Absorption of Energy by an Electron, moves electron away from ground state(AAS)
Emission of Energy by an Electron, moves electron towards ground state (AES)
Light Energy Aimed at the Electron in the Ground State, gives of photon energy and moves electron away from ground state (AFS)
Primary X-radiation hits a Ground State Electron, this electron is kicked out of all the shells, outer shell electrons take it's place as well as the emission of X-ray fluorescence radiation (XRF)
Generation of a Particle II:
Measuring the mass of a charged species after ionisation.
ionising radiation hits electron
emits this electron
outer shell electron is excited and moves in towards the ground state, taking the place of the emitted electron, as well as giving off UV light at the same time
Mass Spec (AFS and XRF)
Generation of a Particle III:
Measuring the electronic kinetic energy after electron emission.
Electron Spectroscopy
Ground state electrons move all the way by gaining kinetic energy (XPS or AES)
Middle state electrons can either bind and move towards the ground state or move towards the outer shell with the kinetic energy (AES)
Excited state electrons don't really move any further (UPS)
Sample in --> nebulised using argon gas (becomes a mist) --> into the spray chamber --> large particles go down into the drain and small particles go up to the torch/spray chamber
plasma gas, nebuliser gas, and coolant gas goes into a Quartz torch made up of concentric tubes.
Surrounded by RF-loaded coils that cause the spark for the reaction with the argon plasma, RF voltage induced rapid oscillation motion of the argon ions which causes heat
sample aerosol is carried through the centre into the plasma
ICP-MS
Inductively - conductive material is heated using a gas with electromagneticcoils
Coupled - combine with
Plasma - one of the four fundamental states of matter, it is the presence of a significant portion of charged particles in any combination of ions or electrons.
Ionisation Process:
uses argon.
electron impact (molecular ion and 2 electrons)
charge transfer (molecular ion and argon)
Penning ionisation (molecular ion, argon and 1 electron) (argon impact causes the excited state that emits an electron)
Ion Extraction:
Samples goes through:
Sample cone --> Skimmer cone --> ion beam is focused and guided using electrostatic lenses.
it is all done under vacuum once the beam has passed through the Skimmer cone so that there is reduced particle collision and reduction of noise in the detector
Types of Interface:
Dual Cone System:
sample cone
Skimmer cone
more distance that is travelled the lower the pressure gets due to the beam divergence. This can be very messy for the cell and the spectrometer
Triple Cone System:
sample cone
Skimmer cone
hyper-Skimmer cone
more distance the beam travels the pressure drops gradually in three steps, this reduces the beam divergence and keeps the cell and spectrometer clean
Photon/Shadow Stop
ion beam is tightly focused by the extraction lenses
beam travels through the shadow stop
photons and neutrals are not deflected so they remain in the beam and are removed
ions of all masses are deflected off of the axis and go to the collisioncell
alternative
Quadrupole Ion Deflector
ions, photon and neutrals travel in the ion beam
the surrounding negative and positive magnetic fields cause the light ions and heavy ions to be deflected at 90 degrees and the photons and neutrals carry on in the ion beam
Non-Spectroscopic Interferences
Matrix Effects:
introduction effects - issues with the aerosol transport efficiency
space-charge effects - high mass remain more focused on the beam whereas lower mass could have the possibility of drifting off
plasma effects - thermal ionisation equilibrium
Instrument Drift
dissolved solids deposit left on the nebuliser cone and causes blockage and therefore signal suppression
temperature of ICP components impactionisation efficiency
Non-Spectroscopic Interferences:
dilution - reduces matrix and concentration and reduces signal
internal standard - element spiking to normalise matrix effects, assumes standard and analyte are the same
chemical purification - enhances analyte matrix ratio, time consuming and complex
Spectroscopic Interferences:
isotopes/isobaric - confuse other analytes with the same m/z
polyatomic - sample and matrix ions recombine after ICP and give same m/z as the analyte
Collision Reaction Cell
Kinetic Energy Discrimination (the removal of polyatomics) depends on:
collision cross section (the differential)
number of collisions
cell pressure and length
Collision Reaction Cell
Dynamic Reaction Cell (remove isobaric and polyatomics)
polyatomics and analyte react with ammonia reaction gas - the rate of reaction with iron is slower than argon oxide
then goes to mass filter
Quadrupole Mass Filter
usescan mode or sim mode
tandem MS
on mass approach - reaction only with the anlyte of interest
mass shift approach - reaction with the analytes that are NOT of interest - keeping the analyte of interest going the the second filter (Q2)
Detectors
faraday cups - metal hollow collectors, open one end and closed the other and electric current is measured to determine the number of ions collected in a specific time period
dynode electron multiplier - electrical pulse for every ion that strikes the inner surface with the sufficient kinetic energy and pulses are counted
Signal
pulse - pulses corresponding to individual particle detection
analogue - signal has a continuous voltage and every intensity of a particle hitting it is detected
Types of Samples:
soft tissue - break down using perchloric acid and then heated
environmental
cells
fluids - alkaline dilution or acid digestion
Configurations/Applications
Single Cell ICP-MS - example cisplatin uptake and resistence
HPLC ICP-MS - example arsenic species in toxicology
Laser Ablation ICP-MS - example iron localisation in Alzheimer's disease brain