Acousto-Optic Filters McCreery, R. L., Raman Spectroscopy for Chemical Analysis, 3rd ed., Wiley, New York: 2000 Wavelength tuning over entire Raman shift.

Slides:



Advertisements
Similar presentations
Bragg’s Law nl=2dsinΘ Just needs some satisfaction!! d Θ l
Advertisements

Electron Diffraction - Introduction Electron diffraction is an important method to characterize materials. The textbook, Transmission Electron Microscopy,
CAVITY RING DOWN SPECTROSCOPY
Microscopy Outline 1.Resolution and Simple Optical Microscope 2.Contrast enhancement: Dark field, Fluorescence (Chelsea & Peter), Phase Contrast, DIC 3.Newer.
1. If this standing wave is 3.2 m long, what is the wavelength? (2.56 m)
TeO2 Polarizing Optics – Glan Prisms. Company "Elent A/Elent Technics" has more than 20 years experience in manufacturing and processing of TeO 2 crystals.
Raman Spectroscopy 1923 – Inelastic light scattering is predicted by A. Smekel 1928 – Landsberg and Mandelstam see unexpected frequency shifts in scattering.
Dual Acousto-Optical Tunable Filter (AOTF) University of California Irvine David Tseng Mentor: Rong Huang PI: Professor Henry Lee.
Sergey Kucheryavski Raman spectroscopy Acquisition, preprocessing and analysis of spectra.
Exam II Review. Review of traveling wave interference Phase changes due to: Optical path length differences sources out of phase General solution.
Raman Spectroscopy 1923 – Inelastic light scattering is predicted by A. Smekel 1928 – Landsberg and Mandelstam see unexpected frequency shifts in scattering.
Raman Spectroscopy 1923 – Inelastic light scattering is predicted by A. Smekel 1928 – Landsberg and Mandelstam see unexpected frequency shifts in scattering.
Fiber-Optic Communications James N. Downing. Chapter 2 Principles of Optics.
Chapter 38 Serway & Beichner 6 th Ed.. Fig 38-4a, p.1207 Diffraction.
Lecture 5 An Introduction to Spectroscopy Electromagnetic radiation, electromagnetic wave Emission, absorption, fluorescence.
Stimulated Raman scattering If high enough powered radiation is incident on the molecule, stimulated Anti-Stokes radiation can be generated. The occurrence.
Raman Spectroscopy 1923 – Inelastic light scattering is predicted by A. Smekel 1928 – Landsberg and Mandelstam see unexpected frequency shifts in scattering.
Neodymium:YAG Laser Nd3+ in yttrium-aluminum-garnet (Y3Al5O12)
Common types of spectroscopy
What is spectroscopy? It is the study of how matter interacts with electromagnetic radiation (gamma rays down to radio waves) Matter can interact with.
Acousto optic modulators Additional details relevant for servos.
Ability to probe living tissue with subcellular resolution enable the visualization of morphological details in tissue that can not be resolved by ultrasound.
Vibrating Strings and Resonance in Air Columns. String Instruments  In many musical instruments, the source sets a string into vibration  Standing waves.
1 Optic Rotation Project I Doppler-free saturated absorption spectrum Lei Huang Department of Physics and Astronomy SUNY at Stony Brook May. 4 th, 2005.
The Nobel Prize in Physics 1930 "for his work on the scattering of light and for the discovery of the effect named after him" Sir Chandrasekhara Venkata.
Fukuoka Univ. A. Nishiyama, A. Matsuba, M. Misono Doppler-Free Two-Photon Absorption Spectroscopy of Naphthalene Assisted by an Optical Frequency Comb.
Raman Spectroscopy Lord Rutherford, 1930 April 10th, 2014.
J.R.Krenn – Nanotechnology – CERN 2003 – Part 3 page 1 NANOTECHNOLOGY Part 3. Optics Micro-optics Near-Field Optics Scanning Near-Field Optical Microscopy.
WAVES Wave motion allows a transfer of energy without a transfer of matter.
IPC Friedrich-Schiller-Universität Jena 1 ASP_MP_S2j Biophotonics Prof. Dr. Rainer Heintzmann Institut für Physikalische Chemie Friedrich-Schiller-Universität.
IPC Friedrich-Schiller-Universität Jena 1 ASP_MP_S2j Biophotonics Prof. Dr. Rainer Heintzmann Institut für Physikalische Chemie Friedrich-Schiller-Universität.
Acousto-Optic Modulators
Accelerating Science Improving Environment and Efficiency Meeting Tomorrow’s Medical Challenges.
SEM- Schematic Overview. Electron Detection Tungsten Filament Electron Source.
Chapter 3 Lattice vibration and crystal thermal properties Shuxi Dai Department of Physics Unit 4 : Experimental measurements of Phonons.
Spectra. White Light Light from many colors mixes to form white light. Different colors have different wavelengths. Shorter wavelengths bend more through.
5.1 Electromagnetic Radiation. Wave motion The transfer of energy without matter is called wave motion Two Types.
PHYSICS CLASS ACTIVITY. CLASS ACTIVITY: TUNING FORK FREQUENCY.
Chapter 24 Physics A First Course Light and Optics.
Near Field Scanning Optical Microscopy (NSOM, SNOM, NFOM) Stephanie Pruzinsky Group Meeting, June 6, 2002.
라만 의 원리와 그의 응용 (Normal,SERS,TERS)
Bruno De Fanti Anel EE230 University of California, Santa Cruz December 2011 LASER SCANNING CONFOCAL MICROENDOSCOPY.
0 Frequency Gain 1/R 1 R 2 R 3 0 Frequency Intensity Longitudinal modes of the cavity c/L G 0 ( ) Case of homogeneous broadening R2R2 R3R3 R1R1 G 0 ( )
Spectroscopy Utilizes the various regions of the electromagnetic spectrum to detect signal.
RAMAN EFFECT.
Ch25 Modern Optics and Matter Waves
Research stoichiometric of heterogeneity of lithium niobate crystals by IR spectroscopy Paranin V.D., Pantelei E.
X-ray spectroscopy Repetition, exercises and more
Ch25 Modern Optics and Matter Waves
3.3 Other types of microscopy
Electromagnetic Spectrum Project
Near-Field Optical Microscopy
Introduction - characterization of materials.
P.J. Caspers, G.W. Lucassen, G.J. Puppels  Biophysical Journal 
Unit 8: Light and Optics Chapter 23: The Physical Nature of Light
Geometrical Optics (Chapter 2)
Radio Astronomy.
Diffraction Diffraction is the spreading out of a wave as it goes passed an obstacle or through an aperture When the wavelength is small compared to the.
Chapter 3-1 Notes: The Electromagnetic Spectrum
Scalar theory of diffraction
Jana Humpolíčková, Aleš Benda, Jörg Enderlein  Biophysical Journal 
5.2 Properties of Light Our goals for learning What is light?
Diffraction Grating calculation of light wavelength
Properties of traveling waves: Acoustics applications
Volume 90, Issue 2, Pages (January 2006)
OCT (Optical Coherence Tomography) Time domain Frequency domain Coherence length.
Properties of Waves Part 2.
P.J. Caspers, G.W. Lucassen, G.J. Puppels  Biophysical Journal 
Anran Li, Jie Lin, Zhongning Huang, Xiaotian Wang, Lin Guo  iScience 
Presentation transcript:

Acousto-Optic Filters McCreery, R. L., Raman Spectroscopy for Chemical Analysis, 3rd ed., Wiley, New York: 2000 Wavelength tuning over entire Raman shift range. Wavelength tuning over entire Raman shift range. TeO 2 crystal is excited acoustically with ultrasonic generator. => Standing wave pattern acts as diffraction grating. TeO 2 crystal is excited acoustically with ultrasonic generator. => Standing wave pattern acts as diffraction grating. Spectrum is scanned by changing ultrasonic frequency in less than 1 s over 0 to 3500 cm -1 shift range. Spectrum is scanned by changing ultrasonic frequency in less than 1 s over 0 to 3500 cm -1 shift range.

Acousto-optic Tunable Filter

Confocal Microscopy Optics McCreery, R. L., Raman Spectroscopy for Chemical Analysis, 3rd ed., Wiley, New York: 2000

Confocal Aperture and Field Depth McCreery, R. L., Raman Spectroscopy for Chemical Analysis, 3rd ed., Wiley, New York: 2000 a nd McCreery, R. L., Raman Spectroscopy for Chemical Analysis, 3rd ed., Wiley, New York: 2000 a nd

Confocal Aperture and Field Depth McCreery, R. L., Raman Spectroscopy for Chemical Analysis, 3rd ed., Wiley, New York: 2000