The dynamics of O(3P) + deuterated hydrocarbons: influences on product rotation and fine-structure state partitioning

2002 ◽  
Vol 4 (3) ◽  
pp. 473-481 ◽  
Author(s):  
Florian Ausfelder ◽  
Hailey Kelso ◽  
Kenneth G. McKendrick
2001 ◽  
Vol 114 (10) ◽  
pp. 4479 ◽  
Author(s):  
M. Kind ◽  
F. Stuhl ◽  
Yi-Ren Tzeng ◽  
Millard H. Alexander ◽  
Paul J. Dagdigian

1983 ◽  
Vol 28 (3) ◽  
pp. 1329-1337 ◽  
Author(s):  
B. G. Zollars ◽  
H. A. Schuessler ◽  
J. W. Parker ◽  
R. H. Hill

1977 ◽  
Vol 38 (18) ◽  
pp. 1018-1020 ◽  
Author(s):  
William D. Phillips ◽  
Charles L. Glaser ◽  
Daniel Kleppner

1985 ◽  
Vol 115 (4-5) ◽  
pp. 353-357 ◽  
Author(s):  
J.G. Balz ◽  
R.A. Bernheim ◽  
W.J. Chen ◽  
L.P. Gold

Author(s):  
John A. Mousel ◽  
Sarah C. Vigmostad ◽  
H. S. Udaykumar ◽  
Krishnan B. Chandran

Cutting edge computational tools are an important component of the future of tasks such as surgical planning of mitral valve repair and the design and evaluation of prosthetic valves. For example, despite half a century of use, mechanical heart valves still require further research to reduce the non-physiologic nature of the flow field, which is the source of potential medical complications, of which the most serious complication is thrombus formation [1]. In fact, there is still a lack of consensus in the literature about which flow pathologies are the most damaging to blood elements [2, 3]. Much computational work has been performed examining the flow around mechanical heart valve devices [4, 5], but because the emphasis has been on correct valve motion and not fine structure detail, only the largest features have been adequately resolved and the forward flow structures are allowed to dissipate on stretched meshes such that the features may not lead to the correct fine structure state as directionality of blood flow changes during the cardiac cycle.


1981 ◽  
Vol 59 (4) ◽  
pp. 548-554 ◽  
Author(s):  
M. Głódz ◽  
J. B. Atkinson ◽  
L. Krause

Cross sections for inelastic transfer between the 82D3/2 and 82D5/2 fine-structure states in rubidium, induced in resonant collisions with ground-state Rb atoms, have been determined using an experimental method involving two-photon excitation of atomic fluorescence. Rubidium vapor in a fluorescence cell was irradiated with pulses of 641 nm radiation from a N2 laser-pumped dye-laser tuned to excite one of the 82D states. The resulting fluorescence included the direct component originating from the optically excited state and a sensitized component arising from the other fine-structure state populated by collisions. Relative intensities of the fluorescent components, determined by photon-counting techniques, yielded the cross sections for excitation transfer: Q(2D3/2 → 2D5/2) = 8.1 × 10−13 cm2; Q(2D3/2 ← 2D5/2) = 5.5 × 1013 cm2; as well as [Formula: see text], the effective quenching cross section. The excitation transfer cross sections which are considered accurate to within ±20% are in the ratio predicted by the principle of detailed balancing.


Author(s):  
W. H. Zucker ◽  
R. G. Mason

Platelet adhesion initiates platelet aggregation and is an important component of the hemostatic process. Since the development of a new form of collagen as a topical hemostatic agent is of both basic and clinical interest, an ultrastructural and hematologic study of the interaction of platelets with the microcrystalline collagen preparation was undertaken.In this study, whole blood anticoagulated with EDTA was used in order to inhibit aggregation and permit study of platelet adhesion to collagen as an isolated event. The microcrystalline collagen was prepared from bovine dermal corium; milling was with sharp blades. The preparation consists of partial hydrochloric acid amine collagen salts and retains much of the fibrillar morphology of native collagen.


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