7782-79-8Relevant academic research and scientific papers
New topology in azide-bridged cobalt(11) complexes: The weak ferromagnet [Co2(N3)4(HexamethylenetetramineKH 2O)]n
Mautner, Franz A.,Oehrstroem, Lars,Sodin, Beate,Vicente, Ramon
, p. 6280 - 6286 (2009)
A new polynuclear azido-bridged Co(11) compound with formula [Co 2(N3)4(HMTA)(H2O)]n (1) (HMTA = hexamethyl-enetetramine) has been structurally and magnetically characterized. The compound 1 crystalli
The rates of the elementary reactions of NH(a1 Δ) with NH3(X) and HN3(X). The temperature dependences
Adam,Hack,Olzmann
, p. 197 - 211 (2005)
The reactions NH(a) + HN3(X) → prod. (1) and NH(a) + NH3(X) → prod. (2) were studied in a quasi-static reaction cell in the temperature range 293 ≤ T/K ≤ 501 at a pressure of 10 mbar and 20 mbar, respectively, with He as the main carrier gas. The electronically excited reactant NH(a) was generated by laser-flash photolysis of HN 3, at λ = 308 nm and detected by laser-induced fluorescence (LIF). Also the ground state species NH(X) was detected by LIF. From the measured concentration-time profiles of NH(a) under pseudo-first order conditions, the rate coefficients k1(T) and k2(T) were obtained. For the rate coefficient k1 a positive temperature dependence was observed: k1(T) = (8.1 ± 0.5) × 10 13 exp[(-0.76 ± 0.05)/RT] cm3/mol s with a small activation energy of EA = 0.76 kJ/mol. For reaction (2) the rate coefficient k2(T) = (8.6 ± 0.6) × 1013 (T/298)-(0.6±0.1) cm3/mol s with a negative temperature dependence was measured indicating that the intermediate N 2H4, which decomposes to 2NH2, is formed without a barrier. The rate of the quenching channel NH(a) + NH3 → NH(X) + NH3 (2q) has the same temperature dependence as the rate of the overall reaction (2). The contribution k2q/k2 = 0.008 over the temperature range 293 ≤ T/K ≤ 501.
Mechanism of the Reaction of NH(1Δ) with NO in Argon Matrix
Yokoyama, Keiichi,Kitaike, Hiroshi,Fueno, Takayuki
, p. 1731 - 1737 (1991)
Matrix-isolated hydrazoic acid HN3 admixed with NO was photolyzed by a low-pressure mercury discharge lamp.Product analysis based on the FTIR spectroscopy has revealed the formations of NH, N2O, OH, HNO, and HONO as photoproducts.From the comparisons of the amount of HN3 consumed with that of N2O produced, we conclude that the reaction of NH(1Δ) with NO proceeds mainly through the process NH(1Δ)+NON2O+H.The quantum yield of N2O is found to be Φ1=0.7+/-0.1.The conclusion is in line with our previous results of the gas phase experiments at room temperature.
Collision-Induced Intersystem Crossing of NH(a1Δ, v''= 0.1) by N2 and Xe: Temperature Dependence (N2) and Product States (N2, Xe)
Hack, W.,Rathmann, K.
, p. 47 - 52 (1992)
The elementary reactions of NM(a1Δ,v''=0) with N2 and Xe have been studied in the gas phase.NH(a,v'') was produced by laser photolysis of HN3 at λl = 248 nm and λL = 308 nm and detected directly by laser-induced fluorescence (LIF) via the c1Π-a1Δ) transition.Time resolution is based on the delay between the photolysis and the probe laser.The reaction rates were determined under pseudo-first-order conditions ( >>a,v'')>0), at different temperatures in the range 290 a,v''=0) + N2 -> products (1), k1 = (3.9 +/- 1.2) * 1011 exp(-(5.4 +/- 1.2) kJ mol-1/RT)cm3/(mol s); NH(a,v''=1) + N2 -> products (2), k2 = (8.6 +/- 2.7) * 1011 exp(-(4.4+/- 2.3) kJ mol-1/RT) cm3/(mol s); ND(a,v''=0) + N2 -> products (3), k3 = (4.7 +/- 1.7) * 1011 exp(-(5.2 +/- 1.1) kJ mol-1/RT) cm3/(mol s).The NH(X,v), which appeared as the product of physical quenching, was detected by LIF with the transition (A3Π-X3Σ-).In the reaction 1, 2, and 3 NH(X) and ND(X), respectively, were formed only in the vibrational ground state.The rate constant for the process NH(a,v''=1) + Xe -> products (5) was determined to be k5 = (7.7 +/- 0.9) * 1012 cm3/(mol s).In the physical quenching of NH(a,v'') (produced at λL = 248 nm) by Xe vibrationally vibrationally excited NH in the electronic ground sate NH(X,v=0,1,2) was detected NH(a,v''=0) (produced at λL = 308 nm) was quenched to NH(X,v=0).The different quenching dynamics of NH(a,v'') by N2 and Xe are discussed.
Phenylborylene: Direct spectroscopic characterization in inert gas matrices
Bettinger, Holger F.
, p. 2534 - 2535 (2006)
The photolysis of bisazidophenylborane isolated in cryogenic matrices results in phenylborylene, a subvalent boron(I) species with a singlet ground state. Broad band irradiation of phenylborylene causes formation of benzoborirene by insertion into an ortho-CH bond. Copyright
Epitaxial growth of inn films by molecular-beam epitaxy using hydrazoic acid (HN3) as an efficient nitrogen source
Chen,Hsiao,Hsu,Wu,Yen,Wei,Chen,Chen
, p. 6755 - 6759 (2007)
Epitaxial InN films have been successfully grown on c-plane GaN template by gas-source molecular-beam epitaxy with hydrazoic acid (HN3) as an efficient nitrogen source. Results in residual-gas analyzer show that the HN3 is highly dissociated to produce nitrogen radicals and can be controlled in the amounts of active nitrogen species by tuning HN3 pressure. A flat and high-purity InN epifilm has been realized at the temperature near 550 °C, and a growth rate of 200 nm/hr is also achieved. Moreover, the epitaxial relationship of the InN(002) on the GaN(002) is reflected in the X-ray diffraction, and the full-width at half-maximum of the InN(002) peak as narrow as 0.05° is related to a high-quality crystallinity. An infrared photoluminescence (PL) emission peak at 0.705 eV and the integrated intensity increasing linearly with excitation power suggest that the observed PL can be attributed to a free-to-bound recombination.
3D azido-bridged cobalt(II) complexes with diazines as coligands
Mautner, Franz A.,Sodin, Beate,Vicente, Ramon
, p. 23 - 27 (2011)
Two new three-dimensional azido-bridged Co(II) compounds with formula [Co(N3)2(2,5-Me2pyz)]n (1) and [Co(N3)2(2-ampym)]n (2) have been structurally and magnetically characterized
A new energy transfer chemical laser at 1.315 μm
Henshaw, Thomas L.,Manke Ii, Gerald C.,Madden, Timothy J.,Berman, Michael R.,Hager, Gordon D.
, p. 537 - 544 (2000)
CW laser action has been demonstrated on the electronic I*(2P1/2)→I(2P 3/2) transition of atomic iodine at 1.315 μm from the NCl (a1Δ)+I(2P 3/2) energy transfer reaction. The stimulated emission was generated in a transverse subsonic flow device when hydrogen azide, HN3, was injected into a flow of iodine and chlorine atoms. The measured laser output power was 180 mW.
Temperature dependence of the UPS and HREELS of HN3 and DN3 on Si(110)
Bu,Chu,Lin
, p. L151 - L156,L151-L156 (1992)
HN3 was used for the first time as a nitrogen source for nitridation of Si surfaces. Its interaction with Si(110) was studied with HREELS and UPS at temperatures between 120 and 1350 K. HN3 was found to adsorb molecularly on the Si surface at 120 K, as all molecular vibrational peaks, such as HN-NN stretching at 150 meV, HNN=N stretching at 265 meV and H-NNN stretching at 414 meV, were clearly observed in HREEL spectra. A similar HREELS study of DN3 was carried out to confirm some of the EELS assignments. Upon warming up to 220 K, HN3 started to dissociate into N2 and NH, which further dissociated to give N and H as the surface was annealed from 580 to 800 K, H adatoms were observed to desorb at T > 800 K, while N remained on the surface, forming Si3N4 at T ? 1350 K.
Binary Zinc Azides
Schulz, Axel,Villinger, Alexander
, p. 2032 - 2038 (2016)
Pure, solvent-free Zn(N3)2 was prepared by reaction of diethyl zinc and hydrazoic acid in aprotic solvents. The single-crystal structure determination, along with the comprehensive characterization of α-Zn(N3)2 and two metastable polymorphs, could be achieved for the first time. Since these data disagree in large parts with the known, previously reported values, all previous syntheses of Zn(N3)2, and for comparison Zn(N3)2×2.5 H2O and Zn(OH)N3 were reinvestigated, indicating that some of the earlier work has to be revised.
