1 Dr Yann Sivry - sivry@ipgp.fr
Aquatic Geochemistry Team - Institut de Physique du Globe de Paris & Université Paris 7 UMR CNRS 7154
1, Rue Jussieu 75238 Paris cedex 05 Tel : +33 (0) 1 83 95 74 55 Fax : +33 (0) 1 83 95 77 08
e-mail : sivry@ipgp.fr
CMIS-1
Comment mesurer les concentrations en éléments traces, ultra- traces… isotopes ?
Inductively Coupled Plasma Mass Spectrometry : ICP-MS
Université Paris Diderot LiPAC
Novembre 2020
Dr Yann Sivry - sivry@ipgp.fr
CMIS-1
Comment mesurer les concentrations en éléments traces, ultra- traces… isotopes ?
Inductively Coupled Plasma Mass Spectrometry : ICP-MS
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Definitions
Spectroscopy = general term used to describe analytical methods based on absoprtion, emission or fluorescence of some molecules (Receptor = eye)
Spectrometry = methods using a dispersive element (Receptor is not the eye)
Spectroscopic methods = methods based on interaction between electromagnetic radiations and matter
Periodic table of elements - Mendeleïev
• Emission: ICP-AES, DP-AES, flame
• Absorption: flame, oven, atomic vapor
• Fluorescence: atomic, X (XRF)
• Mass (+ isotopes): ICP-MS, étincelle, TOF-SIMS
• Core: INAA (neutronic activation)
Elemental analysis
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Analytical range(s)
Reminds on prefixes used
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Introduction: Mass Spectrometry
Analytical tools/methods allowing the detection and quantification of almost all the periodic table elements
This involves free atomes at vapor state (no more included in a molecule)
Thus, the machine will:
o produce atomic vapor from the sample
o induce the molecule destruction = no more information on the nature of initial molecules (except if coupling with speciation technique)
Possible to dose simultaneously all the species of a given element
Mass spectrometry
Measurement of the mass/charge ratio of ionized molecules
Major steps of the measurement:
1) Ionization and extraction of the sampling gas
2) Separation of charged molecules as a function of the m/q ratio:
- Increasing the velocity (v) in an electric potential (U) - Separating in a magnetic field (B)
3) Collection of the charged molecules and creation of an electric current which is amplified then converted into high voltage
Introduction: Mass Spectrometry
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Sample introduction: nebulisation
Cyclonic chamber Scott chamber
Nebulisation/Spray chambers
• Nebulizer reproducibility is essential: flow and size distribution of droplets. Ultrasonic nebulizer is not dependent on pneumatic variations nor turbulances: it will ensure the best reproducibility.
• Nebulization variability will induce analytical variability.
The internal standard method is the best method to correct this bias as the element added is measured exactly simultaneously to the analyte.
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Nebulisation efficiency
• Induced current (ICP) or microwave (MW).
• Coupling Plasma-Generator with a spire from 2 to 4 rolls.
• High frequencey (MHz), high power (kW).
• Plasma (ionized gas) from 6000K to 12000K.
Warming system: the plasma torch
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Warming system: the plasma torch
Warming system: the plasma torch
Inductively Coupled Plasma
= ion source
Mass Spectrometry
= detection
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ICP-MS
• Ar, Ar + , e - , atoms and ions.
• If T increases, ionization increases
• Saha law:
Oxyde rate: M
++ O = MO
+Nebulization
Position of the flame
ICP-MS: Plasma Chemistry
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ICP-MS – The Interface: Extraction
ICP-MS: Separation between ions and neutrals/photons
1/ Quadrupole ion deflector (Perkin)
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ICP-MS: Separation between ions and neutrals/photons
2/ Ion transfer optics (Thermo)
Tiges métalliques Détecteur
Tension AC + DC Faisceau ionique
issue de la source
m/z
ICP-MS: Mass Filter
1/ Quadrupolar (Q-ICP-MS)
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ICP-MS: Mass Filter
2/ Magnetic sector field (HR-ICP-MS)
ICP-MS: detection system
1/ Discrete Dynode Detector
ICP-MS: detection system
2/ Faraday cup
ICP-MS: Global Scheme
1/ The Nexion Triple-Q-ICP-MS (Perkin)
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ICP-MS: Global Scheme
2/ The X-Series Q-ICP-MS (Agilent)
ICP-MS: Global Scheme
3/ The Element II HR-ICP-MS (Thermo)
ICP-MS: Global Scheme
4/ The Neptune Multi-Collector-ICP-MS (Thermo)
2) Separation of charged molecules as a function of the m/q ratio:
- Increasing the velocity (v)
- Separating in a magnetic field (B)
3) Collection of the charged molecules and creation of an electric current which
ICP-MS: Global Scheme
ICP-MS: Global Scheme
General scheme of the Nier’s mass spectrometer
ICP-MS: Global Scheme
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TIMS : Thermal Ionization Mass Spectrometry
MC-ICP-MS: Multi-Collector Inductively Coupled Plasma Mass Spectrometry
Interférences isobariques,
polyatomiques
The atomic core is composed by 2 types of particles: protons and neutrons, also
called nucleons
A X
Z
Z = nb of protons in the core N = nb of neutrons in the core
Z is also equal to the nb of electrons (except for ions) since neutrons are not charged
A = atomic mass nb = N + Z
Reminds: the internal structure of atoms
1 uma = 12 10
-3kg / 12. Na = 1,66055 10
-27kg Na = Avogadro nb = 6,022098 10
23atoms
1 proton = 1.00727647 uma 1 neutron = 1.008665 uma
Same value for Z (protons) not for A Two isotopes have different neutrons
Definition:
1 mole of
12C atoms = 12.00000000…g Atomic mass of C :
Reminds: Isotopes
Reminds: Which isotopes (elements) are analyzed by ICP-MS?
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Z (atomic nb) = nbof protons
Phosphorus isotopes
12 C
127N 137N
13 C
11 C
Reminds: the nuclides table
First step: Chemical preparation of samples
CRUSHING < 60 µm EVAPORATION
AQUEOUS SOLUTION ACID DIGESTION in a clean room
Isolation of the target element (Sr, Zn…) CHEMICAL SEPARATION in a clean room
ISOTOPIC COMPOSITION measurement by mass spectrometry
SAMPLING
0 5 10 15 20 25 30
142 143 144 145 146 147 148 149 150 151 152 153 154
masses
Abundance(%)
Samarium (Sm) Néodyme (Nd)
Why do we need to purify the element?
Isobars may disturb the measurement of 143Nd/144Nd!
The Rubidium – Strontium couple
0 10 20 30 40 50 60 70 80 90
84Sr 86Sr 87Sr 88Sr
Sr isotopes
%
0,56%
9,86% 7,00%
82,58%
Natural abundances (%)
0 10 20 30 40 50 60 70 80
85Rb 87Rb
Isotopes du Rb
%
72,165%
27,835%
Natural abundances (%)
Isobaric interferences
Polyatomic interferences
Work in a clean room
Chemical separation
Cationic exchange resin:
This reaction is associated to a value “K” which is resin, acid and ion dependent.
M++ H-R M-R + H+
Elements et isotopes
Isotope Masse (a.m.u.) Abondance (%) Isotope Masse (a.m.u.) Abondance (%)
1H 1.007825 99.985 31P 30.973763 100
2H (D) 2.014102 0.015 32S 31.972072 95.02
12C 12.000000 98.90 33S 32.971459 0.75
13C 13.003355 1.10 34S 33.967868 4.21
14N 14.003074 99.634 36S 35.967079 0.02
15N 15.000109 0.366 35Cl 34.968853 75.77
16O 15.994915 99.762 37Cl 36.965903 24.23
17O 16.999131 0.038 79Br 78.918336 50.69
18O 17.999159 0.200 81Br 80.916290 49.31
19F 18.998403 100 127I 126.904477 100
Masse
16O proche masse de
32S ou
32S
2+comme
16O
+Interférences polyatomiques
• Plasma: O, H, Cl, C, Ar, O + , Ar + , Cl + , C + ,
…..
• Formation de tous les ions bi moléculaires possibles, quelques tri.
– Ar: 40, 36, 38 – O: 16, 18, 17 – C: 12, 13
– N: 14, 15
• ArC + , ArO + , ArO 2 + , ….
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Interférences courantes
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Calcul de la résolution nécessaire ?
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Isotope Ion interférant Résolution
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Fe
40Ar
160 2500
75
As
40Ar
35Cl 7800
80
Se
40Ar
40Ar 9700
40
Ca
40Ar 193000
Exemples d'interférences
Isotope Ion interférant Résolution
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Fe
40Ar
160 2500
75
As
40Ar
35Cl 7800
80
Se
40Ar
40Ar 9700
40
Ca
40Ar 193000
Interférences isobariques
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Interférences isobariques
Exercice : Si 10^6 coups/ppb quel que soit l’élément
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Q Resolution M/M = 300
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Exemples de prix (Perkin)
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