ch1 spectroscopy
TRANSCRIPT
Ch1 Spectroscopy
1. More than half
of all instrumental
methods of
analysis involve the
absorption or
emission of light.
Thus the
degree of light
absorption and the
intensity of light
emission are
the critical
measurements
2. Characterizing
Light
Particle theory of
light
Wave theory of
light
Electromagnetic
Wave3.
3. Radiant Energy
(Wave theory)
Luminance (亮度)
Φ: 光通量 Ω: 立體角θ: 給定方向與單位面積元 ds 法線方向的夾角Luminous intensity
(發光強度)
Φ: 光通量 Ω: 立體角4.Photon Energy
Wavenumber=1/
(𝒄𝒎)5.AbsorptionExcitationEmission
5.Beer’s Law For liquids For gases𝑇 : Transmission (or transmissivity) 𝛼 : Absorption coefficient of the substance 𝑙 : Path length 𝜀 : Molar
absorptivity (extinction coefficient) of the absorber 𝑐 : Molar concentration of
absorbing species in the material 𝜎 : Absorption cross section 𝑁 : Number density of absorbers 𝛼 = ′ 𝛼ln 10 = 2.303𝛼6. Cuvettemade of plastic,
glass, or fused quartz (for UV light) Beer’s Law PlotWavelength of Maximum Absorbance• The larger the molar absorptivity, the more sensitive the method. The greatest analytical sensitivity occurs at the wavelength at which the absorptivity is a maximum.Ch2Ultravioletvis
ibleSpectrometry
This technique is
complementary 螢光光譜某些物質經某波長入射光照射後,分子被激發從基態到激發態,並在很短時間內去激發從激發態返回基態,發出波長長於入射光的螢光。因此入射光的
能量(hν)需大於螢光能量。Light Sources
Visible light(鎢絲燈UV light 氘燈Ultraviolet-Visible
light(氙弧燈
Xenon Arc LampA
continuous
ultraviolet and
visible emission
contains xenon at a
fairly high pressure
and the light is
formed via a
discharge across a
pair of electrodes
BandwidthandRe
solution
The width of the
band that is
allowed to pass is
called the
bandwidthThe
narrowness of the
band that is
allowed to pass
varies from one
design to another
and is called the
resolution.
Absorption
Filters
Monochromators
An entrance slit, a
dispersing element,
and an exit slit.
Luminescence
Phosphorescence
(燐光):
Luminescence
resulting from a
jump back to
the ground state
after routing
through other
electronic states
(triplet
state,三重激發態) is
called
phosphorescence.
HOMO / LUMO
and Bandgap
HOMO: Highest
occupied molecular
orbital or called
“Valence band”.
LUMO: Lowest
unoccupied
molecular orbital,
or called
“Conduction band”
Bandgap: The
difference of the
energies of the
HOMO and LUMO
The smaller the
energy, the more
easily it will be
excited.
Conjugation
The spectrum on
the below
illustrates that
conjugation of
double and triple
bonds also
shifts the
absorption
maximum to longer
wavelengths. It is clear that each
additional double
bond in the
conjugated π-
electron system
shifts the
absorption
maximum about 30
nm in the same
direction. Increased
conjugation brings
the HOMO and
LUMO orbitals
closer together.
When two double
bonds are
conjugated, the
four π-atomic
orbitals combine to
generate four π-
molecular orbitals
(two are bonding
and two are
antibonding).In a
similar manner, the
three double bonds
of a conjugated
polyene create six
π-molecular
orbitals, half
bonding and half
anti-bonding.
Limitations of
UV-VIS
Spectroscopy
Sample:
works well on
liquids and
solutions solid will
scatter the light
Calibrationand
reference:
Blank reference will
be needed(濃度需夠精準Choice of solvent:
Every solvent has a
UV-vis absorbance
cutoff wavelength
which the solvent
itself absorbs all of
the light
Choice of
container:
also have a UV-vis
absorbance cutoff
Concentration of
solution:
想要得到精準的數據,材料的吸收波峰至少要大於背景值三倍(濃度要夠高才行材料的大小受限制(相
比容器不能太小4.Photoluminesc
ence(PL)
probing the
electronic structure
of materialsOne
way this excess
energy can be
dissipated by
the sample is
through the
emission of light, or
luminescence The
excitation
wavelength should
be lower than the
PL wavelength of
the measured
material.
Relationship to
UV-VIS and PL
在紫外 可見光譜的吸光度與波長的曲線圖是測量從基態躍遷到激發態,而光致發光譜是從激發態躍遷到基態。excitation
spectrum is a
graph of emission
intensity
versus excitation
wavelength
PL在半導體的應用Bandgap
determination
雜質與缺陷量測Recombination
emchanisms
表面結構和excited states
The simplest
photoluminescent
processes are
resonant
radiations, in which
a photon of a
particular
wavelength is
absorbed and an
equivalent photon
is immediately
emitted.
PL在有機的應用Light emission
patterns
Absorption and
Emission
ACQ, TICT and
AIE
Aggregation-
caused quenching
(ACQ):
fluorescence is
weakened with an
increase in its
solution
concentration
Aggregation-
induced emission
(AIE)
exactly opposite to
the ACQ effect
twisted
intramolecular
charge
transfer(TICT)
Excitation
Wavelength
Dependent
入射能量越高,因照射時間越長所造成的紅移現象越明顯,且時間越久,強度越弱
CH4X-Ray
Photoelectron
Spectroscopy
(XPS)
measures the
elemental
composition,
empirical formula,
chemical state and
electronic state of
the elements by
irradiating a
material with a
beam ofX-rays
while
simultaneously
measuring the
kinetic energy and
number of
electrons that
escape from the
top 1 to 10 nm of
the material being
analyzed. XPS
requires ultra-high
vacuum (UHV)
conditions (10 -8
Torr).
Function and
Application
XPS detects all
elements with an
atomic number
(Z) of 3 (lithium)
and above
Detection limits for
most of the
elements are in
the parts per
thousand
range(ppm) Alias Names of
XPS
ESCA: Electron
spectroscopy for
chemical analysis
UPS: Ultraviolet
photoelectron
spectroscopy
PES:
Photoemission
spectroscopy
Electron
Configurations
Fundamental
Theory of XPS𝒉𝝂= 𝑬𝒌 + 𝑬𝒃 + 𝝓𝒔𝒑𝒆𝒄 𝒉𝝂 :
Photon energy from
X-ray source 𝑬𝒌 :
Kinetic energy of
the electron 𝑬𝑩 :
Binding energy of
the sample 𝝓𝒔𝒑𝒆𝒄 : Work
function of
spectrometer Work
function: Energies
required to remove
electrons from the
Fermi to
vacuum levels
可畫出跟 binding
energy 有關的能偕圖XPS Spectrum
XPS spectrum is to
measure intensities
of
photoelectrons vs.
𝑬𝒃Spin Orbital
Splitting
For p, d and f
peaks, two peaks
are observed.The
separation
between the two
peaks are named
spin
orbital splitting,
which is
attributed to L-S
coupling (耦合作用).
L-S coupling
Peak notations
L-S coupling ( 𝑗= 𝑙+ 𝑠 ) 𝑗 : Total
angular
momentum 𝑙 : Orbital angular
momentum 𝑠 : Spin
angular
momentum
Peak Area
Ratios
2p 1/2 electrons
have a smaller
kinetic energy in
comparison to the
2p 3/2 . The
integrated intensity
of the 2p 1/2signal
is half of that of 2p
3/2 due to the
difference of the
energetic
degeneration of
both terms ( 𝟐𝒋+ 𝟏 ). Peak separation is
increased with
heavier atoms.
X-ray Induced
Auger Electrons
Satellite Peak &
Shake-up Peak
During the
emission of a
photoelectron one
may get an
additional
excitation of a
second
electron.The
related distribution
of the energy 𝒉𝝂
to both processes
causes a shift of
the photoelectron
to larger binding
energy, which
yields a satellite
peak. If the second
electron is also
ejected the
satelliteis called a
shake-off peak, if it
is only excited to a
higher electronic
level it is called a
shake-
uppeak.Shake-up
satellites are
observed for Cu(II)-
ions. They have
only partially filled
d-levels,which may
accept an excited
electron from
anions of an
appropriate
compound.
Effect of
Bandgap
If the sample is an
insulator or a
semiconductor with
a large bandgap
∆𝑬𝒈 the intensity
of the XPS signal
goes back to the
level at the leading
edge with a smaller
binding energy for
several eV and
then increases.
This feature mirrors
the bandgap of the
material. For
metals, electrons
may be excitedwith
any energy and no
gap is observed. background
subtraction
by Shirley
method
assumes that the
background
increases with the
binding
energy
proportionally to
the part of the
signal immediately
before a given
energy. For the
background
subtraction, it must
include or correct
for X-ray satellites
chemically shifted
specie Shake-up
peaks Plasmon or
other losses
Quantitative XPS
積分面積 of a peak 𝑰𝒊𝝆𝒊: Average atomic
concentration of
element 𝒊 in the
surface𝑲𝒊: Relative
sensitivity factors
(RSF)