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This issue of
Metrologia collects papers about the results of an
international research project aimed at the determination of the
Avogadro constant,
N
A, by counting the atoms in a silicon crystal highly
enriched with the isotope
28Si. Fifty years ago, Egidi [1] thought about realizing
an atomic mass standard. In 1965, Bonse and Hart [2] operated the
first x-ray interferometer, thus paving the way to the achievement
of Egidi's dream, and soon Deslattes
et al [3] completed the first counting of the atoms in a
natural silicon crystal.
The present project, outlined by Zosi [4] in 1983, began in 2004
by combining the experiences and capabilities of the BIPM, INRIM,
IRMM, NIST, NPL, NMIA, NMIJ and PTB. The start signal, ratified by
a memorandum of understanding, was a contract for the production of
a silicon crystal highly enriched with
28Si. The enrichment process was undertaken by the
Central Design Bureau of Machine Building in St Petersburg.
Subsequently, a polycrystal was grown in the Institute of Chemistry
of High-Purity Substances of the Russian Academy of Sciences in
Nizhny Novgorod and a
28Si boule was grown and purified by the
Leibniz-Institut für Kristallzüchtung in Berlin. Isotope
enrichment made it possible to apply isotope dilution mass
spectroscopy, to determine the Avogadro constant with unprecedented
accuracy, and to fulfil Egidi's dream.
To convey Egidi's 'fantasy' into practice, two
28Si kilogram prototypes shaped as quasi-perfect spheres
were manufactured by the Australian Centre for Precision Optics;
their isotopic composition, molar mass, mass, volume, density and
lattice parameter were accurately determined and their surfaces
were chemically and physically characterized at the atomic scale.
The paper by Andreas
et al reviews the work carried out; it collates all the
findings and illustrates how Avogadro's constant was obtained.
Impurity concentration and gradients in the enriched crystal were
measured by infrared spectroscopy and taken into account; Zakel
et al relate these measurements in detail. Next, Pramann
et al illustrate how the molar mass of the enriched crystal
was measured by exploiting isotopic enrichment and isotope dilution
mass spectrometry. Valkiers
et al report about remeasurement of the molar mass of a
natural Si crystal, a measurement prompted by the exigency of
clarifying the origin of the discrepancy between the
N
A value given in the present issue and the value
obtained using natural Si crystals. A consistency analysis of the
different isotopic-composition determinations is illustrated in the
paper by Bulska
et al. As reported in two papers by Massa
et al, to determine the lattice parameter an x-ray
interferometer was manufactured from the material between the
already mentioned spheres. The measurement result was combined with
lattice comparisons between different crystal samples and with the
impurity gradient to extrapolate the sphere's lattice-parameter.
Ferroglio
et al's contribution analyzes the self-weight deformation of
the x-ray interferometer. Fujimoto
et al report about the lattice-perfection investigations
carried out by a novel self-referencing diffractometer at the
National Laboratory for High-Energy Physics (KEK) in Japan. A
really great effort was made to characterize the sphere surfaces
and to correct for the oxide layer and the contaminating atoms. The
results of these investigations are given by Busch
et al. The sphere diameter and topography were measured by
optical interferometry to nanometer accuracy; the papers of Bartl
et al and Kuramoto
et al describe how the sphere volumes were determined.
Andreas
et al's paper describes the calculation of phase corrections
for the diameter measurements. The results of mass comparisons
against the Pt–Ir standards of the BIPM, NMIJ and PTB are
given by Picard
et al.
The results reported in the present issue need to be completed.
One of the necessary activities is to relate the mass of the
28Si atom to its Compton wavelength to test the
mass–energy–frequency equivalence. Another effort is to
monitor the stability of the Pt–Ir prototype: the
technologies described in the present issue can be refined and
finalized to calculate the mass variation of 1 kg
28Si spheres by monitoring the surface evolution without
weighing them on a balance. The last activity is the determination
of the mass of a
28Si sphere by electrical measurements using a watt
balance and without any reference to the Pt–Ir prototype. In
this framework, it will be necessary to demonstrate the mutual
consistency and the stability of both the electrical and crystal
mise en pratique of a kilogram definition based on a
conventional value of the Planck constant. A related issue is to
develop suitable procedures and protocols to disseminate the unit
of mass from the new realizations.
Since the molar Planck constant is well known via the
measurement of the Rydberg constant, the accurate measurement of
N
A also provides an accurate and independent
determination of the Planck constant,
h. A comparison of the values of the Planck constant
obtained via the watt-balance experiment and the
N
A determination tests quantum mechanics. In fact, the
watt-balance value of
h depends on solid state physics through the theories of
Josephson and quantum Hall effects, whereas the value of
h derived from
N
A depends on atomic physics through the energy level
differences in hydrogen and deuterium, whose associated transition
frequencies yield information on the Rydberg constant.
Grateful thanks are addressed to H-J Pohl for his outstanding
project management in Russia, to A K Kaliteevski and his colleagues
of the Central Design Bureau of Machine Building and the Institute
of Chemistry of High-Purity Substances for their dedication and the
punctual delivery of the enriched material, to H Riemann and his
staff of the Institut für Kristallzüchtung for the
crystal growth, to our directors for their advice and financial
support, and to our colleagues for their daily work.
Special thanks are addressed to Peter Becker, to whom this issue
is dedicated on the occasion of his retirement from work at the
Physikalisch-Technische Bundesanstalt. In 1974, young Peter joined
the PTB's Avogadro group which, under the direction of Peter
Seyfried, followed Bonse's work and improved the measurements of
the lattice parameter and the Avogadro constant [5, 6]. In 2004,
Peter proposed and backed this project by taking on his shoulders
the risks, the management burden and the coordination of the many
relevant activities.
References
[1] Egidi C 1963 Phantasies on a natural unity of mass
Nature
200 61–2
[2] Bonse U and Hart M 1965 An x-ray interferometer
Appl. Phys. Lett.
6 155–6
[3] Deslattes R D
et al 1974 Determination of the Avogadro constant
Phys. Rev. Lett.
33 463–6
[4] Zosi G 1983 A neo-Pythagorean approach towards an atomic
mass standard
Lett. Nuovo Cimento
38 577–80
[5] Becker P
et al 1981 Absolute measurement of the (220) lattice plane
spacing in a silicon crystal
Phys. Rev. Lett.
46 1540–3
[6] Seyfried P
et al 1992 A determination of the Avogadro constant
Z. Phys. B
87 289–98