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  • 1
    Online-Ressource
    Online-Ressource
    Cham :Springer International Publishing AG,
    Schlagwort(e): Statistics. ; Electronic books.
    Beschreibung / Inhaltsverzeichnis: a.
    Materialart: Online-Ressource
    Seiten: 1 online resource (148 pages)
    Ausgabe: 1st ed.
    ISBN: 9783319066325
    Serie: SpringerBriefs in Mathematics Series
    Sprache: Englisch
    Anmerkung: Intro -- Preface -- Acknowledgments -- Contents -- 1 Introduction -- 2 Preliminaries -- 3 Well-Posedness of the Vector-Valued BSEEs -- 4 Well-Posedness Result for the Operator-Valued BSEEs with Special Data -- 5 Sequential Banach-Alaoglu-Type Theorems in the Operator Version -- 6 Well-Posedness of the Operator-Valued BSEEs in the General Case -- 7 Some Properties of the Relaxed Transposition Solutions to the Operator-Valued BSEEs -- 8 Necessary Condition for Optimal Controls, the Case of Convex Control Domains -- 9 Necessary Condition for Optimal Controls, the Case of Non-convex Control Domains -- References.
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  • 2
    Online-Ressource
    Online-Ressource
    Cham :Springer International Publishing AG,
    Schlagwort(e): Stochastic control theory. ; Electronic books.
    Materialart: Online-Ressource
    Seiten: 1 online resource (598 pages)
    Ausgabe: 1st ed.
    ISBN: 9783030823313
    Serie: Probability Theory and Stochastic Modelling Series ; v.101
    DDC: 519.2
    Sprache: Englisch
    Anmerkung: Intro -- Preface -- Contents -- 1 Introduction -- 1.1 Why Stochastic Distributed Parameter Control Systems? -- 1.2 Two Fundamental Issues in Control Theory -- 1.3 Range Inclusion and the Duality Argument -- 1.4 Two Basic Methods in This Book -- 2 Some Preliminaries in Stochastic Calculus -- 2.1 Measures and Probability, Measurable Functions and Random Variables -- 2.2 Integrals and Expectation -- 2.3 Signed/Vector Measures, Conditional Expectation -- 2.3.1 Signed Measures -- 2.3.2 Distribution, Density and Characteristic Functions -- 2.3.3 Vector Measures -- 2.3.4 Conditional Expectation -- 2.4 A Riesz-Type Representation Theorem -- 2.4.1 Proof of the Necessity for a Special Case -- 2.4.2 Proof of the Necessity for the General Case -- 2.4.3 Proof of the Sufficiency -- 2.5 A Sequential Banach-Alaoglu-Type Theorem in the Operator Version -- 2.6 Stochastic Processes -- 2.7 Stopping Times -- 2.8 Martingales -- 2.8.1 Real Valued Martingales -- 2.8.2 Vector-Valued Martingales -- 2.9 Brownian Motions -- 2.9.1 Brownian Motions in Finite Dimensions -- 2.9.2 Construction of Brownian Motions in one Dimension -- 2.9.3 Vector-Valued Brownian Motions -- 2.10 Stochastic Integrals -- 2.10.1 Itô's Integrals w.r.t. Brownian Motions in Finite Dimensions -- 2.10.2 Itô's Integrals w.r.t. Vector-Valued Brownian Motions -- 2.11 Properties of Stochastic Integrals -- 2.11.1 Itô's Formula for Itô's Processes (in a Strong Form) -- 2.11.2 Burkholder-Davis-Gundy Inequality -- 2.11.3 Stochastic Fubini Theorem -- 2.11.4 Itô's Formula for Itô's processes in a Weak Form -- 2.11.5 Martingale Representation Theorem -- 2.12 Notes and Comments -- 3 Stochastic Evolution Equations -- 3.1 Stochastic Evolution Equations in Finite Dimensions -- 3.2 Well-Posedness of Stochastic Evolution Equations -- 3.2.1 Notions of Solutions -- 3.2.2 Well-Posedness in the Sense of Mild Solution. , 3.3 Regularity of Mild Solutions to Stochastic Evolution Equations -- 3.3.1 Burkholder-Davis-Gundy Type Inequality and Time Regularity -- 3.3.2 Space Regularity -- 3.4 Notes and Comments -- 4 Backward Stochastic Evolution Equations -- 4.1 The Case of Finite Dimensions and Natural filtration -- 4.2 The Case of Infinite Dimensions -- 4.2.1 Notions of Solutions -- 4.2.2 Well-Posedness in the Sense of Mild Solution for the Case of Natural Filtration -- 4.3 The Case of General Filtration -- 4.4 The Case of Natural Filtration Revisited -- 4.5 Notes and Comments -- 5 Control Problems for Stochastic Distributed Parameter Systems -- 5.1 An Example of Controlled Stochastic Differential Equations -- 5.2 Control Systems Governed by Stochastic Partial Differential Equations -- 5.3 Some Control Problems for Stochastic Distributed Parameter Systems -- 5.4 Notes and Comments -- 6 Controllability for Stochastic Differential Equations in Finite Dimensions -- 6.1 The Control Systems With Controls in Both Drift and Diffusion Terms -- 6.2 Control System With a Control in the Drift Term -- 6.3 Lack of Robustness for Null/Approximate Controllability -- 6.4 Notes and Comments -- 7 Controllability for Stochastic Linear Evolution Equations -- 7.1 Formulation of the Problems -- 7.2 Well-Posedness of Stochastic Systems With Unbounded Control Operators -- 7.3 Reduction to the Observability of Dual Problems -- 7.4 Explicit Forms of Controls for the Controllability Problems -- 7.5 Relationship Between the Forward and the Backward Controllability -- 7.5.1 The Case of Bounded Control Operators -- 7.5.2 The Case of Unbounded Control Operators -- 7.6 Notes and Comments -- 8 Exact Controllability for Stochastic Transport Equations -- 8.1 Formulation of the Problem and the Main Result -- 8.2 Hidden Regularity and a Weighted Identity. , 8.3 Observability Estimate for Backward Stochastic Transport Equations -- 8.4 Notes and Comments -- 9 Controllability and Observability of Stochastic Parabolic Systems -- 9.1 Formulation of the Problems -- 9.2 Controllability of a Class of Stochastic Parabolic Systems -- 9.2.1 Preliminaries -- 9.2.2 Proof of the Null Controllability -- 9.2.3 Proof of the Approximate Controllability -- 9.3 Controllability of a Class of Stochastic Parabolic Systems by one Control -- 9.3.1 Proof of the Null Controllability Result -- 9.3.2 Proof of the Negative Null Controllability Result -- 9.4 Carleman Estimate for a Stochastic Parabolic-Like Operator -- 9.5 Observability Estimate for Stochastic Parabolic Equations -- 9.5.1 Global Carleman Estimate for Stochastic Parabolic Equations, I -- 9.5.2 Global Carleman Estimate for Stochastic Parabolic Equations, II -- 9.5.3 Proof of the Observability Result -- 9.6 Null and Approximate Controllability of Stochastic Parabolic Equations -- 9.6.1 Global Carleman Estimate for Backward Stochastic Parabolic Equations -- 9.6.2 Proof of the Observability Estimate for Backward Stochastic Parabolic Equations -- 9.7 Notes and Comments -- 10 Exact Controllability for a Refined Stochastic Wave Equation -- 10.1 Formulation of the Problem -- 10.2 Well-Posedness of Stochastic Wave Equations With Boundary Controls -- 10.3 Main Controllability Results -- 10.4 A Reduction of the Exact Controllability Problem -- 10.5 A Fundamental Identity for Stochastic Hyperbolic-Like Operators -- 10.6 Observability Estimate for the Stochastic Wave Equation -- 10.7 Notes and Comments -- 11 Exact Controllability for Stochastic Schrödinger Equations -- 11.1 Formulation of the Problem and the Main Result -- 11.2 Well-Posedness of the Control System -- 11.3 A Fundamental Identity for Stochastic Schrödinger-Like Operators. , 11.4 Observability Estimate for Backward Stochastic Schrödinger Equations -- 11.5 Notes and Comments -- 12 Pontryagin-Type Stochastic Maximum Principle and Beyond -- 12.1 Formulation of the Optimal Control Problem -- 12.2 The Case of Finite Dimensions -- 12.3 Necessary Condition for Optimal Controls for Convex Control Regions -- 12.4 Operator-Valued Backward Stochastic Evolution Equations -- 12.4.1 Notions of Solutions -- 12.4.2 Preliminaries -- 12.4.3 Proof of the Uniqueness Results -- 12.4.4 Well-Posedness Result for a Special Case -- 12.4.5 Proof of the Existence and Stability for the General Case -- 12.4.6 A Regularity Result -- 12.5 Pontryagin-Type Maximum Principle -- 12.6 Sufficient Condition for Optimal Controls -- 12.6.1 Clarke's Generalized Gradient -- 12.6.2 A Sufficient Condition for Optimal Controls -- 12.7 Second Order Necessary Condition for Optimal Controls -- 12.8 Notes and Comments -- 13 Linear Quadratic Optimal Control Problems -- 13.1 Formulation of the Problem -- 13.2 Optimal Feedback for Deterministic LQ Problem in Finite Dimensions -- 13.3 Optimal Feedback for Stochastic LQ Problem in Finite Dimensions -- 13.3.1 Differences Between Deterministic and Stochastic LQ Problems in Finite Dimensions -- 13.3.2 Characterization of Optimal Feedbacks for Stochastic LQ Problems in Finite Dimensions -- 13.4 Finiteness and Solvability of Problem (SLQ) -- 13.5 Pontryagin-Type Maximum Principle for Problem (SLQ) -- 13.6 Transposition Solutions to Operator-Valued Backward Stochastic Riccati Equations -- 13.7 Existence of Optimal Feedback Operator for Problem (SLQ) -- 13.8 Global Solvability of Operator-Valued Backward Stochastic Riccati Equations -- 13.8.1 Some Preliminary Results -- 13.8.2 Proof of the Main Solvability Result -- 13.9 Some Examples -- 13.9.1 LQ Problems for Stochastic Wave Equations. , 13.9.2 LQ problems for Stochastic Schrödinger Equations -- 13.10 Notes and Comments -- References -- Index.
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  • 3
    Materialart: Buch
    Seiten: Seite 46 - 91
    Serie: Past Global Changes Magazine Vol. 27, No. 2
    Sprache: Englisch
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  • 4
    Digitale Medien
    Digitale Medien
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 99 (1995), S. 1768-1775 
    Quelle: ACS Legacy Archives
    Thema: Chemie und Pharmazie , Physik
    Materialart: Digitale Medien
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  • 5
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 107 (1997), S. 8239-8251 
    ISSN: 1089-7690
    Quelle: AIP Digital Archive
    Thema: Physik , Chemie und Pharmazie
    Notizen: Fluorene–Arn complexes formed in a pulsed supersonic jet have been studied in their S1 state using two color REMPI spectroscopy with mass resolved detection. The appearance and shifts of the S1 origins relative to the fluorene monomer are measured for cluster sizes up to n=30. The shifts and appearance of these bands are used to identify multiple conformations at low n and have indicated a shift from two sided clustering by Ar at low n to primarily one sided clustering at large n. The ionic ground state of the smaller clusters (n≤6) are studied using mass analyzed threshold ionization (MATI) spectroscopy. The change of the ionization potentials as a function of cluster size has been determined. In the case of the fluorene–Ar4 cluster, the MATI spectrum of two separate cluster conformations was measured, revealing significantly different ionization potentials. Vibrational dynamics has been studied in several smaller clusters (n≤3) by measuring MATI and ZEKE spectra when pumping vibronic transitions in the fluorene chromophore. Significantly enhanced coupling of the chromophore to van der Waals modes is observed in going from n=1 to n=3. © 1997 American Institute of Physics.
    Materialart: Digitale Medien
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  • 6
    Digitale Medien
    Digitale Medien
    s.l. : American Chemical Society
    Accounts of chemical research 25 (1992), S. 385-392 
    ISSN: 1520-4898
    Quelle: ACS Legacy Archives
    Thema: Chemie und Pharmazie
    Materialart: Digitale Medien
    Standort Signatur Einschränkungen Verfügbarkeit
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  • 7
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 99 (1993), S. 2550-2559 
    ISSN: 1089-7690
    Quelle: AIP Digital Archive
    Thema: Physik , Chemie und Pharmazie
    Notizen: Intramolecular vibrational energy redistribution (IVR) and vibrational predissociation (VP) are measured for a number of vibronic states in the S1 electronic state of the aniline-CH4 complex. The detailed dynamics are monitored using picosecond threshold photoelectron spectroscopy which is shown to be a sensitive probe of van der Waals molecule dynamics. For the lowest vibrational states accessed, the 6a10 and 6a10+24 cm−1 bands, both IVR and VP are observed and their rates are independently determined. At higher excess energy, IVR becomes the rate limiting step and the rate for VP cannot be measured independently. The results are interpreted using a serial dissociation mechanism with a simple kinetic model description. The rates of the reaction are modeled using standard Rice–Ramsperger–Kassel–Marcus (RRKM) theory which qualitatively predicts rates consistent with the experimental observations.
    Materialart: Digitale Medien
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  • 8
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 99 (1993), S. 3133-3136 
    ISSN: 1089-7690
    Quelle: AIP Digital Archive
    Thema: Physik , Chemie und Pharmazie
    Notizen: Studies are performed which measure the lifetime of very high lying molecular Rydberg states which play a central role in high resolution threshold ionization spectroscopy. The molecular systems investigated are styrene, phenol, and phenanthrene as well as the atomic iron system for comparison. It is shown that the lifetimes of the highest lying levels are determined not by intramolecular nonradiative processes but by intermolecular Rydberg–ion or Rydberg–Rydberg interactions. Under low fluence laser excitation, the highest lying Rydberg states are observed to have a lifetime greater than 25 μs but under high fluence the observed lifetime is ∼4 μs. The long Rydberg lifetimes are utilized to implement a simplified spectrometer for mass analyzed threshold ionization (MATI) spectroscopy.
    Materialart: Digitale Medien
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  • 9
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 97 (1992), S. 2843-2860 
    ISSN: 1089-7690
    Quelle: AIP Digital Archive
    Thema: Physik , Chemie und Pharmazie
    Notizen: Zero electron kinetic energy threshold photoelectron spectroscopy is applied to jet cooled aniline and the van der Waals molecules aniline–Ar, aniline–(Ar)2, and aniline–CH4. The monomer cation spectrum is assigned and more precise values of the vibrational frequencies are determined. The spectra of the cation complexes reveal significant vibronic activity indicative of a significant change in complex geometry upon ionization. The change in complex binding energy upon ionization is obtained from a determination of the complex ionization potentials. For the first time zero electron kinetic energy is used to probe van der Waals complex predissociation on the S1 electronic surface. Both reactants (complex) and products (monomer) of the reaction are observed in the photoelectron spectrum. Details of the mechanism of the zero electron kinetic energy threshold photoionization process and its impact on the observation of van der Waals molecules are discussed.
    Materialart: Digitale Medien
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  • 10
    Digitale Medien
    Digitale Medien
    s.l. : American Chemical Society
    Journal of the American Chemical Society 114 (1992), S. 3147-3148 
    ISSN: 1520-5126
    Quelle: ACS Legacy Archives
    Thema: Chemie und Pharmazie
    Materialart: Digitale Medien
    Standort Signatur Einschränkungen Verfügbarkeit
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