Circular dichroism (CD) is the difference in light
absorbance between left- (L-CPL) and right-circularly
polarised light (R-CPL) and circular dichroism
spectrometers (spectrophotometers) are highly
specialised variations of the absorbance
spectrophotometer.
A circular dichroism spectrophotometer is also commonly
termed a circular dichroism spectropolarimeter or a
circular dichrograph. Most modern circular dichroism
instruments operate on the same principles, which is
demonstrated in the slide show at the bottom of the page.
There is a source of monochromatic linearly polarised light
which can be turned into either left- or right-circularly
polarised light by passing it through a quarter-wave plate
whose unique axis is at 45 degrees to the linear polarisation
plane as described in the section about polarised light.
Instead of a static quarter-wave plate, a circular dichroism
spectrophotometer has a specialised optical element called
a photo-elastic modulator (PEM). This is a piezoelectric
element cemented to a block of fused silica. At rest, when
the piezoelectric element is not oscillating, the silica block is
not birefringent; when driven, the piezoelectric element
oscillates at its resonance frequency (typically around 50
kHz), and induces stress in the silica in such a way that it
becomes birefringent. The alternating stress turns the fused
silica element into a dynamic quarter-wave plate, retarding
first vertical with respect to horizontal components of the
incident linearly polarised light by a quarter-wave and then
vice versa, producing left- and then right- circularly polarised
light at the drive frequency. The amplitude of the oscillation
is tuned so that the retardation is appropriate for the
wavelength of light passing through the silica block.
On the other side of the sample position there is a light
detector. When there is no circularly dichroic sample in the
light path, the light hitting the detector is constant. If there is a
circularly dichroic sample in the light path, the recorded light
intensity will be different for right- and left-CPL. Using a lock-
in amplifier tuned to the frequency of the PEM, it is possible
to measure the difference in intensity between the two
circular polarisations (vAC). The average total light intensity
across many PEM oscillations (vDC) can be used to scale
the size of the lock-in amplifier signal to take into account
variations in total light level. Both signals can be recorded
and from them the circular dichroism signal can be
calculated easily by dividing the vAC component by the vDC
signal.
G is a calibration-scaling factor to provide either ellipticity or
differential absorbance. The section about CD Units and
their inter-conversion explains how ellipticity and differential
absorbance are related.
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http://newdrugapprovals.org/
DRUG APPROVALS BY DR ANTHONY MELVIN CRASTO
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At the top of Preikestolen with view over the Lysefjord, Norway
Norway - Bergen Cityscape by AgiVega
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