Results for 'No-cloning theorem'

965 found
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  1.  38
    (1 other version)Classical Cloning and No-cloning.Nicholas J. Teh - unknown
    It is part of information theory folklore that, while quantum theory prohibits the generic cloning of states, such cloning is allowed by classical information theory. Indeed, many take the phenomenon of no-cloning to be one of the features that distinguishes quantum mechanics from classical mechanics. In this paper, we use symplectic geometry to argue that pace conventional wisdom, in the case where one does not include a machine system, there is an analog of the no-cloning (...) for classical systems. However, upon adjoining a non-trivial machine system one finds that, pace the quantum case, the obstruction to cloning disappears for pure states. We then discuss the difference between this result and the quantum case, and show that it can be explained in terms of the rigidity of the theories' respective geometries. Finally, we discuss the relationship between this result and classical no-cloning arguments in the context of symmetric monoidal categories and statistical classical mechanics. (shrink)
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  2.  46
    Imperfect Cloning Operations in Algebraic Quantum Theory.Yuichiro Kitajima - 2015 - Foundations of Physics 45 (1):62-74.
    No-cloning theorem says that there is no unitary operation that makes perfect clones of non-orthogonal quantum states. The objective of the present paper is to examine whether an imperfect cloning operation exists or not in a C*-algebraic framework. We define a universal \ -imperfect cloning operation which tolerates a finite loss \ of fidelity in the cloned state, and show that an individual system’s algebra of observables is abelian if and only if there is a universal (...)
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  3. Quantum no-go theorems and consciousness.Danko Georgiev - 2013 - Axiomathes 23 (4):683-695.
    Our conscious minds exist in the Universe, therefore they should be identified with physical states that are subject to physical laws. In classical theories of mind, the mental states are identified with brain states that satisfy the deterministic laws of classical mechanics. This approach, however, leads to insurmountable paradoxes such as epiphenomenal minds and illusionary free will. Alternatively, one may identify mental states with quantum states realized within the brain and try to resolve the above paradoxes using the standard Hilbert (...)
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  4.  16
    Causality and no-go theorems.Paolo Casella & Canio Noce - 2023 - Science and Philosophy 11 (2):95-108.
    The aim of the paper is to investigate the role played by causality, and more specifically the no-signaling condition, in the assessment of the quantum theory. To this end, we discuss why it is important that even a non-relativistic theory such as Quantum Mechanics doesn’t imply a violation of this condition. Then, we use this argument to prove an original result stating that the destructive behaviour of the measurement process on the entanglement properties of quantum systems is a necessary and (...)
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  5.  92
    (1 other version)A New Problem for Quantum Mechanics.Alexander Meehan - 2020 - British Journal for the Philosophy of Science:000-000.
    In this article I raise a new problem for quantum mechanics, which I call the control problem. Like the measurement problem, the control problem places a fundamental constraint on quantum theories. The characteristic feature of the problem is its focus on state preparation. In particular, whereas the measurement problem turns on a premise about the completeness of the quantum state ('no hidden variables'), the control problem turns on a premise about our ability to prepare or control quantum states. After raising (...)
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  6.  37
    There is No New Problem for Quantum Mechanics.Lev Vaidman - 2020 - Foundations of Physics 50 (11):1728-1734.
    A recent claim by Meehan that quantum mechanics has a new “control problem” that puts limits on our ability to prepare quantum states and revises our understanding of the no-cloning theorem is examined. We identify flaws in Meehan’s analysis and argue that such a problem does not exist.
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  7.  68
    Thou Shalt Not Clone One Bit!John Conway & Simon Kochen - 2010 - Foundations of Physics 40 (4):430-433.
    We prove a no-triplets theorem for spin 1 particles, which implies a strengthened form of the no-cloning theorem.
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  8. The emancipation of chemistry.Gerald F. Thomas - 2011 - Foundations of Chemistry 14 (2):109-155.
    In his classic work The Mind and its Place in Nature published in 1925 at the height of the development of quantum mechanics but several years after the chemists Lewis and Langmuir had already laid the foundations of the modern theory of valence with the introduction of the covalent bond, the analytic philosopher C. D. Broad argued for the emancipation of chemistry from the crass physicalism that led physicists then and later—with support from a rabblement of philosophers who knew as (...)
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  9.  81
    Modal Quantum Theory.Benjamin Schumacher & Michael D. Westmoreland - 2012 - Foundations of Physics 42 (7):918-925.
    We present a discrete model theory similar in structure to ordinary quantum mechanics, but based on a finite field instead of complex amplitudes. The interpretation of this theory involves only the “modal” concepts of possibility and necessity rather than quantitative probability measures. Despite its simplicity, our model theory includes entangled states and has versions of both Bell’s theorem and the no cloning theorem.
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  10.  52
    Quantum Teleportation and Grover’s Algorithm Without the Wavefunction.Gerd Niestegge - 2017 - Foundations of Physics 47 (2):274-293.
    In the same way as the quantum no-cloning theorem and quantum key distribution in two preceding papers, entanglement-assisted quantum teleportation and Grover’s search algorithm are generalized by transferring them to an abstract setting, including usual quantum mechanics as a special case. This again shows that a much more general and abstract access to these quantum mechanical features is possible than commonly thought. A non-classical extension of conditional probability and, particularly, a very special type of state-independent conditional probability are (...)
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  11. Local Hidden Variables Underpinning of Entanglement and Teleportation.A. Kalev, A. Mann & M. Revzen - 2007 - Foundations of Physics 37 (1):125-143.
    Entangled states whose Wigner functions are non-negative may be viewed as being accounted for by local hidden variables (LHV). Recently, there were studies of Bell’s inequality violation (BIQV) for such states in conjunction with the well known theorem of Bell that precludes BIQV for theories that have LHV underpinning. We extend these studies to teleportation which is also based on entanglement. We investigate if, to what extent, and under what conditions may teleportation be accounted for via LHV theory. Our (...)
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  12. Schroedinger's Register: Foundational Issues and Physical Realization.Stephen Pink & Stanley Martens - manuscript
    This work-in-progress paper consists of four points which relate to the foundations and physical realization of quantum computing. The first point is that the qubit cannot be taken as the basic unit for quantum computing, because not every superposition of bit-strings of length n can be factored into a string of n-qubits. The second point is that the “No-cloningtheorem does not apply to the copying of one quantum register into another register, because the mathematical representation of this (...)
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  13.  49
    Evidence for the Epistemic View of Quantum States: A Toy Theory.Robert W. Spekkens - 2007 - Physical Review A 75:032110.
    We present a toy theory that is based on a simple principle: the number of questions about the physical state of a system that are answered must always be equal to the number that are unanswered in a state of maximal knowledge. Many quantum phenomena are found to have analogues within this toy theory. These include the noncommutativity of measurements, interference, the multiplicity of convex decompositions of a mixed state, the impossibility of discriminating nonorthogonal states, the impossibility of a universal (...)
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  14.  8
    No-Lose Theorems and the Pursuitworthiness of Experiments.Enno Fischer - unknown
    No-lose theorems state that---no matter what the result of an experiment will be---there will be a relevant epistemic gain if the experiment is performed. Here I provide an analysis of such theorems, looking at examples from particle physics. I argue that no-lose theorems indicate the pursuitworthiness of experiments by partially decoupling the expected epistemic gain of an experiment from the ex-ante probability that the primarily intended outcome is achieved. While an experiment's pursuitworthiness typically depends on the ex-ante probability that the (...)
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  15. Common Origin of No-Cloning and No-Deleting Principles Conservation of Information.Michał Horodecki, Ryszard Horodecki, Aditi Sen & Ujjwal Sen - 2005 - Foundations of Physics 35 (12):2041-2049.
    We discuss the role of the notion of information in the description of physical reality. We consider theories for which dynamics is linear with respect to stochastic mixing. We point out that the no-cloning and no-deleting principles emerge in any such theory, if law of conservation of information is valid, and two copies contain more information than one copy. We then describe the quantum case from this point of view.
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  16.  63
    No-Go Theorems Face Background-Based Theories for Quantum Mechanics.Louis Vervoort - 2016 - Foundations of Physics 46 (4):458-472.
    Recent experiments have shown that certain fluid-mechanical systems, namely oil droplets bouncing on oil films, can mimic a wide range of quantum phenomena, including double-slit interference, quantization of angular momentum and Zeeman splitting. Here I investigate what can be learned from these systems concerning no-go theorems as those of Bell and Kochen-Specker. In particular, a model for the Bell experiment is proposed that includes variables describing a ‘background’ field or medium. This field mimics the surface wave that accompanies the droplets (...)
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  17. Reconsidering No-Go Theorems from a Practical Perspective.Michael E. Cuffaro - 2018 - British Journal for the Philosophy of Science 69 (3):633-655.
    I argue that our judgements regarding the locally causal models that are compatible with a given constraint implicitly depend, in part, on the context of inquiry. It follows from this that certain quantum no-go theorems, which are particularly striking in the traditional foundational context, have no force when the context switches to a discussion of the physical systems we are capable of building with the aim of classically reproducing quantum statistics. I close with a general discussion of the possible implications (...)
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  18.  52
    No-Go Theorems and the Foundations of Quantum Physics.Andrea Oldofredi - 2018 - Journal for General Philosophy of Science / Zeitschrift für Allgemeine Wissenschaftstheorie 49 (3):355-370.
    In the history of quantum physics several no-go theorems have been proved, and many of them have played a central role in the development of the theory, such as Bell’s or the Kochen–Specker theorem. A recent paper by F. Laudisa has raised reasonable doubts concerning the strategy followed in proving some of these results, since they rely on the standard framework of quantum mechanics, a theory that presents several ontological problems. The aim of this paper is twofold: on the (...)
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  19. No-Forcing and No-Matching Theorems for Classical Probability Applied to Quantum Mechanics.Ehtibar N. Dzhafarov & Janne V. Kujala - 2014 - Foundations of Physics 44 (3):248-265.
    Correlations of spins in a system of entangled particles are inconsistent with Kolmogorov’s probability theory (KPT), provided the system is assumed to be non-contextual. In the Alice–Bob EPR paradigm, non-contextuality means that the identity of Alice’s spin (i.e., the probability space on which it is defined as a random variable) is determined only by the axis $\alpha _{i}$ chosen by Alice, irrespective of Bob’s axis $\beta _{j}$ (and vice versa). Here, we study contextual KPT models, with two properties: (1) Alice’s (...)
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  20.  54
    A no-go theorem about rotation in relativity theory.David B. Malament - unknown
    Within the framework of general relativity, in some cases at least, it is a delicate and interesting question just what it means to say that an extended body is or is not "rotating". It is so for two reasons. First, one can easily think of different criteria of rotation. Though they agree if the background spacetime structure is sufficiently simple, they do not do so in general. Second, none of the criteria fully answers to our classical intuitions. Each one exhibits (...)
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  21.  25
    (1 other version)Two No-Go Theorems for Modal Interpretations of Quantum Mechanics.Pieter E. Vermaas - 1998 - Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics 30 (3):403-431.
    Modal interpretations take quantum mechanics as a theory which assigns at all times definite values to magnitudes of quantum systems. In the case of single systems, modal interpretations manage to do so without falling prey to the Kochen and Specker no-go theorem, because they assign values only to a limited set of magnitudes. In this paper I present two further no-go theorems which prove that two modal interpretations become nevertheless problematic when applied to more than one system. The first (...)
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  22. Two no-go theorems for modal interpretations of quantum mechanics.E. P. - 1999 - Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics 30 (3):403-431.
    Modal interpretations take quantum mechanics as a theory which assigns at all times definite values to magnitudes of quantum systems. In the case of single systems, modal interpretations manage to do so without falling prey to the Kochen and Specker no-go theorem, because they assign values only to a limited set of magnitudes. In this paper I present two further no-go theorems which prove that two modal interpretations become nevertheless problematic when applied to more than one system. The first (...)
     
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  23.  53
    The 'No-Supervenience' Theorem and its Implications for Theories of Consciousness.Catherine M. Reason - 2024 - Journal of Consciousness Studies 31 (1):138-148.
    The 'no-supervenience' theorem (Reason, 2019; Reason and Shah, 2021) is a proof that no fully self-aware system can entirely supervene on any objectively observable system. I here present a simple, non-technical summary of the proof and demonstrate its implications for four separate theories of consciousness: the 'property dualism' theory of David Chalmers; the 'reflexive monism' of Max Velmans; Galen Strawson's 'realistic monism'; and the 'illusionism' of Keith Frankish. It is shown that all are ruled out in their current form (...)
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  24.  24
    Interpreting cosmic no hair theorems: Is fatalism about the far future of expanding cosmological models unavoidable?Juliusz Doboszewski - 2019 - Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics 66:170-179.
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  25.  47
    No-go theorems: What are they good for?Radin Dardashti - 2021 - Studies in History and Philosophy of Science Part A 86 (C):47-55.
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  26.  65
    A No-Trade Theorem under Knightian Uncertainty with General Preferences.Chenghu Ma - 2001 - Theory and Decision 51 (2/4):173-181.
    This paper derives a no-trade theorem under Knightian uncertainty, which generalizes the theorem of Milgrom and Stokey by allowing general preference relations. It is shown that the no-trade theorem holds true as long as agents' preferences are dynamically consistent in the sense of Machina and Schmeidler, and satisfies the so-called piece-wise monotonicity axiom. A preference satisfying the piece-wise monotonicity axiom does not necessarily imply the additive utility representation, nor is necessarily based on beliefs.
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  27.  12
    A No-Go Theorem for $$\psi$$-Ontic Models? Yes! Response to Criticisms.Gabriele Carcassi, Andrea Oldofredi & Christine A. Aidala - 2024 - Foundations of Physics 55 (1):1-9.
    This short note addresses the criticisms recently proposed by Shan Gao against our article “On the Reality of the Quantum State Once Again: A No-Go Theorem for $$\psi$$ -Ontic Models” (Found. Phys. 54:14). The essay aims to respond to such objections and to show once again that the theorem proved in our paper is correct, and therefore true—contrary to Gao’s claims. Philosophical consequences of this fact are briefly discussed.
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  28.  87
    The No-Signalling Theorems: A Nitpicking Distinction.Kent A. Peacock - unknown
    It seems to me that it is among the most sure-footed of quantum physicists, those who have it in their bones, that one finds the greatest impatience with the idea that the ‘foundations of quantum mechanics’ might need some attention. Knowing what is right by instinct, they can become a little impatient with nitpicking distinctions between theorems and assumptions. —John Stewart Bell [4, p. 33].
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  29.  22
    On the Reality of the Quantum State Once Again: A No-Go Theorem for $$\psi$$ -Ontic Models?Shan Gao - 2024 - Foundations of Physics 54 (4):1-6.
    In a recent paper (Found Phys 54:14, 2024), Carcassi, Oldofredi and Aidala concluded that the \(\psi\) -ontic models defined by Harrigan and Spekkens cannot be consistent with quantum mechanics, since the information entropy of a mixture of non-orthogonal states are different in these two theories according to their information theoretic analysis. In this paper, I argue that this no-go theorem for \(\psi\) -ontic models is false by explaining the physical origin of the von Neumann entropy in quantum mechanics.
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  30. Screening-Off and Causal Incompleteness: A No-Go Theorem.Elliott Sober & Mike Steel - 2013 - British Journal for the Philosophy of Science 64 (3):513-550.
    We begin by considering two principles, each having the form causal completeness ergo screening-off. The first concerns a common cause of two or more effects; the second describes an intermediate link in a causal chain. They are logically independent of each other, each is independent of Reichenbach's principle of the common cause, and each is a consequence of the causal Markov condition. Simple examples show that causal incompleteness means that screening-off may fail to obtain. We derive a stronger result: in (...)
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  31.  27
    Aumann's “No Agreement” Theorem Generalized.Matthias Hild, Richard Jeffrey & Mathias Risse - 1999 - In Cristina Bicchieri, Richard C. Jeffrey & Brian Skyrms (eds.), The logic of strategy. New York: Oxford University Press. pp. 92--100.
  32. Another no‐go theorem for hidden variable models of inaccurate spin 1 measurements.Thomas Breuer - 2002 - Philosophy of Science 70 (5):1368-1379.
    Uncertainty about the actual orientation of the measurement device has been claimed to open a loophole for hidden variable models of quantum mechanics. In this paper I describe the statistics of inaccurate spin measurements by unsharp spin observables. A no‐go theorem for hidden variable models of the inaccurate measurement statistics follows: There is a finite set of directions for which not all results of inaccurate spin measurements can be predetermined in a non‐contextual way. In contrast to an earlier (...) (Breuer 2002) this result does not rely on the assigment of approximate truth values, and it holds under weaker assumptions on the measurement inaccuracy. (shrink)
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  33.  39
    How the Natural Interpretation of QM Avoids the Recent No-Go Theorem.Anthony Rizzi - 2020 - Foundations of Physics 50 (3):204-215.
    A recent no-go theorem gives an extension of the Wigner’s Friend argument that purports to prove the “Quantum theory cannot consistently describe the use of itself.” The argument is complex and thought provoking, but fails in a straightforward way if one treats QM as a statistical theory in the most fundamental sense, i.e. if one applies the so-called ensemble interpretation. This explanation is given here at an undergraduate level, which can be edifying for experts and students alike. A recent (...)
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  34.  18
    Taking Mermin's Relational Interpretation of QM Beyond Cabello's and Seevinck's No-Go Theorems.Christian de Ronde, Raimundo Fernández Mouján & Massri Cesar - unknown
    In this paper we address a deeply interesting debate that took place at the end of the last millennia between David Mermin, Adan Cabello and Michiel Seevinck, regarding the meaning of relationalism within quantum theory. In a series of papers, Mermin proposed an interpretation in which quantum correlations were considered as elements of physical reality. Unfortunately, the very young relational proposal by Mermin was too soon tackled by specially suited no-go theorems designed by Cabello and Seevinck. In this work we (...)
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  35.  18
    Two-Qubit Operators in No-Splitting Theorems.B. Shravan Kumar & S. Balakrishnan - 2022 - Foundations of Physics 52 (3):1-14.
    Applications of quantum mechanics in the computational and information processing tasks is a recent research interest among the researchers. Certain operations which are impossible to achieve in the description of quantum mechanics are known as no-go theorems. One such theorem is no-splitting theorem of quantum states. The no-splitting theorem states that the information in an unknown quantum bit is an inseparable entity and cannot be split into two complementary qubits. In this work, we try to find out (...)
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  36.  25
    A SQUID No-Go theorem without macrorealism: What SQUID's really tell us about nature. [REVIEW]Sara Foster & Andrew Elby - 1991 - Foundations of Physics 21 (7):773-785.
    Without invoking macrorealism, we derive a contradiction between the quantum mechanical predictions forsquid's and two intuitive conditions. First, we assume that asquid can be measured without significantly disturbing its subsequent macroscopic behavior. Second, we assume a trivial realism condition much weaker than Leggett's macrorealism. Quantum mechanics itself obeys our realism assumption. This proof suggests that althoughsquid experiments cannot rule out macrorealism, they can rule out most theories that allow noninvasive measurements.
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  37.  64
    Higher complexity search problems for bounded arithmetic and a formalized no-gap theorem.Neil Thapen - 2011 - Archive for Mathematical Logic 50 (7):665-680.
    We give a new characterization of the strict $$\forall {\Sigma^b_j}$$ sentences provable using $${\Sigma^b_k}$$ induction, for 1 ≤ j ≤ k. As a small application we show that, in a certain sense, Buss’s witnessing theorem for strict $${\Sigma^b_k}$$ formulas already holds over the relatively weak theory PV. We exhibit a combinatorial principle with the property that a lower bound for it in constant-depth Frege would imply that the narrow CNFs with short depth j Frege refutations form a strict hierarchy (...)
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  38. The no-free-lunch theorems of supervised learning.Tom F. Sterkenburg & Peter D. Grünwald - 2021 - Synthese 199 (3-4):9979-10015.
    The no-free-lunch theorems promote a skeptical conclusion that all possible machine learning algorithms equally lack justification. But how could this leave room for a learning theory, that shows that some algorithms are better than others? Drawing parallels to the philosophy of induction, we point out that the no-free-lunch results presuppose a conception of learning algorithms as purely data-driven. On this conception, every algorithm must have an inherent inductive bias, that wants justification. We argue that many standard learning algorithms should rather (...)
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  39.  30
    Virtual reality: Consequences of no-go theorems for the modal interpretation of quantum mechanics.Guido Bacciagaluppi & Pieter E. Vermaas - 1999 - In Maria Luisa Dalla Chiara (ed.), Language, Quantum, Music. Springer. pp. 117--128.
  40.  83
    Bell, Bohm, and von Neumann: some philosophical inequalities concerning no-go theorems and the axiomatic method.Michael Stoeltzner - 2002 - In Tomasz Placek & Jeremy Butterfield (eds.), Non-locality and Modality. Dordrecht and Boston: Kluwer Academic Publishers. pp. 37--58.
    The present paper investigates the philosophical relationship between John von Neumann’s Nohidden-variable theorem and Bell’s inequalities. Bell erroneously takes the axiomatic method as implying a finality claim and thus ignores von Neumann’s strongly pragmatist stance towards mathematical physics. If one considers, however, Hilbert’s axiomatic method as a critical enterprise, Bell’s theorem improves von Neumann’s by defining a more appropriate notion of ‘ hidden variable’ that permits one to include Bohm’s interpretation which recovers the predictive content of quantum mechanics. (...)
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  41.  47
    Human Cloning: A Case of no Harm Done?M. A. Roberts - 1996 - Journal of Medicine and Philosophy 21 (5):537-554.
    Some have objected to the laboratory cloning of human preembryos on the grounds that the procedure would violate the dignity of and respect owed to human preembryos. Others have argued that human cloning ought be permitted if it will predictably benefit, or at least not burden, individuals who are, unlike the human preembryo, clearly entitled to our respect and concern. Taking this latter position, the legal theorist John A. Robertson has argued that, since cloning does not harm (...)
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  42. The End Times of Philosophy.François Laruelle - 2012 - Continent 2 (3):160-166.
    Translated by Drew S. Burk and Anthony Paul Smith. Excerpted from Struggle and Utopia at the End Times of Philosophy , (Minneapolis: Univocal Publishing, 2012). THE END TIMES OF PHILOSOPHY The phrase “end times of philosophy” is not a new version of the “end of philosophy” or the “end of history,” themes which have become quite vulgar and nourish all hopes of revenge and powerlessness. Moreover, philosophy itself does not stop proclaiming its own death, admitting itself to be half dead (...)
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  43.  40
    On the Reality of the Quantum State Once Again: A No-Go Theorem for ψ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\psi$$\end{document}-Ontic Models. [REVIEW]Christine A. Aidala, Andrea Oldofredi & Gabriele Carcassi - 2024 - Foundations of Physics 54 (1):1-15.
    In this paper we show that ψ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\psi$$\end{document}-ontic models, as defined by Harrigan and Spekkens (HS), cannot reproduce quantum theory. Instead of focusing on probability, we use information theoretic considerations to show that all pure states of ψ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\psi$$\end{document}-ontic models must be orthogonal to each other, in clear violation of quantum mechanics. Given that (i) Pusey, Barrett and Rudolph (PBR) previously showed that ψ\documentclass[12pt]{minimal} \usepackage{amsmath} (...)
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  44. No More Cloning Around.Arthur Caplan - 2008 - Free Inquiry 28:20-20.
     
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  45.  62
    No Free Lunch Theorem, Inductive Skepticism, and the Optimality of Meta-induction.Gerhard Schurz - 2017 - Philosophy of Science 84 (5):825-839.
    The no free lunch theorem is a radicalized version of Hume’s induction skepticism. It asserts that relative to a uniform probability distribution over all possible worlds, all computable prediction algorithms—whether ‘clever’ inductive or ‘stupid’ guessing methods —have the same expected predictive success. This theorem seems to be in conflict with results about meta-induction. According to these results, certain meta-inductive prediction strategies may dominate other methods in their predictive success. In this article this conflict is analyzed and dissolved, by (...)
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  46.  50
    No Escape from Vardanyan's theorem.Albert Visser & Maartje de Jonge - 2006 - Archive for Mathematical Logic 45 (5):539-554.
    Vardanyan's theorem states that the set of PA-valid principles of Quantified Modal Logic, QML, is complete Π0 2. We generalize this result to a wide class of theories. The crucial step in the generalization is avoiding the use of Tennenbaum's Theorem.
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  47.  93
    The No Free Lunch Theorem: Bad News for (white's Account of) the Problem of Induction.Gerhard Schurz - 2021 - Episteme 18 (1):31-45.
    White (2015) proposes an a priori justification of the reliability of inductive prediction methods based on his thesis of induction-friendliness. It asserts that there are by far more induction-friendly event sequences than induction-unfriendly event sequences. In this paper I contrast White's thesis with the famous no free lunch (NFL) theorem. I explain two versions of this theorem, the strong NFL theorem applying to binary and the weak NFL theorem applying to real-valued predictions. I show that both (...)
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  48.  36
    The Implications of the No-Free-Lunch Theorems for Meta-induction.David H. Wolpert - 2023 - Journal for General Philosophy of Science / Zeitschrift für Allgemeine Wissenschaftstheorie 54 (3):421-432.
    The important recent book by Schurz ( 2019 ) appreciates that the no-free-lunch theorems (NFL) have major implications for the problem of (meta) induction. Here I review the NFL theorems, emphasizing that they do not only concern the case where there is a uniform prior—they prove that there are “as many priors” (loosely speaking) for which any induction algorithm _A_ out-generalizes some induction algorithm _B_ as vice-versa. Importantly though, in addition to the NFL theorems, there are many _free lunch_ theorems. (...)
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    Response to Special Section: “Cloning: Technology, Policy, and Ethics” (CQ Vol 7, No 2) But What If We Feel That Cloning Is Wrong? [REVIEW]Matti Häyry - 2001 - Cambridge Quarterly of Healthcare Ethics 10 (2):205-208.
    The idea of cloning adult human beings often gives rise to objections involving mad dictators producing copies of themselves, or deranged billionaires who want to live forever. But what about situations where we can more readily understand and accept the reasons for creating a clone? Consider, for instance, the case of parents who have simultaneously lost their newly born child and found out that they cannot have any more children of their own by other known methods. Would it be (...)
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  50. No one knows the date or the hour: An unorthodox application of rev. Bayes's theorem.Paul Bartha & Christopher Hitchcock - 1999 - Philosophy of Science 66 (3):353.
    Carter and Leslie (1996) have argued, using Bayes's theorem, that our being alive now supports the hypothesis of an early 'Doomsday'. Unlike some critics (Eckhardt 1997), we accept their argument in part: given that we exist, our existence now indeed favors 'Doom sooner' over 'Doom later'. The very fact of our existence, however, favors 'Doom later'. In simple cases, a hypothetical approach to the problem of 'old evidence' shows that these two effects cancel out: our existence now yields no (...)
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