1. Transition dipole moment

Size: px
Start display at page:

Download "1. Transition dipole moment"

Transcription

1 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 spectra have similar shape but the spectrum of A is 1.2 times broader than the spectrum of B. Maximum optical density A is 1.67 times larger than that of B. The absorption reaches is maximum at ν max = cm -1. Fluorescence lifetime τ fl (A) = 1 ns; fluorescence yield Φ fl (A) =Φ fl (B)= 0.3; a) Calculate the transition dipole moment of A in Debye (µ A =?) b) Calculate the transition dipole moment of B in Debye (µ B =?) c) Calculate fluorescence lifetime of B (τ fl (B) =?) 2. Jablonski diagram/sms Jablonski diagram of a dye molecule is given at the figure. The rates are: k IC = 0.5 ns -1 k fl = 0.5 ns -1 k ISC = 0.25 ns -1 k T = 0.1 ms -1 a) Calculate Φ fl ; Φ ISC ; Φ IC b) Fluorescence intensity of a single molecule of this dye is monitored by a fluorescence microscope. Fluorescence blinking is observed. What is the characteristic time the molecule stays in dark, non-fluorescent states? 3. Fluorescence decay Fluorescence decay of a sample without quencher (Φ fl =1) is shown at the figure. a) What is the fluorescence radiative lifetime of the chromophores? b) A dynamic quencher was added to the initial sample so that Φ fl =0.33; Draw the fluorescence decay at the same graph c) A static quencher was added to the initial sample. 50% of all dye molecules form complexes with the quenchers. Draw the fluorescence decay at the same graph d) To the solution obtained in (c) a dynamic quencher was added so that the fluorescence lifetime become 1 ns. Draw the fluorescence decay at the same graph e) Calculate fluorescence quantum yield for the case d)

2 4. Electron transfer Molecules of a dye are attached to TiO 2 nanoparticles via a spacer. Changing the spacer allows to change the distance r between the dye and the particle. When the dye is close to the nanoparticle an electron transfer reaction occurs. The distance parameter of electron transfer β=10 nm -1. For r=0.2 nm the electron transfer rate k ET = s -1. The free dye in solution has fluorescence lifetime τ fl = 1 ns and fluorescence quantum yield Φ fl = 0.5. a) Calculate Φ fl and τ fl for r = 0.2 nm b) Calculate k EL, Φ fl and τ fl for r = 1 nm 5. Förster energy transfer Donor (D) and acceptor (A) chromophores are separated by distance r= 4.24 nm. The orientation of the transition dipole moments of the molecules are shown at the figure where α=45 o. Molecules of D without A has fluorescence yield Φ D =1 and fluorescence lifetime τ D =4 ns Molecules of A without D has fluorescence yield Φ A =1 Förster radius for energy transfer from D to A for random orientations of the molecules is R 0 Random =5 nm For the pair of molecules shown at the figure calculate: a) Förster radius R 0 b) Efficiency of energy transfer from D to A c) Fluorescence lifetime of the donor 6. Fluorescence anisotropy Your sample (a frozen solution of a chromophore) has two strong absorption bands (see the figure). The one at 350 nm corresponds to absorption to S 2 state; the other at 550 nm is absorption to S 1 state. So, you can excite fluorescence by excitation via 350 band or 550 nm band. You know, that the transition dipole moment of optical transition between S 0 and S 1 is perpendicular to the dipole moment of optical transition between S 0 and S 2. a) What will be the fluorescence anisotropy when excited at 550 nm? b) What will be the fluorescence anisotropy when excited at 350 nm? c) You increase the temperature and the solvent become liquid. Fluorescence lifetime is 4 ns; rotation correlation time of the molecules is 1 ns at these conditions. Calculate fluorescence anisotropy for 550 and 350 nm excitation wavelengths.

3 7. Practical Spectroscopy You have 2 spectra of a sample obtained with different excitations (λ ex1 and λ ex2 ) with a grating spectrometer (see the figure). The excitation light is a narrow laser line (linewidth < 0.1 nm). The resolution of the spectrometer is 0.1 nm. a) Identify the features in the spectrum (second order of light diffraction on the grating; Raman scattering, fluorescence) b) Determine λ ex1 and λ ex2 c) Calculate the frequency (in cm -1 ) of the molecular vibration giving the Raman line observed in the spectra d) Draw how the spectrum A would look like if the both slits of the spectrometer are increases up to 5 mm. Liner dispersion is dx/dλ=1 mm/1nm. Draw the spectrum at the same graph where the spectrum A is shown. 8. Lasers What should be the output mirror reflectivity to reach critical inversion of 2*10 17 cm -3 for a 9 cm long laser media with the cross-section of 4*10-19 cm 2 and a regular highly reflecting mirror (R=0.999)? 9. Coherent techniques Consider three Gaussian Fourier-transform limited pulses. The spectrum of one pulse is centered at 500 nm with FWHM of 35 nm, the second is centered at 700 nm with FWHM of 75 nm and the third is centered at 900 nm with FWHM of 110 nm. Which pulse is the shortest and which is the longest? 10. Quantum mechanics We have a coherent state: α = exp n 1 2 α ( α ) n 2 n n! Explain the physical meaning of the parameter α. Explain why in most of the laser experiments one can describe the laser generated electric field classically. Calculate the probability of finding n photons in the single-mode coherent state. 11. Surface science and spectroscopy The conventional three dimensional FCC (face centered cubic) unit cell of copper has a lattice constant of 3.61 Å (length of the cube). Draw a two dimensional surface unit cell for the (100), (110) and (111) surfaces and determine the size of the unit cell.

4 To problem 1 ε A B 2000 ν To problem 2 k ISC S 1 T 1 k IC k 0 fl k T S 0 To problem 5 D α A α r To problem 6 Absorptio Fluorescenc λ

5

single-molecule fluorescence resonance energy transfer

single-molecule fluorescence resonance energy transfer single-molecule fluorescence resonance energy transfer (2) determing the Förster radius: quantum yield, donor lifetime, spectral overlap, anisotropy michael börsch 26/05/2004 1 fluorescence (1) absorbance

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

CHEM Outline (Part 15) - Luminescence 2013

CHEM Outline (Part 15) - Luminescence 2013 CHEM 524 -- Outline (Part 15) - Luminescence 2013 XI. Molecular Luminescence Spectra (Chapter 15) Kinetic process, competing pathways fluorescence, phosphorescence, non-radiative decay Jablonski diagram

More information

Fluorescence (Notes 16)

Fluorescence (Notes 16) Fluorescence - 2014 (Notes 16) XV 74 Jablonski diagram Where does the energy go? Can be viewed like multistep kinetic pathway 1) Excite system through A Absorbance S 0 S n Excite from ground excited singlet

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

Application of IR Raman Spectroscopy

Application of IR Raman Spectroscopy Application of IR Raman Spectroscopy 3 IR regions Structure and Functional Group Absorption IR Reflection IR Photoacoustic IR IR Emission Micro 10-1 Mid-IR Mid-IR absorption Samples Placed in cell (salt)

More information

Fluorescence 2009 update

Fluorescence 2009 update XV 74 Fluorescence 2009 update Jablonski diagram Where does the energy go? Can be viewed like multistep kinetic pathway 1) Excite system through A Absorbance S 0 S n Excite from ground excited singlet

More information

Lecture 10. Lidar Effective Cross-Section vs. Convolution

Lecture 10. Lidar Effective Cross-Section vs. Convolution Lecture 10. Lidar Effective Cross-Section vs. Convolution q Introduction q Convolution in Lineshape Determination -- Voigt Lineshape (Lorentzian Gaussian) q Effective Cross Section for Single Isotope --

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

XV 74. Flouorescence-Polarization-Circular-Dichroism- Jablonski diagram Where does the energy go?

XV 74. Flouorescence-Polarization-Circular-Dichroism- Jablonski diagram Where does the energy go? XV 74 Flouorescence-Polarization-Circular-Dichroism- Jablonski diagram Where does the energy go? 1) Excite system through A Absorbance S 0 S n Excite from ground excited singlet S = 0 could be any of them

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

10. 6 Photochemistry. Out-class reading: Levine, pp photochemistry

10. 6 Photochemistry. Out-class reading: Levine, pp photochemistry Out-class reading: Levine, pp. 800-804 photochemistry 6.1 Brief introduction of light 1) Photochemistry The branch of chemistry which deals with the study of chemical reaction initiated by light. 2) Energy

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

Skoog Chapter 6 Introduction to Spectrometric Methods

Skoog Chapter 6 Introduction to Spectrometric Methods Skoog Chapter 6 Introduction to Spectrometric Methods General Properties of Electromagnetic Radiation (EM) Wave Properties of EM Quantum Mechanical Properties of EM Quantitative Aspects of Spectrochemical

More information

Molecular spectroscopy

Molecular spectroscopy Molecular spectroscopy Origin of spectral lines = absorption, emission and scattering of a photon when the energy of a molecule changes: rad( ) M M * rad( ' ) ' v' 0 0 absorption( ) emission ( ) scattering

More information

Chemical Analysis on complex biological systems by Raman spectroscopy. Janina Kneipp

Chemical Analysis on complex biological systems by Raman spectroscopy. Janina Kneipp Chemical Analysis on complex biological systems by Raman spectroscopy Janina Kneipp Analytical Strategies J. Kneipp Nov 2014 1 Raman scattering and resonant Raman scattering S 1 resonant Raman scattering

More information

What is spectroscopy?

What is spectroscopy? Absorption Spectrum What is spectroscopy? Studying the properties of matter through its interaction with different frequency components of the electromagnetic spectrum. With light, you aren t looking directly

More information

PHOTOCHEMISTRY NOTES - 1 -

PHOTOCHEMISTRY NOTES - 1 - - 1 - PHOTOCHEMISTRY NOTES 1 st Law (Grotthus-Draper Law) Only absorbed radiation produces chemical change. Exception inelastic scattering of X- or γ-rays (electronic Raman effect). 2 nd Law (Star-Einstein

More information

Singlet. Fluorescence Spectroscopy * LUMO

Singlet. Fluorescence Spectroscopy * LUMO Fluorescence Spectroscopy Light can be absorbed and re-emitted by matter luminescence (photo-luminescence). There are two types of luminescence, in this discussion: fluorescence and phosphorescence. A

More information

(2) A two-dimensional solid has an electron energy band of the form, . [1]

(2) A two-dimensional solid has an electron energy band of the form, . [1] (1) The figure shows a two-dimensional periodic lattice, containing A atoms (white) and B atoms (black). The section of lattice shown makes a 3a 4a rectangle, as shown (measured from A atom to A atom).

More information

Wavelength λ Velocity v. Electric Field Strength Amplitude A. Time t or Distance x time for 1 λ to pass fixed point. # of λ passing per s ν= 1 p

Wavelength λ Velocity v. Electric Field Strength Amplitude A. Time t or Distance x time for 1 λ to pass fixed point. # of λ passing per s ν= 1 p Introduction to Spectroscopy (Chapter 6) Electromagnetic radiation (wave) description: Wavelength λ Velocity v Electric Field Strength 0 Amplitude A Time t or Distance x Period p Frequency ν time for 1

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

Supplementary Materials

Supplementary Materials Supplementary Materials Sample characterization The presence of Si-QDs is established by Transmission Electron Microscopy (TEM), by which the average QD diameter of d QD 2.2 ± 0.5 nm has been determined

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

5.33 Lecture Notes: Introduction to Spectroscopy

5.33 Lecture Notes: Introduction to Spectroscopy 5.33 Lecture Notes: ntroduction to Spectroscopy What is spectroscopy? Studying the properties of matter through its interaction with different frequency components of the electromagnetic spectrum. Latin:

More information

CHEM*3440. Photon Energy Units. Spectrum of Electromagnetic Radiation. Chemical Instrumentation. Spectroscopic Experimental Concept.

CHEM*3440. Photon Energy Units. Spectrum of Electromagnetic Radiation. Chemical Instrumentation. Spectroscopic Experimental Concept. Spectrum of Electromagnetic Radiation Electromagnetic radiation is light. Different energy light interacts with different motions in molecules. CHEM*344 Chemical Instrumentation Topic 7 Spectrometry Radiofrequency

More information

4 Single molecule FRET

4 Single molecule FRET 4 Single molecule FRET FRET basics Energie Dipole-dipole interaction Teil I SM Fluo, Kap. 4 FRET FRET basics transfer rate (from Fermis Golden Rule) k t = 1 0 1 r 6 apple 2 9 ln(10) n 4 N A 128 5 Z d f

More information

Chemistry 2. Molecular Photophysics

Chemistry 2. Molecular Photophysics Chemistry 2 Lecture 12 Molecular Photophysics Assumed knowledge Electronic states are labelled using their spin multiplicity with singlets having all electron spins paired and triplets having two unpaired

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

Lecture 5. Anisotropy decay/data analysis. Enrico Gratton

Lecture 5. Anisotropy decay/data analysis. Enrico Gratton Lecture 5. Anisotropy decay/data analysis Enrico Gratton Anisotropy decay Energy-transfer distance distributions Time resolved spectra Excited-state reactions Basic physics concept in polarization The

More information

CHAPTER 13 Molecular Spectroscopy 2: Electronic Transitions

CHAPTER 13 Molecular Spectroscopy 2: Electronic Transitions CHAPTER 13 Molecular Spectroscopy 2: Electronic Transitions I. General Features of Electronic spectroscopy. A. Visible and ultraviolet photons excite electronic state transitions. ε photon = 120 to 1200

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

Figure 1 Relaxation processes within an excited state or the ground state.

Figure 1 Relaxation processes within an excited state or the ground state. Excited State Processes and Application to Lasers The technology of the laser (Light Amplified by Stimulated Emission of Radiation) was developed in the early 1960s. The technology is based on an understanding

More information

Linear and nonlinear spectroscopy

Linear and nonlinear spectroscopy Linear and nonlinear spectroscopy We ve seen that we can determine molecular frequencies and dephasing rates (for electronic, vibrational, or spin degrees of freedom) from frequency-domain or timedomain

More information

Chem Homework Set Answers

Chem Homework Set Answers Chem 310 th 4 Homework Set Answers 1. Cyclohexanone has a strong infrared absorption peak at a wavelength of 5.86 µm. (a) Convert the wavelength to wavenumber.!6!1 8* = 1/8 = (1/5.86 µm)(1 µm/10 m)(1 m/100

More information

CD Basis Set of Spectra that is used is that derived from comparing the spectra of globular proteins whose secondary structures are known from X-ray

CD Basis Set of Spectra that is used is that derived from comparing the spectra of globular proteins whose secondary structures are known from X-ray CD Basis Set of Spectra that is used is that derived from comparing the spectra of globular proteins whose secondary structures are known from X-ray crystallography An example of the use of CD Modeling

More information

LABORATORY OF ELEMENTARY BIOPHYSICS

LABORATORY OF ELEMENTARY BIOPHYSICS LABORATORY OF ELEMENTARY BIOPHYSICS Experimental exercises for III year of the First cycle studies Field: Applications of physics in biology and medicine Specialization: Molecular Biophysics Fluorescence

More information

Chem 442 Review of Spectroscopy

Chem 442 Review of Spectroscopy Chem 44 Review of Spectroscopy General spectroscopy Wavelength (nm), frequency (s -1 ), wavenumber (cm -1 ) Frequency (s -1 ): n= c l Wavenumbers (cm -1 ): n =1 l Chart of photon energies and spectroscopies

More information

Radiation in the Earth's Atmosphere. Part 1: Absorption and Emission by Atmospheric Gases

Radiation in the Earth's Atmosphere. Part 1: Absorption and Emission by Atmospheric Gases Radiation in the Earth's Atmosphere Part 1: Absorption and Emission by Atmospheric Gases Electromagnetic Waves Electromagnetic waves are transversal. Electric and magnetic fields are perpendicular. In

More information

Modern Optical Spectroscopy

Modern Optical Spectroscopy Modern Optical Spectroscopy With Exercises and Examples from Biophysics and Biochemistry von William W Parson 1. Auflage Springer-Verlag Berlin Heidelberg 2006 Verlag C.H. Beck im Internet: www.beck.de

More information

UV-vis (Electronic) Spectra Ch.13 Atkins, Ch.19 Engel

UV-vis (Electronic) Spectra Ch.13 Atkins, Ch.19 Engel XV 74 UV-vis (Electronic) Spectra-2014 -Ch.13 Atkins, Ch.19 Engel Most broadly used analytical tech / especially bio-applic. inexpensive optics / solvent & cell usually not problem intense transitions

More information

Self-assembled Nanoscale DNA-porphyrin Complex for. Artificial Light-harvesting

Self-assembled Nanoscale DNA-porphyrin Complex for. Artificial Light-harvesting Supporting Information for Self-assembled Nanoscale DNA-porphyrin Complex for Artificial Light-harvesting Jakob G. Woller, Jonas K. Hannestad, and Bo Albinsson Department of Chemical and Biological Engineering/Physical

More information

What the Einstein Relations Tell Us

What the Einstein Relations Tell Us What the Einstein Relations Tell Us 1. The rate of spontaneous emission A21 is proportional to υ 3. At higher frequencies A21 >> B(υ) and all emission is spontaneous. A 21 = 8π hν3 c 3 B(ν) 2. Although

More information

This document contains the following supporting information: 1. Wide field scanning electron microscope image

This document contains the following supporting information: 1. Wide field scanning electron microscope image Supporting information for Self-assembled nanoparticle dimer antennas for plasmonic-enhanced single-molecule fluorescence detection at micromolar concentrations Deep Punj, Raju Regmi, Alexis Devilez, Robin

More information

What happens when light falls on a material? Transmission Reflection Absorption Luminescence. Elastic Scattering Inelastic Scattering

What happens when light falls on a material? Transmission Reflection Absorption Luminescence. Elastic Scattering Inelastic Scattering Raman Spectroscopy What happens when light falls on a material? Transmission Reflection Absorption Luminescence Elastic Scattering Inelastic Scattering Raman, Fluorescence and IR Scattering Absorption

More information

Spectral Resolution. Spectral resolution is a measure of the ability to separate nearby features in wavelength space.

Spectral Resolution. Spectral resolution is a measure of the ability to separate nearby features in wavelength space. Spectral Resolution Spectral resolution is a measure of the ability to separate nearby features in wavelength space. R, minimum wavelength separation of two resolved features. Delta lambda often set to

More information

Laserphysik. Prof. Yong Lei & Dr. Yang Xu. Fachgebiet Angewandte Nanophysik, Institut für Physik

Laserphysik. Prof. Yong Lei & Dr. Yang Xu. Fachgebiet Angewandte Nanophysik, Institut für Physik Laserphysik Prof. Yong Lei & Dr. Yang Xu Fachgebiet Angewandte Nanophysik, Institut für Physik Contact: yong.lei@tu-ilmenau.de; yang.xu@tu-ilmenau.de Office: Heisenbergbau V 202, Unterpörlitzer Straße

More information

Comments to Atkins: Physical chemistry, 7th edition.

Comments to Atkins: Physical chemistry, 7th edition. Comments to Atkins: Physical chemistry, 7th edition. Chapter 16: p. 483, Eq. (16.1). The definition that the wave number is the inverse of the wave length should be used. That is much smarter. p. 483-484.

More information

Supporting Information

Supporting Information Supporting Information Cyclodextrin Supramolecular Complex as Water Soluble Ratiometric Sensor for ferric Ion Sensing Meiyun Xu, Shuizhu Wu,* Fang Zeng, Changmin Yu College of Materials Science & Engineering,

More information

Electronic Transition Spectra of Thiophenoxy and Phenoxy Radicals in Hollow cathode discharges

Electronic Transition Spectra of Thiophenoxy and Phenoxy Radicals in Hollow cathode discharges Electronic Transition Spectra of Thiophenoxy and Phenoxy Radicals in Hollow cathode discharges Tokyo Univ. Science Mitsunori ARAKI, Hiromichi WAKO, Kei NIWAYAMA and Koichi TSUKIYAMA 2014/06/16 2015/2/20

More information

24/ Rayleigh and Raman scattering. Stokes and anti-stokes lines. Rotational Raman spectroscopy. Polarizability ellipsoid. Selection rules.

24/ Rayleigh and Raman scattering. Stokes and anti-stokes lines. Rotational Raman spectroscopy. Polarizability ellipsoid. Selection rules. Subject Chemistry Paper No and Title Module No and Title Module Tag 8/ Physical Spectroscopy 24/ Rayleigh and Raman scattering. Stokes and anti-stokes lines. Rotational Raman spectroscopy. Polarizability

More information

Understanding Nanoplasmonics. Greg Sun University of Massachusetts Boston

Understanding Nanoplasmonics. Greg Sun University of Massachusetts Boston Understanding Nanoplasmonics Greg Sun University of Massachusetts Boston Nanoplasmonics Space 100pm 1nm 10nm 100nm 1μm 10μm 100μm 1ns 100ps 10ps Photonics 1ps 100fs 10fs 1fs Time Surface Plasmons Surface

More information

Pre-Lab Exercises Lab 2: Spectroscopy

Pre-Lab Exercises Lab 2: Spectroscopy Pre-Lab Exercises Lab 2: Spectroscopy 1. Which color of visible light has the longest wavelength? Name Date Section 2. List the colors of visible light from highest frequency to lowest frequency. 3. Does

More information

Advanced Spectroscopy Laboratory

Advanced Spectroscopy Laboratory Advanced Spectroscopy Laboratory - Raman Spectroscopy - Emission Spectroscopy - Absorption Spectroscopy - Raman Microscopy - Hyperspectral Imaging Spectroscopy FERGIELAB TM Raman Spectroscopy Absorption

More information

Optical and Photonic Glasses. Lecture 31. Rare Earth Doped Glasses I. Professor Rui Almeida

Optical and Photonic Glasses. Lecture 31. Rare Earth Doped Glasses I. Professor Rui Almeida Optical and Photonic Glasses : Rare Earth Doped Glasses I Professor Rui Almeida International Materials Institute For New Functionality in Glass Lehigh University Rare-earth doped glasses The lanthanide

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

Introduction to Spectroscopic methods

Introduction to Spectroscopic methods Introduction to Spectroscopic methods Spectroscopy: Study of interaction between light* and matter. Spectrometry: Implies a quantitative measurement of intensity. * More generally speaking electromagnetic

More information

Lecture 3: Light absorbance

Lecture 3: Light absorbance Lecture 3: Light absorbance Perturbation Response 1 Light in Chemistry Light Response 0-3 Absorbance spectrum of benzene 2 Absorption Visible Light in Chemistry S 2 S 1 Fluorescence http://www.microscopyu.com

More information

1. Strahlungsgesetze, Ableitung der Planck-schen Strahlungsformel, Einstein-Koeffizienten, Extinktinskoeffizient, Oszillatorenstärke

1. Strahlungsgesetze, Ableitung der Planck-schen Strahlungsformel, Einstein-Koeffizienten, Extinktinskoeffizient, Oszillatorenstärke 1. Strahlungsgesetze, Ableitung der Planck-schen Strahlungsformel, Einstein-Koeffizienten, Extinktinskoeffizient, Oszillatorenstärke Einheiten in diesem Kapitel: diesmal cgs. Energy volume density of blackbody

More information

Optical Spectroscopy. Steady State and Time Dependent Fluorescence Measurements. Kai Wen Teng. October 8 th PHYS 403 Fall 2013

Optical Spectroscopy. Steady State and Time Dependent Fluorescence Measurements. Kai Wen Teng. October 8 th PHYS 403 Fall 2013 Optical Spectroscopy Steady State and Time Dependent Fluorescence Measurements Kai Wen Teng October 8 th 2013 PHYS 403 Fall 2013 EM Spectrum of molecules Rotational Energy Infrared Vibrational Energy Near

More information

Chemistry 524--Final Exam--Keiderling Dec. 12, pm SES

Chemistry 524--Final Exam--Keiderling Dec. 12, pm SES Chemistry 524--Final Exam--Keiderling Dec. 12, 2002 --4-8 pm -- 238 SES Please answer all questions in the answer book provided. Calculators, rulers, pens and pencils are permitted plus one 8.5 x 11 sheet

More information

Förster Energy Transfer - AKA - Fluorescence Resonance Energy Transfer

Förster Energy Transfer - AKA - Fluorescence Resonance Energy Transfer örster Energy Transfer - K - luorescence esonance Energy Transfer 1. Origins: Theory of Energy Transfer developed by T. örster (örster. 1948. nnalen der Physi. :55-75.). evelopment of ET as a Spectroscopic

More information

Luminescence. Photoluminescence (PL) is luminescence that results from optically exciting a sample.

Luminescence. Photoluminescence (PL) is luminescence that results from optically exciting a sample. Luminescence Topics Radiative transitions between electronic states Absorption and Light emission (spontaneous, stimulated) Excitons (singlets and triplets) Franck-Condon shift(stokes shift) and vibrational

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION SUPPLEMENTARY INFORMATION Electroluminescence from a single nanotube-molecule-nanotube junction Christoph W. Marquardt, Sergio Grunder, Alfred Błaszczyk, Simone Dehm, Frank Hennrich, Hilbert v. Löhneysen,

More information

Measurement Examples. Excitation and Emission Scans. Steady State Fluorescence Anisotropy. Kinetic Measurements

Measurement Examples. Excitation and Emission Scans. Steady State Fluorescence Anisotropy. Kinetic Measurements Measurement Examples A division of Edinburgh Instruments Ltd. Excitation and Emission Scans Excitation and emission spectra are standard measurements in fluorescence spectroscopy. The figure demonstrates

More information

Fundamentals of Spectroscopy for Optical Remote Sensing. Course Outline 2009

Fundamentals of Spectroscopy for Optical Remote Sensing. Course Outline 2009 Fundamentals of Spectroscopy for Optical Remote Sensing Course Outline 2009 Part I. Fundamentals of Quantum Mechanics Chapter 1. Concepts of Quantum and Experimental Facts 1.1. Blackbody Radiation and

More information

Fluorescence Quenching

Fluorescence Quenching Summary Fluorescence Quenching The emission of light from the excited state of a molecule (fluorescence or phosphorescence) can be quenched by interaction with another molecule. The stationary and time-dependent

More information

IR Spectrography - Absorption. Raman Spectrography - Scattering. n 0 n M - Raman n 0 - Rayleigh

IR Spectrography - Absorption. Raman Spectrography - Scattering. n 0 n M - Raman n 0 - Rayleigh RAMAN SPECTROSCOPY Scattering Mid-IR and NIR require absorption of radiation from a ground level to an excited state, requires matching of radiation from source with difference in energy states. Raman

More information

Fluorescence Resonance Energy Transfer (FRET) Microscopy

Fluorescence Resonance Energy Transfer (FRET) Microscopy Fluorescence Resonance Energy Transfer () Microscopy Mike Lorenz Optical Technology Development mlorenz@mpi-cbg.de -FLM course, May 2009 What is fluorescence? Stoke s shift Fluorescence light is always

More information

Energy transfer and optical gain studies of FDS: Rh B dye mixture investigated under CW laser excitation

Energy transfer and optical gain studies of FDS: Rh B dye mixture investigated under CW laser excitation Energy transfer and optical gain studies of FDS: Rh B dye mixture investigated under CW laser excitation M. Kailasnath *a, G. Ajith Kumar, V.P.N Nampoori b International School of Photonics, Cochin University

More information

A few Experimental methods for optical spectroscopy Classical methods Modern methods. Remember class #1 Generating fast LASER pulses

A few Experimental methods for optical spectroscopy Classical methods Modern methods. Remember class #1 Generating fast LASER pulses A few Experimental methods for optical spectroscopy Classical methods Modern methods Shorter class Remember class #1 Generating fast LASER pulses, 2017 Uwe Burghaus, Fargo, ND, USA W. Demtröder, Laser

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

Solution set for EXAM IN TFY4265/FY8906 Biophysical microtechniques

Solution set for EXAM IN TFY4265/FY8906 Biophysical microtechniques ENGLISH NORWEGIAN UNIVERSITY OF SCIENCE AND TECHNOLOGY DEPARTMENT OF PHYSICS Contact during exam: Magnus Borstad Lilledahl Telefon: 73591873 (office) 92851014 (mobile) Solution set for EXAM IN TFY4265/FY8906

More information

Elements of Quantum Optics

Elements of Quantum Optics Pierre Meystre Murray Sargent III Elements of Quantum Optics Fourth Edition With 124 Figures fya Springer Contents 1 Classical Electromagnetic Fields 1 1.1 Maxwell's Equations in a Vacuum 2 1.2 Maxwell's

More information

Chapter 2 Energy Transfer Review

Chapter 2 Energy Transfer Review Chapter 2 Energy Transfer Review In this chapter, we discuss the basic concepts of excitation energy transfer, making the distinction between radiative and nonradiative, and giving a brief overview on

More information

Implementation and evaluation of data analysis strategies for time-resolved optical spectroscopy

Implementation and evaluation of data analysis strategies for time-resolved optical spectroscopy Supporting information Implementation and evaluation of data analysis strategies for time-resolved optical spectroscopy Chavdar Slavov, Helvi Hartmann, Josef Wachtveitl Institute of Physical and Theoretical

More information

Road map (Where are we headed?)

Road map (Where are we headed?) Road map (Where are we headed?) oal: Fairly high level understanding of carrier transport and optical transitions in semiconductors Necessary Ingredients Crystal Structure Lattice Vibrations Free Electron

More information

Laser Physics OXFORD UNIVERSITY PRESS SIMON HOOKER COLIN WEBB. and. Department of Physics, University of Oxford

Laser Physics OXFORD UNIVERSITY PRESS SIMON HOOKER COLIN WEBB. and. Department of Physics, University of Oxford Laser Physics SIMON HOOKER and COLIN WEBB Department of Physics, University of Oxford OXFORD UNIVERSITY PRESS Contents 1 Introduction 1.1 The laser 1.2 Electromagnetic radiation in a closed cavity 1.2.1

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

Emission Spectrum of Atomic Gases. Prelab Questions

Emission Spectrum of Atomic Gases. Prelab Questions Emission Spectrum of Atomic Gases Prelab Questions Before this coming to this lab, please review your text for the physics of the spectrum of visible light and of diffraction grating spectrometer.. Which

More information

P. Lambrev October 10, 2018

P. Lambrev October 10, 2018 TIME-RESOLVED OPTICAL SPECTROSCOPY Petar Lambrev Laboratory of Photosynthetic Membranes Institute of Plant Biology The Essence of Spectroscopy spectro-scopy: seeing the ghosts of molecules Kirchhoff s

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

Excited State Processes

Excited State Processes Excited State Processes Photophysics Fluorescence (singlet state emission) Phosphorescence (triplet state emission) Internal conversion (transition to singlet gr. state) Intersystem crossing (transition

More information

Aula 5 e 6 Transferência de Energia e Transferência de Elétron Caminhos de espécies fotoexcitadas

Aula 5 e 6 Transferência de Energia e Transferência de Elétron Caminhos de espécies fotoexcitadas Fotoquímica Aula 5 e 6 Transferência de Energia e Transferência de Elétron Prof. Amilcar Machulek Junior IQ/USP - CEPEMA Caminhos de espécies fotoexcitadas 1 Diagrama de Jablonski S 2 Relaxation (τ < 1ps)

More information

MEFT / Quantum Optics and Lasers. Suggested problems Set 4 Gonçalo Figueira, spring 2015

MEFT / Quantum Optics and Lasers. Suggested problems Set 4 Gonçalo Figueira, spring 2015 MEFT / Quantum Optics and Lasers Suggested problems Set 4 Gonçalo Figueira, spring 05 Note: some problems are taken or adapted from Fundamentals of Photonics, in which case the corresponding number is

More information

Fluorescence Spectroscopy

Fluorescence Spectroscopy Fluorescence Spectroscopy Steady State and Time Dependent Fluorescence Measurements Kai Wen Teng PHYS 403 Fall 15 EM Spectrum of molecules Rotational Energy Infrared Vibrational Energy Near Infrared Electronic

More information

Lecture 0. NC State University

Lecture 0. NC State University Chemistry 736 Lecture 0 Overview NC State University Overview of Spectroscopy Electronic states and energies Transitions between states Absorption and emission Electronic spectroscopy Instrumentation Concepts

More information

Abstract... I. Acknowledgements... III. Table of Content... V. List of Tables... VIII. List of Figures... IX

Abstract... I. Acknowledgements... III. Table of Content... V. List of Tables... VIII. List of Figures... IX Abstract... I Acknowledgements... III Table of Content... V List of Tables... VIII List of Figures... IX Chapter One IR-VUV Photoionization Spectroscopy 1.1 Introduction... 1 1.2 Vacuum-Ultraviolet-Ionization

More information

PRINCIPLES OF NONLINEAR OPTICAL SPECTROSCOPY

PRINCIPLES OF NONLINEAR OPTICAL SPECTROSCOPY PRINCIPLES OF NONLINEAR OPTICAL SPECTROSCOPY Shaul Mukamel University of Rochester Rochester, New York New York Oxford OXFORD UNIVERSITY PRESS 1995 Contents 1. Introduction 3 Linear versus Nonlinear Spectroscopy

More information

APEX CARE INSTITUTE FOR PG - TRB, SLET AND NET IN PHYSICS

APEX CARE INSTITUTE FOR PG - TRB, SLET AND NET IN PHYSICS Page 1 1. Within the nucleus, the charge distribution A) Is constant, but falls to zero sharply at the nuclear radius B) Increases linearly from the centre, but falls off exponentially at the surface C)

More information

Ultraviolet-Visible and Infrared Spectrophotometry

Ultraviolet-Visible and Infrared Spectrophotometry Ultraviolet-Visible and Infrared Spectrophotometry Ahmad Aqel Ifseisi Assistant Professor of Analytical Chemistry College of Science, Department of Chemistry King Saud University P.O. Box 2455 Riyadh 11451

More information

Supplementary information for. Observation of photovoltaic action from photoacid-modified Nafion due to light-driven ion transport

Supplementary information for. Observation of photovoltaic action from photoacid-modified Nafion due to light-driven ion transport Supplementary information for Observation of photovoltaic action from photoacid-modified Nafion due to light-driven ion transport William White, a# Christopher D. Sanborn, a# Ronald S. Reiter, a David

More information

Absorption and scattering

Absorption and scattering Absorption and scattering When a beam of radiation goes through the atmosphere, it encounters gas molecules, aerosols, cloud droplets, and ice crystals. These objects perturb the radiation field. Part

More information

CHEM6416 Theory of Molecular Spectroscopy 2013Jan Spectroscopy frequency dependence of the interaction of light with matter

CHEM6416 Theory of Molecular Spectroscopy 2013Jan Spectroscopy frequency dependence of the interaction of light with matter CHEM6416 Theory of Molecular Spectroscopy 2013Jan22 1 1. Spectroscopy frequency dependence of the interaction of light with matter 1.1. Absorption (excitation), emission, diffraction, scattering, refraction

More information

High Resolution Laser Microscopy: a fascinating method to explore the molecular world

High Resolution Laser Microscopy: a fascinating method to explore the molecular world High Resolution Laser Microscopy: a fascinating method to explore the molecular world Alfred J. Meixner Physical and Theoretical Chemistry Laboratory University of Siegen Single-molecule spectroscopy and

More information

Frequency- and Time-Domain Spectroscopy

Frequency- and Time-Domain Spectroscopy Frequency- and Time-Domain Spectroscopy We just showed that you could characterize a system by taking an absorption spectrum. We select a frequency component using a grating or prism, irradiate the sample,

More information

MOLECULAR SPECTROSCOPY

MOLECULAR SPECTROSCOPY MOLECULAR SPECTROSCOPY First Edition Jeanne L. McHale University of Idaho PRENTICE HALL, Upper Saddle River, New Jersey 07458 CONTENTS PREFACE xiii 1 INTRODUCTION AND REVIEW 1 1.1 Historical Perspective

More information

E L E C T R O P H O S P H O R E S C E N C E

E L E C T R O P H O S P H O R E S C E N C E Organic LEDs part 4 E L E C T R O P H O S P H O R E S C E C E. OLED efficiency 2. Spin 3. Energy transfer 4. Organic phosphors 5. Singlet/triplet ratios 6. Phosphor sensitized fluorescence 7. Endothermic

More information

Rotational Brownian motion; Fluorescence correlation spectroscpy; Photobleaching and FRET. David A. Case Rutgers, Spring 2009

Rotational Brownian motion; Fluorescence correlation spectroscpy; Photobleaching and FRET. David A. Case Rutgers, Spring 2009 Rotational Brownian motion; Fluorescence correlation spectroscpy; Photobleaching and FRET David A. Case Rutgers, Spring 2009 Techniques based on rotational motion What we studied last time probed translational

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