Gerhard Herzberg 2026-10-24
Figure 1.
Portrait of Gerhard Herzberg
. GFHund; photograph from Friedrich Hund's estate, held by Gerhard Hund. CC BY 3.0, via Wikimedia Commons. Source.
Hyperfine structure Created 2026-10-14 Updated 2026-10-18
Small splittings of energy eigenvalues due to interactions involving nuclear spin.
J. A. Bearden Created 2026-10-20 Updated 2026-10-31
Joseph von Fraunhofer Created 2026-10-13 Updated 2026-10-31
Figure 1. . Unknown artist; Berlin-Brandenburg Academy archive source. Public domain (PD-old as declared on Commons). Source and usage information on the linked Wikimedia file page. Source.
On 10 July 1908, Heike Kamerlingh Onnes's Leiden laboratory circulated purified helium through liquid air and evaporatively cooled liquid-hydrogen precooling, a regenerative heat exchanger, and an expansion valve. Returning helium cooled incoming helium; liquid collected in a transparent vacuum vessel. Reflected light revealed its liquid meniscus, crossed by thermocouple wires. Subsequent mass density and spectroscopy checks tested contamination.[ref]
Figure 1. . Original functional diagram of the reported sequence. Arrows show stream direction and heat transfer; positions do not represent the apparatus geometry. Compression and heat rejection close the refrigeration cycle. Source. Details.
A constant-volume helium gas thermometer below the valve supplied the temperature indication. An oxygen boiling reference check disagreed with its expected reading; the real gas correction to thermodynamic temperature remained provisional. A temperature plateau suggested immersion before the liquid meniscus was recognized.[ref]
The measurement principles separate two questions. A visible liquid meniscus establishes an interface; a gas thermometer estimates temperature through an equation of state. A stationary temperature trace can also result from a steady state without phase coexistence, so it cannot replace the interface observation. Conversely, seeing a liquid does not calibrate a thermometer. Thermometer calibration, the gas thermometer dead-space correction, departures from the ideal gas law and incomplete thermal equilibrium all matter when assigning an absolute temperature. A check far from the intended measurement range tests the instrument but does not by itself bound every low-temperature error.
Leonard C. Maximon Created 2026-10-14 Updated 2026-10-31
Albert Abraham Michelson's 1907 lecture, Recent Advances in Spectroscopy, pp. 171–172, connects counting interference fringes with a reproducible length standard. Broad or multiple spectral lines obscured fringes at large path differences; red cadmium emission supplied a suitable source. His 1907 Nobel Prize in Physics recognized optical precision instruments and their spectroscopy and metrology applications.[ref]
His authored account of the metre comparison at Sèvres describes a heated, evacuated cadmium discharge tube and a spectrometer selecting one spectral line. A movable reference mirror was compared with pairs of silvered parallel surfaces defining intermediate standards. Counted interference fringes established a short interval; repeated comparisons extended it to a decimetre and then a metre. White-light fringes located surface coincidence, while monochromatic fringes supplied counts and fractional orders. A thermally shielding box, firm pier, calibrated translation screw and tested thermometers controlled drafts, vibration, travel and temperature. Uniform temperature mattered in comparisons; the final standard required an absolute temperature reading. Optical microscopes made the final comparison to the marked metre bar, limiting the whole result.[ref]
This is a measurement chain, rather than one enormous unchecked fringe count: short intervals establish whole orders; fractional-order readings refine each longer comparison. The optical coherence envelope helps locate white-light coincidence, whereas the carrier phase difference measures small departures from it. Repetition checks counting mistakes, but agreement alone cannot exclude shared systematic errors. The general lesson of metrology is to preserve the link from the optical ruler through each transfer and control to the final length.
Molecular beam Created 2026-10-14 Updated 2026-10-18
A directed stream of molecules used to prepare samples for spectroscopy.
A molecular beam also includes a stream of chemical atoms, then called an atomic beam. An oven supplies particles; aligned slits restrict their directions, and a vacuum limits subsequent collisions. Narrowing the directions does not by itself make every particle's speed equal. This gives a useful separation of tasks: prepare a path, select or measure speed, apply an interaction, and read the resulting particle counts or deflection.
The advantage is unusually tangible. A magnetic field can separate spin components in the Stern-Gerlach experiment; even gravity can sort a beam by flight time. The effusive beam speed distribution explains which particles leave the source, while gravity deflection of an atomic beam explains how that distribution becomes a pattern on a detector.
Figure 1.
Two ways of measuring molecular beam speeds: rotating openings and gravitational flight
. Original functional schematics, not historical apparatus drawings. The lower panel exaggerates the fall for visibility; all numerical settings used in the text are chosen model inputs. Details.
Nicolaas Bloembergen Created 2026-10-18 Updated 2026-10-31
Figure 1. . Rob Herber; attribution requested on Commons: Pinoccio at Dutch Wikipedia. CC BY-SA 2.5, via Wikimedia Commons. Source.
Albert Abraham Michelson received the award for precise optical instruments and their use in spectroscopy and metrology.[ref] The Michelson interferometer converts relative wave phase into a readout for precise length measurements.