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9780198515722

The Feynman Integral and Feynman's Operational Calculus

by ;
  • ISBN13:

    9780198515722

  • ISBN10:

    0198515723

  • Edition: Reprint
  • Format: Paperback
  • Copyright: 2002-03-28
  • Publisher: Clarendon Press

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Summary

The aim of this book is to make accessible to mathematicians, physicists and other scientists interested in quantum theory, the mathematically beautiful but difficult subjects of the Feynman integral and Feynman's operational calculus. Some advantages of the four approaches to the Feynman integral which are given detailed treatment in this book are the following: the existence of the Feynman integral is established for very general potentials in all four cases; under more restrictive but still broad conditions, three of these Feynman integrals agree with one another and with the unitary group from the usual approach to quantum dynamics; these same three Feynman integrals possess pleasant stability properties. Much of the material covered here was previously only in the research literature, and the book also contains some new results. The background material in mathematics and physics that motivates the study of the Feynman integral and Feynman's operational calculus is discussed and detailed proofs are provided for the central results.

Table of Contents

Introduction
1(23)
General introductory comments
1(7)
Feynman's path integral
1(3)
Feynman's operational calculus
4(1)
Feynman's operational calculus via the Feynman and Wiener integrals
5(2)
Feynman's operational calculus and evolution equations
7(1)
Further work on or related to the Feynman integral: Chapter 20
8(1)
Recurring themes and their connections with the Feynman integral and Feynman's operational calculus
8(9)
Product formulas and applications to the Feynman integral
8(2)
Feynman--Kac formula: Analytic continuation in time and mass
10(2)
The role of operator theory
12(1)
Connections between the Feynman--Kac and Trotter product formulas
13(1)
Evolution equations
13(2)
Functions of noncommuting operators
15(1)
Time-ordered perturbation series
15(1)
The use of measures
16(1)
Relationship with the motivating physical theories: background and quantum-mechanical models
17(7)
Physical background
17(1)
Highly singular potentials
18(1)
Time-dependent potentials
19(1)
Phenomenological models: complex and nonlocal potentials
19(2)
Prerequisites, new material, and organization of the book
21(3)
The physical phenomenon of Brownian motion
24(7)
A brief historical sketch
24(4)
Einstein's probabilistic formula
28(3)
Wiener measure
31(31)
There is no reasonable translation invariant measure on Wiener space
32(2)
Construction of Wiener measure
34(8)
Wiener's integration formula and applications
42(9)
Finitely based functions
43(2)
Applications
45(6)
Axiomatic description of the Wiener process
51(1)
Nondifferentiability of Wiener paths
51(6)
d-dimensional Wiener measure and Wiener process
57(1)
Appendix: Converse measurability results
57(3)
Appendix: B(X x Y) = B(X) B(Y)
60(2)
Scaling in Wiener space and the analytic Feynman integral
62(27)
Quadratic variation of Wiener paths
63(4)
Scale change in Wiener space
67(7)
Translation pathologies
74(3)
Scale-invariant measurable functions
77(2)
The scalar-valued analytic Feynman integral
79(3)
The nonexistence of Feynman's ``measure''
82(3)
Appendix: Some useful Gaussian-type integrals
85(2)
Appendix: Proof of formula (4.2.3a)
87(2)
Stochastic processes and the Wiener process
89(5)
Stochastic processes and probability measures on function spaces
89(1)
The Kolmogorov consistency theorem
90(2)
Two realizations of the Wiener process
92(2)
Quantum dynamics and the Schrodinger equation
94(5)
Hamiltonian approach to quantum dynamics
94(1)
Transition amplitudes and measurement
95(1)
The Heisenberg uncertainty principle
96(1)
Hamiltonian for a system of particles
97(2)
The Feynman integral: heuristic ideas and mathematical difficulties
99(22)
Introduction
99(2)
Feynman's formula
101(5)
Connections with classical mechanics: The method of stationary phase
105(1)
Heuristic derivation of the Schrodinger equation
106(3)
Feynman's approximation formula
109(2)
Nelson's approach via the Trotter product formula
111(4)
The Trotter product formula
114(1)
The approach via analytic continuation
115(6)
Semigroups of operators: an informal introduction
121(6)
Linear semigroups of operators
127(25)
Infinitesimal generator
127(7)
Integral equation
129(1)
Evolution equation
130(1)
Closed unbounded operators
130(4)
Examples of semigroups and their generators
134(4)
The translation semigroup
134(1)
The heat semigroup
135(2)
The Poisson semigroup
137(1)
The resolvent
138(2)
Generation theorems
140(3)
The Hille--Yosida theorem
140(1)
Dissipative operators and the Lumer--Phillips theorem
141(2)
Uniformly continuous and weakly continuous semigroups
143(1)
Self-adjoint operators, unitary groups and Stone's theorem
144(3)
Perturbation theorems
147(5)
Unbounded self-adjoint operators and quadratic forms
152(45)
Spectral theorem for unbounded self-adjoint operators
153(8)
Multiplication operators
153(2)
Three useful forms of the spectral theorem
155(6)
Applications of the spectral theorem
161(15)
The free Hamiltonian H0
161(2)
The heat semigroup and unitary group
163(8)
Standard cores for the free Hamiltonian
171(3)
Imaginary resolvents
174(2)
Representation theorems for unbounded quadratic forms
176(17)
Basic definitions and properties
176(7)
Representation theorems for quadratic forms
183(7)
The form sum of operators
190(3)
Conditions on the potential V for H0-form boundedness
193(4)
Product formulas with applications to the Feynman integral
197(75)
Trotter and Chernoff product formulas
198(6)
Product formula for unitary groups
203(1)
Feynman integral via the Trotter product formula
204(16)
Criteria for essential self-adjointness of positive operators
204(1)
A brief outline of distribution theory
205(1)
Kato's distributional inequality
206(4)
Essential self-adjointness of the Hamiltonian H = H0 + V
210(5)
Conditions on the potential V for H0-operator boundedness
215(2)
Feynman integral via the Trotter product formula for unitary groups
217(3)
Product formula for imaginary resolvents
220(12)
Hypotheses and statement of the main result
220(2)
Proof of the product formula
222(7)
Consequences, extensions and open problems
229(3)
Application to the modified Feynman integral
232(13)
Modified Feynman integral and Schrodinger equation with singular potential
233(8)
Extensions: Riemannian manifolds and magnetic vector potentials
241(4)
Dominated convergence theorem for the modified Feynman integral
245(14)
Preliminaries
247(1)
Perturbation of form sums of self-adjoint operators
248(4)
Application to a general dominated convergence theorem for Feynman integrals
252(7)
The modified Feynman integral for complex potentials
259(7)
Product formula for imaginary resolvents of normal operators
260(3)
Application to dissipative quantum systems
263(3)
Appendix: Extended Vitali's theorem with application to unitary groups
266(6)
Extension of Vitali's theorem for sequences for analytic functions
266(3)
Analytic continuation and product formula for unitary groups
269(3)
The Feynman-Kac formula
272(21)
The Feynman-Kac formula, the heat equation and the Wiener integral
273(3)
Proof of the Feynman--Kac formula
276(14)
Bounded potentials
276(6)
Monotone convergence theorems for forms and integrals
282(2)
Unbounded potentials
284(6)
Consequences
290(3)
Analytic-in-time or-mass operator-valued Feynman integrals
293(81)
Introduction
293(5)
The analytic-in-time operator-valued Feynman integral
298(2)
Proof of existence
300(3)
The Feynman integrals compared with one another and with the unitary group. Application to stability theorems
303(5)
The analytic-in-mass operator-valued Feynman integral
308(23)
Definition of the analytic-in-mass operator-valued Feynman integral
309(3)
Nelson's results
312(9)
Haugsby's result for time-dependent, complex-valued potentials
321(2)
Further extensions via a product formula for semigroups
323(8)
The analytic-in-mass modified Feynman integral
331(27)
Existence of the analytic-in-mass modified Feynman integral
334(3)
Product formula for resolvents: The case of imaginary mass
337(8)
Comparison with other analytic-in-mass Feynman integrals
345(1)
Highly singular central potentials---the attractive inverse-square potential
346(12)
The analytic-in-time operator-valued Feynman integral via additive functionals of Brownian motion
358(16)
Introductory remarks
359(1)
The parallel with Section 13.3
359(2)
Generalized signed measures
361(1)
The generalized Kato class
361(1)
Capacity on Rd
362(1)
Smooth measures
363(1)
Positive continuous additive functionals of Brownian motion
364(1)
The relationship between smooth measures and PCAFs
365(2)
The analytic-in-time operator-valued Feynman integral exists for μ = μ+ - μ_ S -- GKd
367(1)
Examples
368(6)
Feynman's operational calculus for noncommuting operators: an introduction
374(30)
Functions of operators
375(1)
The rules for Feynman's operational calculus
376(7)
Feynman's time-ordering convention
377(1)
Feynman's heuristic rules
377(1)
Two elementary examples
378(5)
Time-ordered Perturbation series
383(11)
Perturbation series via Feynman's operational calculus
383(6)
Perturbation series via a path integral
389(4)
The origins of Feynman's operational calculus rigorous
393(1)
Making Feynman's operational calculus rigorous
394(3)
Rigor via path integrals
394(1)
Well-defined and useful formulas arrived at via Feynman's heuristic rules
395(1)
A general theory of Feynman's operational calculus with computations which are rigorous at each stage
396(1)
Feynman's operational calculus via Wiener and Feynman integrals: Comments on Chapter 15--18
397(7)
Generalized Dyson series, the Feynman integral and Feynman's operational calculus
404(58)
Introduction
404(3)
The analytic operator-valued Feynman integral
407(9)
Notation and definitions
407(3)
The analytic (in mass) operator-valued Feynman integral Ktλ(·)
410(3)
Preliminary results
413(3)
A simple generalized Dyson series (η = μ + ωδτ)
416(10)
The classical Dyson series
424(2)
Generalized Dyson series: The general case
426(8)
Disentangling via perturbation expansions: Examples
434(12)
A single measure and potential
435(7)
Several measures and potentials
442(4)
Generalized Feynman diagrams
446(5)
Commutative Banach algebras of functionals: The disentangling algebras
451(11)
The disentangling algebras At
452(3)
The time-reversal map on At and the natural physical ordering
455(4)
Connections with Feynman's operational calculus
459(3)
Stability results
462(15)
Stability in the potentials
462(2)
Stability in the measures
464(13)
The Feynman--Kac formula with a Lebesgue--Stieltjes measure and Feynman's operational calculus
477(53)
Introduction
477(3)
Notation and hypotheses
478(2)
The Feynman--Kac formula with a Lebesgue--Stieltjes measure: Finitely supported discrete part v
480(6)
Integral equation (Integrated form of the evolution equation)
480(1)
Differential equation (differential form of the evolution equation)
481(1)
Discontinuities (in time) of the solution
482(1)
Propagator and explicit solution
483(3)
Derivation of the integral equation in a simple case (η = μ + ωδτ)
486(10)
Sketch of the proof when v is finitely supported
495(1)
Discontinuities of the solution to the evolution equation
496(3)
The time discontinuities
496(1)
Differential equation and change of initial condition
497(2)
Explicit solution and physical interpretations
499(8)
Continuous measure: Uniqueness of the solution
500(1)
Measure with finitely supported discrete part: Propagator and explicit solution
501(2)
Physical interpretations in the quantum-mechanical case
503(1)
Physical interpretations in the diffusion case
504(1)
Further connections with Feynman's Operational calculus
505(2)
The Feynman--Kac formula with a Lebesgue--Stieltjes measure: The general case (arbitrary measure η)
507(23)
Integral equation (integrated form of the evolution equation)
507(2)
Basic properties of the solution to the integral equation
509(2)
Quantum-mechanical case: Reformulation in the interaction (or Dirac) picture
511(3)
Product integral representation of the solution
514(3)
Distributional differential equation (true differential form of the evolution equation)
517(2)
Unitary propagators
519(1)
Scattering matrix and improper product integral
520(1)
Sketch of the proof of the integral equation
521(9)
Noncommutative operations on Wiener functionals, disentangling algebras and Feynman's operational calculus
530(32)
Introduction
530(2)
Preliminaries: maps, measures and measurability
532(3)
The noncommutative operations * and +
535(5)
The functional integrals Ktλ(·) and the operations * and +
540(4)
The disentangling algebras At, the operations * and +, and the disentangling process
544(9)
Examples: Trigonometric, binomial and exponential formulas
552(1)
Appendix: Quantization, axiomatic Feynman's operational calculus, and generalized functional integral
553(9)
Algebraic and analytic axioms
554(2)
Consequences of the axioms
556(3)
Examples: the disentangling algebras and analytic Feynman integrals
559(3)
Feynman's operational calculus and evolution equations
562(47)
Introduction and hypotheses
562(6)
Feynman's operational calculus as a generalized path integral
562(1)
Exponentials of sums of noncommuting operators
563(1)
Disentangling exponentials of sums via perturbation series
563(2)
Local and nonlocal potentials
565(1)
Hypotheses
566(2)
Disentangling exp{--tα + ∫t0 β(s)μ(ds)}
568(5)
Disentangling exp{-tα + ∫t0 β1(s)μ1(ds) + ... + ∫t0 βn(s)μn(ds)}
573(8)
Convergence of the disentangled series
581(6)
The evolution equation
587(9)
Uniqueness of the solution to the evolution equation
596(3)
Further examples of the disentangling process
599(10)
Nonlocal potentials relevant to phenomenological nuclear theory
604(5)
Further work on or related to the Feynman integral
609(88)
Transform approaches to the Feynman integral. References to further approaches
609(28)
The Fresnel integral and other transform approaches to the Feynman integral
610(1)
The Fresnel integral
610(1)
Properties of the Fresnel integral
611(2)
An approach to the Feynman integral via the Fresnel integral
613(1)
Advantages and disadvantages of Fresnel integral approaches to the Feynman integral
613(2)
The Feynman map
615(1)
The Poison process and transforms
616(1)
A ``Fresnel integral'' on classical Wiener space
616(4)
The Banach algebras S and F(H1) are the same
620(1)
Consequences of the close relationship between S and F(H1)
621(1)
More functions in F(H1)
622(1)
A unified theory of Fresnel integrals: Introductory remarks
623(1)
Background material
624(2)
A unified theory of Fresnel integrals (continued)
626(3)
The Fresnel classes along with quadratic forms
629(1)
The classes Gq(H) and Gq(B)
630(1)
Quadratic forms extended
631(1)
Functions in the Fresnel class of an abstract Wiener space: Examples of abstract Wiener spaces
632(4)
Fourier--Feynman transforms, convolution, and the first variation for functions in S
636(1)
References to further approaches to the Feynman integral
636(1)
The influence of heuristic Feynman integrals on contemporary mathematics and physics: Some examples
637(60)
The heuristic Feynman path integral
638(1)
Knot invariants and low-dimentional topology
639(1)
The Jones polynomial invariant for knots and links
639(2)
Witten's topological invariants via Feynman path integrals
641(13)
Further developments: Vassiliev invariants and the Kontsevich integral
654(5)
Further comments and references on subjects related to the Feynman integral
659(1)
Supersymmetric Feynman path integrals and the Atiyah--Singer index theorem
659(15)
Deformation quantization: Star products and perturbation series
674(8)
Gauge field theory and Feynman path integrals
682(6)
String theory, Feynman--Polyakov integrals, and dualities
688(7)
What lies ahead? Towards a geometrization of Feynman path integrals?
695(2)
References 697(48)
Index of symbols 745(5)
Author index 750(6)
Subject index 756

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