5,294 research outputs found

    Consistent nonparametric Bayesian inference for discretely observed scalar diffusions

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    We study Bayes procedures for the problem of nonparametric drift estimation for one-dimensional, ergodic diffusion models from discrete-time, low-frequency data. We give conditions for posterior consistency and verify these conditions for concrete priors, including priors based on wavelet expansions.Comment: Published in at http://dx.doi.org/10.3150/11-BEJ385 the Bernoulli (http://isi.cbs.nl/bernoulli/) by the International Statistical Institute/Bernoulli Society (http://isi.cbs.nl/BS/bshome.htm

    Nucleation in sheared granular matter

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    We present an experiment on crystallization of packings of macroscopic granular spheres. This system is often considered to be a model for thermally driven atomic or colloidal systems. Cyclically shearing a packing of frictional spheres, we observe a first order phase transition from a disordered to an ordered state. The ordered state consists of crystallites of mixed FCC and HCP symmetry that coexist with the amorphous bulk. The transition, initiated by homogeneous nucleation, overcomes a barrier at 64.5% volume fraction. Nucleation consists predominantly of the dissolving of small nuclei and the growth of nuclei that have reached a critical size of about ten spheres

    Stop Yer Tickling, Jock!

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    https://digitalcommons.library.umaine.edu/mmb-vp/6761/thumbnail.jp

    The historical individuality of the Christian faith (movement)

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    Thesis (M. A.)--Boston University, 1936. This item was digitized by the Internet Archive

    Vhf Studies Of The Lower Ionosphere

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    Crossed molecular beam: I. Photoionization studies of hydrogen sulfide and its dimer and trimer, II. A rotating source crossed molecular beam apparatus

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    Photoionization efficiency data for H(,2)S(\u27+), S(\u27+) and HS(\u27+) have been obtained in the region 645-1190 (ANGSTROM) using the molecular beam method. The ionization energy of H(,2)S was determined to be 10.4607 (+OR-) 0.0026 eV (1185.25 (+OR-) 0.30 (ANGSTROM)). The observed autoionizing vibrational progressions are tentatively assigned to the Rydberg transitions: 5a(,1) (---\u3e) nsa(,1) (n = 5 and 6) and 2b(,2) (---\u3e) nda(,1) (n = 4 and 5). The internal energy effects and the energetics of the ion-molecule reactions H(,2)S(\u27+) + H(,2)S (---\u3e) S(,2)(\u27+) + 2H(,2), HS(,2)(\u27+) + H(,2) + H, H(,3)S(\u27+) + HS, and H(,3)S(,2)(\u27+) + H have been studied by photoionization of hydrogen sulfide dimers which were synthesized by the molecular beam method. The appearance energy (AE) for H(,3)S(\u27+) from (H(,2)S)(,2) was determined to be 10.249 (+OR-) 0.012 eV (1209.7 (+OR-) 1.5 (ANGSTROM)). This value allows the calculation of the absolute proton affinity for H(,2)S at 0 K to be 167.2 (+OR-) 1.4 kcal/mol. Using the measured ionization energies for (H(,2)S)(,2)(\u27+) (9.596 (+OR-) 0.022 eV) and (H(,2)S)(,3)(\u27+) (0.467 (+OR-) 0.022 eV) and the estimated bonding energies for H(,2)S(.)H(,2)S and (H(,2)S)(,2)(.)H(,2)S(0.05 eV), the bond dissociation energies for H(,2)S(\u27+)(.)H(,2)S and (H(,2)S)(,2)(\u27+)(.)H(,2)S are deduced to be 0.92 (+OR-) 0.04 and 0.18 (+OR-) 0.04 eV, respectively. The AE for H(,3)S(\u27+)(.)H(,2)S from (H(,2)S)(,3) (9.84 (+OR-) 0.04 eV) also makes possible the calculation of the bond dissociation energy for H(,3) H(,3)S(\u27+)(.)H(,2)S to be 0.46 (+OR-) 0.10 eV;In the second part, a unique experimental apparatus is described for crossed neutral-neutral molecular beam studies; a rotating source crossed molecular beam apparatus. Each of the two independently rotatable beam sources is provided with two stages of differential pumping. The present beam source chambers permit any molecular beam crossing angle between 180 and 60 degrees. The detector chamber has three differentially pumped regions, the innermost of which contains the electron bombardment ionizer, quadrupole mass filter, and ion counting system which constitute the detector. This stationary detector chamber permits strong differential pumping in all regions and allows the entire detector to be translated, in vacuo over a distance of (TURN)60 cm beginning (TURN)27 cm from the beam crossing region. A particularly attractive feature of;this flexible design is the expected ease with which techniques utilizing lasers may be incorporated; (\u271)USDOE Report IS-T-1113. This work was performed under Contract W-7405-Eng-82 with the U.S. Department of Energy
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