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Lectures on Quantum Field Theory
QUANTUM FIELD THEORY Notes taken from a course of R. E. Borcherds, Fall 2001, Berkeley Richard E. Borcherds, Mathematics department, Evans Hall, UC Berkeley, CA 94720, U.S.A. e–mail: [email protected] home page: www.math.berkeley.edu/~reb Alex Barnard, Mathematics department, Evans Hall, UC Berkeley, CA 94720, U.S.A. e–mail: [email protected] home page: www.math.berkeley.edu/~barnard Contents 1 Introduction 4 1.1 Life Cycle of a Theoretical Physicist . ....... 4 1.2 Historical Survey of the Standard Model . ....... 5 1.3 SomeProblemswithNeutrinos . ... 9 1.4 Elementary Particles in the Standard Model . ........ 10 2 Lagrangians 11 arXiv:math-ph/0204014v1 8 Apr 2002 2.1 WhatisaLagrangian?.............................. 11 2.2 Examples ...................................... 11 2.3 The General Euler–Lagrange Equation . ...... 13 3 Symmetries and Currents 14 3.1 ObviousSymmetries ............................... 14 3.2 Not–So–ObviousSymmetries . 16 3.3 TheElectromagneticField. 17 1 3.4 Converting Classical Field Theory to Homological Algebra........... 19 4 Feynman Path Integrals 21 4.1 Finite Dimensional Integrals . ...... 21 4.2 TheFreeFieldCase ................................ 22 4.3 Free Field Green’s Functions . 23 4.4 TheNon-FreeCase................................. 24 5 0-Dimensional QFT 25 5.1 BorelSummation.................................. 28 5.2 OtherGraphSums................................. 28 5.3 TheClassicalField............................... 29 5.4 TheEffectiveAction ............................... 31 6 Distributions and Propagators 35 6.1 EuclideanPropagators . 36 6.2 LorentzianPropagators . 38 6.3 Wavefronts and Distribution Products . ....... 40 7 Higher Dimensional QFT 44 7.1 AnExample..................................... 44 7.2 Renormalisation Prescriptions . ....... 45 7.3 FiniteRenormalisations . 47 7.4 A Group Structure on Finite Renormalisations . ........ 50 7.5 More Conditions on Renormalisation Prescriptions . -
Predeterminism and Moral Agency in the Hodayot
Predeterminism and Moral Agency in the Hodayot Carol A. Newsom 1 Introduction For reasons that are not yet entirely clear, sharp disagreements about pre- determinism and free will became a significant feature of Jewish theological stances in the Hellenistic and Roman periods. Josephus provides the most ex- plicit consideration of these issues in ancient Jewish sources, as he attempts to distinguish the positions of the three major Jewish sects with respect to the philosophical category of “fate” (εἱμαρμένη). Josephus identifies the position of the Essenes as believing strongly in fate, to the apparent exclusion of free will (Ant. 13.172). Similarly, modern scholarly treatments of the Qumran yaḥad have acknowledged the very strong predeterminist element in their thinking, attested in a variety of sectarian or closely related texts.1 At the same time, there has been a degree of perplexity as to what to do with the obviously volun- tarist statements and assumptions that are present in these same documents. A variety of suggestions have been made, mostly to the effect that the sectar- ians were inconsistent or not fully systematic in their beliefs.2 This may in- deed be the case, though Jonathan Klawans argues that, properly understood, all deterministic systems are consistent with voluntarism in a rather minimal 1 I take the Qumran yaḥad movement to be Essene, though I consider it possible that the term “Essene” may also have referred to groups not formally part of the yaḥad. For examinations of the phenomenon of predestination in Qumran sectarian literature and closely related texts, see J. Licht, “The Concept of Free Will in the Writings of the Sect of the Judean Desert,” in Studies in the Dead Sea Scrolls: Lectures Delivered at the Third Annual Conference (1957) in Memory of E. -
Edward Close Response IQNJ Nccuse V5.2 ED 181201
One Response to “An Evaluation of TDVP” With Explanations of Fundamental Concepts Edward R. Close, PhD, PE, DF (ECA), DSPE) and With Vernon M Neppe, MD, PhD, Fellow Royal Society (SA), DPCP (ECA), DSPE a b ABSTRACT Dr. Vernon M. Neppe and I first published an innovative, consciousness-based paradigm in a volume entitled Reality Begins with Consciousness in 2012.1 It was the combination of many years of independent research by us, carried out before we met, and then initially about 3 years of direct collaboration, that has now stretched beyond a decade. Hailed by some peer reviewers as the next major paradigm shift, the Triadic Dimensional Vortical Paradigm (TDVP) has been further developed and expanded over the past seven years in a number of papers and articles published outside of mainstream scientific journals because of the unspoken taboo against including consciousness in mathematical physics. This article is a response to criticisms leveled in the article, “An Evaluation of TDVP,” published in Telicom XXX, no. 5 (Oct-Dec 2018), by physicists J. E. F. Kaan and Simon Olling Rebsdorf.2 This article, along with Dr. Neppe’s rejoinder (which immediately follows this article), underlines the difficulty that mainstream scientists have had in understanding the basics and implications of TDVP. In addition to replying to the criticisms in Kaan and Rebsdorf’s article, this article contains explanations of some of the basic ideas that make TDVP a controversial shift from materialistic physicalism to a comprehensive consciousness-based scientific paradigm. 1.0 INTRODUCTION a Dr. Close PhD, DPCP (ECAO), DSPE is a Physicist, Mathematician, Cosmologist, Environmental Engineer and Dimensional Biopsychophysicist. -
Nöroetik Prensipler 5
Türk Dünyası Uygulama ve Araştırma Merkezi Sinir Bilim Dergisi No. 2018/1-2 B ö l ü m Nöroetik Prensipler 5 Etik ilkeler konusunda öneriler Etiksel kavramları daha somut boyuta getirerek prensiplerin ilkeleştirilmesi hedeflenmiştir. öroetik konusunda etiksel anlamda ilkeleşme, tüm insanı ve insanlığı kapsadığı için, tüm etik ilkeleri bünyesinde toplamaktadır. N Nöroetik olarak konunun yeniden gözden geçirilmesi ve ilkeleştirilmesi yukarıdaki kapsam altında gerekli olmadığı anlaşılacaktır. Ancak, olayın özetlenmesi açısından ilkelerde toparlamanın mümkün olabileceği varsayılmaktadır. Her bir yaklaşımda belirli esasların oluşturulması önceliklidir. Bir konu ele alınırken, o konuda bilgi sorgulaması öncesinde, belirli bir planın yapılması gerekir. Planlama olmadan rastgele alınan bilgiler, belirli bir bilgi kirliliğine neden olabilecektir. Birbiri ile çelişen durumlar ve bilgileri çözmek imkansızlaştığı gibi, belirli sorunlara da neden olabilecektir. Bu açıdan nöroetik kavramı üzerinde değinilmeden önce, bu konuda temel yaklaşımlar, belirli bir felsefe içinde ele alınmasını gerekli kılmaktadır. Öncelikle konuyu ele alma biçimi, olayı yrumlama ve algılama düzeyi ortaya konulmalıdır. Bu amaçla nöroetik konusunda bir genel yaklaşım esasları oluşturulmaya çalışılmıştır. Aşağıda bir ilkeleme çalışması görülecektir. Nöroetik Prensipler/İlkeler TANIMLAMALAR Etik Tıp Bilimi temelde insanı birey olarak ele almakta ve onun haklarının öncelikli olduğu ve otonomisinin her türlü durumda korunmasının hukuksal açıdan da ilke olarak ele alınması gerektiğinin bilincindedir. Sayfa. 252 Türk Dünyası Uygulama ve Araştırma Merkezi Sinir Bilim Dergisi No. 2018/1-2 Birey, insan olmanın gerektiği modelinde, ruhsal, sosyal ve kültürel anlamda da toplumsal bir kişiliği olduğunun kavramı olarak da algılanmalıdır. Hekimlik mesleği, bireyin özerkliği ve kendi haklarını belirleme çerçevesinde, tıp biliminin uygulanması yanında sanatsal ve felsefe bilimler anlamında da bir bütünlüğü gerekli kılmaktadır. Tüm diğer özellikler hukuksal esaslar yanında etik ilkeler boyutunda da olmalıdır. -
The Two Bell's Theorems of John Bell
The two Bell's theorems of John Bell Author Wiseman, HM Published 2014 Journal Title Journal of Physics A: Mathematical and Theoretical Version Accepted Manuscript (AM) DOI https://doi.org/10.1088/1751-8113/47/42/424001 Copyright Statement © 2014 Institute of Physics Publishing. This is the author-manuscript version of this paper. Reproduced in accordance with the copyright policy of the publisher.Please refer to the journal's website for access to the definitive, published version. Downloaded from http://hdl.handle.net/10072/65174 Griffith Research Online https://research-repository.griffith.edu.au The Two Bell’s Theorems of John Bell H. M. Wiseman Centre for Quantum Computation and Communication Technology (Australian Research Council), Centre for Quantum Dynamics, Griffith University, Brisbane, Queensland 4111, Australia Abstract. Many of the heated arguments about the meaning of “Bell’s theorem” arise because this phrase can refer to two different theorems that John Bell proved, the first in 1964 and the second in 1976. His 1964 theorem is the incompatibility of quantum phenomena with the dual assumptions of locality and determinism. His 1976 theorem is the incompatibility of quantum phenomena with the unitary property of local causality. This is contrary to Bell’s own later assertions, that his 1964 theorem began with that single, and indivisible, assumption of local causality (even if not by that name). While there are other forms of Bell’s theorems — which I present to explain the relation between Jarrett-completeness, “fragile locality”, and EPR-completeness — I maintain that Bell’s two versions are the essential ones. Although the two Bell’s theorems are logically equivalent, their assumptions are not, and the different versions of the theorem suggest quite different conclusions, which are embraced by different communities. -
Quantum Mechanics Propagator
Quantum Mechanics_propagator This article is about Quantum field theory. For plant propagation, see Plant propagation. In Quantum mechanics and quantum field theory, the propagator gives the probability amplitude for a particle to travel from one place to another in a given time, or to travel with a certain energy and momentum. In Feynman diagrams, which calculate the rate of collisions in quantum field theory, virtual particles contribute their propagator to the rate of the scattering event described by the diagram. They also can be viewed as the inverse of the wave operator appropriate to the particle, and are therefore often called Green's functions. Non-relativistic propagators In non-relativistic quantum mechanics the propagator gives the probability amplitude for a particle to travel from one spatial point at one time to another spatial point at a later time. It is the Green's function (fundamental solution) for the Schrödinger equation. This means that, if a system has Hamiltonian H, then the appropriate propagator is a function satisfying where Hx denotes the Hamiltonian written in terms of the x coordinates, δ(x)denotes the Dirac delta-function, Θ(x) is the Heaviside step function and K(x,t;x',t')is the kernel of the differential operator in question, often referred to as the propagator instead of G in this context, and henceforth in this article. This propagator can also be written as where Û(t,t' ) is the unitary time-evolution operator for the system taking states at time t to states at time t'. The quantum mechanical propagator may also be found by using a path integral, where the boundary conditions of the path integral include q(t)=x, q(t')=x' . -
Quantum Riemannian Geometry of Phase Space and Nonassociativity
Demonstr. Math. 2017; 50: 83–93 Demonstratio Mathematica Open Access Research Article Edwin J. Beggs and Shahn Majid* Quantum Riemannian geometry of phase space and nonassociativity DOI 10.1515/dema-2017-0009 Received August 3, 2016; accepted September 5, 2016. Abstract: Noncommutative or ‘quantum’ differential geometry has emerged in recent years as a process for quantizing not only a classical space into a noncommutative algebra (as familiar in quantum mechanics) but also differential forms, bundles and Riemannian structures at this level. The data for the algebra quantisation is a classical Poisson bracket while the data for quantum differential forms is a Poisson-compatible connection. We give an introduction to our recent result whereby further classical data such as classical bundles, metrics etc. all become quantised in a canonical ‘functorial’ way at least to 1st order in deformation theory. The theory imposes compatibility conditions between the classical Riemannian and Poisson structures as well as new physics such as n typical nonassociativity of the differential structure at 2nd order. We develop in detail the case of CP where the i j commutation relations have the canonical form [w , w¯ ] = iλδij similar to the proposal of Penrose for quantum twistor space. Our work provides a canonical but ultimately nonassociative differential calculus on this algebra and quantises the metric and Levi-Civita connection at lowest order in λ. Keywords: Noncommutative geometry, Quantum gravity, Poisson geometry, Riemannian geometry, Quantum mechanics MSC: 81R50, 58B32, 83C57 In honour of Michał Heller on his 80th birthday. 1 Introduction There are today lots of reasons to think that spacetime itself is better modelled as ‘quantum’ due to Planck-scale corrections. -
Winter 2017/18)
Thorsten Ohl 2018-02-07 14:05:03 +0100 subject to change! i Relativistic Quantum Field Theory (Winter 2017/18) Thorsten Ohl Institut f¨urTheoretische Physik und Astrophysik Universit¨atW¨urzburg D-97070 W¨urzburg Personal Manuscript! Use at your own peril! git commit: c8138b2 Thorsten Ohl 2018-02-07 14:05:03 +0100 subject to change! i Abstract 1. Symmetrien 2. Relativistische Einteilchenzust¨ande 3. Langrangeformalismus f¨urFelder 4. Feldquantisierung 5. Streutheorie und S-Matrix 6. Eichprinzip und Wechselwirkung 7. St¨orungstheorie 8. Feynman-Regeln 9. Quantenelektrodynamische Prozesse in Born-N¨aherung 10. Strahlungskorrekturen (optional) 11. Renormierung (optional) Thorsten Ohl 2018-02-07 14:05:03 +0100 subject to change! i Contents 1 Introduction1 Lecture 01: Tue, 17. 10. 2017 1.1 Limitations of Quantum Mechanics (QM).......... 1 1.2 (Special) Relativistic Quantum Field Theory (QFT)..... 2 1.3 Limitations of QFT...................... 3 2 Symmetries4 2.1 Principles ofQM....................... 4 2.2 Symmetries inQM....................... 6 2.3 Groups............................. 6 Lecture 02: Wed, 18. 10. 2017 2.3.1 Lie Groups....................... 7 2.3.2 Lie Algebras...................... 8 2.3.3 Homomorphisms.................... 8 2.3.4 Representations.................... 9 2.4 Infinitesimal Generators.................... 10 2.4.1 Unitary and Conjugate Representations........ 12 Lecture 03: Tue, 24. 10. 2017 2.5 SO(3) and SU(2) ........................ 13 2.5.1 O(3) and SO(3) .................... 13 2.5.2 SU(2) .......................... 15 2.5.3 SU(2) ! SO(3) .................... 16 2.5.4 SO(3) and SU(2) Representations........... 17 Lecture 04: Wed, 25. 10. 2017 2.6 Lorentz- and Poincar´e-Group................ -
Free Will: Hail and Farewell
Essays in the Philosophy of Humanism © 2019 The American Humanist Association volume 27 (2019), article 6, 98-124. ISSN 1522-7340 (print), 2052-8388 (online) Free Will: Hail and Farewell James A. Montanye Independent scholar, Falls Church, VA [email protected] This essay traces the evolution of the free will concept, from Plato to the present. It examines interpretations offered by theologians, political philosophers, philosophers of mind and consciousness, neuroscientists, evolutionists, legal scholars, and economists. The essay illuminates the concept’s instrumental use as an artifice for manipulating behavioral adaptations to the scarcity of economic resources. Macroeconomic and ngram data reveal these manipulations as having locked Western civilization into centuries of social and economic stagnation. Keywords: free will, consciousness, economics, prosperity, scarcity, competition, neuroscience, compatibilism, incompatibilism, ngrams “The persistence of the traditional free will problem in philosophy seems to me something of a scandal. After all these centuries of writing about free will, it does not seem to me that we have made very much progress.” John Searle (2007, 37) “A flood of ink has been spilled, especially in the modern era, on how to understand the concept of being able to do otherwise.” Timothy O’Connor (2016) “...the whole arcane issue about free will is a miscast concept, based on social and psychological beliefs held at particular times in human history that have not been borne out and/or are at odds with modern scientific knowledge about the nature of our universe.” Michael Gazzaniga (2011, 219) “...if we no longer entertain the luxury of a belief in the ‘magic of the soul,’ then there is little else to offer in support of the concept of free will.” Anthony Cashmore (2010, 1) [98] 1. -
INFORMATION– CONSCIOUSNESS– REALITY How a New Understanding of the Universe Can Help Answer Age-Old Questions of Existence the FRONTIERS COLLECTION
THE FRONTIERS COLLECTION James B. Glattfelder INFORMATION– CONSCIOUSNESS– REALITY How a New Understanding of the Universe Can Help Answer Age-Old Questions of Existence THE FRONTIERS COLLECTION Series editors Avshalom C. Elitzur, Iyar, Israel Institute of Advanced Research, Rehovot, Israel Zeeya Merali, Foundational Questions Institute, Decatur, GA, USA Thanu Padmanabhan, Inter-University Centre for Astronomy and Astrophysics (IUCAA), Pune, India Maximilian Schlosshauer, Department of Physics, University of Portland, Portland, OR, USA Mark P. Silverman, Department of Physics, Trinity College, Hartford, CT, USA Jack A. Tuszynski, Department of Physics, University of Alberta, Edmonton, AB, Canada Rüdiger Vaas, Redaktion Astronomie, Physik, bild der wissenschaft, Leinfelden-Echterdingen, Germany THE FRONTIERS COLLECTION The books in this collection are devoted to challenging and open problems at the forefront of modern science and scholarship, including related philosophical debates. In contrast to typical research monographs, however, they strive to present their topics in a manner accessible also to scientifically literate non-specialists wishing to gain insight into the deeper implications and fascinating questions involved. Taken as a whole, the series reflects the need for a fundamental and interdisciplinary approach to modern science and research. Furthermore, it is intended to encourage active academics in all fields to ponder over important and perhaps controversial issues beyond their own speciality. Extending from quantum physics and relativity to entropy, conscious- ness, language and complex systems—the Frontiers Collection will inspire readers to push back the frontiers of their own knowledge. More information about this series at http://www.springer.com/series/5342 For a full list of published titles, please see back of book or springer.com/series/5342 James B. -
Quarks and Gluons in the Phase Diagram of Quantum Chromodynamics
Dissertation Quarks and Gluons in the Phase Diagram of Quantum Chromodynamics Christian Andreas Welzbacher July 2016 Justus-Liebig-Universitat¨ Giessen Fachbereich 07 Institut fur¨ theoretische Physik Dekan: Prof. Dr. Bernhard M¨uhlherr Erstgutachter: Prof. Dr. Christian S. Fischer Zweitgutachter: Prof. Dr. Lorenz von Smekal Vorsitzende der Pr¨ufungskommission: Prof. Dr. Claudia H¨ohne Tag der Einreichung: 13.05.2016 Tag der m¨undlichen Pr¨ufung: 14.07.2016 So much universe, and so little time. (Sir Terry Pratchett) Quarks und Gluonen im Phasendiagramm der Quantenchromodynamik Zusammenfassung In der vorliegenden Dissertation wird das Phasendiagramm von stark wechselwirk- ender Materie untersucht. Dazu wird im Rahmen der Quantenchromodynamik der Quarkpropagator ¨uber seine quantenfeldtheoretischen Bewegungsgleichungen bes- timmt. Diese sind bekannt als Dyson-Schwinger Gleichungen und konstituieren einen funktionalen Zugang, welcher mithilfe des Matsubara-Formalismus bei endlicher Tem- peratur und endlichem chemischen Potential angewendet wird. Theoretische Hin- tergr¨undeder Quantenchromodynamik werden erl¨autert,wobei insbesondere auf die Dyson-Schwinger Gleichungen eingegangen wird. Chirale Symmetrie sowie Confine- ment und zugeh¨origeOrdnungsparameter werden diskutiert, welche eine Unterteilung des Phasendiagrammes in verschiedene Phasen erm¨oglichen. Zudem wird der soge- nannte Columbia Plot erl¨autert,der die Abh¨angigkeit verschiedener Phasen¨uberg¨ange von der Quarkmasse skizziert. Zun¨achst werden Ergebnisse f¨urein System mit zwei entarteten leichten Quarks und einem Strange-Quark mit vorangegangenen Untersuchungen verglichen. Eine Trunkierung, welche notwendig ist um das System aus unendlich vielen gekoppelten Gleichungen auf eine endliche Anzahl an Gleichungen zu reduzieren, wird eingef¨uhrt. Die Ergebnisse f¨urdie Propagatoren und das Phasendiagramm stimmen gut mit vorherigen Arbeiten ¨uberein. Einige zus¨atzliche Ergebnisse werden pr¨asentiert, wobei insbesondere auf die Abh¨angigkeit des Phasendiagrammes von der Quarkmasse einge- gangen wird. -
Classical/Quantum Dynamics in a Uniform Gravitational Field: A
Classical/Quantum Dynamics in a Uniform Gravitational Field: A. Unobstructed Free Fall Nicholas Wheeler, Reed College Physics Department August 2002 Introduction. Every student of mechanics encounters discussion of the idealized one-dimensional dynamical systems 0:free particle F (x)=mx¨ with F (x)= −mg : particle in free fall −kx : harmonic oscillator at a very early point in his/her education, and with the first & last of those systems we are never done: they are—for reasons having little to do with their physical importance—workhorses of theoretical mechanics, traditionally employed to illustrated formal developments as they emerge, one after another. But—unaccountably—the motion of particles in uniform gravitational fields1 is seldom treated by methods more advanced than those accessible to beginning students. It is true that terrestrial gravitational forces are so relatively weak that they can—or could until recently—usually be dismissed as irrelevant to the phenomenology studied by physicists in their laboratories.2 But the free fall 1 It is to avoid that cumbersome phrase that I adopt the “free fall” locution, though technically free fall presumes neither uniformity nor constancy of the ambient gravitational field. If understood in the latter sense, “free fall” lies near the motivating heart of general relativity, which is certainly not a neglected subject. 2 There are exceptions: I am thinking of experiments done several decades ago where neutron diffraction in crystals was found to be sensitive to the value of g. And of experiments designed to determine whether antiparticles “fall up” (they don’t). 2 Classical/quantum motion in a uniform gravitational field: free fall problem—especially if construed quantum mechanically, with an eye to the relation between the quantum physics and classical physics—is itself a kind of laboratory, one in which striking clarity can be brought to a remarkable variety of formal issues.