Sensitivity of the joint survival probability for reinsurance schemes

2013 ◽  
Vol 37 (2) ◽  
pp. 289-295 ◽  
Author(s):  
Eleni E. Roumelioti ◽  
Michael A. Zazanis ◽  
Nikos E. Frangos
Keyword(s):  
Survival Probability ◽  
Joint Survival Probability

Joint survival probability via truncated invariant copula

2016 ◽  
Vol 85 ◽  
pp. 68-76 ◽  
Author(s):  
Jeong-Hoon Kim ◽  
Yong-Ki Ma ◽  
Chan Yeol Park
Keyword(s):  
Survival Probability ◽  
Joint Survival Probability

Temporal variation in annual survival probability of the Eurasian woodcock Scolopax rusticola wintering in France

2002 ◽  
Vol 8 (1) ◽  
pp. 21-30 ◽  
Author(s):  
Giacomo Tavecchia ◽  
Roger Pradel ◽  
François Gossmann ◽  
Claudine Bastat ◽  
Yves Ferrand ◽  
...  
Keyword(s):  
Temporal Variation ◽  
Survival Probability ◽  
Annual Survival ◽  
Scolopax Rusticola

Scattering of Low-Energy (5-12 eV) C2D4•+ Ions from Room-Temperature Carbon Surfaces

2008 ◽  
Vol 73 (6-7) ◽  
pp. 755-770 ◽  
Author(s):  
Andriy Pysanenko ◽  
Ján Žabka ◽  
Zdeněk Herman
Keyword(s):  
Survival Probability ◽  
Room Temperature ◽  
Incident Angle ◽  
Pyrolytic Graphite ◽  
Carbon Surface ◽  
Translational Energy ◽  
Energy Distributions ◽  
Surface Mass ◽  
Fragment Ions ◽  
Product Ions

The scattering of the hydrocarbon radical cation C2D4•+ from room-temperature carbon (highly oriented pyrolytic graphite, HOPG) surface was investigated at low incident energies of 6-12 eV. Mass spectra, angular and translational energy distributions of product ions were measured. From these data, information on processes at surfaces, absolute ion survival probability, and kinematics of the collision was obtained. The projectile ion showed both inelastic, dissociative and reactive scattering, namely the occurrence of H-atom transfer reaction with hydrocarbons present on the room-temperature carbon surface. The absolute survival probability of the ions for the incident angle of 30° (with respect to the surface) decreased from about 1.0% (16 eV) towards zero at incident energies below 10 eV. Estimation of the effective surface mass involved in the collision process led to m(S)eff of about 57 a.m.u. for inelastic non-dissociative collisions of C2D4•+ and of about 115 a.m.u. for fragment ions (C2D3+, C2D2•+) and ions formed in reactive surface collisions (C2D4H+, C2D2H+, contributions to C2D3+ and C2D2•+). This suggested a rather complex interaction between the projectile ion and the hydrocarbon-covered surface during the collision.

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