1975
DOI: 10.1128/aem.29.2.293-294.1975
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Effect of L-Histidine on the Survival of a T-Strain of Mycoplasma

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Cited by 5 publications
(8 citation statements)
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“…Without this wavelength region, spectral fits to the data will not account for the Werner lines, biasing the results toward very low energy electron distributions. As the threshold energies for the Lyman and Werner bands are 11.37 and 12.41 eV (Ajello et al 1984), respectively, Lyman band continuum emission in the absence of discrete Werner band lines requires a highly-tuned electron distribution. Because Lyα production from the dissociation of H 2 drops sharply at 14.7eV (Ajello et al 1991), discrete lines should be even more important relative to the continuum at very low electron energies.…”
Section: Outstanding Issues Regarding Electron-impactmentioning
confidence: 99%
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“…Without this wavelength region, spectral fits to the data will not account for the Werner lines, biasing the results toward very low energy electron distributions. As the threshold energies for the Lyman and Werner bands are 11.37 and 12.41 eV (Ajello et al 1984), respectively, Lyman band continuum emission in the absence of discrete Werner band lines requires a highly-tuned electron distribution. Because Lyα production from the dissociation of H 2 drops sharply at 14.7eV (Ajello et al 1991), discrete lines should be even more important relative to the continuum at very low electron energies.…”
Section: Outstanding Issues Regarding Electron-impactmentioning
confidence: 99%
“…This mechanism requires stellar X-rays to create a distribution of photoelectrons that pump the molecules into excited electronic states. The H 2 then relaxes, producing a characteristic far-UV cascade spectrum of discrete emission lines and quasi-continuous spectral features during the dissociation of H 2 (Ajello et al 1984;Abgrall et al 1997). Ingleby et al (2009) proposed this mechanism to explain a portion of the low-resolution far-UV spectra from a sample of classical and weak-lined (low gas content) T Tauri stars observed with the Hubble Space Telescope-ACS and -STIS.…”
Section: Introductionmentioning
confidence: 99%
“…In the general form, Equation A1 must also be summed over the possible redistribution over rotational (∆J = ±1, 0) states, however, the present case is simplified due to the parity selection rules that forbid Q branch (∆J = 0) transitions to mix with R (∆J = -1) and P (∆J = +1) branches. The predissociation fraction for the Werner bands is zero (ξ C = 0; Ajello et al, 1984).…”
Section: O VI Flux Limitsmentioning
confidence: 99%
“…In the case of AU Mic, we are concerned with Werner band emission (n ′ -n ′′ = C -X ≡ C 1 Π u -X 1 Σ + g ), v ′ = 1, and v ′′ = 3 and 4 for the 1119.08 and 1163.81Å lines, respectively. The predissociation fraction for the Werner bands is zero (ξ C = 0; Ajello et al, 1984).…”
Section: Total Emitted H 2 Fluxmentioning
confidence: 99%