8,707 research outputs found
Correspondence between J. R. Boyd, Jr. and Zebulon Weaver, 1932
No full textZebulon Weaver (1872-1948) was a lawyer and U.S. Representative from western North Carolina. He was a member of the North Carolina Park Commission and was involved in the land acquisition process that went towards establishment of the Great Smoky Mountain National Park and development of the Blue Ridge Parkway.
This set of letters represent correspondence related to establishing the boundaries for the park. Following are brief summaries of each of the letters:
J. R. Boyd, Jr. to Zebulon Weaver, April 18, 1932
In this letter Boyd asks Weaver to consider the issue of setting up of boundaries for the park and offers some of his own suggestions of establishing the boundaries at the mouth of the Cataloochee that would include some of the finest sceneries in the area while protecting the watershed of the Pigeon River.
J. R. Boyd, Jr. to Zebulon Weaver, April 25, 1932
In this letter Boyd again urges Weaver to establish the park boundaries as the previously suggested boundaries near the mouth of the Catalooche had already been occupied by the Carolina Light and Power Company. Zebulon Weaver to J. R. Boyd, May 2, 1932
In this letter Weaver acknowledges receiving Boyd’s letter of the 25th but confesses to not clearly understanding the issue that Mr. Boyd was interested in with regards to the park boundaries. Weaver reiterated North Carolina and Tennessee’s contribution of 428000 acres for the park and he hoped the Cataloochee basin and further lands with these boundaries could be acquired by the government for park purposes
ROTC
No full textAir Force ROTC Members shown are row one: cadets: Scott T. Jolley, Hugo A Ramos, Faye F Hamrick, Gaye Brinton, Cadet 2 Lt. Bradely Orton, Capt. Francis J. Wyborski, Commandant of Cadets. Row two: Cadetts: Samuel R. Clarke, Gary L. Sjoblom, Alan B. Warby, Blaine H. John Johnson Jr., Michael R. Clark. Row three: SSgt. Howard P. Schmuhl, NCO Administration & Supply, Cadets: Rulon L. Brough, Lynn H. Hatch, Boyd E. Fife, John E. Clarke, Jerald R. DeMille, Grant A Gabriel
Measurement of the ratio of prompt χ c to J / ψ production in pp collisions at √s = 7 TeV
Full text linkThe prompt production of charmonium χ c and J / ψ states is studied in proton-proton collisions at a centre-of-mass energy of √s = 7 TeV at the Large Hadron Collider. The χ c and J / ψ mesons are identified through their decays χ c → J / ψ γ and J / ψ → μ + μ - using 36 pb - 1 of data collected by the LHCb detector in 2010. The ratio of the prompt production cross-sections for χ c and J / ψ, σ (χ c → J / ψ γ) / σ (J / ψ), is determined as a function of the J / ψ transverse momentum in the range 2 < p T J / ψ < 15 GeV / c. The results are in excellent agreement with next-to-leading order non-relativistic expectations and show a significant discrepancy compared with the colour singlet model prediction at leading order, especially in the low p T J / ψ region
Beta-oxidation in the free-living stages of the entomophilic nematode Romanomermis culicivorax
No full textPT: J; CR: BAILEY CH, 1973, J INVERTEBR PATHOL, V22, P435 BARRETT J, 1971, COMP BIOCH PHYSL B, V38, P279 BARRETT J, 1976, INT J PARASITOL, V6, P155 BARRETT J, 1977, INT J PARASITOL, V7, P419 GORDON R, 1979, COMP BIOCH PHYSL B, V64, P369 GREEN DE, 1954, J BIOL CHEM, V206, P1 IMBRIANI JL, 1981, J NEMATOLOGY, V12, P226 ITTYCHERIAH PI, 1977, NEMATOLOGICA, V23, P165 KORNBERG A, 1953, J BIOL CHEM, V204, P329 KORTING W, 1971, J PARASITOL, V57, P1153 KORTING W, 1972, J PARASITOL, V58, P45 LOWRY OH, 1951, J BIOL CHEM, V193, P265 PETERSEN JJ, 1973, EXPT PARASITOLOGY, V33, P239 POINAR GO, 1979, NEMATODES BIOL CONTR RUTHERFORD TA, 1974, J PARASITOL, V60, P804 RUTHERFORD TA, 1976, 1ST P INT C INV PATH, P272 RUTHERFORD TA, 1977, CANADIAN J ZOOLOGY, V55, P1173 STADTMAN ER, 1957, METHOD ENZYMOL, V3, P931 STERN JR, 1955, METHOD ENZYMOL, V1, P581 STERN JR, 1956, J BIOL CHEM, V218, P971 WAKIL SJ, 1954, J BIOL CHEM, V207, P631 WARD CW, 1970, DEV BIOL, V22, P366 WARD CW, 1970, J PARASITOL, V56, P1009; NR: 23; TC: 4; J9: PARASITOLOGY; PG: 7; GA: MV921Source type: Electronic(1
[Photograph 2012.201.B0119.0549]
No full textPhotograph used for a story in the Daily Oklahoman newspaper. Caption: "W. R. Boyd Jr.-executive vice president of the American Petroleum Institute, Artell J. Byles, president of the A. P. I. and "Frank Buttram
Shrimp culture in inland low salinity waters
No full textInland aquaculture of shrimp in low salinity waters is widespread in many regions worldwide. Owing to its ability to grow and survive in low salinity environments the Pacific white shrimp, (Litopenaeusvannamei Boone) has become the candidate of choice for low salinity culture. Remediation techniques have been developed to improve the osmoregulatory capacity of shrimp reared in low salinity waters. These techniques have evaluated water modification strategies that improve low salinity waters used for production by adding potassium and magnesium fertilizers and dietary approaches that involve modification of the feeds offered to shrimp with supplements that might improve osmoregulatory capacity. Based on our own experience as well as what we found predominantly in the literature, it appears that modification of the rearing medium with potassium and magnesium fertilizers is more effective than dietary modification techniques at improving the growth, survival and osmoregulatory capacity of shrimp reared in low salinity waters. © 2010 Blackwell Publishing Asia Pty Ltd.AldaySanz V, 2010, SHRIMP BOOK, P1; Alvarez AL, 2004, AQUACULTURE, V237, P237, DOI 10.1016-j.aquaculture.2004.03.029; Araneda M, 2008, AQUACULTURE, V283, P13, DOI 10.1016-j.aquaculture.2008.06.030; Atwood HL, 2003, J WORLD AQUACULT SOC, V34, P518, DOI 10.1111-j.1749-7345.2003.tb00091.x; Bidwell J. P., 1985, ARTIFICIAL SEAWATERS; Bliss D. E., 1983, BIOL CRUSTACEA, V5, P54; BOWSER PR, 1981, AQUACULTURE, V23, P11, DOI 10.1016-0044-8486(81)90003-X; Boyd C. 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MAGNETIC MOLECULES IN MATRICES
No full textW. Weltner, Jr., R.J. Van Zee, and S. Li. J. Phys. Chem. 99, 6277 (1995). Y.M. Hamrick and W. Weltner, Jr.,. J. Chem. Phys. 94 3371 (1991). R.J. Van Zee and W. Weltner, Jr., Chem. Phys. Lett (accepted). S. Li, H.A. Weimer, R.J. Van Zee, and W. Weltner, Jr., J. Chem. Phys. (accepted)Author Institution: Department of Chemistry, University of FloridaMagneto-infrared and electron-skip-resonance (ESR) spectroscopies have been applied to trapped molecules and ions hin rare-gas matrices. Topics to be discussed may include zero-field quenching of orbital angular and phonon $effects.^{d}
Elastic energy and staging in intercalation compounds
No full textPT: J; CR: BERLINSKY AJ, 1979, SOLID STATE COMMUN, V31, P135 DAHN DC, UNPUB DAHN JR, 1981, SOLID STATE COMMUN, V40, P245 HARRIS AB, 1979, CAN J PHYS, V57, P1859 LEE CR, 1980, J PHYS SOC JPN, V49, P870 MCKINNON WR, 1980, SOLID STATE IONICS, V1, P111 NAGELBERG AS, 1981, J SOLID STATE CHEM, V38, P321 OHNISHI S, 1980, SOLID STATE COMMUN, V36, P823 OSORIO R, J PHYS CHEM SOLIDS PIESL H, 1978, HYDROGEN METALS, V1 SAFRAN SA, 1980, PHYS REV B, V22, P606 SAFRAN SA, 1980, PHYS REV LETT, V44, P937 SCHOLZ GA, 1980, MATER RES BULL, V15, P1703 SEZERMAN O, 1980, SOLID STATE COMM, V40, P245 THOMPSON AH, 1981, SOLID STATE IONICS, V3, P175 WAGNER H, 1978, HYDROGEN METALS, V1 WHITTINGHAM MS, 1975, MATER RES B, V10, P363; NR: 17; TC: 97; J9: SOLID STATE COMMUN; PG: 5; GA: NL648Source type: Electronic(1
Evidence for the decay B0→J/ψω and measurement of the relative branching fractions of meson decays to J/ψη and J/ψη′
Full text linkFirst evidence of the B 0 → J / ψ ω decay is found and the B s 0 → J / ψ η and B s 0 → J / ψ η ′ decays are studied using a dataset corresponding to an integrated luminosity of 1.0 fb -1 collected by the LHCb experiment in proton-proton collisions at a centre-of-mass energy of sqrt(s) = 7 TeV. The branching fractions of these decays are measured relative to that of the B 0 → J / ψ ρ 0 decay:frac(B (B 0 → J / ψ ω), B (B 0 → J / ψ ρ 0)) = 0.89 ± 0.19 (stat) - 0.13 + 0.07 (syst),frac(B (B s 0 → J / ψ η), B (B 0 → J / ψ ρ 0)) = 14.0 ± 1.2 (stat) - 1.5 + 1.1 (syst) - 1.0 + 1.1 (frac(f d, f s)),frac(B (B s 0 → J / ψ η ′), B (B 0 → J / ψ ρ 0)) = 12.7 ± 1.1 (stat) - 1.3 + 0.5 (syst) - 0.9 + 1.0 (frac(f d, f s)), where the last uncertainty is due to the knowledge of f d / f s, the ratio of b-quark hadronization factors that accounts for the different production rate of B 0 and B s 0 mesons. The ratio of the branching fractions of B s 0 → J / ψ η ′ and B s 0 → J / ψ η decays is measured to befrac(B (B s 0 → J / ψ η ′), B (B s 0 → J / ψ η)) = 0.90 ± 0.09 (stat) - 0.02 + 0.06 (syst)
DIATOMIC MOLECULES FORMED BY Mo AND W WITH Cu, Ag, AND Au
No full text Baumann, R. J. Van Zee, and W. Weltner, JR., J. Chem. Phys, 79, 5272 (1983).""Author Institution: Department of Chemistry, University of FloridaThe ground states of MoCu, MoAg, MoAu, WCu, WAg, and WAu were determined to be with zero-field splitting parameters . Hyperfine splittings and nuclear quadrupole coupling constants (in molecules containing Au) were determined. Bonding and electron spin distribution will be discussed and related to earlier studies of the corresponding Cr $diatomics.^{1}
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