department - UNS 1 Planetary model of atom Positive charge is concentrated in the center of the atom (nucleus) Atom has zero net charge:
Physics of light-to-electric-signal conversion in carbon nanotubes PIs: Slava V. Rotkin *, Ivan Biaggio *, Alma E. Wickenden # Alma E. Wickenden # Other.
ROTATIONAL SPECTROSCOPY
Controlled Neutralization of Anions in Cryogenic Matrices by Photodetachment Ryan M. Ludwig, David T. Moore Chemistry Department, Lehigh University Bethlehem,
SIMULTANEOUS COUNTER-ION CO- DEPOSITION: A TECHNIQUE ENABLING MATRIX ISOLATION SPECTROSCOPY STUDIES USING LOW-ENERGY BEAMS OF MASS-SELECTED IONS Ryan M.
Photo-Electronic Modulation of Nafion-gated Single-Walled Carbon Nanotube FETs Happiness Munedzimwe 3, S. V. Rotkin 1,2 1 Physics Department 2 Center for.
Electromagnetic Waves
Notes Over 2.1 Graphing a Linear Equation Graph the equation.
Proving lines parallel Chapter 3 Section 5. converse corresponding angles postulate If two lines are cut by a transversal so that corresponding angles.
Raman Spectroscopy A) Introduction IR Raman
Waves, Light & Quanta Tim Freegarde Web Gallery of Art; National Gallery, London.
1. band structure of pristine SWCNTs abstrac t abstrac t Effect of Helical Perturbation on Exciton Binding Energy in Semiconducting Carbon Nanotubes Benjamin.
atomic excitation and ionisation
Roberto Fuentes Badilla University of Arizona Acknowledgements: Dr. Sumit Mazumdar Dr. Zhendong Wang U.S. N.S.F.
Sep 13, nd NIRT Meeting, DuPontSlava V Rotkin Band structure of single-wall carbon nanotube modulated by DNA wrap Physics Department & Center for.
6.1.2 Energy Levels Photons in / Photons out. Ionization IONIZATION ENERGIES Energy needed to liberate electron from that level. GROUND STATE Lowest possible.
基 督 再 來 (一). 經文: 1 你們心裡不要憂愁;你們信神,也當信我。 2 在我父的家裡有許多住處;若是沒有,我就早 已告訴你們了。我去原是為你們預備地去 。 3 我 若去為你們預備了地方,就必再來接你們到我那 裡去,我在 那裡,叫你們也在那裡, ] ( 約 14 : 1-3)
Geometry Review on Algebra 1
of single-wall nanotube DNA hybrids
ШАПКА DNA-Single Walled Carbon Nanotube Hybrids:
A. Jagota. , M. Zheng#, Y-M. Chiang+, S. V. Rotkin. , C. Kiely
Geometry Today: Check Up 3.4 Instruction Practice
Structural and electronic characterization
أ/عبير السريحي.
Novel Scattering Mechanisms for Nanotube-Silicon Devices
Thermal Interface between Carbon Nanotubes and Polar Materials
Optical Methods to Identify Nanotube-DNA hybrids
'. \s\s I. '.. '... · \ \ \,, I.
Introduction to the coordinate Plane
Day 7 – Parallel and Perpendicular lines
EP324 Applied Optics Topic X ABSORPTION REFLECTION TRANSMISSION
TYPES OF TRANSITIONS: In U.V spectroscopy molecule undergo electronic transition involving σ, π and n electrons. Four types of electronic transition.
Nanotube Fluorescence Spectroscopy
Слайд-дәріс Қарағанды мемлекеттік техникалық университеті
Geometry 3-6 Parallel and Perpendicular Lines
Raman Spectroscopy A) Introduction IR Raman
.. -"""--..J '. / /I/I =---=-- -, _ --, _ = :;:.
II //II // \ Others Q.
I1I1 a 1·1,.,.,,I.,,I · I 1··n I J,-·
' '· \ ·' ,,,,
Volume by Cross-sectional Areas A.K.A. - Slicing
Graphing.
3.5 Parallel and PerpendicularLines in the Coordinate Plane
Warm Up Graph the pre-image and image of ΔABC with vertices A(4, 0), B(2, -1) and C(-1, 2) that is translated along vector 2. Graph the lines:
Atomic emission spectrum
3.5 Energy levels and spectra
Chapter – 8 Fluorescence
Synthesis and Characterization of Novel Donor/Acceptor
. '. '. I;.,, - - "!' - -·-·,Ii '.....,,......, -,
Atomic Spectra Imaging Science Fundamentals

Raman Spectroscopy A) Introduction IR Raman

Presentation transcript:

Optical Identification of Helical ss-DNA Wrapping on the Nanotube Slava V. Rotkin, Physics Department and Center for Advanced Materials and Nanotechnology, Lehigh University, Bethlehem, PA 18015 Small v.4, p.1284-6, Aug 2008 AR of PhysChem, v.61, 2010 in perp polarization (vertical energy axis): new line appears at much lower energy in II polarization: the line shift Eg= E11=1.43 eV Egpert = 1.33 eV 3D view of the hybrids 3.5 2.5 1.5 Bare [7,0] tube DNA-wrapped tube Perp. Absorption Energy (eV) Parallel Emission Energy (eV) 0.8 1.8 2.8 Lifting of the optical selection rules changes the spectrum qualitatively: Old transitions in the perpendicular polarization are present (but shifted); new ones appear that are prohibited for the pristine nanotube.