Rydberg constant

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Rydberg constant

(rĭd`bərg), physical constant used in studies of the spectrumspectrum,
arrangement or display of light or other form of radiation separated according to wavelength, frequency, energy, or some other property. Beams of charged particles can be separated into a spectrum according to mass in a mass spectrometer (see mass spectrograph).
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 of a substance. Its value for hydrogen is 109,737.3 cm−1.
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Rydberg constant

The most accurately measured of the fundamental constants; it is a universal scaling factor for any spectroscopic transition and an important cornerstone in the determination of other constants.

This constant was introduced empirically. J. Balmer's formula described the visible spectral lines of atomic hydrogen, while J. Rydberg's formula applied to the spectra of many elements. Their results may be summarized by Eq. (1),

where λ is the wavelength of the spectral line and R is a constant. In Balmer's account of the visible hydrogen spectrum, n1 was equal to 2, while n2 took on the integer values 3, 4, 5, and so forth. In Rydberg's more general work, n1 and n2 differed slightly from integer values. A remarkable result of Rydberg's work was that the constant R was the same for all spectral series he studied, regardless of the element. This constant R has come to be known as the Rydberg constant.

Applied to hydrogen, Niels Bohr's atomic model leads to Balmer's formula with a predicted value for the Rydberg constant given by Eq. (2),

where me is the electron mass, e is the electron charge, h is Planck's constant, ε0 is the permittivity of vacuum, and c is the speed of light. The equation expresses the Rydberg constant in SI units. To express it in cgs units, the right-hand side must be multiplied by (4&pgr;ε0)2. The subscript ∞ means that this is the Rydberg constant corresponding to an infinitely massive nucleus.

E. Schrödinger's wave mechanics predicts the same energy levels as the simple Bohr model, but the relativistic quantum theory of P. A. M. Dirac introduces small corrections or fine-structure splittings. The modern theory of quantum electrodynamics predicts further corrections. Additional small hyperfine-structure corrections account for the interaction of the electron and nuclear magnetic moments. See Fine structure (spectral lines), Hyperfine structure

The Rydberg constant is determined by measuring the wavelength or frequency of a spectral line of a hydrogenlike atom or ion. The highest resolution and accuracy has been achieved by the method of Doppler-free two-photon spectroscopy, which permits the observation of very sharp resonance transitions between long-living states. The 2002 adjustment of the fundamental constants, taking into account different measurements, adopted the value R = 10,973,731.568,525 ± 0.000,073 m-1 for the Rydberg constant. The measurements provide an important cornerstone for fundamental tests of basic laws of physics. See Atomic structure and spectra, Fundamental constants, Laser, Laser spectroscopy

McGraw-Hill Concise Encyclopedia of Physics. © 2002 by The McGraw-Hill Companies, Inc.
The following article is from The Great Soviet Encyclopedia (1979). It might be outdated or ideologically biased.

Rydberg Constant


(R), a physical constant introduced by J. R. Rydberg in 1890 in the study of atomic spectra.

The Rydberg constant is found in the expressions for energy levels and emission frequencies of atoms. If the mass of a nucleus of an atom is taken as infinitely great relative to the mass of an electron (the nucleus is stationary), then, according to quantum-mechanical calculation, R = 2π2me4/ch3 = 10,973,731.77 ± 0.83 m-1 (as of 1976), where e and m are the charge and mass of an electron, c is the velocity of light, and h is Planck’s constant, if the movement of the nucleus is taken into account, the mass of an electron is replaced by the reduced mass of the electron and nucleus, and then Ri = R/(1 + m/M), where M is the mass of the nucleus. For light atoms (hydrogen H, deuterium D, and helium 4He), the Rydberg constant has the following values (in m-1): RH = 10,967,759.3, RD = 10,970,741.7, and R4He = 10,972,226.7.


Taylor, B., W. Parker, and D. Langenberg. Fundamental’nye konstanty i kvantovaia elektrodinamika. Moscow, 1972. (Translated from English.)
The Great Soviet Encyclopedia, 3rd Edition (1970-1979). © 2010 The Gale Group, Inc. All rights reserved.

Rydberg constant

[′rid‚bərg ‚kän·stənt]
(atomic physics)
The most accurately measured of the fundamental constants, which enters into the formulas for wave numbers of atomic spectra and serves as a universal scaling factor for any spectroscopic transition and as an important cornerstone in the determination of other constants; it is equal to α2 mc /(2 h), or, in International System (SI) units, to me 4/(8 h 3ε02 c), where α is the fine-structure constant, m and e are the electron mass and charge, c is the speed of light, h is Planck's constant, and ε0 is the electric constant; numerically, it is equal to 10,973,731.568 549 ± 0.000 083 inverse meters. Symbolized R.
For any atom, the Rydberg constant (first definition) divided by 1 + m / M, where m and M are the masses of an electron and of the nucleus.
McGraw-Hill Dictionary of Scientific & Technical Terms, 6E, Copyright © 2003 by The McGraw-Hill Companies, Inc.
References in periodicals archive ?
(c) An optical frequency comb for producing ultraprecise colors of light can trigger quantum energy jumps useful for accurately measuring the Rydberg constant. Image courtesy of National Institute of Standards and Technology (NIST).
This atom is important not only as a model system that tests the limits of atomic theory and experiment, but it also provides information on fundamental physical constants, such as the Rydberg constant. In the past decade, the precision of the experiments has been improving rapidly, and improvements in the theory have been necessary to keep pace.
The analytic value of Rydberg constant is [[R.sub.[infinity]]] = (1/4[pi][E.sup.3])[l.sup.-1] = 3.0922328 x [10.sup.-8][l.sup.-1], the experimentally obtained value of the constant is ([R.sub.[infinity]]) = 109737.311 [+ or -] [+ or -]0.012[cm.sup.-1].
The Cowan-code result for the mean kinetic energy of an electron in the 5d orbital of the [5d.sup.9][6s.sup.2] configuration is T = 19.32 hc[R.sub.[infty], where [R.sub.[infty]] is the Rydberg constant. Using this value, we obtain a theoretical value of [g.sub.J](D), including the Breit-Margenau correction, of 1.199 85, which disagrees with the the experimental value by 1.85 X [10.sup.-3], which is 2.6 times the estimated experimental uncertainty of Ref.