Schopenhauer on Space, Time, Causality and Matter: a Physical Re-Examination
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Introduction to Dynamical Triangulations
Introduction to Dynamical Triangulations Andrzej G¨orlich Niels Bohr Institute, University of Copenhagen Naxos, September 12th, 2011 Andrzej G¨orlich Causal Dynamical Triangulation Outline 1 Path integral for quantum gravity 2 Causal Dynamical Triangulations 3 Numerical setup 4 Phase diagram 5 Background geometry 6 Quantum fluctuations Andrzej G¨orlich Causal Dynamical Triangulation Path integral formulation of quantum mechanics A classical particle follows a unique trajectory. Quantum mechanics can be described by Path Integrals: All possible trajectories contribute to the transition amplitude. To define the functional integral, we discretize the time coordinate and approximate each path by linear pieces. space classical trajectory t1 time t2 Andrzej G¨orlich Causal Dynamical Triangulation Path integral formulation of quantum mechanics A classical particle follows a unique trajectory. Quantum mechanics can be described by Path Integrals: All possible trajectories contribute to the transition amplitude. To define the functional integral, we discretize the time coordinate and approximate each path by linear pieces. quantum trajectory space classical trajectory t1 time t2 Andrzej G¨orlich Causal Dynamical Triangulation Path integral formulation of quantum mechanics A classical particle follows a unique trajectory. Quantum mechanics can be described by Path Integrals: All possible trajectories contribute to the transition amplitude. To define the functional integral, we discretize the time coordinate and approximate each path by linear pieces. quantum trajectory space classical trajectory t1 time t2 Andrzej G¨orlich Causal Dynamical Triangulation Path integral formulation of quantum gravity General Relativity: gravity is encoded in space-time geometry. The role of a trajectory plays now the geometry of four-dimensional space-time. All space-time histories contribute to the transition amplitude. -
Causality and Determinism: Tension, Or Outright Conflict?
1 Causality and Determinism: Tension, or Outright Conflict? Carl Hoefer ICREA and Universidad Autònoma de Barcelona Draft October 2004 Abstract: In the philosophical tradition, the notions of determinism and causality are strongly linked: it is assumed that in a world of deterministic laws, causality may be said to reign supreme; and in any world where the causality is strong enough, determinism must hold. I will show that these alleged linkages are based on mistakes, and in fact get things almost completely wrong. In a deterministic world that is anything like ours, there is no room for genuine causation. Though there may be stable enough macro-level regularities to serve the purposes of human agents, the sense of “causality” that can be maintained is one that will at best satisfy Humeans and pragmatists, not causal fundamentalists. Introduction. There has been a strong tendency in the philosophical literature to conflate determinism and causality, or at the very least, to see the former as a particularly strong form of the latter. The tendency persists even today. When the editors of the Stanford Encyclopedia of Philosophy asked me to write the entry on determinism, I found that the title was to be “Causal determinism”.1 I therefore felt obliged to point out in the opening paragraph that determinism actually has little or nothing to do with causation; for the philosophical tradition has it all wrong. What I hope to show in this paper is that, in fact, in a complex world such as the one we inhabit, determinism and genuine causality are probably incompatible with each other. -
Existentialism Principles As Seen in the Character of Satoru Nakata in Haruki Murakami’S Kafka on the Shore
PLAGIAT MERUPAKAN TINDAKAN TIDAK TERPUJI EXISTENTIALISM PRINCIPLES AS SEEN IN THE CHARACTER OF SATORU NAKATA IN HARUKI MURAKAMI’S KAFKA ON THE SHORE AN UNDERGRADUATE THESIS Presented as Partial Fulfillment of the Requirements for the degree of Sarjana Sastra in English Letters By Bayu Kusuma Student Number: 144214095 DEPARTMENT OF ENGLISH LETTERS FACULTY OF LETTERS UNIVERSITAS SANATA DHARMA YOGYAKARTA 2018 PLAGIAT MERUPAKAN TINDAKAN TIDAK TERPUJI EXISTENTIALISM PRINCIPLES AS SEEN IN THE CHARACTER OF SATORU NAKATA IN HARUKI MURAKAMI’S KAFKA ON THE SHORE AN UNDERGRADUATE THESIS Presented as Partial Fulfillment of the Requirements for the degree of Sarjana Sastra in English Letters By Bayu Kusuma Student Number: 144214095 DEPARTMENT OF ENGLISH LETTERS FACULTY OF LETTERS UNIVERSITAS SANATA DHARMA YOGYAKARTA 2018 ii PLAGIAT MERUPAKAN TINDAKAN TIDAK TERPUJI iii PLAGIAT MERUPAKAN TINDAKAN TIDAK TERPUJI iv PLAGIAT MERUPAKAN TINDAKAN TIDAK TERPUJI STATEMENT OF ORIGINALITY I certify that this undergraduate thesis contains no material which has been previously submitted for the award of any other degree at any university, and that, to the best of my knowledge, this undergraduate thesis contains no material previously written by any other person except where due reference is made in the text of the undergraduate thesis Yogyakarta, December 5, 2018 Bayu Kusuma v PLAGIAT MERUPAKAN TINDAKAN TIDAK TERPUJI LEMBAR PERNYATAAN PERSETUJUAN PUBLIKASI KARYA ILMIAH UNTUK KEPENTINGAN AKADEMIS Yang bertanda tangan di bawah ini, saya mahasiswa Universitas Sanata -
Causality in Quantum Field Theory with Classical Sources
Causality in Quantum Field Theory with Classical Sources Bo-Sture K. Skagerstam1;a), Karl-Erik Eriksson2;b), Per K. Rekdal3;c) a)Department of Physics, NTNU, Norwegian University of Science and Technology, N-7491 Trondheim, Norway b) Department of Space, Earth and Environment, Chalmers University of Technology, SE-412 96 G¨oteborg, Sweden c)Molde University College, P.O. Box 2110, N-6402 Molde, Norway Abstract In an exact quantum-mechanical framework we show that space-time expectation values of the second-quantized electromagnetic fields in the Coulomb gauge, in the presence of a classical source, automatically lead to causal and properly retarded elec- tromagnetic field strengths. The classical ~-independent and gauge invariant Maxwell's equations then naturally emerge and are therefore also consistent with the classical spe- cial theory of relativity. The fundamental difference between interference phenomena due to the linear nature of the classical Maxwell theory as considered in, e.g., classical optics, and interference effects of quantum states is clarified. In addition to these is- sues, the framework outlined also provides for a simple approach to invariance under time-reversal, some spontaneous photon emission and/or absorption processes as well as an approach to Vavilov-Cherenkovˇ radiation. The inherent and necessary quan- tum uncertainty, limiting a precise space-time knowledge of expectation values of the quantum fields considered, is, finally, recalled. arXiv:1801.09947v2 [quant-ph] 30 Mar 2019 1Corresponding author. Email address: [email protected] 2Email address: [email protected] 3Email address: [email protected] 1. Introduction The roles of causality and retardation in classical and quantum-mechanical versions of electrodynamics are issues that one encounters in various contexts (for recent discussions see, e.g., Refs.[1]-[14]). -
Time and Causality in General Relativity
Time and Causality in General Relativity Ettore Minguzzi Universit`aDegli Studi Di Firenze FQXi International Conference. Ponta Delgada, July 10, 2009 FQXi Conference 2009, Ponta Delgada Time and Causality in General Relativity 1/8 Light cone A tangent vector v 2 TM is timelike, lightlike, causal or spacelike if g(v; v) <; =; ≤; > 0 respectively. Time orientation and spacetime At every point there are two cones of timelike vectors. The Lorentzian manifold is time orientable if a continuous choice of one of the cones, termed future, can be made. If such a choice has been made the Lorentzian manifold is time oriented and is also called spacetime. Lorentzian manifolds and light cones Lorentzian manifolds A Lorentzian manifold is a Hausdorff manifold M, of dimension n ≥ 2, endowed with a Lorentzian metric, that is a section g of T ∗M ⊗ T ∗M with signature (−; +;:::; +). FQXi Conference 2009, Ponta Delgada Time and Causality in General Relativity 2/8 Time orientation and spacetime At every point there are two cones of timelike vectors. The Lorentzian manifold is time orientable if a continuous choice of one of the cones, termed future, can be made. If such a choice has been made the Lorentzian manifold is time oriented and is also called spacetime. Lorentzian manifolds and light cones Lorentzian manifolds A Lorentzian manifold is a Hausdorff manifold M, of dimension n ≥ 2, endowed with a Lorentzian metric, that is a section g of T ∗M ⊗ T ∗M with signature (−; +;:::; +). Light cone A tangent vector v 2 TM is timelike, lightlike, causal or spacelike if g(v; v) <; =; ≤; > 0 respectively. -
Studies on Causal Explanation in Naturalistic Philosophy of Mind
tn tn+1 s s* r1 r2 r1* r2* Interactions and Exclusions: Studies on Causal Explanation in Naturalistic Philosophy of Mind Tuomas K. Pernu Department of Biosciences Faculty of Biological and Environmental Sciences & Department of Philosophy, History, Culture and Art Studies Faculty of Arts ACADEMIC DISSERTATION To be publicly discussed, by due permission of the Faculty of Arts at the University of Helsinki, in lecture room 5 of the University of Helsinki Main Building, on the 30th of November, 2013, at 12 o’clock noon. © 2013 Tuomas Pernu (cover figure and introductory essay) © 2008 Springer Science+Business Media (article I) © 2011 Walter de Gruyter (article II) © 2013 Springer Science+Business Media (article III) © 2013 Taylor & Francis (article IV) © 2013 Open Society Foundation (article V) Layout and technical assistance by Aleksi Salokannel | SI SIN Cover layout by Anita Tienhaara Author’s address: Department of Biosciences Division of Physiology and Neuroscience P.O. Box 65 FI-00014 UNIVERSITY OF HELSINKI e-mail [email protected] ISBN 978-952-10-9439-2 (paperback) ISBN 978-952-10-9440-8 (PDF) ISSN 1799-7372 Nord Print Helsinki 2013 If it isn’t literally true that my wanting is causally responsible for my reaching, and my itching is causally responsible for my scratching, and my believing is causally responsible for my saying … , if none of that is literally true, then practically everything I believe about anything is false and it’s the end of the world. Jerry Fodor “Making mind matter more” (1989) Supervised by Docent Markus -
Truth and Transcendence Turning the Tables on the Liar Paradox
11 Truth and Transcendence Turning the Tables on the Liar Paradox GILA SHER 11.1. AMethodological Turnaround Confrontingthe liar paradox is commonly viewed as a prerequisite for developing a theory of truth. As soon as the truth theorist accepts one of the most minimal principles of truth, the equivalence principle, which in one of its forms is often formulated(schematically) by (E) <P> is true iff(if and only if) P, where "P" stands for any sentence and" <P>" stands for a name of that sentence, the liar paradox arises. And it is only after the truth theorist incorporates some device Oike a Tarskian hierarchy or a K.ripkeangrounding process) forblocking the paradox that he is entitled to continue developing his theory. In this chapter I would like to turn the tables on this traditional conception of the relation between the liar paradox and the theory of truth. I would like to show that the theorist of truth need not worry about the liar paradox in developing her theory, that if she focuses deeply enough on the "material" adequacy of her theory (i.e., whether it adequately accounts for the nature of truth) as distinct from its "formal" adequacy (i.e., whether it is a consistent theory), the liar challenge is unlikely to arise for her theory at all. 1 In approaching the liar challenge in this way, we are treating the theory of truth like most other theories. Consider a physical, psychological, geometrical, or moral theory. Normally, the theorist in any of these fields is aware that his theory must sati�fy certain norms of formal adequacy. -
Causation As Folk Science
1. Introduction Each of the individual sciences seeks to comprehend the processes of the natural world in some narrow do- main—chemistry, the chemical processes; biology, living processes; and so on. It is widely held, however, that all the sciences are unified at a deeper level in that natural processes are governed, at least in significant measure, by cause and effect. Their presence is routinely asserted in a law of causa- tion or principle of causality—roughly, that every effect is produced through lawful necessity by a cause—and our ac- counts of the natural world are expected to conform to it.1 My purpose in this paper is to take issue with this view of causation as the underlying principle of all natural processes. Causation I have a negative and a positive thesis. In the negative thesis I urge that the concepts of cause as Folk Science and effect are not the fundamental concepts of our science and that science is not governed by a law or principle of cau- sality. This is not to say that causal talk is meaningless or useless—far from it. Such talk remains a most helpful way of conceiving the world, and I will shortly try to explain how John D. Norton that is possible. What I do deny is that the task of science is to find the particular expressions of some fundamental causal principle in the domain of each of the sciences. My argument will be that centuries of failed attempts to formu- late a principle of causality, robustly true under the introduc- 1Some versions are: Kant (1933, p.218) "All alterations take place in con- formity with the law of the connection of cause and effect"; "Everything that happens, that is, begins to be, presupposes something upon which it follows ac- cording to a rule." Mill (1872, Bk. -
Causality in the Quantum World
VIEWPOINT Causality in the Quantum World A new model extends the definition of causality to quantum-mechanical systems. by Jacques Pienaar∗ athematical models for deducing cause-effect relationships from statistical data have been successful in diverse areas of science (see Ref. [1] and references therein). Such models can Mbe applied, for instance, to establish causal relationships between smoking and cancer or to analyze risks in con- struction projects. Can similar models be extended to the microscopic world governed by the laws of quantum me- chanics? Answering this question could lead to advances in quantum information and to a better understanding of the foundations of quantum mechanics. Developing quantum Figure 1: In statistics, causal models can be used to extract extensions of causal models, however, has proven challeng- cause-effect relationships from empirical data on a complex ing because of the peculiar features of quantum mechanics. system. Existing models, however, do not apply if at least one For instance, if two or more quantum systems are entangled, component of the system (Y) is quantum. Allen et al. have now it is hard to deduce whether statistical correlations between proposed a quantum extension of causal models. (APS/Alan them imply a cause-effect relationship. John-Mark Allen at Stonebraker) the University of Oxford, UK, and colleagues have now pro- posed a quantum causal model based on a generalization of an old principle known as Reichenbach’s common cause is a third variable that is a common cause of both. In the principle [2]. latter case, the correlation will disappear if probabilities are Historically, statisticians thought that all information conditioned to the common cause. -
Stanford Encyclopedia of Philosophy) Stanford Encyclopedia of Philosophy Arthur Schopenhauer
03/05/2017 Arthur Schopenhauer (Stanford Encyclopedia of Philosophy) Stanford Encyclopedia of Philosophy Arthur Schopenhauer First published Mon May 12, 2003; substantive revision Sat Nov 19, 2011 Among 19th century philosophers, Arthur Schopenhauer was among the first to contend that at its core, the universe is not a rational place. Inspired by Plato and Kant, both of whom regarded the world as being more amenable to reason, Schopenhauer developed their philosophies into an instinctrecognizing and ultimately ascetic outlook, emphasizing that in the face of a world filled with endless strife, we ought to minimize our natural desires for the sake of achieving a more tranquil frame of mind and a disposition towards universal beneficence. Often considered to be a thoroughgoing pessimist, Schopenhauer in fact advocated ways — via artistic, moral and ascetic forms of awareness — to overcome a frustrationfilled and fundamentally painful human condition. Since his death in 1860, his philosophy has had a special attraction for those who wonder about life's meaning, along with those engaged in music, literature, and the visual arts. 1. Life: 1788–1860 2. The Fourfold Root of the Principle of Sufficient Reason 3. Schopenhauer's Critique of Kant 4. The World as Will 5. Transcending the Human Conditions of Conflict 5.1 Aesthetic Perception as a Mode of Transcendence 5.2 Moral Awareness as a Mode of Transcendence 5.3 Asceticism and the Denial of the WilltoLive 6. Schopenhauer's Later Works 7. Critical Reflections 8. Schopenhauer's Influence Bibliography Academic Tools Other Internet Resources Related Entries 1. Life: 1788–1860 Exactly a month younger than the English Romantic poet, Lord Byron (1788–1824), who was born on January 22, 1788, Arthur Schopenhauer came into the world on February 22, 1788 in Danzig [Gdansk, Poland] — a city that had a long history in international trade as a member of the Hanseatic League. -
The Passive Personality Principle
The Catholic University of America, Columbus School of Law CUA Law Scholarship Repository Scholarly Articles and Other Contributions Faculty Scholarship 1993 The Passive Personality Principle Geoffrey R. Watson The Catholic University of America, Columbus School of Law Follow this and additional works at: https://scholarship.law.edu/scholar Part of the Constitutional Law Commons, and the International Law Commons Recommended Citation Geoffrey R. Watson, The Passive Personality Principle, 28 TEX. INT’L L. J. 1 (1993). This Article is brought to you for free and open access by the Faculty Scholarship at CUA Law Scholarship Repository. It has been accepted for inclusion in Scholarly Articles and Other Contributions by an authorized administrator of CUA Law Scholarship Repository. For more information, please contact [email protected]. ARTICLES The Passive Personality Principle GEOFFREY R. WATSONt SUMMARY I. INTRODUCTION ..................................... 2 Ii. THE EVOLUTION OF PASSIVE PERSONALITY JURISDICTION IN UNITED STATES PRACTICE ............................ 4 III. PASSIVE PERSONALITY JURISDICTION IN INTERNATIONAL LAW . 14 A. Intrusion on Sovereignty .......................... 15 B. Fairness to the Defendant ......................... 22 C. Evidentiary and Logistical Objections to Passive Personality Jurisdiction ................................... 25 IV. PASSIVE PERSONALITY JURISDICTION IN UNITED STATES LAW... 30 A. Passive PersonalityJurisdiction and the Constitution ...... 30 B. Implementation of Passive PersonalityJurisdiction ........ 34 V. RETHINKING THE JURISPRUDENCE OF JURISDICTION: A SYSTEMIC APPROACH ....................................... 38 VI. CONCLUSION ..................................... 45 t Assistant Professor of Law, University of Puget Sound School of Law, B.A., Yale University, 1982; J.D., Harvard Law School, 1986; Attorney-Adviser, Office of the Legal Adviser, U.S. Dept. of State, 1987-91. TEXAS INTERNATIONAL LAW JOURNAL [Vol. 28:1 I. INTRODUCTION The relationship between state and citizen is a central problem of international law. -
Moritz Schlick and Bas Van Fraassen: Two Different Perspectives on Causality and Quantum Mechanics Richard Dawid1
Moritz Schlick and Bas van Fraassen: Two Different Perspectives on Causality and Quantum Mechanics Richard Dawid1 Moritz Schlick’s interpretation of the causality principle is based on Schlick’s understanding of quantum mechanics and on his conviction that quantum mechanics strongly supports an empiricist reading of causation in his sense. The present paper compares the empiricist position held by Schlick with Bas van Fraassen’s more recent conception of constructive empiricism. It is pointed out that the development from Schlick’s understanding of logical empiricism to constructive empiricism reflects a difference between the understanding of quantum mechanics endorsed by Schlick and the understanding that had been established at the time of van Fraassen’s writing. 1: Introduction Moritz Schlick’s ideas about causality and quantum mechanics dealt with a topic that was at the forefront of research in physics and philosophy of science at the time. In the present article, I want to discuss the plausibility of Schlick’s ideas within the scientific context of the time and compare it with a view based on a modern understanding of quantum mechanics. Schlick had already written about his understanding of causation in [Schlick 1920] before he set out to develop a new account of causation in “Die Kausalität in der gegenwärtigen Physik” [Schlick 1931]. The very substantial differences between the concepts of causality developed in the two papers are due to important philosophical as well as physical developments. Philosophically, [Schlick 1931] accounts for Schlick’s shift from his earlier position of critical realism towards his endorsement of core tenets of logical empiricism.