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T&M Conference Johannesburg 07.10.2013(1)
"Redetermination of the Avogadro Constant for the new Definition of the mole and the kilogram”
Detlef Schiel, Bernd Güttler, Axel Pramann, Olaf RienitzPhysikalisch-Technische Bundesanstalt, 38116 Braunschweig, Germany
T&M Conference Johannesburg 07.10.2013(2)
Speed of light
Definition of Si units by fundamental constants
Boltzmann-constant
Avogadro-constant
Luminous efficacy Planck- constant
Atomic transitions
Elementary charge
cd
K
s
kg
m
mol
A
T&M Conference Johannesburg 07.10.2013(3)
Mass values of the prototypes in 1889, 1950 and 199 0
-100
-80
-60
-40
-20
0
20
40
60
80
100
1880 1900 1920 1940 1960 1980 2000
year
∆∆ ∆∆m/µ
gred: International Prototypegreen: BIPM, Official Copies
orange: no.25, BIPM , for special useblack: national prototypes
„Stability“ of the Kilogram Prototype
50 µg
T&M Conference Johannesburg 07.10.2013(4)
Precondition for new defintion
Measurement challenge :
u(NA) or u(h) ≤ present situation
Three measurement results of NA or h availableone of them should have a rel. stand. uncertainty of 2· 10-8 andtwo should have a rel. standard uncertainty of 5· 10-8
T&M Conference Johannesburg 07.10.2013(5)
International Avogadro Coordination (IAC)CCM Working Group on the Avogadro Constant (WGAC)
2010 Grenoble
T&M Conference Johannesburg 07.10.2013(6)
Measurement of NA
N = VSphere/ VAtom
n = N / NA = m / M
NA = (M / m) (VSphere/ VAtom)
http://www.msm.cam.ac.uk/phase-trans/2003/MP1.crystals/MP1.crystals.html
3
sphere
A
8
am
VMN
⋅⋅⋅=
T&M Conference Johannesburg 07.10.2013(7)
International Avogadro Coordination
Multicollector ICPMS
X-Ray Interferometer
Optical sphere interferometer
3sphere
sphere
A
8
am
VMN
⋅⋅⋅=
Mass comparator
Surface layer : XRR, XRF, XPS,opt. ellipsometry
Impurities: IR, NAA
T&M Conference Johannesburg 07.10.2013(8)
Material for the NA measurement
Isotopically enriched Si(28) material
T&M Conference Johannesburg 07.10.2013(9)
Interferometrical volume determination
camera 1 camera 2
mK-temperature stabilisation
diode laser
collimator
Fizeau-Objective 1
Fizeau-Objective 2
thousands of diameters are measured simultaneously
T&M Conference Johannesburg 07.10.2013(10)
Interferometrical volume determination
PTB‘s sphere interferometer with spherical symmetry
PTB‘s sphere interferometer enables complete topographies of spheres, ndiameter ≈ 600 000.
The radius uncertainty is 0.7 nm or 8 ×10-9
Radius topography of 28Si-sphere S8. Peak to valley deviations from roundness amount to 99 nm.
T&M Conference Johannesburg 07.10.2013(11)
This image cannot currently be displayed.This image cannot currently be displayed.
Combined optical and x-ray interferometry
1 cm
∆s
INRIM X-ray interferometer
T&M Conference Johannesburg 07.10.2013(12)
Mass comparison in air and under vacuum on the 28Si sphere S5
87730
87740
87750
87760
87770
87780
87790
87800
87810
87820
87830
02/2008 06/2008 09/2008 12/2008 03/2009 07/2009 10/2009 01/2010 05/2010 08/2010date (Month/Year)
Mas
s (v
alue
-1kg
) (µ
g)
PTB air (hydrostatic department) NMIJ air (hydrostatic department)
NMIJ air (mass department) NMIJ vacuum
BIPM air BIPM vacuum
PTB air (mass department) PTB vacuum (mass department)
IAC vacuum (Weighted mean) IAC air (Weighted mean)
1.10-8
Values in air are corrected by the amount of water adsorbed
The error bars represent the combined uncertainty (k=1)
S5
ur(m): 4 ×10-9
Mass comparison
T&M Conference Johannesburg 07.10.2013(13)
Oxid layer (PTB, NMIJ, METAS, BIPM)
X-ray reflectometry at BESSY II:Determination of layer thickness (absolute)
X-ray spectroscopy (METAS, BESSYII, PTB):Stoichometry, impurities, mass density
Spectral ellipsometry (PTB, NMIJ):Topography of layer thickness
Influences and Risks:
• Optical constants• Contamination• Surface quality
Total uncertainty: 0,3 nm14 µg
T&M Conference Johannesburg 07.10.2013(14)
Determination of the molar mass of silicon
● three isotopes: 28Si, 29Si, 30Si● amount fractions x ↔ isotope ratios R● Challenge: Target uncertainty of uM,rel ≤ 1·10-8
( ) ( )[ ]∑=
⋅=30
28
SiSi)Si(i
ii MxM
( )∑=
=30
28
Si
jj
ii
R
Rx
T&M Conference Johannesburg 07.10.2013(15)
92.2 %
4.7 %3.1 %
28Si 29Si 30Si
Measurement challenge I
nat. Si
R 28/28 1
R 29/28 5.0 · 10-2
R 30/28 3.4 · 10-2
Isotopic ratios
U < 10-7
Natural Si
T&M Conference Johannesburg 07.10.2013(16)
Measurement challenge II
nat. Sienriched
Si-28
R 28/28 1 1
R 29/28 5.0 · 10-2 4.1 · 10-5
R 30/28 3.4 · 10-2 1,3 · 10-6
Isotopic ratios
U < 10-7 U ≈ 10-3
nat. Si
R 28/28 1
R 29/28 5.0 · 10-2
R 30/28 3.4 · 10-2
> 99.99 %
0.0041 %0.00013 %
28Si 29Si 30Si
„Si28“
T&M Conference Johannesburg 07.10.2013(17)
New concept
w30+29 = wimp = =m29 + m30
m28+m29+m30
mimpm28+mimp
30S29Si
28Si
w 30+29� 29Si and 30Si treated like a virtual two-isotop-element impurity in the isotopically enriched Si (28) matrix
�Measurement of the mass fraction w30+29 by IDMS
T&M Conference Johannesburg 07.10.2013(19)
Measurement procedure
Si (crystal)
alkaline dissolution
Si-solution
ID ICPMS-measurement
Isotopic composition of the sample
Molar Mass
T&M Conference Johannesburg 07.10.2013(20)
Measurement technique
Multicollector-Inductively-Coupled-Plasma Mass Spectrometer (MC-ICP-MS)
28Si29Si 30Si
Sample
MagnetFaraday-Detectors
Neptune (Thermo-Finnigan)
T&M Conference Johannesburg 07.10.2013(21)
Mass interference
High resolution scan of WASO17 and IDMS blend ("28- Si"/"30-Si")
0.000
0.005
0.010
0.015
0.020
0.025
0.030
0.035
0.040
0.045
0.050
28.945 28.950 28.955 28.960 28.965 28.970 28.975 28.980
M /(g/mol)
ion
sign
al/V
IDMS 29Si
WASO17 29Si
29Si
28SiH
T&M Conference Johannesburg 07.10.2013(22)
PTB results (using NaOH)
27.9769690
27.9769692
27.9769694
27.9769696
27.9769698
27.9769700
27.9769702
27.9769704
27.9769706
27.9769708
27.9769710
4.4
5.B2.
1.4
5.B3.
1.1.
3
5.B4.
1.1.
4
7.1.
2.3
7.2.
4.5
8.A2.
1.4
8.B4.
1.1.
3
9.8
sample
M/(
g/m
ol)
urel = 8.2·10-9
T&M Conference Johannesburg 07.10.2013(23)
27.9769680
27.9769685
27.9769690
27.9769695
27.9769700
27.9769705
27.9769710
PTB 2011 NRC 2012 NIST 2013 (S5) NIST 2013 (S8) PTB 2013
M/(
g/m
ol)
Current situation of results
urel = 6·10-9
Molar Mass of „Si28“
∆Mrel = 6.5·10-8
∆Mrel = 1.1·10-8
NaOH NaOH TMAH TMAH TMAH
T&M Conference Johannesburg 07.10.2013(24)
NA = 6.022 140 84(18) · 1023 mol -1
Avogadro constant
Received from Si crystal experiment
T&M Conference Johannesburg 07.10.2013(25)
Intended redefinition of mole and kilogram
• Definitions• Realizations• Consequences (?)
T&M Conference Johannesburg 07.10.2013(26)
The amount of substance of a system which contains as many elementary entities1 as there are atoms in 0.012 kilogram of carbon (12).
Current definition of the mole
1Elementary entities must be specified and may be atoms, molecules, ions, electrons, other particles, or specified groups of such particles
Indentification
NA is derived from the kghas to be measured and
has an uncertainty
12 g (12C) = 1 mol ( 12C){NA} atoms in 1 mol
T&M Conference Johannesburg 07.10.2013(27)
Macroscopic level
Atomic level
NA NA
Current definition of the mole
Definitions: M(12C) = 12 g/molAr(12C) = 12
Furthermore: Mu = mu NA g/mol
M(A) = Ar(A) Mu g/mol
m(12C) mu
M(12C) Mu
Mu = 1 g/molu(Mu) = 0 g/molNA measured mol -1
u(NA) measured mol -1
m(A) = Ar(A) mu g/mol
Ar( 12C)M(A)
Ar(A)
Ar( 12C)m(A)
Ar(A)
T&M Conference Johannesburg 07.10.2013(28)
Intended new definition of the kilogram
kg
h definedU(h) = 0
The kilogram, kg, is the SI unit of mass; its magnitude is set by fixing the numerical value of the Planck constant to be equal to exactly 6.626 068X ·10-34 when it is expressed in the unit s-1 m2
kg, which is equal to J s.
Foto: OkerlandarchivFoto: OkerlandarchivFoto: Okerlandarchiv
T&M Conference Johannesburg 07.10.2013(29)
Intended new definition of the mole
mol kg
NA definedU(NA) = 0
h definedU(h) = 0
The mole, mol, is the unit of amount of substance of a specifiedelementary entity, which may be an atom, molecule, ion, electron, any other particle or a specified group of such particles; its magnitude is set by fixing the numerical value of the Avogadro constant to be equal to exactly 6.022 141X·1023 when it isexpressed in the unit mol-1.
Foto: OkerlandarchivFoto: OkerlandarchivFoto: Okerlandarchiv
?
T&M Conference Johannesburg 07.10.2013(30)
Intended new definition of the mole
mol kg
NA definedU(NA) = 0
h definedU(h) = 0
∞
=R
MecAhN ur
A 2
)( 2α
c light velocity, Ar(e) relative mass of the electron, Mu = (10-3 kg mol-1), α fine structure constant, R∞ Rydberg constant, e elementary charge
The mole, mol, is the unit of amount of substance of a specified elementary entity, which may be an atom, molecule, ion, electron, any other particle or a specified group of such particles; its magnitude is set by fixing the numerical value of the Avogadro constant to be equal to exactly 6.022 14129 *1023 when it is expressed in the unit mol-1.
Foto: OkerlandarchivFoto: OkerlandarchivFoto: Okerlandarchiv
The mole, mol, is the unit of amount of substance of a specifiedelementary entity, which may be an atom, molecule, ion, electron, any other particle or a specified group of such particles; its magnitude is set by fixing the numerical value of the Avogadro constant to be equal to exactly 6.022 14129 *1023 when it isexpressed in the unit mol-1.
T&M Conference Johannesburg 07.10.2013(31)
After new definition of the mole
New definition: NA = 6.0221X·1023 g/molu(NA) = 0 g/mol
Therefore: Mu measuredu(Mu) ≈ 1.4 x 10-9 g/mol
2)(
2
αecA
RhNM
r
Au
∞=
Macroscopic level
Atomic levelAr( 12C)
Ar( 12C)
NA NA
M(A) = Ar(A) Mu g/mol
m(12C) mu
M(12C) Mu
m(A) = Ar(A) mu g/mol
T&M Conference Johannesburg 07.10.2013(32)
Summary of the changes
After defintion• Number of entities in a mole is fixed (and equal to NA exactly)
• Molar masses are uncertain (u(Mu) = 1.4·10-9 )
At present• The mass scale fixed ( Mu is 1 g/mol exactly)
• Number of entities in a mole is an uncertain value (u(NA) = 3·10-8 )
T&M Conference Johannesburg 07.10.2013(33)
Experiments for definition NA and h
● Counting atoms :
Determination of the Avogadro constant with silicon
crystal method,
Current value: urel(NA) = 3· 10-8
● Generating standard forces :
Determination of Planck constant with Watt balance
experiment,
Current value: urel(NA) ~ 6· 10-8
T&M Conference Johannesburg 07.10.2013(34)
Present situation of NA results
6.022138
6.022139
6.022140
6.022141
6.022142
6.022143
6.022144
1990 1995 2000 2005 2010 2015
NA
in 1
023
mol
-1
Year of publication
NPL
NISTNIST
NPL
NPL
IAC
NRC
NISTpreliminaryMETAS
T&M Conference Johannesburg 07.10.2013(35)
Possible realization by XRCD experiment
N / NA = n Is an absolute measurement of amountof substance without using weighing
Realization of the mole
1) VSphere/ Vatom = N N / NA = n
2) m / M = n
N / NA = m / M
T&M Conference Johannesburg 07.10.2013(36)
Consequences for chemists
No Change
except that the relative uncertaintyof an amount of substance valuecannot be smaller than 1.4·10-9
Barry Taylor, Metrologia 46 (2009) L16-L19
n = m / M
T&M Conference Johannesburg 07.10.2013(37)
Dissemination and uncertainty propagation
Reference standards ofE1accredited laboratoriesReference standards of
E1accredited laboratories
National standards of NMIsNational standards of NMIs
BIPM reference standardsBIPM reference standards
BIPM Working standardsBIPM Working standards
Secondary standards of NMIs and best standards according to CMCSecondary standards of NMIs and best standards according to CMC
Standards of customers of E1 accredited laboratories
Standards of customers of E1 accredited laboratories
0 µg
6 µg
14 µg
25 µg
≤ 83 µg (E1)
6 µg
Present system After redefinition
20 µg
44 µg
Ex. 1 (CCM req.)
30 µg
85 µg (E2)
Ex. 2
30 µg
71 µg
71 µg
77 µg
Best realisation of the kilogramBest realisation of the kilogram 50 µg
Ex. 3
42 µg
43 µg
32 µg
53 µg
≤ 83 µg (E1) 100 µg (E2)
30 µg
30 µg 43 µg
43 µg
71 µg
71 µg
Reference standards ofE1accredited laboratoriesReference standards of
E1accredited laboratories
National standards of NMIsNational standards of NMIs
BIPM reference standardsBIPM reference standards
BIPM Working standardsBIPM Working standards
Secondary standards of NMIs and best standards according to CMCSecondary standards of NMIs and best standards according to CMC
Standards of customers of E1 accredited laboratories
Standards of customers of E1 accredited laboratories
0 µg
6 µg
14 µg
25 µg
≤ 83 µg (E1)
6 µg
Present system After redefinition
20 µg
44 µg
Ex. 1 (CCM req.)
30 µg
85 µg (E2)
Ex. 2
30 µg
71 µg
71 µg
77 µg
Best realisation of the kilogramBest realisation of the kilogram 50 µg
Ex. 3
42 µg
43 µg
32 µg
53 µg
≤ 83 µg (E1) 100 µg (E2)
30 µg
30 µg 43 µg
43 µg
71 µg
71 µg
6 µg
6 µg
w
T&M Conference Johannesburg 07.10.2013(38)
Acknowledgement
Molar mass measurements:
Olaf RienitzAxel Pramann Avogadro team leader:
Peter BeckerHorst Bettin
T&M Conference Johannesburg 07.10.2013(40)
XRCD experiment for link to the kg
N · M / NA = m abs. measurement of the mass of thesphere without weighing
M / NA = m(Si) absolute mass of a Si-atom
Realization of the link to the kg
1) VSphere/ Vatom = N N / NA = n
2) m / M = n
N / NA = m / M
T&M Conference Johannesburg 07.10.2013(41)
Realization (traceability chain)
Measurement Uncertainty
SIThe mol is that amount-of-substance
which contains as many entities as there are in 12 g 12C. [n] = 1 mol
Values
n (Cu, X)Amount of copper in XSample X
... Y)(Cu,
)X Cu,(=
n
n
Referencematerial Y
n (Cu, Y)Amount of copper in Y
...Z) (Cu,
) YCu,(=
n
n
Primary (national)standard Z
n (Cu, Z)Amount of copper in a material Z
=)ZCu,(nCu
pur M
*wm
Peter Becker: The Avogadro Project: a 25 Year Quest, 20 Mai 2011, NIST
T&M Conference Johannesburg 07.10.2013(42)
Traceability system for elemental analysis in Germany
Matschat, R., Kipphardt, H., Rienitz, O., Schiel, D., Gernand, W., Oeter D.: Accreditation and Quality Assurance, 10 (2006), S. 633-639
Dissolution
Precision measurementCertification of
commercial solutions
Primary elemental standards Primary elemental solutions
Commercial solutions Transfer solutions
T&M Conference Johannesburg 07.10.2013(43)
m(Cu) = n(Cu)·M(Cu) m(Si) = n(Si)·M(Si)
n(Cu) = n(Si) · Ar(Si))/Ar(Cu) or
N(Cu) = N(Si) · Ar(Si))/Ar(Cu)
„Idea“ for link on primary level
T&M Conference Johannesburg 07.10.2013(44)
XRCD experiment after the new defintion
N = VSphere/ VAtom
n = N / NA = m / M
m / N = m(Si) absolute mass of a Si-atom
M (Si) molar mass (isotope composition)
Remeasurement of the molar mass unitallows to verify e.g. if the mass of a mol 12C is still 12g
T&M Conference Johannesburg 07.10.2013(45)
O. Rienitz, A. Pramann, D. Schiel: Novel concept for the mass spectrometric determination of absolute isotopicabundances with improved measurement uncertainty: Part 1 – theoreticalderivation and feasibility study, Int. J. Mass Spectrom. 289 (2010) 47
G. Mana, O. Rienitz:The calibration of Si isotope ratio measurements, Int. J. Mass Spectrom. 291 (2010) 55.
A. Pramann, O. Rienitz, D. Schiel, B. Güttler: Novel concept for the mass spectrometric determination of absolute isotopicabundances with improved measurement uncertainty: Part 2 – Development of an experimental procedure for the determination of the molar mass of silicon usingMC−ICP−MS, Int. J. Mass Spectrom. 299 (2011) 78.
A. Pramann, O. Rienitz, D. Schiel, B. Güttler, S. Valkiers: Novel concept for the mass spectrometric determination of absolute isotopicabundances with improved measurement uncertainty: Part 3 – Absolute molar massof silicon highly enriched in 28Si, Int. J. Mass Spectrom. 305 (2011) 58.
Literature
T&M Conference Johannesburg 07.10.2013(46)
Traceability system for elemental analysis
Measurement of the test laboratory
Precison measurement for the certification
Precision measurement of the element content
Purity determination
Gravimetrical preparation of the primary solution
sample X
Sample solution wX(E)
Secundary standard Y
Commercial sol., Urel= 0,3% wY(E)
Transferstandard T
Transfer solution, Urel= 0,1% wT(E)
SI
kg and mol NA
Primary standard
Primary solution, Urel= 0,05% wS(E)
Pure material, Urel= 0,01% wpur
diss
emin
atio
n
T&M Conference Johannesburg 07.10.2013(47)
Isotopic composition of SiF 4 by Gas-MS
FaradaydetectorsFaradaydetectors
AmplifierhousingAmplifierhousing
MagnetMagnet
Ion sourceIon source
Faradaydetectors
Amplifierhousing
Magnet
Ion source
MAT 253MC-IRMS
T&M Conference Johannesburg 07.10.2013(48)
Preparation of SiF 4 - reference gases
42 SiFF 2 Si →+
SiF4
Linde.
0
100
200
300
400
500
600
700
800
900
1000
9200 9300 9400 9500 9600 9700 9800 9900 10000
inte
nsi
ty/
mV
magnet current/steps
SiF4 (Russ92), quartz vs. sapphire tube, cup config.: SiF3_1,2,3 (cup2), norm m/z = 86
SiF4 (Russ92), quartz tube
SiF4 (Russ92), sapphire tube
28Si19F3+
29Si19F3+
30Si19F3+
Ar2+
T&M Conference Johannesburg 07.10.2013(49)
0.000 005 ≤ R ≤ 1
28Si 29Si 30Si
R
Classical Concept
0.1 ≤ R ≤ 70
IDMS
w(VE)
29Si 30Si
VE
R
28Si
Novel Concept
M(Si)
Virtual element
modified IDMS:virtual element
T&M Conference Johannesburg 07.10.2013(50)
Why u(NA) = 2 x 10-8?Dissemination and uncertainty propagation
Reference standards ofE1accredited laboratoriesReference standards of
E1accredited laboratories
National standards of NMIsNational standards of NMIs
BIPM reference standardsBIPM reference standards
BIPM Working standardsBIPM Working standards
Secondary standards of NMIs and best standards according to CMCSecondary standards of NMIs and best standards according to CMC
Standards of customers of E1 accredited laboratories
Standards of customers of E1 accredited laboratories
0 µg
6 µg
14 µg
25 µg
≤ 83 µg (E1)
6 µg
Present system After redefinition
20 µg
44 µg
Ex. 1 (CCM req.)
30 µg
85 µg (E2)
Ex. 2
30 µg
71 µg
71 µg
77 µg
Best realisation of the kilogramBest realisation of the kilogram 50 µg
Ex. 3
42 µg
43 µg
32 µg
53 µg
≤ 83 µg (E1) 100 µg (E2)
30 µg
30 µg 43 µg
43 µg
71 µg
71 µg
Reference standards ofE1accredited laboratoriesReference standards of
E1accredited laboratories
National standards of NMIsNational standards of NMIs
BIPM reference standardsBIPM reference standards
BIPM Working standardsBIPM Working standards
Secondary standards of NMIs and best standards according to CMCSecondary standards of NMIs and best standards according to CMC
Standards of customers of E1 accredited laboratories
Standards of customers of E1 accredited laboratories
0 µg
6 µg
14 µg
25 µg
≤ 83 µg (E1)
6 µg
Present system After redefinition
20 µg
44 µg
Ex. 1 (CCM req.)
30 µg
85 µg (E2)
Ex. 2
30 µg
71 µg
71 µg
77 µg
Best realisation of the kilogramBest realisation of the kilogram 50 µg
Ex. 3
42 µg
43 µg
32 µg
53 µg
≤ 83 µg (E1) 100 µg (E2)
30 µg
30 µg 43 µg
43 µg
71 µg
71 µg
6 µg
6 µg
w
T&M Conference Johannesburg 07.10.2013(51)
New concept II
Precondition: Si-material consists only of 28Si, 29Si and 30Si
1 = w28 + w30/29
M = x28 M28 + x29 M29 + x30 M30
R30/29 = n30 / n29
IDMS
Int. J. Mass Spectrom. 289 (2010) 47Int. J. Mass Spectrom. 291 (2010) 55.
. Int. J. Mass Spectrom. 299 (2011) 78Int. J. Mass Spectrom. 305 (2011) 58
T&M Conference Johannesburg 07.10.2013(52)
-0.01
0.04
0.09
0.14
0.19
0.24
0.29
28.94 28.95 28.96 28.97 28.98 28.99 29 29.01 29.02 29.03 29.04
M /(g/mole)
ion
sign
al/V
Signal at mass 29 for natural material
200 ppb natural Si
29Si N2H
COH
T&M Conference Johannesburg 07.10.2013(53)
Consequences
• Mu ≠ 1g/mol exact: lost of the direct relation between mol and kg
• NA has no more defined by kg
• Difference Mu(at present) und Mu(new) smaller than its uncertainty
• Probably a lost of understandability
T&M Conference Johannesburg 07.10.2013(54)
Before and after definiton
M(A) = Ar(A) Mu g/mol molar mass
Mu = mu NA = 1 g/mol; U(Mu) = 0 molar mass const.
mu = m(12C)/12 g atomic mass const.
2)(
2
αecA
RhNM
r
Au
∞= U(Mu) ≠ 0after
defintion
Definition: M(12C) = 12 g/molFurthermore: Ar(12C) = 12Therefore: Mu = 1 g/mol
U(Mu) = 0 g/mol
T&M Conference Johannesburg 07.10.2013(55)
First introduced by Ostwald 1893
Ar(A) relativ atomic masses (dimensionless)Mu molar mass constant (10-3 kg/mol)
Molar mass
Wilhelm Ostwald
Ulrich Stille
1808 Dalton: Hypothesis of atomistic nature of substances1893 Ostwald: Introduction of the molar mass1909 Einstein: Prove of the existence of atoms1955 Ulrich Stille: Introduction of the term „amount of substance“1967 Mole becomes the 7th SI unit
John Dalton
Albert Einstein
T&M Conference Johannesburg 07.10.2013(56)
International Units System
Liminous intensity: candela
Amount of substance: mol
Temperature: kelvin
Electric current: ampere
Time: second
Mass: kilogram
Length : meter
T&M Conference Johannesburg 07.10.2013(57)
History of NA-Measurement results
Loschmidt:Brown motion in gas
Einstein:Diffusion theory
Millikan:elementary charge
Bearden
Deslattes
∼∼∼∼10-1/15 a
year
rel.
unce
rtai
nty
Bragg:crystals
Silicon crystals
target: 2 ⋅⋅⋅⋅ 10-8
Peter Becker: The Avogadro Project: a 25 Year Quest, 20 Mai 2011, NIST
T&M Conference Johannesburg 07.10.2013(58)
Zonefloating
N
H He
Li Be B C O F Ne
Na Mg Al Si P S Cl Ar
K Ca Sc Ti V Cr Mn Fe Co Ni Cu Zn Ga Ge As Se Br Kr
Rb Sr Y Zr Nb Mo Tc Ru Rh Pd Ag Cd In Sn Sb Te I Xe
Cs Ba La Hf Ta W Re Os Ir Pt Au Hg Tl Pb Bi Po At Rn
Fr Ra Ac
Ce Pr Nd Pm Sm Eu Gd Tb Dy Ho Er Tm Yb Lu
Th Pa U
NB C O
Al Si P S
Ga Ge As Se
In Sn Sb Te
IR measured
depleted
Purity characterization
Sum electrical conductivity and parameter: crystal perfection
T&M Conference Johannesburg 07.10.2013(59)
Na Mg Al Si P S Cl Ar
K Ca Sc Ti V Cr Mn Fe Co Ni Cu Zn Ga Ge As Se Br Kr
Rb Sr Y Zr Nb Mo Tc Ru Rh Pd Ag Cd In Sn Sb Te I Xe
Cs Ba La Hf Ta W Re Os Ir Pt Au Hg Tl Pb Bi Po At Rn
Fr Ra Ac
Ce Pr Nd Pm Sm Eu Gd Tb Dy Ho Er Tm Yb Lu
Th Pa U
N
H He
Li Be B C O F Ne
LoD in the range of 10-6 –10-12 g/gPossible partner for
NAA: INRIMGDMS: PTB
Impurity determination by NAA and GDMS
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60
mi
Rb1
Rz,28RzRx
Rbx
38.2 %
25.6 % 23.5 %
Uncertainty Calculation of Molar Mass: example budget
Uncertainty budget
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Conclusion
Advantages• Solely R30/29 need to be measured• Only one chemical conversion• Blank substraction possible
Difficulties:• Extremly small 30Si and 29Si signals due to limited Si content of
the solutions (solubility, nebulizer capacity)• 29Si - 28SiH signal separation
Future work• Validation of the method
International cooperation, CCQM comparison• Gas mass spectrometry• New enriched material
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Experimental
29 30 31 32
0.000
0.001
0.002
0.003
0.004
0.005
16O+
2
30Si+29Si
+U /
V
M / (g/mol)
H3 cup scan
„Si28“inw(NaOH) = 0.001 g/gvs.
NaOH(w = 0.001 g/g)
„Broadband interference“ induced by Na scattering
A. Pramann, O. Rienitz, D. Schiel: Anal. Chem. 84 (2012) 10175
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Isotope dilution mass spectrometry
● primary method● analyte content
206Pb 208Pb
206Pb 208Pb
w(Pb)
1208/206 ≈R
206Pb 208Pb
X
Y
B206Pb 208Pb
206Pb 208Pb
w(Pb)
1208/206 ≈R
206Pb 208Pb
X
Y
B
Pb
Pb
PbPb
Pb IDMS
w(Pb)Pb
Pb
PbPb
Pb IDMS
w(Pb)
Metrologia 47 (2010) 460-463
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Experimental
Main Improvement: Application of sodium-free solvents:
using tetramethylammonium hydroxide (TMAH)* instead of NaOH
TMAH
2-4
4- H2SiOOH 4 Si +→+
*Robert Vocke, Jr., Savelas Rabb, Gregory Turk: private communication (NIST, USA) 2011
Advantages of TMAH● higher signal intensity (factor 5)● MS does not suffer from clogging etc.● stable intensity over days● no more sodium in the plasma
(no scattering/broadband interference)
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LatticeLatticeLatticeLattice parameterparameterparameterparameter determinationdeterminationdeterminationdetermination: : : : PrinciplePrinciplePrinciplePrinciple
This image cannot currently be displayed.This image cannot currently be displayed.
Combined optical and x-ray interferometry
1 cm
∆s
Deslattes 1973
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Calibration
Mass discremination and fractionation requires calibration(Determination of K-factors)
R = I30/I29
Rmess= Imess,30/Imess,29
Imess,29 Imess,30
R / Rmess= K
ICPB
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Calibration + IDMS
blend bxRbx
mw2
mx
mz1my1
blend b2Rb2
blend b1Rb1
myx
mz2
material yRy, Ry,28
material zRz, Rz,28
29Si 30Si28Si 29Si 30Si28Si
material wRw, Rw,28
29Si 30Si28Si
material xRx
29Si 30Si28Si
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Partner Institute Method Status Publication
NIM (China) IDMS almost finished ?
NIST (USA) IDMS finished to be submitted
NMIJ (Japan) IDMS almost finished ?
NRC (Canada) IDMS finished published
PTB (Germany) IDMS finished published
International cooperation
68
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Further interpretation of the XRCD experiment
• 12.058…….cm3 of 28Si at 20 oC in vacuum is 1 molwith an uncertainty of 2·10-8
• 2.152……..1025 atoms of 28Si are 1 kg with an uncertainty of 2·10-8
• 35.747……mol of 28Si atoms are 1 kg with an uncertainty of 2·10-8
1) VSphere/ Vatom = N N / NA = n
2) m / M = n
N / NA = m / M
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Watt balance experiment
In the weighing experiment, a mass and a coil are suspended from a balance. The coil (wire length L) is placed in a magnetic field of flux density B. The gravitational force on the mass m is balanced by an equal and opposite electromagnetic force on the coil by sending a current I through it:m g = I L B
In the moving experiment, the coil is moved at a vertical speed v through the magnetic field so that a voltage U is induced:U = B L v
Scematic principle taken from the BIPM website http://www.bipm.org/en/scientific/elec/watt_balance/wb_principle.html
NIST Watt balancehttp://www.google.de/imgres?imgurl=http://upload.wikimedia.org/wikipedia/commons/a/af/Watt_balance,_
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Torch (sapphire body, BN shield)
„Si-free“ equipment
spray chamber (Peak and PFA body)
15 cm
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Experimental
Sample preparation
● Cleaning & Etching of Si crystals
● Mass determination
● Dissolution in aqueous TMAH
Transformation in a single step!
2-4
4- H2SiOOH 4 Si +→+
OH 2H2SiFHF 6SiO 2-2
62 ++→+ +
OH HHNOSiFHHF 6HNOSi 222623 +++→++
400 mg
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Experimental
0.0
1.0
2.0
3.0
4.0
5.0
6.0
7.0
8.0
H2O NaOH (0.01%) Merck
NaOH (0.1%) Merck
NaOH (0.1%) Fluka
NaOH (0.4%) Merck
NaOH (4%) Merck
NaOH (25%) Merck
30S
i/29S
i/(V
/V)
solvent
isotope ratios of aqueous NaOH: R = f(wNaOH)
R(30Si/29Si)
R(30Si/29Si)av (Sinat)
Isotope ratio dependence from w(NaOH)
30Si/29Si
average 30Si/29Si (natural Si)
A. Pramann, O. Rienitz, D. Schiel: Anal. Chem. 84 (2012) 10175
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Two routes of measurement
Si (crystal)
Chemical conversion e.g. HF, BrF5
SiF4 (gaseous )
Gas MSmeasurement
Isotopic composition
Molar mass
Si (crystal)
Alkaline dissolutione.g. NaOH or TMAH
Si-solution (liquid )
ICP-MS measurement
Isotopic composition
Molar mass