Quantum Dots (DQ) Imaging for Thermal flow studies

Size: px
Start display at page:

Download "Quantum Dots (DQ) Imaging for Thermal flow studies"

Transcription

1 AerE 545 class notes #43 Quantum Dots (DQ) Imaging for Thermal flow studies Hui Hu Department of Aerospace Engineering, Iowa State University Ames, Iowa 511, U.S.A

2 Quantum Dots Quantum dots are chemically synthesized semiconductor nanoparticles that can exhibit unique quantum confinement behavior. Size dependent emission: Smaller particles emit high-energy (shorter wavelength) radiation Larger particles emit low-energy (longer wavelength) radiation. Adjustable hydrophilic or hydrophobic properties: The surface layer can be designed to be either hydrophilic or hydrophobic allowing the nanoparticles to be solubilized in a variety of liquids (i.e. polar and nonpolar). The structure of a (CdSe)ZnS quantum dot 2.3nm 5.5nm

3 Introduction The propose of the present study is to explore the possibility of Quantum dots (QDs)) for thermofluid diagnostics. Compared to commonly-used fluorescent dyes such as Fluorescein and Rhodamine B, the photophysical properties of (CdSe)ZnS( QDs will be investigated: Absorption and emission spectra. Stability against photobleaching under different laser excitations. Temperature sensitivity under different laser excitations. The applications of QDs for thermofluid diagnostics Individual QDs as particle tracers for velocimetry in micro flows: Single Quantum Dot (QD) Velocimetry by Pouya et al. Experiments in Fluids, 26. QDs as fluorescent tracers: Flow visualization and concentration c measurements in a pulsed jet flow. Temperature distribution mapping in a stratified flow.

4 Absorption and Emission Spectra of (CdSe)ZnS Quantum Dots Absorption spectrum: wide range of absorption various laser can be used as excitation source Emission spectrum: emission peak wavelength is adjustable by controlling the size of QDs emission spectrum is symmetrical to the emission peak emission concentrates near emission peak with FWHM only 3~4 nmn Quantum Dots QD-1 QD-2 QD-3 QD-4 Emission Peak 57 nm 593 nm 63 nm 65 nm Emission Full-Width Half-Maximum 33 nm 34 nm 36 nm 4 nm absorption (relative intensity) absorption QD-1 emission QD-2 QD wavelength (nm) QD emission (relative intensity)

5 QD imaging for flow velocity measurements Image of 6 nm (CdSe)ZnS( quantum dots in aqueous solution within 1 nm of the surface. Field of view is 153 lm 93 lm Taken from Single quantum dot (QD) imaging of fluid flow near surfaces By Shahram Pouya Æ Manoochehr Koochesfahani Preston Snee, Moungi Bawendi, Daniel Nocera, Experiments in Fluids (25) 39: Superposition of four consecutive frames showing the movement of two single QDs appearing in three frames. Mean flow is from left to right. Field of view is 37 lm 37 lm

6 Photophysical stability against photobleaching Same volume (2ml) of QD, Fluorescein and Rhodamine B solutions were prepared. Concentration of the Fluorescein and Rhodamine B aqueous solution is M. The solvent of QD is Hexane. The absolute molar concentration of QD is unknown, but it has the e same initial fluorescence emission intensity as the Rohdamine B M solution. mirror optics laser beam CCD camera stirring rod excitation laser test solution digital delay generator (SRS DG535) host computer Experimental setup for the photoluminescence p stability test

7 Photoluminescence stability against photobleaching (Comparison of QD with Fluorescein and Rhodamine B) excitation laser source: pulsed excimer UV laser (38nm ) Normalized fluorescence intensity QD 4 - laser energy: 2mJ/pulse QD 4 - laser enrgy: 15mJ/pulse Rhodamine B - laser energy: 2mJ/pulse Rhodamine B - laser energy: 15mJ/pulse Rhodamine B - laser energy 1mJ/ulse Fluorescein - laser energy: 2mJ/pulse Fluorescein - laser energy 15mJ/pulse Fluorescein - laser energy 1mJ/pulse Number of laser pulse Normalized Fluorescence intensity QD 4 (laser power 2mJ/pulse) QD 4 (laser power 15mJ/pluse) Flourescein (laser power 2mJ/pulse) Fluorescein (laser power 15mJ/pulse) Fluorescein ( laser pulser 1mJ/pulse) Rhodamine B( laser power 2mJ/pluse) Rhodamine B (Laser power 15mJ/pulse) Rhodamine B (laser Power 1mJ/pulse) Total enegy input from the exicitation laser (J)

8 Photoluminescence stability against photobleaching (Comparison of QD with Fluorescein and Rhodamine B) excitation laser source: Argon-ion laser (514.5 nm ) Normalized fluorescence intensity QD-4 (laser power 1.5w) Rhodamine B (laser power 1.w) Rhodamine B (laser power 1.5w) Flourescein (laser power 1.5 W) Flourescein (laser power 1. W) Normalized fluorescence intensity QD-4 (laser power 1.5w) Rhodamine B (laser power 1.w) Rhodamine B (laser power 1.5w) Flourescein (laser power 1.5 W) Flourescein (laser power 1. W) Excitation time (second) Total input energy from the excitation laser (J)

9 Temperature Sensitivity Test mirror RTD probe laser sheet optics 12-bit gated intensified CCD camera (DiCam-Pro) stirring rod Excitation laser QD solution digital delay generator (SRS DG535) heating plate host computer Experimental setup for temperature sensitivity test

10 Temperature sensitive of QD, Fluorescein and Rhodamine B Normalized fluorescence intensity QD Rhodamine B Fluorescein QD-3 (514nm) QD-3 (488nm) QD-3 (38nm) Normalized fluorescence intensity Rhodamine B (514nm) Rhodamine B (488nm) Rhodamine B (38nm) Normalized fluorescence intensity Fluorescein (514nm) Fluorescein (488nm) Fluorescein (38nm) Temperature ( o C) Temperature ( o C) Temperature ( o C) 38nm Excimer laser 488nm Argon-ion laser 514nm Argon-ion laser QD % per C (5 C ~ 65 C) -4% per C (5 C ~ 65 C) -1.5% per C (5 C ~ 65 C) Rhodamine B -1.57% per C (5 C ~ 65 C) -% per C (5 C ~ 65 C) Kim & Khim (21) % per C (15 C ~ 4 C) -1.52% per C (5 C ~ 65 C) Coppeta & Roger(1998) % per C (2 C ~ 6 C) Fluorescein -.45% per C (5 C ~ 65 C) -.25% per C (5 C ~ 65 C) Coppeta & Roger(1998) -.16 % per C (2 C ~ 6 C) +2.25% per C (5 C ~ 65 C) Coppeta & Roger(1998) % per C (2 C ~ 6 C)

11 Applications of Quantum Dots for Thermofluid Diagnostics: (Flow visualization and quantitative concentration measurements) burette QD-3 solution mirror optics Laser sheet CCD Camera Argon-ion Laser ( wavelength = 514.4nm) Experimental setup host computer

12 Application Quantum Dots for Thermofluid Diagnostics: (Flow visualization and quantitative concentration measurements) concentration. 1. a. t = t b. t = t +.2 s c. t = t +.4 s

13 Application Quantum Dots for Thermofluid Diagnostics (Temperature measurements in a Stratified Flow) 5mm QD-3 3 solution (temperature is 23 o C at t = s) mirror optics Ambient temperature amb = 23 o C) (T amb Laser sheet Y test cell (made from glass) 1mm CCD Camera X Argon-ion Laser ( wavelength = 514.4nm) Chilled plate (T( surface =. O C) Coolant flow in Heat exchanger Coolant flow out host computer

14 Application Quantum Dots for Thermofluid Diagnostics (Temperature measurements in a Stratified Flow) Ymm Temperature ( o C) Ymm Temperature ( o C) Ymm Temperature ( o C) Xmm Xmm 1 minute later 5 minutes later 1 minutes later Xmm Ymm Temperature ( o C) Ymm Temperature ( o C) Ymm Temperature ( o C) Xmm Copyright by Dr. Hui Xmm Xmm 15 minutes later Iowa State University. All Rights Reserved! 2 minutes later 3 minutes later

15 Application Quantum Dots for Thermofluid Diagnostics (Temperature profiles in the center of the test cell) 65 Ymm Temperature ( o C) Xmm Distance away from the bottom plate (mm) t = 1 minute t = 5 minutes t = 1 minutes t = 15 minutes t = 2 minutes t = 25 minutes t = 3 minutes Temperature ( o C) Temperature profiles along the vertical line in the center of the test cell.

Laser Induced Fluorescence (LIF) Technique Part - 3

Laser Induced Fluorescence (LIF) Technique Part - 3 AerE 545 class notes #37 Laser Induced Fluorescence (LIF) Technique Part - 3 Hui Hu Department o Aerospace Engineering, Iowa State University Ames, Iowa 500, U.S.A Introduction Instantaneous, quantitative,

More information

FLOW VISUALIZATION AND SIMULTANEOUS VELOCITY AND TEMPERATURE MEASUREMENTS IN THE WAKE OF A HEATED CYLINDER

FLOW VISUALIZATION AND SIMULTANEOUS VELOCITY AND TEMPERATURE MEASUREMENTS IN THE WAKE OF A HEATED CYLINDER TH INTERNATIONAL SYMPOSIUM ON FLOW VISUALIZATION August -,, University of Notre Dame, Notre Dame, Indiana, USA FLOW VISUALIZATION AND SIMULTANEOUS VELOCITY AND TEMPERATURE MEASUREMENTS IN THE WAKE OF A

More information

Detection of toxic mercury ions using a ratiometric CdSe/ZnS nanocrystal sensor

Detection of toxic mercury ions using a ratiometric CdSe/ZnS nanocrystal sensor Supporting Information for Detection of toxic mercury ions using a ratiometric CdSe/ZnS nanocrystal sensor Leah E. Page, Xi Zhang, Ali M. Jawaid, and Preston T. Snee * Department of Chemistry, University

More information

Chapter 6 Photoluminescence Spectroscopy

Chapter 6 Photoluminescence Spectroscopy Chapter 6 Photoluminescence Spectroscopy Course Code: SSCP 4473 Course Name: Spectroscopy & Materials Analysis Sib Krishna Ghoshal (PhD) Advanced Optical Materials Research Group Physics Department, Faculty

More information

SIMULTANEOUS VELOCITY AND CONCENTRATION MEASUREMENTS OF A TURBULENT JET MIXING FLOW

SIMULTANEOUS VELOCITY AND CONCENTRATION MEASUREMENTS OF A TURBULENT JET MIXING FLOW Proceedings of International Symposium on Visualization and Image in Transport Phenomena, Turkey, -9 Oct. SIMULTANEOUS VELOCITY AND CONCENTRATION MEASUREMENTS OF A TURBULENT JET MIXING FLOW Hui HU a, Tetsuo

More information

Simultaneous Velocity and Concentration Measurements of a Turbulent Jet Mixing Flow

Simultaneous Velocity and Concentration Measurements of a Turbulent Jet Mixing Flow Simultaneous Velocity and Concentration Measurements of a Turbulent Jet Mixing Flow HUI HU, a TETSUO SAGA, b TOSHIO KOBAYASHI, b AND NOBUYUKI TANIGUCHI b a Department of Mechanical Engineering, Michigan

More information

Visualization of Xe and Sn Atoms Generated from Laser-Produced Plasma for EUV Light Source

Visualization of Xe and Sn Atoms Generated from Laser-Produced Plasma for EUV Light Source 3rd International EUVL Symposium NOVEMBER 1-4, 2004 Miyazaki, Japan Visualization of Xe and Sn Atoms Generated from Laser-Produced Plasma for EUV Light Source H. Tanaka, A. Matsumoto, K. Akinaga, A. Takahashi

More information

Molecular Tagging Techniques Part - 2

Molecular Tagging Techniques Part - 2 AerE 545X class ntes #4 Mlecular Tagging Techniques Part - 2 Hui Hu Department f Aerspace Engineering, Iwa State University Ames, Iwa 500, U.S.A Cpyright by Dr. Hui Hu @ Iwa State University. All Rights

More information

Laser Doppler Velocimetry (LDV) Part - 01

Laser Doppler Velocimetry (LDV) Part - 01 AerE 545 class notes #21 Laser Doppler Velocimetry (LDV) Part - 01 Hui Hu Department of Aerospace Engineering, Iowa State University Ames, Iowa 50011, U.S.A Techniques for Flow Velocity Measurements Intrusive

More information

Supporting Information. A Facile Methodology for Engineering the Morphology of CsPbX 3 Perovskite Nanocrystals under Ambient Condition

Supporting Information. A Facile Methodology for Engineering the Morphology of CsPbX 3 Perovskite Nanocrystals under Ambient Condition Supporting Information A Facile Methodology for Engineering the Morphology of CsPbX 3 Perovskite Nanocrystals under Ambient Condition Sudipta Seth and Anunay Samanta School of Chemistry, University of

More information

Semiconductor quantum dots

Semiconductor quantum dots Semiconductor quantum dots Quantum dots are spherical nanocrystals of semiconducting materials constituted from a few hundreds to a few thousands atoms, characterized by the quantum confinement of the

More information

CHAPTER 7 SUMMARY OF THE PRESENT WORK AND SUGGESTIONS FOR FUTURE WORK

CHAPTER 7 SUMMARY OF THE PRESENT WORK AND SUGGESTIONS FOR FUTURE WORK 161 CHAPTER 7 SUMMARY OF THE PRESENT WORK AND SUGGESTIONS FOR FUTURE WORK 7.1 SUMMARY OF THE PRESENT WORK Nonlinear optical materials are required in a wide range of important applications, such as optical

More information

Laboratory 3: Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown, and Twiss Setup for Photon Antibunching

Laboratory 3: Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown, and Twiss Setup for Photon Antibunching Laboratory 3: Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown, and Twiss Setup for Photon Antibunching Jonathan Papa 1, * 1 Institute of Optics University of Rochester, Rochester,

More information

Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown and Twiss Photon Antibunching Setup

Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown and Twiss Photon Antibunching Setup 1 Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown and Twiss Photon Antibunching Setup Abstract Jacob Begis The purpose of this lab was to prove that a source of light can be

More information

In a metal, how does the probability distribution of an electron look like at absolute zero?

In a metal, how does the probability distribution of an electron look like at absolute zero? 1 Lecture 6 Laser 2 In a metal, how does the probability distribution of an electron look like at absolute zero? 3 (Atom) Energy Levels For atoms, I draw a lower horizontal to indicate its lowest energy

More information

Application of 2-D LIF temperature measurements in water using a Nd : YAG laser

Application of 2-D LIF temperature measurements in water using a Nd : YAG laser Experiments in Fluids 27 (1999) 420 426 Springer-Verlag 1999 Application of 2-D LIF temperature measurements in water using a Nd : YAG laser M. C. J. Coolen, R. N. Kieft, C. C. M. Rindt, A. A. van Steenhoven

More information

1. Transition dipole moment

1. Transition dipole moment 1. Transition dipole moment You have measured absorption spectra of aqueous (n=1.33) solutions of two different chromophores (A and B). The concentrations of the solutions were the same. The absorption

More information

Laboratory 3&4: Confocal Microscopy Imaging of Single-Emitter Fluorescence and Hanbury Brown and Twiss setup for Photon Antibunching

Laboratory 3&4: Confocal Microscopy Imaging of Single-Emitter Fluorescence and Hanbury Brown and Twiss setup for Photon Antibunching Laboratory 3&4: Confocal Microscopy Imaging of Single-Emitter Fluorescence and Hanbury Brown and Twiss setup for Photon Antibunching Jose Alejandro Graniel Institute of Optics University of Rochester,

More information

Chemistry Instrumental Analysis Lecture 5. Chem 4631

Chemistry Instrumental Analysis Lecture 5. Chem 4631 Chemistry 4631 Instrumental Analysis Lecture 5 Light Amplification by Stimulated Emission of Radiation High Intensities Narrow Bandwidths Coherent Outputs Applications CD/DVD Readers Fiber Optics Spectroscopy

More information

Laser heating of noble gas droplet sprays: EUV source efficiency considerations

Laser heating of noble gas droplet sprays: EUV source efficiency considerations Laser heating of noble gas droplet sprays: EUV source efficiency considerations S.J. McNaught, J. Fan, E. Parra and H.M. Milchberg Institute for Physical Science and Technology University of Maryland College

More information

Lecture # 12: Illumination, imaging, and particle image velocimetry

Lecture # 12: Illumination, imaging, and particle image velocimetry AerE 344 Lecture Notes Lecture # 12: Illumination, imaging, and particle image velocimetry Dr. Hui Hu Department of Aerospace Engineering Iowa State University Ames, Iowa 50011, U.S.A Sources/ Further

More information

NANOSCIENCE: TECHNOLOGY AND ADVANCED MATERIALS

NANOSCIENCE: TECHNOLOGY AND ADVANCED MATERIALS UNIVERSITY OF SOUTHAMPTON PHYS6014W1 SEMESTER 2 EXAMINATIONS 2012-2013 NANOSCIENCE: TECHNOLOGY AND ADVANCED MATERIALS DURATION 120 MINS (2 Hours) This paper contains 8 questions Answer ALL questions in

More information

TECHNICAL INFORMATION. Quantum Dot

TECHNICAL INFORMATION. Quantum Dot Quantum Dot Quantum Dot is the nano meter sized semiconductor crystal with specific optical properties originates from the phenomenon which can be explained by the quantum chemistry and quantum mechanics.

More information

PASSIVE CONTROL ON JET MIXING FLOWS BY USING VORTEX GENERATORS

PASSIVE CONTROL ON JET MIXING FLOWS BY USING VORTEX GENERATORS Proceedings of the Sixth Triennial International Symposium on Fluid Control, Measurement and Visualization, Sherbrooke, Canada, August -7,. PASSIVE CONTROL ON JET MIXING FLOWS BY USING VORTEX GENERATORS

More information

Determination of bandwidth and beamwidth of a Rhodamine 6G dye laser using different optical setups

Determination of bandwidth and beamwidth of a Rhodamine 6G dye laser using different optical setups Practicum Spectroscopy HS 2 Determination of bandwidth and beamwidth of a Rhodamine 6G dye laser using different optical setups DLA Jorge Ferreiro, study degree Chemistry, 5 th semester, fjorge@student.ethz.ch

More information

Lab 3 and 4: Single Photon Source

Lab 3 and 4: Single Photon Source Lab 3 and 4: Single Photon Source By: Justin Deuro, December 10 th, 2009 Abstract We study methods of single photon emission by exciting single colloidal quantum dot (QD) samples. We prepare the single

More information

Supporting Information

Supporting Information Supporting Information Decorating Graphene Sheets with Gold Nanoparticles Ryan Muszynski, Brian Seeger and, Prashant V. Kamat* Radiation Laboratory, Departments of Chemistry & Biochemistry and Chemical

More information

Fundamental Mechanisms, Predictive Modeling, and Novel Aerospace Applications of Plasma Assisted Combustion

Fundamental Mechanisms, Predictive Modeling, and Novel Aerospace Applications of Plasma Assisted Combustion Fundamental Mechanisms, Predictive Modeling, and Novel Aerospace Applications of Plasma Assisted Combustion Walter R. Lempert, Igor V. Adamovich, J. William Rich, Jeffrey A. Sutton Department of Mechanical

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION Supplementary Information Speckle-free laser imaging using random laser illumination Brandon Redding 1*, Michael A. Choma 2,3*, Hui Cao 1,4* 1 Department of Applied Physics, Yale University, New Haven,

More information

Controlled Assembly of Organic Whispering Gallery Mode Microlasers as Highly Sensitive Chemical Sensors

Controlled Assembly of Organic Whispering Gallery Mode Microlasers as Highly Sensitive Chemical Sensors Electronic Supplementary Material (ESI) for ChemComm. This journal is The Royal Society of Chemistry 2017 Electronic Supplementary Information Controlled Assembly of Organic Whispering Gallery Mode Microlasers

More information

Effects of Temperature and Concentration on the Rate of Photo-bleaching of Erythrosine in Water

Effects of Temperature and Concentration on the Rate of Photo-bleaching of Erythrosine in Water Supporting Information for: Effects of Temperature and Concentration on the Rate of Photo-bleaching of Erythrosine in Water Joshua K. G. Karlsson, Owen J. Woodford, Roza Al-Aqar and Anthony Harriman* Molecular

More information

Optics and Spectroscopy

Optics and Spectroscopy Introduction to Optics and Spectroscopy beyond the diffraction limit Chi Chen 陳祺 Research Center for Applied Science, Academia Sinica 2015Apr09 1 Light and Optics 2 Light as Wave Application 3 Electromagnetic

More information

Synthesis of ternary chalcogenide colloidal nanocrystals in aqueous medium

Synthesis of ternary chalcogenide colloidal nanocrystals in aqueous medium Journal of Physics: Conference Series PAPER OPEN ACCESS Synthesis of ternary chalcogenide colloidal nanocrystals in aqueous medium To cite this article: D S Mazing et al 28 J. Phys.: Conf. Ser. 38 25 View

More information

LAB 3: Confocal Microscope Imaging of single-emitter fluorescence. LAB 4: Hanbury Brown and Twiss setup. Photon antibunching. Roshita Ramkhalawon

LAB 3: Confocal Microscope Imaging of single-emitter fluorescence. LAB 4: Hanbury Brown and Twiss setup. Photon antibunching. Roshita Ramkhalawon LAB 3: Confocal Microscope Imaging of single-emitter fluorescence LAB 4: Hanbury Brown and Twiss setup. Photon antibunching Roshita Ramkhalawon PHY 434 Department of Physics & Astronomy University of Rochester

More information

Supporting Information

Supporting Information Supporting Information Study of Diffusion Assisted Bimolecular Electron Transfer Reactions: CdSe/ZnS Core Shell Quantum Dot acts as an Efficient Electron Donor as well as Acceptor. Somnath Koley, Manas

More information

Model Answer (Paper code: AR-7112) M. Sc. (Physics) IV Semester Paper I: Laser Physics and Spectroscopy

Model Answer (Paper code: AR-7112) M. Sc. (Physics) IV Semester Paper I: Laser Physics and Spectroscopy Model Answer (Paper code: AR-7112) M. Sc. (Physics) IV Semester Paper I: Laser Physics and Spectroscopy Section I Q1. Answer (i) (b) (ii) (d) (iii) (c) (iv) (c) (v) (a) (vi) (b) (vii) (b) (viii) (a) (ix)

More information

DEVELOPMENT OF NANO PARTICLE SIZING SYSTEM USING FLUORESCENCE POLARIZATION

DEVELOPMENT OF NANO PARTICLE SIZING SYSTEM USING FLUORESCENCE POLARIZATION XX IMEKO World Congress Metrology for Green Growth September 9 14, 2012, Busan, Republic of Korea DEVELOPMENT OF NANO PARTICLE SIZING SYSTEM USING FLUORESCENCE POLARIZATION Terutake Hayashi, Masaki Michihata,

More information

Calibration of Laser Induced Fluorescence Thermometry Using 2'7' Dichlorofluorescein and Sulforhodamine B

Calibration of Laser Induced Fluorescence Thermometry Using 2'7' Dichlorofluorescein and Sulforhodamine B OREGON STATE UNIVERSITY Calibration of Laser Induced Fluorescence Thermometry Using 2'7' Dichlorofluorescein and Sulforhodamine B PH 403 Senior Thesis With Dr. Vinod Narayanan Jaryd Ulbricht 5/30/2012

More information

Chapter 15 Molecular Luminescence Spectrometry

Chapter 15 Molecular Luminescence Spectrometry Chapter 15 Molecular Luminescence Spectrometry Two types of Luminescence methods are: 1) Photoluminescence, Light is directed onto a sample, where it is absorbed and imparts excess energy into the material

More information

Laser Types Two main types depending on time operation Continuous Wave (CW) Pulsed operation Pulsed is easier, CW more useful

Laser Types Two main types depending on time operation Continuous Wave (CW) Pulsed operation Pulsed is easier, CW more useful Main Requirements of the Laser Optical Resonator Cavity Laser Gain Medium of 2, 3 or 4 level types in the Cavity Sufficient means of Excitation (called pumping) eg. light, current, chemical reaction Population

More information

Chlorophyll and other naturally occurring tracer dyes for laser-induced fluorescence in liquid flow applications

Chlorophyll and other naturally occurring tracer dyes for laser-induced fluorescence in liquid flow applications Chlorophyll and other naturally occurring tracer dyes for laser-induced fluorescence in liquid flow applications Katharina Zähringer * Lehrstuhl für Strömungsmechanik und Strömungstechnik, Universität

More information

Natallia Strekal. Plasmonic films of noble metals for nanophotonics

Natallia Strekal. Plasmonic films of noble metals for nanophotonics Natallia Strekal Plasmonic films of noble metals for nanophotonics The aim of our investigation is the mechanisms of light interactions with nanostructure and High Tech application in the field of nanophotonics

More information

Ultrafast Dynamics and Single Particle Spectroscopy of Au-CdSe Nanorods

Ultrafast Dynamics and Single Particle Spectroscopy of Au-CdSe Nanorods Supporting Information Ultrafast Dynamics and Single Particle Spectroscopy of Au-CdSe Nanorods G. Sagarzazu a, K. Inoue b, M. Saruyama b, M. Sakamoto b, T. Teranishi b, S. Masuo a and N. Tamai a a Department

More information

Laser-produced extreme ultraviolet (EUV) light source plasma for the next generation lithography application

Laser-produced extreme ultraviolet (EUV) light source plasma for the next generation lithography application Laser-produced extreme ultraviolet (EUV) light source plasma for the next generation lithography application EUV light source plasma Tin icrodroplet Main pulse (CO2 laser pulse) Pre-pulse (Nd:YAG laser

More information

Detection of Single Photon Emission by Hanbury-Brown Twiss Interferometry

Detection of Single Photon Emission by Hanbury-Brown Twiss Interferometry Detection of Single Photon Emission by Hanbury-Brown Twiss Interferometry Greg Howland and Steven Bloch May 11, 009 Abstract We prepare a solution of nano-diamond particles on a glass microscope slide

More information

Fang Chen, Haixing Li & Hui Hu

Fang Chen, Haixing Li & Hui Hu Molecular tagging techniques and their applications to the study of complex thermal flow phenomena Fang Chen, Haixing Li & Hui Hu Acta Mechanica Sinica ISSN 0567-7718 Acta Mech. Sin. DOI 10.1007/s10409-015-0464-z

More information

Raman and stimulated Raman spectroscopy of chlorinated hydrocarbons

Raman and stimulated Raman spectroscopy of chlorinated hydrocarbons Department of Chemistry Physical Chemistry Göteborg University KEN140 Spektroskopi Raman and stimulated Raman spectroscopy of chlorinated hydrocarbons WARNING! The laser gives a pulsed very energetic and

More information

Effect of Addition Au Nanoparticles on Emission Spectra of Laser Dye

Effect of Addition Au Nanoparticles on Emission Spectra of Laser Dye International Journal of Applied Engineering Research ISSN 973-462 Volume 2, Number 24 (27) pp. 4833-484 Effect of Addition Au Nanoparticles on Emission Spectra of Laser Dye Sara Ali Razzak, Lazem Hassan

More information

29:006 FINAL EXAM FRIDAY MAY 11 3:00 5:00 PM IN LR1 VAN

29:006 FINAL EXAM FRIDAY MAY 11 3:00 5:00 PM IN LR1 VAN L 33 Modern Physics [1] 29:006 FINAL EXAM FRIDAY MAY 11 3:00 5:00 PM IN LR1 VAN Introduction- quantum physics Particles of light PHOTONS The photoelectric effect Photocells & intrusion detection devices

More information

Electronic Supplementary Information

Electronic Supplementary Information Electronic Supplementary Material (ESI) for Journal of Materials Chemistry C. This journal is The Royal Society of Chemistry 2017 Electronic Supplementary Information Polymorphism and microcrystal shape

More information

LASER BASED DIAGNOSTIC SYSTEM FOR SPRAY MEASUREMENTS

LASER BASED DIAGNOSTIC SYSTEM FOR SPRAY MEASUREMENTS Journal of KONES Powertrain and Transport, Vol. 22, No. 3 2015 LASER BASED DIAGNOSTIC SYSTEM FOR SPRAY MEASUREMENTS Łukasz Jan Kapusta, Piotr Jaworski, Andrzej Teodorczyk Warsaw University of Technology,

More information

Modern optics Lasers

Modern optics Lasers Chapter 13 Phys 322 Lecture 36 Modern optics Lasers Reminder: Please complete the online course evaluation Last lecture: Review discussion (no quiz) LASER = Light Amplification by Stimulated Emission of

More information

Confocal Microscope Imaging of Single emitter fluorescence and Observing Photon Antibunching Using Hanbury Brown and Twiss setup. Lab.

Confocal Microscope Imaging of Single emitter fluorescence and Observing Photon Antibunching Using Hanbury Brown and Twiss setup. Lab. Submitted for the partial fulfilment of the course PHY 434 Confocal Microscope Imaging of Single emitter fluorescence and Observing Photon Antibunching Using Hanbury Brown and Twiss setup Lab. 3 and 4

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION SUPPLEMENTARY INFORMATION DOI: 10.1038/NNANO.2012.63 Bright infrared quantum-dot light-emitting diodes through inter-dot spacing control Liangfeng Sun, Joshua J. Choi, David Stachnik, Adam C. Bartnik,

More information

Fluorescence Workshop UMN Physics June 8-10, 2006 Quantum Yield and Polarization (1) Joachim Mueller

Fluorescence Workshop UMN Physics June 8-10, 2006 Quantum Yield and Polarization (1) Joachim Mueller Fluorescence Workshop UMN Physics June 8-10, 2006 Quantum Yield and Polarization (1) Joachim Mueller Quantum yield, polarized light, dipole moment, photoselection, dipole radiation, polarization and anisotropy

More information

Applications of Laser Spectroscopy to Highly Sensitive Analyses

Applications of Laser Spectroscopy to Highly Sensitive Analyses G u e s t F o r u m Guest Forum Series of Lectures by Screening Committees of the Second Masao Horiba Awards Applications of Laser Spectroscopy to Highly Sensitive Analyses Cavity Ring-Down Spectroscopy

More information

EUV lithography and Source Technology

EUV lithography and Source Technology EUV lithography and Source Technology History and Present Akira Endo Hilase Project 22. September 2017 EXTATIC, Prague Optical wavelength and EUV (Extreme Ultraviolet) VIS 13.5nm 92eV Characteristics of

More information

Shear instabilities in a tilting tube

Shear instabilities in a tilting tube Abstract Shear instabilities in a tilting tube Edmund Tedford 1, Jeff Carpenter 2 and Greg Lawrence 1 1 Department of Civil Engineering, University of British Columbia ttedford@eos.ubc.ca 2 Institute of

More information

6. A solution of red Kool-Aid transmits light at a wavelength range of nm.

6. A solution of red Kool-Aid transmits light at a wavelength range of nm. I. Multiple Choice (15 pts) 1. FRET stands for a. Fluorescence Recovery Electron Transfer b. Fluorescence Resonance Energy Transfer c. Fluorescence Recovery Energy Transfer 2. Fluorescence involves the

More information

Modern Physics- Introduction. L 35 Modern Physics [1] ATOMS and classical physics. Newton s Laws have flaws! accelerated charges radiate energy

Modern Physics- Introduction. L 35 Modern Physics [1] ATOMS and classical physics. Newton s Laws have flaws! accelerated charges radiate energy L 35 Modern Physics [1] Introduction- quantum physics Particles of light PHOTONS The photoelectric effect Photocells & intrusion detection devices The Bohr atom emission & absorption of radiation LASERS

More information

ScienceDirect. Gas flow visualization using laser-induced fluorescence

ScienceDirect. Gas flow visualization using laser-induced fluorescence Available online at www.sciencedirect.com ScienceDirect Procedia Engineering 106 (2015 ) 92 96 Dynamics and Vibroacoustics of Machines (DVM2014) Gas flow visualization using laser-induced fluorescence

More information

MEASUREMENT OF TEMPORAL RESOLUTION AND DETECTION EFFICIENCY OF X-RAY STREAK CAMERA BY SINGLE PHOTON IMAGES

MEASUREMENT OF TEMPORAL RESOLUTION AND DETECTION EFFICIENCY OF X-RAY STREAK CAMERA BY SINGLE PHOTON IMAGES Proceedings of IBIC212, Tsukuba, Japan MEASUREMENT OF TEMPORAL RESOLUTION AND DETECTION EFFICIENCY OF X-RAY STREAK CAMERA BY SINGLE PHOTON IMAGES A. Mochihashi, M. Masaki, S. Takano, K. Tamura, H. Ohkuma,

More information

Chapter 17: Fundamentals of Spectrophotometry

Chapter 17: Fundamentals of Spectrophotometry Chapter 17: Fundamentals of Spectrophotometry Spectroscopy: the science that deals with interactions of matter with electromagnetic radiation or other forms energy acoustic waves, beams of particles such

More information

The molecules that will be studied with this device will have an overall charge of

The molecules that will be studied with this device will have an overall charge of The Basics of the Rotation of Polarized Light The molecules that will be studied with this device will have an overall charge of zero but will have localized polarities that can be used to orient the molecule.

More information

Synthesis of Zinc Sulphide Nanoparticles

Synthesis of Zinc Sulphide Nanoparticles Synthesis of Zinc Sulphide Nanoparticles The procedure shown here was adapted from an adaption by Paul Hansen and George Lisensky from Kurt Winkelmann, Thomas Noviello, and Steven Brooks, "Preparation

More information

Applications of Quantum Dots to Biosensing

Applications of Quantum Dots to Biosensing Applications of Quantum Dots to Biosensing CHEM 681 Student Seminar Series March 17 th, 2003 Heechang Ye Advisor : Dr. Richard M. Crooks Introduction Quantum dots (QDs) are semiconductor particles that

More information

Pressure Measurement Techniques and Instrumentation

Pressure Measurement Techniques and Instrumentation AerE 344 class notes Lecture # 04 Pressure Measurement Techniques and Instrumentation Hui Hu Department of Aerospace Engineering, Iowa State University Ames, Iowa 50011, U.S.A Measurement Techniques for

More information

Dynamics of Large Scale Motions in Bubble-Driven Turbulent Flow

Dynamics of Large Scale Motions in Bubble-Driven Turbulent Flow Dynamics of Large Scale Motions in Bubble-Driven Turbulent Flow Kyung Chun Kim School of Mechanical Engineering, Pusan National University Jangjeon-dong, Geumjeong-gu, Pusan, 609-735, Korea kckim@pusan.ac.kr

More information

Excimer Lasers Currently best UV laser sources Consist two atom types which repel each other eg nobel gas and halide or oxide which normally do not

Excimer Lasers Currently best UV laser sources Consist two atom types which repel each other eg nobel gas and halide or oxide which normally do not Excimer Lasers Currently best UV laser sources Consist two atom types which repel each other eg nobel gas and halide or oxide which normally do not bond But when excited/ionized these atoms attract Bound

More information

Application of magnetic/phosphorescent nanoparticles in immunoassays

Application of magnetic/phosphorescent nanoparticles in immunoassays Application of magnetic/phosphorescent nanoparticles in immunoassays Ian M. Kennedy and Dosev Dosev, Mikaela Nichkova, Bruce Hammock, Shirley Gee, R. Dumas, Kai Liu Department of Mechanical and Aeronautical

More information

Chapter 18. Fundamentals of Spectrophotometry. Properties of Light

Chapter 18. Fundamentals of Spectrophotometry. Properties of Light Chapter 18 Fundamentals of Spectrophotometry Properties of Light Electromagnetic Radiation energy radiated in the form of a WAVE caused by an electric field interacting with a magnetic field result of

More information

Femtosecond laser microfabrication in. Prof. Dr. Cleber R. Mendonca

Femtosecond laser microfabrication in. Prof. Dr. Cleber R. Mendonca Femtosecond laser microfabrication in polymers Prof. Dr. Cleber R. Mendonca laser microfabrication focus laser beam on material s surface laser microfabrication laser microfabrication laser microfabrication

More information

ATTO 565 and ATTO 590

ATTO 565 and ATTO 590 ATTO 565 and ATTO 590 General Information ATTO 565 and ATTO 590 are fluorescent labels belonging to the well known rhodamine dyes. A common feature of all rhodamine dyes is a carboxyphenyl substituent

More information

A novel method for instantaneous, quantitative measurement of molecular mixing in gaseous flows

A novel method for instantaneous, quantitative measurement of molecular mixing in gaseous flows A novel method for instantaneous, quantitative measurement of molecular mixing in gaseous flows H. Hu, M.M. Koochesfahani Experiments in Fluids 33 (2002) 202 209 DOI 10.1007/s00348-002-0452-5 202 Abstract

More information

FLUORESCENCE APPLICATIONS

FLUORESCENCE APPLICATIONS FLUORESCENCE APPLICATIONS CORRECTION OF EMISSION SPECTRA USING THE PERKINELMER MODEL LS-50 LUMINESCENCE SPECTROMETER Spectra collected on luminescence spectrometers consist of true spectral information

More information

Dual-Wavelength Lasing from Organic Dye Encapsulated Metal-Organic Framework Microcrystals

Dual-Wavelength Lasing from Organic Dye Encapsulated Metal-Organic Framework Microcrystals Electronic Supplementary Material (ESI) for ChemComm. This journal is The Royal Society of Chemistry 2019 Electronic Supplementary Information Dual-Wavelength Lasing from Organic Dye Encapsulated Metal-Organic

More information

RESEARCH ON THE MIXING ENHANCEMENT PERFORMANCE OF LOBED NOZZLES BY USING PIV AND LIF

RESEARCH ON THE MIXING ENHANCEMENT PERFORMANCE OF LOBED NOZZLES BY USING PIV AND LIF Proceedings of FEDSM 98 1998 ASME Fluids Engineering Division Summer Meeting June 21-25,1998, Washington, DC FEDSM98-4994 RESEARCH ON THE MIXING ENHANCEMENT PERFORMANCE OF LOBED NOZZLES BY USING PIV AND

More information

Scienza e Tecnologia dei Materiali Ceramici. Modulo 2: Materiali Nanostrutturati

Scienza e Tecnologia dei Materiali Ceramici. Modulo 2: Materiali Nanostrutturati Università degli Studi di Trieste Dipartimento di Ingegneria e Architettura A.A. 2016-2017 Scienza e Tecnologia dei Materiali Ceramici Modulo 2: Materiali Nanostrutturati - Lezione 5 - Vanni Lughi vlughi@units.it

More information

Anti-Bunching from a Quantum Dot

Anti-Bunching from a Quantum Dot Anti-Bunching from a Quantum Dot Gerardo I. Viza 1, 1 Department of Physics and Astronomy, University of Rochester, Rochester, NY 14627 We study the nature of non-classical single emitter light experimentally

More information

Quick Review. 1. Kinetic Molecular Theory. 2. Average kinetic energy and average velocity. 3. Graham s Law of Effusion. 4. Real Gas Behavior.

Quick Review. 1. Kinetic Molecular Theory. 2. Average kinetic energy and average velocity. 3. Graham s Law of Effusion. 4. Real Gas Behavior. Quick Review 1. Kinetic Molecular Theory. 2. Average kinetic energy and average velocity. 3. Graham s Law of Effusion. 4. Real Gas Behavior. Emission spectra Every element has a unique emission spectrum

More information

Lecture 11, May 11, 2017

Lecture 11, May 11, 2017 Lecture 11, May 11, 2017 This week: Atomic Ions for QIP Ion Traps Vibrational modes Preparation of initial states Read-Out Single-Ion Gates Two-Ion Gates Introductory Review Articles: D. Leibfried, R.

More information

Lecture # 09: Technical Basis for Optical Instrumentation

Lecture # 09: Technical Basis for Optical Instrumentation AerE 344 Lecture Notes Lecture # 09: Technical Basis for Optical Instrumentation Dr. Hui Hu Department of Aerospace Engineering Iowa State University Ames, Iowa 50011, U.S.A The nature of light According

More information

Laser-Dye Imaging of the ph Field in a Laboratory Experiment

Laser-Dye Imaging of the ph Field in a Laboratory Experiment Journal of Oceanography, Vol. 6, pp. 789 to 795, 24 Laser-Dye Imaging of the ph Field in a Laboratory Experiment SATOSHI SOMEYA *, SHIGERU BANDO 2, YONGCHEN SONG, BAIXIN CHEN and MASAHIRO NISHIO National

More information

Fluorescence Spectroscopy

Fluorescence Spectroscopy Fluorescence Spectroscopy Frequency and time dependent emission Emission and Excitation fluorescence spectra Stokes Shift: influence of molecular vibrations and solvent Time resolved fluorescence measurements

More information

Colloidal Single-Layer Quantum Dots with Lateral Confinement Effects on 2D Exciton

Colloidal Single-Layer Quantum Dots with Lateral Confinement Effects on 2D Exciton Supporting Information Colloidal Single-Layer Quantum Dots with Lateral Confinement Effects on 2D Exciton Ho Jin,, Minji Ahn,,,, Sohee Jeong,,, Jae Hyo Han,,, Dongwon Yoo,, Dong Hee Son, *, and Jinwoo

More information

Supporting Information for. Long-Distance Charge Carrier Funneling in Perovskite Nanowires Enable by Built-in Halide Gradient

Supporting Information for. Long-Distance Charge Carrier Funneling in Perovskite Nanowires Enable by Built-in Halide Gradient Supporting Information for Long-Distance Charge Carrier Funneling in Perovskite Nanowires Enable by Built-in Halide Gradient Wenming Tian, Jing Leng, Chunyi Zhao and Shengye Jin* State Key Laboratory of

More information

Chapter 17: Fundamentals of Spectrophotometry

Chapter 17: Fundamentals of Spectrophotometry Chapter 17: Fundamentals of Spectrophotometry Spectroscopy: the science that deals with interactions of matter with electromagnetic radiation or other forms energy acoustic waves, beams of particles such

More information

Distribution of Delay Times in Laser Excited CdSe-ZnS Core-Shell Quantum Dots

Distribution of Delay Times in Laser Excited CdSe-ZnS Core-Shell Quantum Dots Distribution of Delay Times in Laser Excited CdSe-ZnS Core-Shell Quantum Dots Andrei Vajiac Indiana University South Bend Mathematics, Computer Science Advisor: Pavel Frantsuzov, Physics Abstract This

More information

Investigation of Heat Transfer in Mini Channels using Planar Laser Induced Fluorescence

Investigation of Heat Transfer in Mini Channels using Planar Laser Induced Fluorescence Aalborg Universitet Investigation of Heat Transfer in Mini Channels using Planar Laser Induced Fluorescence Bøgild, Morten Ryge; Poulsen, Jonas Lundsted; Rath, Emil Zacho; Sørensen, Henrik Published in:

More information

Chemistry 524--Final Exam--Keiderling May 4, :30 -?? pm SES

Chemistry 524--Final Exam--Keiderling May 4, :30 -?? pm SES Chemistry 524--Final Exam--Keiderling May 4, 2011 3:30 -?? pm -- 4286 SES Please answer all questions in the answer book provided. Calculators, rulers, pens and pencils are permitted. No open books or

More information

High resolution method for measuring local quantum yield of photoluminescence and phototransformation using confocal scanning microscope

High resolution method for measuring local quantum yield of photoluminescence and phototransformation using confocal scanning microscope High resolution method for measuring local quantum yield of photoluminescence and phototransformation using confocal scanning microscope * Viktor Zakharov 1) and Andrei Veniaminov 2) National Research

More information

Chemistry Instrumental Analysis Lecture 17. Chem 4631

Chemistry Instrumental Analysis Lecture 17. Chem 4631 Chemistry 4631 Instrumental Analysis Lecture 17 Introduction to Optical Atomic Spectrometry From molecular to elemental analysis there are three major techniques used for elemental analysis: Optical spectrometry

More information

Exploring different speckle reduction techniques for double pass ocular imaging. Donatus Halpaap Advisers: Meritxell Vilaseca, Cristina Masoller

Exploring different speckle reduction techniques for double pass ocular imaging. Donatus Halpaap Advisers: Meritxell Vilaseca, Cristina Masoller Exploring different speckle reduction techniques for double pass ocular imaging Donatus Halpaap Advisers: Meritxell Vilaseca, Cristina Masoller Biophysics by the Sea, Alcúdia, Mallorca, October 12, 2018

More information

Near-Infrared Spectroscopy of Nitride Heterostructures EMILY FINAN ADVISOR: DR. OANA MALIS PURDUE UNIVERSITY REU PROGRAM AUGUST 2, 2012

Near-Infrared Spectroscopy of Nitride Heterostructures EMILY FINAN ADVISOR: DR. OANA MALIS PURDUE UNIVERSITY REU PROGRAM AUGUST 2, 2012 Near-Infrared Spectroscopy of Nitride Heterostructures EMILY FINAN ADVISOR: DR. OANA MALIS PURDUE UNIVERSITY REU PROGRAM AUGUST 2, 2012 Introduction Experimental Condensed Matter Research Study of large

More information

Electronic Supplementary Information. Ultrafast Charge Separation in Supramolecular Tetrapyrrole- Graphene Hybrids

Electronic Supplementary Information. Ultrafast Charge Separation in Supramolecular Tetrapyrrole- Graphene Hybrids Electronic Supplementary Information Ultrafast Charge Separation in Supramolecular Tetrapyrrole- Graphene Hybrids Chandra Bikram, K.C, a Sushanta Das, a Kei Ohkubo, b Shunichi Fukuzumi, b,c,* and Francis

More information

Interaction mechanism for energy transfer from Ce to Tb ions in silica

Interaction mechanism for energy transfer from Ce to Tb ions in silica Interaction mechanism for energy transfer from Ce to Tb ions in silica HAA Seed Ahmed 1,2, W-S Chae 3, OM Ntwaeaborwa 1 and RE Kroon 1 1 Department of Physics, University of the Free State, South Africa

More information

Department of Chemistry Physical Chemistry Göteborg University

Department of Chemistry Physical Chemistry Göteborg University Department of Chemistry Physical Chemistry Göteborg University &RQVWUXFWLRQRIDSXOVHGG\HODVHU 3OHDVHREVHUYHWKDWWKHVDIHW\SUHFDXWLRQVRQSDJHPXVW EHIROORZHGRWKHUZLVHWKHUHLVDULVNRIH\HGDPDJH Renée Andersson -97,

More information

Instrumentation. Dr. Hui Hu Dr. Rye Waldman. Department of Aerospace Engineering Iowa State University Ames, Iowa 50011, U.S.A

Instrumentation. Dr. Hui Hu Dr. Rye Waldman. Department of Aerospace Engineering Iowa State University Ames, Iowa 50011, U.S.A AerE 344 Lecture Notes Lecture # 05: elocimetry Techniques and Instrumentation Dr. Hui Hu Dr. Rye Waldman Department of Aerospace Engineering Iowa State University Ames, Iowa 500, U.S.A Sources/ Further

More information

Single Emitter Detection with Fluorescence and Extinction Spectroscopy

Single Emitter Detection with Fluorescence and Extinction Spectroscopy Single Emitter Detection with Fluorescence and Extinction Spectroscopy Michael Krall Elements of Nanophotonics Associated Seminar Recent Progress in Nanooptics & Photonics May 07, 2009 Outline Single molecule

More information

Time-Resolved Velocity and ph Mapping in T-shaped Microchannel

Time-Resolved Velocity and ph Mapping in T-shaped Microchannel Lisbon, Portugal, 26-29 June, 26 Paper No. #134 Time-Resolved Velocity and ph Mapping in T-shaped Microchannel Mitsuhisa ICHIYANAGI 1, Yohei SATO 2, Koichi HISHIDA 3 1: Department of System Design Engineering,

More information