Everything about Raman Spectroscopy totally explained
Raman spectroscopy is a
spectroscopic technique used in
condensed matter physics and
chemistry to study vibrational, rotational, and other low-frequency modes in a system. It relies on
inelastic scattering, or
Raman scattering of monochromatic light, usually from a
laser in the
visible,
near infrared, or
near ultraviolet range. The laser light interacts with
phonons or other excitations in the system, resulting in the energy of the laser photons being shifted up or down. The shift in energy gives information about the phonon modes in the system.
Infrared spectroscopy yields similar, but complementary information.
Typically, a sample is illuminated with a laser beam. Light from the illuminated spot is collected with a
lens and sent through a
monochromator. Wavelengths close to the laser line, due to elastic
Rayleigh scattering, are filtered out while the rest of the collected light is dispersed onto a detector.
Spontaneous
Raman scattering is typically very weak, and as a result the main difficulty of Raman spectroscopy is separating the weak inelastically scattered light from the intense Rayleigh scattered laser light. Raman
spectrometers typically use holographic
diffraction gratings and multiple dispersion stages to achieve a high degree of laser rejection. In the past,
PMTs were the detectors of choice for dispersive Raman setups, which resulted in long acquisition times. However, the recent uses of
CCD detectors have made dispersive Raman spectral acquisition much more rapid.
Raman spectroscopy has a stimulated version, analogous to
stimulated emission, called stimulated Raman scattering.
Basic theory
The Raman effect occurs when light impinges upon a
molecule and interacts with the electron cloud of the bonds of that molecule. The incident
photon excites one of the electrons into a virtual state. For the spontaneous Raman effect, the molecule will be excited from the ground state to a virtual energy state, and relax into a vibrational excited state, which generates Stokes Raman scattering. If the molecule was already in an elevated vibrational energy state, the Raman scattering is then called anti-Stokes Raman scattering.
A molecular polarizability change, or amount of deformation of the electron cloud, with respect to the
vibrational coordinate is required for the molecule to exhibit the Raman effect. The amount of the polarizability change will determine the Raman scattering intensity, whereas the Raman shift is equal to the vibrational level that's involved.
History
Although the inelastic scattering of light was predicted by Smekal in 1923, it wasn't until 1928 that it was observed in practice. The Raman effect was named after one of its discoverers, the Indian scientist
Sir C. V. Raman who observed the effect by means of sunlight (1928, together with K. S. Krishnan and independently by
Grigory Landsberg and
Leonid Mandelstam).
Raman spectroscopy can be used to investigate the chemical composition of historical documents such as the
Book of Kells and contribute to knowledge of the social and economic conditions at the time the documents were produced. This is especially helpful because Raman spectroscopy offers a non-invasive way to determine the best course of
preservation or
conservation treatment for such materials.
Raman microspectroscopy
Raman spectroscopy offers several advantages for
microscopic analysis. Since it's a scattering technique, specimens don't need to be fixed or sectioned. Raman spectra can be collected from a very small volume (< 1 µm in diameter); these spectra allow the identification of species present in that volume. Water doesn't interfere very strongly. Thus, Raman spectroscopy is suitable for the microscopic examination of
minerals, materials such as polymers and ceramics,
cells and
proteins. A Raman microscope begins with a standard optical microscope, and adds an excitation laser, a
monochromator, and a sensitive detector (such as a
charge-coupled device (CCD), or
photomultiplier tube (PMT)).
FT-Raman has also been used with microscopes.
In
direct imaging, the whole field of view is examined for scattering over a small range of wavenumbers (Raman shifts). For instance, a wavenumber characteristic for cholesterol could be used to record the distribution of cholesterol within a cell culture.
The other approach is
hyperspectral imaging or
chemical imaging, in which thousands of Raman spectra are acquired from all over the field of view. The data can then be used to generate images showing the location and amount of different components. Taking the cell culture example, a hyperspectral image could show the distribution of cholesterol, as well as proteins, nucleic acids, and fatty acids. Sophisticated signal- and image-processing techniques can be used to ignore the presence of water, culture media, buffers, and other interferents.
Raman microscopy, and in particular
confocal microscopy, has very high spatial resolution. For example, the lateral and depth resolutions were 250 nm and 1.7 µm, respectively, using a confocal Raman microspectrometer with the 632.8 nm line from a He-Ne
laser with a pinhole of 100 µm diameter.
Since the objective lenses of microscopes focus the laser beam to several micrometres in diameter, the resulting photon flux is much higher than achieved in conventional Raman setups. This has the added benefit of enhanced
fluorescence quenching. However, the high photon flux can also cause sample degradation, and for this reason some setups require a thermally conducting substrate (which acts as a heat sink) in order to mitigate this process.
By using Raman microspectroscopy,
in vivo time- and space-resolved Raman spectra of microscopic regions of samples can be measured. As a result, the
fluorescence of water, media, and buffers can be removed. Consequently
in vivo time- and space-resolved Raman spectroscopy is suitable to examine
proteins,
cells and
organs.
Raman microscopy for biological and medical specimens generally uses
near-infrared (NIR) lasers (785 nm diodes and 1064 nm Nd:YAG are especially common). This reduces the risk of damaging the specimen by applying high power. However, the intensity of NIR Raman is low (owing to the ω
-4 dependence of Raman scattering intensity), and most detectors required very long collection times. Recently, more sensitive detectors have become available, making the technique better suited to general use. Raman microscopy of inorganic specimens, such as rocks and ceramics and polymers, can use a broader range of excitation wavelengths.
Variations
Several variations of Raman spectroscopy have been developed. The usual purpose is to enhance the sensitivity (for example, surface-enhanced Raman), to improve the spatial resolution (Raman microscopy), or to acquire very specific information (resonance Raman).
- Surface Enhanced Raman Spectroscopy (SERS) - Normally done in a silver or gold colloid or a substrate containing silver or gold. Surface plasmons of silver and gold are excited by the laser, resulting in an increase in the electric fields surrounding the metal. Given that Raman intensities are proportional to the electric field, there's large increase in the measured signal (by up to 1011). This effect was originally observed by Fleishman but the prevailing explanation was proposed by Van Duyne in 1977.
Hyper Raman - A non-linear effect in which the vibrational modes interact with the second harmonic of the excitation beam. This requires very high power, but allows the observation of vibrational modes which are normally "silent". It frequently relies on SERS-type enhancement to boost the sensitivity.
Resonance Raman spectroscopy - The excitation wavelength is matched to an electronic transition of the molecule or crystal, so that vibrational modes associated with the excited electronic state are greatly enhanced. This is useful for studying large molecules such as polypeptides, which might show hundreds of bands in "conventional" Raman spectra. It is also useful for associating normal modes with their observed frequency shifts.
Spontaneous Raman Spectroscopy - Used to study the temperature dependence of the Raman spectra of molecules.
Optical Tweezers Raman Spectroscopy (OTRS) - Used to study individual particles, and even biochemical processes in single cells trapped by optical tweezers.
Stimulated Raman Spectroscopy - A two color pulse transfers the population from ground to a rovibrationally excited state, if the difference in energy corresponds to an allowed Raman transition. Two photon UV ionization, applied after the population transfer but before relaxation, allows the intra-molecular or inter-molecular Raman spectrum of a gas or molecular cluster (indeed, a given conformation of molecular cluster) to be collected. This is a useful molecular dynamics technique.
Spatially Offset Raman Spectroscopy (SORS) - The Raman scatter is collected from regions laterally offset away from the excitation laser spot, leading to significantly lower contributions from the surface layer than with traditional Raman spectroscopy.
Coherent anti-Stokes Raman spectroscopy (CARS) - Two laser beams are used to generate a coherent anti-Stokes frequency beam, which can be enhanced by resonance.Further Information
Get more info on 'Raman Spectroscopy'.
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