51,062 research outputs found
The thermal decomposition of diazirines: 3-(3-methyldiazirin-3-yl)propan-1-ol and 3-(3-methyldiazirin-3-yl)propanoic acid
PT: J; CR: BIGOT B, 1978, J AM CHEM SOC, V100, P6575 BRIDGE MR, 1969, J CHEM SOC A, P91 CHURCH RFR, 1970, J ORG CHEM, V35, P2465 CLOSS GL, 1965, J AM CHEM SOC, V87, P4270 EFFIO A, 1980, J AM CHEM SOC, V102, P1734 FIGUERA JM, 1976, AN QUIM, V72, P737 FIGUERA JM, 1978, J CHEM SOC F1, V74, P809 FIGUERA JM, 1979, J PHOTOCHEM, V10, P473 FREY HM, 1963, J CHEM SOC, P3514 FREY HM, 1964, J CHEM SOC, P4700 FREY HM, 1965, J CHEM SOC, P1700 FREY HM, 1965, J CHEM SOC, P3101 FREY HM, 1966, J CHEM SOC A, P968 FREY HM, 1977, J CHEM SOC F1, V73, P2010 FREY HM, 1979, J CHEM SOC A, P1916 GANZER GA, 1986, J AM CHEM SOC, V108, P1517 GRILLER D, 1982, J AM CHEM SOC, V104, P5549 LAL D, 1974, J AM CHEM SOC, V96, P6355 LIU MTH, 1972, INT J CHEM KINET, V4, P229 LIU MTH, 1972, J PHYS CHEM-US, V76, P797 LIU MTH, 1973, CAN J CHEM, V51, P2393 LIU MTH, 1974, J CHEM SOC P2, P937 LIU MTH, 1977, CAN J CHEM, V55, P3596 LIU MTH, 1982, CHEM SOC REV, V11, P127 LIU MTH, 1984, J CHEM SOC CHEM COMM, P1062 LIU MTH, 1984, TETRAHEDRON, V40, P887 LIU MTH, 1985, J CHEM SOC CHEM COMM, P982 LIU MTH, 1986, J CHEM SOC PERK T 2, P211 LIU MTH, 1987, CHEM DIAZIRINES, V1, P111 MANSOOR AM, 1966, TETRAHEDRON LETT, P1753 MANSOOR M, 1967, THESIS U SOUTHAMPTON MOSS RA, 1984, TETRAHEDRON LETT, V25, P1023 NEUVARAND EW, 1967, J PHYS CHEM-US, V71, P1229 SCHMID P, 1979, INT J CHEM KINET, V11, P333 SHERIDAN RS, 1984, J AM CHEM SOC, V106, P436 SKELL PS, 1972, TETRAHEDRON, V28, P3571 SMITH NP, 1979, J CHEM SOC P2, P213 SMITH RAG, 1975, J CHEM SOC P2, P686 VOIGT E, 1975, CHEM BER, V108, P3326; NR: 39; TC: 8; J9: J CHEM SOC PERKIN TRANS 2; PG: 7; GA: DD960Source type: Electronic(1
on the thermal decomposition of diazirines
PT: J; CR: BIGOT B, 1978, J AM CHEM SOC, V100, P6576 BRADLEY GF, 1977, J CHEM SOC P2, P1214 BRUNNER J, 1980, J BIOL CHEM, V255, P3313 DIDERICH G, 1972, HELV CHIM ACTA, V55, P2103 FLEMING I, 1980, FRONTIER ORBITALS OR GRILLER D, 1982, J AM CHEM SOC, V104, P5549 JENNINGS BM, 1976, J AM CHEM SOC, V98, P6416 LAHMANI F, 1976, J PHYS CHEM-US, V80, P2623 LANGANIS ED, 1983, J AM CHEM SOC, V105, P7457 LIU MTH, 1972, J PHYS CHEM-US, V76, P797 LIU MTH, 1973, CAN J CHEM, V51, P2393 LIU MTH, 1974, J CHEM SOC P2, P937 LIU MTH, 1977, CAN J CHEM, V55, P3596 LIU MTH, 1982, CHEM SOC REV, V11, P127 MOORE CB, 1964, J CHEM PHYS, V41, P3504 SCHMITZ E, 1965, CHEM BER, V98, P2509 SCHMITZ E, 1967, CHEM BER, V100, P2093 SCHMITZ E, 1971, 23RD INT C PUR ALL C, V2, P283 SHEPARD RA, 1967, J ORG CHEM, V32, P3197 SHILOV AE, 1968, TETRAHEDRON LETT, P4177 SMITH NP, 1979, J CHEM SOC P2, P213 SMITH RAG, 1975, J CHEM SOC P2, P686 SNYDER JP, 1972, TETRAHEDRON LETT, P4347 TAYLOR EC, 1979, CHEM REV, V79, P181 TURRO NJ, 1980, J AM CHEM SOC, V102, P7576 TURRO NJ, 1982, J AM CHEM SOC, V104, P1754 VOIGT E, 1975, CHEM BER, V108, P3326 ZOLLINGER H, 1978, ANGEW CHEM INT EDIT, V17, P141; NR: 28; TC: 8; J9: J CHEM SOC PERKIN TRANS 2; PG: 4; GA: A2035Source type: Electronic(1
Effect of diazirine concentration on the reaction of 3-benzyl-3-chlorodiazirine with methanol
PT: J; CR: GRAHAM WH, 1965, J AM CHEM SOC, V87, P4396 GRILLER D, 1982, J AM CHEM SOC, V104, P5549 LIU MTH, 1984, J CHEM SOC CHEM COMM, P1062 LIU MTH, 1985, J CHEM SOC CHEM COMM, P982 LIU MTH, 1985, J ORG CHEM, V50, P3218 LIU MTH, 1985, TETRAHEDRON LETT, V26, P3071 LIU MTH, 1986, J CHEM SOC PERK T 2, P1233 LIU MTH, 1986, J PHYS CHEM-US, V90, P75 LIU MTH, 1987, CHEM DIAZIRINES, V1, CH5 TOMIOKA H, 1984, J AM CHEM SOC, V106, P454 TOMIOKA H, 1986, J CHEM SOC CHEM COMM, P1364; NR: 11; TC: 5; J9: J CHEM SOC PERKIN TRANS 2; PG: 3; GA: L7207Source type: Electronic(1
Substituent and temperature effects on the reactions of benzylchlorocarbene with alcohol
PT: J; CR: DOLBY LJ, 1966, J ORG CHEM, V31, P110 FRENKING G, 1984, TETRAHEDRON, V40, P2123 GRAHAM WH, 1965, J AM CHEM SOC, V87, P4396 GRILLER D, UNPUB GRILLER D, 1982, J AM CHEM SOC, V104, P5549 GRILLER D, 1984, J AM CHEM SOC, V106, P198 KIRMSE W, 1971, CARBENE CHEM KIRMSE W, 1981, J AM CHEM SOC, V103, P5935 LIU MTH, 1984, J CHEM SOC CHEM COMM, P1062 LIU MTH, 1985, J CHEM SOC CHEM COMM, P982 MARCH J, 1985, ADV ORG CHEM, P244 MOSS RA, 1975, CARBENES, V1 MOSS RA, 1975, CARBENES, V2 MOSS RA, 1983, TETRAHEDRON LETT, V24, P685 MUROV SL, 1973, HDB PHOTOCHEMISTRY, P147 PLATZ MS, 1982, J AM CHEM SOC, V104, P6494 SCHLOSSER M, 1967, CHEM BER, V100, P3901 SCHMID GH, 1978, J ORG CHEM, V43, P777 SENTHILNATHAN VP, 1980, J AM CHEM SOC, V102, P7637 TANAKA R, 1971, TETRAHEDRON, V27, P2651 TOMIOKA H, 1983, J AM CHEM SOC, V105, P5053 TOMIOKA H, 1984, J AM CHEM SOC, V106, P454 TOMIOKA H, 1984, J CHEM SOC CHEM COMM, P476 TOMIOKA H, 1984, TETRAHEDRON LETT, V25, P4413 WARNER P, 1984, J ORG CHEM, V49, P3666 WARNER PM, 1984, J AM CHEM SOC, V106, P5366 WRIGHT BB, 1984, J AM CHEM SOC, V106, P4175; NR: 27; TC: 9; J9: J CHEM SOC PERKIN TRANS 2; PG: 8; GA: D7012Source 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′
First 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)
Measurement of the B0–B0 oscillation frequency Δmd with the decays B0→D−π+ and B0→ J/ψK∗0
The B
0
–B
0
oscillation frequency Δmd is measured by the LHCb experiment using a dataset corresponding
to an integrated luminosity of 1.0 fb−1
of proton–proton collisions at √
s = 7 TeV, and is found to be
Δmd
=0.5156±0.0051 (stat.)±0.0033 (syst.) ps−1
. The measurement is based on results from analyses
of the decays B
0
→ D
−π
+ (D
−
→ K
+π
−π
−) and B
0
→ J/ψK
∗0
(J/ψ →μ
+μ
−,K
∗0
→ K
+π
−) and
their charge conjugated modes
Search for the rare decays J/y -> D-s(-) rho(+) and J/psi -> <(D)over bar(0)<(K)over bar*(0)
A search for the rare decays of J/psi -> D-S(-) rho(+) + c.c. and J/psi -> D-S(-)rho(+) + c.c.) <1.3 x 10(-5) and beta(J/psi -
A convenient synthesis of some arylated phenylsulfonylacetonitriles and ethyl cyanoacetates using organoiron complexes.
A general method for the synthesis of some arylated phenylsulphonylacetonitriles 6a–g, 10a, b and 16 and ethyl cyanoacetates 7a-d and 11a, b is described. Nucleophilic substitution of the cyclopentadienyliron complexes of chloroarenes 1a–g with phenylsulphonylacetonitrile 2 or ethyl cyanoacetate 3 in the presence of potassium carbonate in DMF, at room temperature under a nitrogen atmosphere gave cyclopentadienyliron complexes of arylated phenylsulphonylacetonitriles 4a–g, 8a, b and 15 and ethyl cyanoacetates 5a–d and 9a, b in very good yields (71–94%). Photolysis of these complexes liberated the arenes (70–91%). To demonstrate the versatility of this methodological approach, reactions of both carbon nucleophiles 2, 3 with dimethyl chlorobenzene complexes 1h, j gave the desired products 8a, 9a, 12 and 13 without significant steric effect. This synthesis is advantageous over all those previously reported and should be a practical route to a variety of alkanoic acid and heterocyclic precursors
A 2 h periodic variation in the low-mass X-ray binary Ser X-1
Spectroscopy of the low-mass X-ray binary Ser X-1 using the Gran Telescopio Canarias have revealed a ?2 h periodic variability that is present in the three strongest emission lines. We tentatively interpret this variability as due to orbital motion, making it the first indication of the orbital period of Ser X-1. Together with the fact that the emission lines are remarkably narrow, but still resolved, we show that a main-sequence K dwarf together with a canonical 1.4 M? neutron star gives a good description of the system. In this scenario, the most likely place for the emission lines to arise is the accretion disc, instead of a localized region in the binary (such as the irradiated surface or the stream-impact point), and their narrowness is due instead to the low inclination (?10°) of Ser X-1
Search for the weak decays J/psi -> D-s(()*()-) e(+)nu(e) + c.c.
Using a sample of 2.25 x 10(8) J/psi events collected with the BESIII detector at the BEPCII collider, we search for the J/psi semileptonic weak decay J/psi -> D-s(-) e(+)nu(e) +c.c. with a much higher sensitivity than previous searches. We also perform the first search for J/psi -> D-s(*-) e(+) nu(e) + c.c. No significant excess of a signal above background is observed in either channel. At the 90% confidence level, the upper limits are determined to be B(J/psi -> D-s(-) e(+) nu(e) + c.c.) D-s*(-) e(+) nu(e) + c.c.) <1.8 x 10(-6), respectively. Both are consistent with Standard Model predictions
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