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CHEM 4396 (W237) Physical Chemistry Laboratory Fall 2009 Absorption Spectra of Nano-particles Instructor: Dr. Aleksey I. Filin Absorption Spectra of Nano-particles CHEM 4396 (W237) Physical Chemistry Laboratory Fall 2009 Introduction Conduction band Energy gap Electron energy Electron energy band structure in semiconductor - Forbidden band Valence band Eph>Eg If the photon energy is higher than the energy gap the electron can be excited We work with CdSe nanostructures (quantum dots) Energy gap of bulk CdSe is Eg = 1.829 eV @ room temperature Instructor: Dr. Aleksey I. Filin Absorption Spectra of Nano-particles CHEM 4396 (W237) Physical Chemistry Laboratory Fall 2009 Introduction Conduction band Energy gap Electron energy Electron energy band structure in semiconductor + Forbidden band Valence band Electron being excited left in the valence band positively charged quasi-particle known as the electronic hole, or the hole. Positively charged hole interacts with negatively charged electron by Coulomb interaction. Instructor: Dr. Aleksey I. Filin Absorption Spectra of Nano-particles CHEM 4396 (W237) Physical Chemistry Laboratory Fall 2009 Introduction Conduction band Energy gap Electron energy Electron energy band structure in semiconductor + Forbidden band Valence band Exciton: Large and strongly interactive particles formed when an electron, excited by a photon into the conduction band of a semiconductor, binds with the positively charged hole it left behind in the valence band. Exciton Bohr radius is the smallest possible orbit for the electron, that with the lowest energy, is most likely to be found at a distance from the hole Instructor: Dr. Aleksey I. Filin Absorption Spectra of Nano-particles CHEM 4396 (W237) Physical Chemistry Laboratory Fall 2009 Introduction Electron energy band structure in semiconductor F ma a F Why the effective charge of the hole is positive? Lack of mass Lack of charge m is negative! negative mass negative charge Instructor: Dr. Aleksey I. Filin CHEM 4396 (W237) Physical Chemistry Laboratory Fall 2009 Absorption Spectra of Nano-particles Introduction A Quantum Dot is: A crystal of semiconductor compound (eg. CdSe, PbS) with a diameter on the order of the compound's Exciton Bohr Radius Or: A nanostructure that confines the motion of Excitons in all three spatial directions Exciton is an atomic-like quasi-particle, so, its energy spectrum is similar to that for Hydrogen atom Instructor: Dr. Aleksey I. Filin Absorption Spectra of Nano-particles CHEM 4396 (W237) Physical Chemistry Laboratory Fall 2009 Introduction Low dimensional structures 3D 2D 1D y y y z x Bulk: motion is not confined at all z x Quantum well: motion is not confined in 2 dimensions y z x Quantum wire: motion is not confined in 1 dimensions 0D z x Quantum Dot: motion is confined in all dimensions Instructor: Dr. Aleksey I. Filin Absorption Spectra of Nano-particles CHEM 4396 (W237) Physical Chemistry Laboratory Fall 2009 Introduction Energy Wavefunction of Electron in Quantum Well WF of electron in QW can contain only integer number of half wavelength -> Energy spectrum of electron in QW is discrete Instructor: Dr. Aleksey I. Filin Absorption Spectra of Nano-particles CHEM 4396 (W237) Physical Chemistry Laboratory Fall 2009 Introduction Energy Wavefunction of Electron in Quantum Well Energy level shifts towards higher energy for smaller size Instructor: Dr. Aleksey I. Filin Absorption Spectra of Nano-particles CHEM 4396 (W237) Physical Chemistry Laboratory Fall 2009 Absorption Spectra Absorbance (in diagram form) Bulk Single QD in theory 0 Eg Photon energy Lowest exciton state Energy spectrum of exciton in QD is discrete (or quantized) (similar to spectrum of electron in QW) Instructor: Dr. Aleksey I. Filin Absorption Spectra of Nano-particles CHEM 4396 (W237) Physical Chemistry Laboratory Fall 2009 Absorption Spectra Position of lowest exciton state (as well as other states) depends on particle size: energy level shifts towards higher energy for smaller size (similar to electron in quantum well) Absorbance (in diagram form) Average size Bigger size Smaller size Each sample contains mostly the particles of certain average size. There is also some amount of particles of bigger and smaller sizes. 0 Absorption lines are broadened due to particles size distribution: Eg Photon energy Absorption lines have near-Gaussian shape due to nearGaussian particles size distribution Instructor: Dr. Aleksey I. Filin Absorption Spectra of Nano-particles CHEM 4396 (W237) Physical Chemistry Laboratory Fall 2009 Absorption Spectra Absorbance (in diagram form) 0 Eg Photon energy Lowest exciton state For each sample, the lowest exciton state position is defined by average particle size Instructor: Dr. Aleksey I. Filin Absorption Spectra of Nano-particles CHEM 4396 (W237) Physical Chemistry Laboratory Fall 2009 Absorption Spectra Absorbance (in diagram form) 1hr 2hrs 4hrs 0.5hrs 0 Photon energy Samples were heat treated @7000C for different times (0.5, 1, 2 and 4 hrs). Average particle size increases with increasing of heat treatment time. Absorption peak position shifts towards lower energy with average particle size increasing. Instructor: Dr. Aleksey I. Filin Absorption Spectra of Nano-particles CHEM 4396 (W237) Physical Chemistry Laboratory Fall 2009 Typical absorption spectra of CdSe nanoparticles Real experimental lines are broadened due to particles size distribution Instructor: Dr. Aleksey I. Filin Absorption Spectra of Nano-particles CHEM 4396 (W237) Physical Chemistry Laboratory Fall 2009 Our goals: • investigate the absorption spectra of nanoparticles (QDs) embedded in glass; • define the lowest exciton absorption peak position for each sample; • analyze the data and calculate an average particle size for each sample. Instructor: Dr. Aleksey I. Filin Absorption Spectra of Nano-particles CHEM 4396 (W237) Physical Chemistry Laboratory Fall 2009 Measurements Spectrophotometer measures absorbance vs. wavelength Absorbance Absorbance Theory works with absorbance vs. photon energy 0 0 Wavelength Photon energy Lowest exciton state To transfer wavelength into energy, use the formula: 1240 E[eV ] [nm] Instructor: Dr. Aleksey I. Filin Absorption Spectra of Nano-particles CHEM 4396 (W237) Physical Chemistry Laboratory Fall 2009 Data Analysis Gaussian Parabola y Gaussian + Parabola y y + = x x x Maximum of (Gaussian + Parabola) curve is shifted in comparison with that for the Gaussian curve. To find the correct position of Gaussian we have to subtract the background from the summary curve Instructor: Dr. Aleksey I. Filin Absorption Spectra of Nano-particles CHEM 4396 (W237) Physical Chemistry Laboratory Fall 2009 Data Analysis Absorbance Parabola (result of your fit) Gaussian + Parabola (your experimental curve) Gaussian 0 Wavelength •Pick 2 points on the left and 2 points on the right shoulders of the peak •Fit this 4 points with parabola •Subtract the parabola from the experimental curve •You get the unshifted position of the lowest exciton absorption peak •Find the wavelength, corresponding to the maximum position •Calculate the energy, corresponding to this wavelength Instructor: Dr. Aleksey I. Filin Absorption Spectra of Nano-particles CHEM 4396 (W237) Physical Chemistry Laboratory Fall 2009 Data Analysis Energy can be calculated using formula E[eV]=1240/[nm] In theory, dependence of the shift of lowest exciton absorption state Ex on nanoparticle radius r can be approximately expressed as: Ex = Eg + 0.038[eV]+ 2.4[eV*nm2]/r2 (After Ekimov et al, J. Opt. Soc. Am. B10, January 1993) Energy gap of bulk CdSe is Eg = 1.829 eV So, you know the Ex for the particle, you can calculate the particle size as: r[nm] 2.4[eV nm 2 ] E x [eV ] E g [eV ] 0.038eV Instructor: Dr. Aleksey I. Filin Absorption Spectra of Nano-particles CHEM 4396 (W237) Physical Chemistry Laboratory Fall 2009 Summary We measure the absorption spectra of CdSe nanoparticles in glass We define the energy of lowest exciton absorption peak position We estimate the average size of the nanoparticles in each sample Instructor: Dr. Aleksey I. Filin