2000
DOI: 10.1088/0264-9381/17/9/302
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A general worldline quantum inequality

Abstract: Worldline quantum inequalities provide lower bounds on weighted averages of the renormalised energy density of a quantum field along the worldline of an observer. In the context of real, linear scalar field theory on an arbitrary globally hyperbolic spacetime, we establish a worldline quantum inequality on the normal ordered energy density, valid for arbitrary smooth timelike trajectories of the observer, arbitrary smooth compactly supported weight functions and arbitrary Hadamard quantum states. Normal orderi… Show more

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Cited by 134 publications
(282 citation statements)
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“…The work described in this section, conducted with Verch [18] and building on earlier work [8,43], uncovers a circle of connections between stability conditions operating at three different scales: the microscopic (Hadamard condition/microlocal spectrum condition), mesoscopic (QEIs) and macroscopic (thermodynamic stability, expressed by the notion of passivity [40]). Each connection takes the form of a rigorous theorem; the reader should be cautioned, however, that the conclusions and hypotheses of successive links do not match perfectly.…”
Section: Stability At Three Scalesmentioning
confidence: 97%
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“…The work described in this section, conducted with Verch [18] and building on earlier work [8,43], uncovers a circle of connections between stability conditions operating at three different scales: the microscopic (Hadamard condition/microlocal spectrum condition), mesoscopic (QEIs) and macroscopic (thermodynamic stability, expressed by the notion of passivity [40]). Each connection takes the form of a rigorous theorem; the reader should be cautioned, however, that the conclusions and hypotheses of successive links do not match perfectly.…”
Section: Stability At Three Scalesmentioning
confidence: 97%
“…They have since been established for the free Klein-Gordon [22,24,26,38,10,16,8,19,47,20], Dirac [47,17,12], Maxwell [26,37,14] and Proca [14] quantum fields in both flat and curved spacetimes, the RaritaSchwinger field in Minkowski space [49], and also for general unitary positiveenergy conformal field theories in two-dimensional Minkowski space [11]. We will not give a full history of the development of the subject, referring the reader to the recent reviews [9,42].…”
Section: Quantum Energy Inequalitiesmentioning
confidence: 99%
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“…Since φ [F T ] = φ ( f T ) (see (10)), this means that the Hawking radiation flux measured by a distant detector is highly entangled with field observables 15 Negative energy fluxes of stress-energy or negative energy densities can occur in quantum field theory even for fields that classically satisfy the dominant energy condition, see e.g. [32,34]. 16 Of course, the approximate description leading to this prediction should be valid only when M M P , where M P denotes the Planck mass (∼ 10 −5 gm), but modifications to the evaporation process at this stage (including the possibility of Planck mass remnants) would not significantly alter the discussion below.…”
Section: C) Hawking Effectmentioning
confidence: 99%