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Lecture Date: January 18 th , 2007 Introduction to Spectroscopy

Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

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Page 1: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

Lecture Date: January 18th, 2007

Introduction to Spectroscopy

Page 2: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

What is Spectroscopy?

The study of the interaction between radiation and matter

“Analytical spectroscopy”, as defined in this class, covers applications of spectroscopy to chemical analysis

Page 3: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

History of Analytical Spectroscopy

1666: Isaac Newton (England) shows that white light can be dispersed into constituent colors, and coins the term “spectrum”

– Newton also produced the first “spectroscope” based on lenses, a prism, and a screen

1800: W. Herschel and J. W. Ritter show that infrared (IR) and ultraviolet (UV) light are part of the spectrum

1814: Joseph Fraunhofer noticed that the sun’s spectrum contains a number of dark lines, developed the diffraction grating

1859: G. Kirchoff obtains spectra of the elements, explains the sun’s spectrum

Page 4: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

The Visible Spectrum of the Sun

(Black lines are absorption by elements in the cooler outer region of the star)

Figure from National Optical Astronomy Observatory/Association of Universities for Research in Astronomy/National Science Foundation, http://www.noao.edu/image_gallery/html/im0600.html

Page 5: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

History of Analytical Spectroscopy

1870: J. C. Maxwell formalizes and combines the laws of electricity and magnetism

1900 to present: More than 25 Nobel prizes awarded to spectroscopists, including:

– 1902: H. A. Lorentz and P. Zeeman

– 1919: J. Stark

– 1933: P. A. M. Dirac and E. Schrodinger

– 1945: W. Pauli

….

– 1999: A. Zewail

Page 6: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

Introduction to Spectroscopy

Figures from NASA (www.nasa.gov)

The electromagnetic spectrum

Each color you see is a specific (narrow) range of frequencies in this spectrum

Page 7: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

The Electromagnetic Spectrum

Modern life (not just analytical spectroscopy) revolves around the EM spectrum!

Page 8: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

Properties of Electromagnetic Radiation

Wave/particle duality

Perpendicular E and B components

– E = electric field

– B = magnetic field

Wave properties:– Wavelength (frequency)

– Amplitude

– Phase

1 2 3 4 5

-1

-0.5

0.5

1

1 2 3 4 5

-1

-0.5

0.5

1

Long wavelength(low frequency)

Short wavelength(high frequency)

c = the speed of light (~3.00 x 108 m/s) = the frequency in cycles/second (Hz) = the wavelength in meters/cycle

c

Note – this figure shows polarized radiation!

Page 9: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

Interference of Radiation

Monochromatic: radiation containing a single frequency

Polychromatic: radiation containing multiple frequencies

Constructive interference: when two waves reinforce each other

Destructive interference: when two waves cancel each other

Page 10: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

The Interaction of Radiation and Matter

Electromagnetic radiation travels fastest in a vacuum

When not travelling in a vacuum, radiation and matter can interact in a number of ways

Some key processes (for spectroscopy):

– Diffraction

– Refraction

– Scattering

– Polarization

– Absorption

Page 11: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

Transmission of Radiation

The velocity at which radiation travels (or propagates) through a medium is dependent on the medium itself

When radiation travels through a medium and does not undergo a frequency change, it cannot be undergoing a permanent energy transfer

However, radiation can still interact with the medium

– Radiation, an EM field, polarizes the electron clouds of atoms in the medium

– Polarization is a temporary deformation of the electron clouds

Page 12: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

Transmission and Refraction

The refractive index (ni) of a medium is given by:

ii

c n

c = the speed of light (~3.00 x 108 m/s) i = the velocity of the radiation in the medium in m/sni = the refractive index at the frequency i

Refractive index measures the degree of interaction between the radiation and the medium– Liquids: ni ~ 1.3 to 1.8

– Solids: ni ~ 1.3 to 2.5

Refractive index can be used to identify pure liquid substances

Page 13: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

Refraction

When radiation passes through an interface between two media with different refractive indices, it can abruptly change direction

Snell’s law:

1

2

2

1

2

1

sin

sin

v

v

n

n

1 = the velocity of the radiation in medium 1 in m/sn1 = the refractive index in medium 1

Snell’s law is a consequence of the change in velocity in the media

Reflection always occurs at an interface. Its extent depends on the refractive indices of the media

1

2

Medium 1

Medium 2

Page 14: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

Diffraction

Fraunhofer diffraction:

– Also known as far-field diffraction, parallel beam diffraction

– Important in optical microscopy

Fresnel diffraction

– Also known as near-field diffraction

Page 15: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

Diffraction

Diffraction gratings:

– Widely used in spectroscopic instruments to separate frequencies (can be made precisely)

sin2d n

http://www.astro.virginia.edu/research/observatories/40inch/fobos/images/grating.jpg

Bragg diffraction – multiple slit Fraunhofer diffraction:

– Important for instrument design, crystallography

Page 16: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

Scattering

Rayleigh scattering (an elastic process):

– Scattering of small amounts of radiation by molecules and atoms (whose size is near to the wavelength of the radiation)

Mie scattering: applies to large particles, involves scattering in different directions.

– Practical use in particle size analysis

4

1

scattering

Page 17: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

Polarization

Polarization of EM radiation – a simple classical picture:

Figure from Sears, et al., “University Physics”, 7th Ed., 1988

Page 18: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

Coherent Radiation

Coherent radiation fulfils two conditions: (1) it has the same frequency or set of frequencies, and (2) it has a well-defined and constant phase relationship

– Coherent radiation is “cross-corelated” in that the properties of one beam can be used to predict those of the other beam

Examples of coherent radiation:

– Lasers

– Microwave sources (masers)

Coherent radiation: different frequencies (colors) with a defined

phase relationship interfere to produce a pulse

Diagram from wikipedia.org (public domain)

Page 19: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

Incoherent Radiation

Produced by “random” emission, e.g. individual atoms in a large sample emitting photons

Actually is coherent, but just to a tiny (undetectable) extent

Also known as “continuous” radiation

Examples of incoherent radiation:

– Incandescent light bulbs

– Filament sources

– Deuterium lamps

Incoherent radiation: different frequencies (colors) combined to produce continuous radiation with

varying phase, frequency and amplitude

Diagram from wikipedia.org (public domain)

Page 20: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

More Properties of Electromagnetic Radiation

Wave and particle behavior: photons behave as both waves and particles

– Quantum mechanics developed around the concept of the photon, the elementary unit of radiation

Planck’s law:

E is the energy of the photon in joules h is Planck's constant (6.624 x 10-34 joule seconds) is the frequency of the radiation

hE

Page 21: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

Absorption and Emission

Absorption is a process accompanied by an energy change

– involves energy transfer of EM radiation to a substance, usually at specific frequencies corresponding to natural atomic or molecular energies

Emission occurs when matter releases energy in the form of radiation (photons

E = h

Higher energy

Lower energy

Absorption Emission

Page 22: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

Energy Levels

Several types of quantum-mechanical energy levels occur in nature:

– Electronic

– Rotational

– Vibrational (including phonons and heat)

– Nuclear

For each of these, a discrete quantum “state” and energy-driven transitions between these “states” can be studied (as opposed to a continuous range of energies)

Page 23: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

The Uncertainty of Measurements

Because the lifetimes of quantum states can persist for short periods, it can be difficult to measure their energies accurately

This is usually stated in the form of an “energy-time uncertainty”:

tE

Page 24: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

The Uncertainty Principle

The uncertainty principle: it is not possible to know both the location and the momentum of a particle exactly – a fundamental limit on all measurements

In Heisenberg’s terms, the act of measuring a particle’s position affects its momentum, and vice versa

In equation form:

– In other words, if you know the position of a particle to within x, then you can specify its momentum along x to px

– As the uncertainty in x increases (x ), that of px decreases (x ), and vice versa

px x 21

Page 25: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

Spectra and Spectrometers

Spectra are usually plotted as frequency vs. amplitude

– Instead of energy, wavelength or energy (related properties) can also be used

– The choice of x- and y-axes is often dependent on the particular technique, its history, etc…

– Key parameter is frequency/energy/wavelength resolution

Spectrometers: instruments that measure the interaction of radiation with matter, so the properties of such interactions can be studied

Page 26: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

Spectroscopy in Analytical Chemistry

Widely used approach for characterizing systems ranging from chemical physics to biology, from individual atoms to the largest molecules

Some of the most common techniques are:

– UV-Visible spectroscopy

– IR spectroscopy

– Raman spectroscopy

– X-ray spectroscopy

– NMR spectroscopy

– EPR spectroscopy

Page 27: Lecture Date: January 18 th, 2007 Introduction to Spectroscopy

Further Reading

P. W. Atkins and R. S. Friedman, Molecular Quantum Mechanics, 3rd Ed. Oxford, New York (2003)

R. P. Feynman, R. B. Leighton, M. Sands, The Feynman Lectures on Physics, Addison-Wesley, Reading MA (1977)

Any good physics text!