1998
DOI: 10.1103/physrevb.58.2383
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Molecular hydrogen internuclear distance in high-pressure fluid and solid phases at room temperature

Abstract: Pure rotational Raman-scattering spectra have been measured in fluid and solid hydrogen at room temperature and at pressures from 0.3 to 20 GPa. The frequency position of the four molecular rotational lines S 0 (0), S 0 (1), S 0 (2), S 0 (3) has been determined as a function of pressure. The analysis of these data has permitted the extraction of the density dependence of the hydrogen internuclear distance. In the fluid phase, this quantity shows a marked decrease in the density range from 50 mol/l to the freez… Show more

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Cited by 20 publications
(10 citation statements)
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“…3 we report the effective internuclear distance r m = r −2 −1/2 = (4πµcB 0 /h) −1/2 . In the same figure, we show data referring to the gas at room temperature [21][22][23], to the isolated molecule [33] and to the low pressure solid [10]. The marked decrease of the internuclear distance, already seen in ref.…”
mentioning
confidence: 67%
“…3 we report the effective internuclear distance r m = r −2 −1/2 = (4πµcB 0 /h) −1/2 . In the same figure, we show data referring to the gas at room temperature [21][22][23], to the isolated molecule [33] and to the low pressure solid [10]. The marked decrease of the internuclear distance, already seen in ref.…”
mentioning
confidence: 67%
“…The 3 low-frequency bands (358, 589, and 815 cm Ϫ1 ) are easily identified as the S 0 (0), S 0 (1), and S 0 (2) rotational bands of H 2 (30). The comparison with a compressed H 2 /Ar mixture (top spectrum of After the last irradiation, the sample is monitored for several hours by measuring the Raman spectrum of different regions without observing any change in the reaction products composition.…”
Section: Resultsmentioning
confidence: 99%
“…The Raman spectra of the bubbles in the 200-1200 cm À1 frequency region (Figure 2 A) are dominated by four sharp bands, identified as the S 0 (0) (355 cm À1 ), S 0 (1) (589 cm À1 ), S 0 (2) (816 cm À1 ), and S 0 (3) (1033.5 cm À1 ) rotational bands of H 2 . [23] Other product bands, broader and weaker, which are the only signals observed in the transparent areas, also appears in some bubbles (traces e, h, and l). The Raman spectra of the transparent areas in the 200-1200 cm À1 frequency region show product bands with peak frequencies measured at 428, 526, 805, 898, 941, 1005 (shoulder), 1022, and 1135 cm À1 (Figure 2 B, traces d, x, y, and z).…”
Section: Matteo Ceppatelli* Roberto Bini Maria Caporali and Maurizmentioning
confidence: 92%