14,191 research outputs found
Portrait of Siegmund Hess.
No full textLBISiegmund Hess was born in 1838 in Gross Muehlingen, the son of a musical family. In 1885 he moved to Gardelegen, Saxony, where he remained until his death in 1912. He held the honorary title of Koenigl. Musikmeister (Royal Music Master). Siegmund’s son, Richard Hess (b. 1873) became director of the Hess music school in 1910, until he was forced to resign in 1935.Ruth Neubec
Siegmund Hess Collection circa 1860-1938
No full textThis collection contains a variety of items from the career of composor and director Siegmund Hess (1838-1912) of Mühlingen, Germany. The earliest item in the collection appears to be a schedule with classes from his musical education; followed by a composition entitled "Deutschland 1870," a calling card, personal letters pertaining to concerts, programs from concerts, and newspaper clippings including Hess's obituary.Included in the collection but with uncertain correlation is a hand copied birth certificate from 1938 for Bertha Wiesenthal, born 1850 in Dessau.Siegmund Hess was born in 1838 in Mühlingen, the son of a musical family. In 1885 he moved to Gardelegen, Saxony, where he remained until his death in 1912. He held the honorary title of Königlich Musikmeister (Royal Music Master). Siegmund’s son, Richard Hess (b. 1873) became director of the Hess music school in 1910, until he was forced to resign in 1935.Processed for digitizatio
Viscosity data for hydrous peraluminous granitic melts: comparison with a metaluminous model
No full textWe performed 27 viscosity determinations on dry and water-bearing peraluminous haplogranitic melts. The dry melt compositions cover the range of normative corundum to be expected in peraluminous granitic melts in nature. The compositions are based on addition
of Al2O3 to a haplogranitic melt (HPG8) whose composition is near that of the projection
of the 2 kbar H2O-saturated minimum melt composition into the system NaAlSi3O8-
KAlSi3O8-SiO2. The H2O contents of the hydrous melts were analyzed using Karl Fischer titration ranging from 1 to 3 wt%. The viscosity determinations were performed using a
modified micropenetration method in the viscosity range of 1010 to 1011 Pa·s, at 1 atm
pressure, and in the temperature ranges of 880–940 °C and 470–640 °C for the dry and wet melts, respectively. For the dry peraluminous melts in this high viscosity range, addition of the first few percent of normative corundum to a metaluminous granitic melt increases the viscosity, which remains nearly constant despite further addition of Al2O3.
Thus a viscosity maximum is inferred for dry slightly peraluminous granitic melts. The hydrous melt viscosity data were compared with the recent calculational model of Hess and Dingwell (1996), which was based on and designed for metaluminous melt viscosities.
That model is capable of describing the viscosities of hydrous peraluminous granitic melts within the uncertainties stated for its application in metaluminous melts
Adsorption of CO on TiO2(110) studied by means of a cluster model surrounded by multipoles obtained from slab calculations
No full textAn array of point multipoles is used to mimic the long-range Coulomb interactions in a TiO56- cluster model designed to describe the adsorption of CO on a rutile surface. The multipoles are derived from the electron density and the concomitant electrostatic potential of a slab model of the (110) surface of rutile as calculated in a periodic Hartree-Fock approach. The motivation for the use of a cluster model is the possibility of inclusion of electron correlation by means of quantum-chemical methods, which is to date not easily possible in periodic Hartree-Fock calculations. In contrast to an array of point charges based on a Mulliken population analysis of the periodic charge distribution, the distributed multipoles show good agreement of adsorption properties as compared to a slab calculation. Surface relaxation has a significant influence on the binding of the adsorbate
Action Painting
No full textCatalog from the exhibition, "Action Painting," March 4–April 13, 1958, held by the Dallas Museum for Contemporary Arts.
Includes: a conversation between Thomas B. Hess and Harold Rosenberg, a list of artists and artworks in the exhibition, some images
Compte rendu de S. Menetrey, B. Hess (dir.) Les dialogues des juges en Europe
No full textMenetrey (S.), Hess (B.) (dir.), Les dialogues des juges en Europe", Bruxelles, Bruylant, 2014. 396 p. ISBN : 978280447170
1945-49 -- Correspondence, Unsorted -- letter, 1948-05-15
No full textLetter from Hess, William E. to Sabin, Albert B. dated 1948-05-15.Sabin Collection Fair Use Policy</a
Utlization of a modified B&L autoplot to perform the Hess-Lancaster test
No full textUtlization of a modified B&L autoplot to perform the Hess-Lancaster tes
Branching fraction and CP asymmetry of the decays B+→K0Sπ+ and B+→K0SK+
No full textAn analysis of B+ → K0
Sπ+ and B+ → K0
S K+ decays is performed with the LHCb experiment. The pp
collision data used correspond to integrated luminosities of 1 fb−1 and 2 fb−1 collected at centre-ofmass
energies of
√
s = 7 TeV and
√
s = 8 TeV, respectively. The ratio of branching fractions and the
direct CP asymmetries are measured to be B(B+ → K0
S K+
)/B(B+ → K0
Sπ+
) = 0.064 ± 0.009 (stat.) ±
0.004 (syst.), ACP(B+ → K0
Sπ+
) = −0.022 ± 0.025 (stat.) ± 0.010 (syst.) and ACP(B+ → K0
S K+
) =
−0.21 ± 0.14 (stat.) ± 0.01 (syst.). The data sample taken at
√
s = 7 TeV is used to search for
B+
c
→ K0
S K+ decays and results in the upper limit ( fc · B(B+
c
→ K0
S K+
))/( fu · B(B+ → K0
Sπ+
)) <
5.8 × 10−2 at 90% confidence level, where fc and fu denote the hadronisation fractions of a ¯b
quark
into a B+
c or a B+ meson, respectively
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