Modelling Systems with Intentional Dynamics: a Lesson from Quantum Mechanics
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31 Diffraction and Interference.Pdf
Diffraction and Interference Figu These expar new .5 wave oday Isaac Newton is most famous for his new v accomplishments in mechanics—his laws of Tmotion and universal gravitation. Early in his career, however, he was most famous for his work on light. Newton pictured light as a beam of ultra-tiny material particles. With this model he could explain reflection as a bouncing of the parti- cles from a surface, and he could explain refraction as the result of deflecting forces from the surface Interference colors. acting on the light particles. In the eighteenth and nineteenth cen- turies, this particle model gave way to a wave model of light because waves could explain not only reflection and refraction, but everything else that was known about light at that time. In this chapter we will investigate the wave aspects of light, which are needed to explain two important phenomena—diffraction and interference. As Huygens' Principle origin; 31.1 pie is I constr In the late 1600s a Dutch mathematician-scientist, Christian Huygens, dimen proposed a very interesting idea about waves. Huygens stated that light waves spreading out from a point source may be regarded as die overlapping of tiny secondary wavelets, and that every point on ' any wave front may be regarded as a new point source of secondary waves. We see this in Figure 31.1. In other words, wave fronts are A made up of tinier wave fronts. This idea is called Huygens' principle. Look at the spherical wave front in Figure 31.2. Each point along the wave front AN is the source of a new wavelet that spreads out in a sphere from that point. -
Degruyter Opphil Opphil-2020-0010 147..160 ++
Open Philosophy 2020; 3: 147–160 Object Oriented Ontology and Its Critics Simon Weir* Living and Nonliving Occasionalism https://doi.org/10.1515/opphil-2020-0010 received November 05, 2019; accepted February 14, 2020 Abstract: Graham Harman’s Object-Oriented Ontology has employed a variant of occasionalist causation since 2002, with sensual objects acting as the mediators of causation between real objects. While the mechanism for living beings creating sensual objects is clear, how nonliving objects generate sensual objects is not. This essay sets out an interpretation of occasionalism where the mediating agency of nonliving contact is the virtual particles of nominally empty space. Since living, conscious, real objects need to hold sensual objects as sub-components, but nonliving objects do not, this leads to an explanation of why consciousness, in Object-Oriented Ontology, might be described as doubly withdrawn: a sensual sub-component of a withdrawn real object. Keywords: Graham Harman, ontology, objects, Timothy Morton, vicarious, screening, virtual particle, consciousness 1 Introduction When approaching Graham Harman’s fourfold ontology, it is relatively easy to understand the first steps if you begin from an anthropocentric position of naive realism: there are real objects that have their real qualities. Then apart from real objects are the objects of our perception, which Harman calls sensual objects, which are reduced distortions or caricatures of the real objects we perceive; and these sensual objects have their own sensual qualities. It is common sense that when we perceive a steaming espresso, for example, that we, as the perceivers, create the image of that espresso in our minds – this image being what Harman calls a sensual object – and that we supply the energy to produce this sensual object. -
Prelab 5 – Wave Interference
Musical Acoustics Lab, C. Bertulani PreLab 5 – Wave Interference Consider two waves that are in phase, sharing the same frequency and with amplitudes A1 and A2. Their troughs and peaks line up and the resultant wave will have amplitude A = A1 + A2. This is known as constructive interference (figure on the left). If the two waves are π radians, or 180°, out of phase, then one wave's crests will coincide with another waves' troughs and so will tend to cancel itself out. The resultant amplitude is A = |A1 − A2|. If A1 = A2, the resultant amplitude will be zero. This is known as destructive interference (figure on the right). When two sinusoidal waves superimpose, the resulting waveform depends on the frequency (or wavelength) amplitude and relative phase of the two waves. If the two waves have the same amplitude A and wavelength the resultant waveform will have an amplitude between 0 and 2A depending on whether the two waves are in phase or out of phase. The principle of superposition of waves states that the resultant displacement at a point is equal to the vector sum of the displacements of different waves at that point. If a crest of a wave meets a crest of another wave at the same point then the crests interfere constructively and the resultant crest wave amplitude is increased; similarly two troughs make a trough of increased amplitude. If a crest of a wave meets a trough of another wave then they interfere destructively, and the overall amplitude is decreased. This form of interference can occur whenever a wave can propagate from a source to a destination by two or more paths of different lengths. -
A Simple Proof That the Many-Worlds Interpretation of Quantum Mechanics Is Inconsistent
A simple proof that the many-worlds interpretation of quantum mechanics is inconsistent Shan Gao Research Center for Philosophy of Science and Technology, Shanxi University, Taiyuan 030006, P. R. China E-mail: [email protected]. December 25, 2018 Abstract The many-worlds interpretation of quantum mechanics is based on three key assumptions: (1) the completeness of the physical description by means of the wave function, (2) the linearity of the dynamics for the wave function, and (3) multiplicity. In this paper, I argue that the combination of these assumptions may lead to a contradiction. In order to avoid the contradiction, we must drop one of these key assumptions. The many-worlds interpretation of quantum mechanics (MWI) assumes that the wave function of a physical system is a complete description of the system, and the wave function always evolves in accord with the linear Schr¨odingerequation. In order to solve the measurement problem, MWI further assumes that after a measurement with many possible results there appear many equally real worlds, in each of which there is a measuring device which obtains a definite result (Everett, 1957; DeWitt and Graham, 1973; Barrett, 1999; Wallace, 2012; Vaidman, 2014). In this paper, I will argue that MWI may give contradictory predictions for certain unitary time evolution. Consider a simple measurement situation, in which a measuring device M interacts with a measured system S. When the state of S is j0iS, the state of M does not change after the interaction: j0iS jreadyiM ! j0iS jreadyiM : (1) When the state of S is j1iS, the state of M changes and it obtains a mea- surement result: j1iS jreadyiM ! j1iS j1iM : (2) 1 The interaction can be represented by a unitary time evolution operator, U. -
Lecture 9, P 1 Lecture 9: Introduction to QM: Review and Examples
Lecture 9, p 1 Lecture 9: Introduction to QM: Review and Examples S1 S2 Lecture 9, p 2 Photoelectric Effect Binding KE=⋅ eV = hf −Φ energy max stop Φ The work function: 3.5 Φ is the minimum energy needed to strip 3 an electron from the metal. 2.5 2 (v) Φ is defined as positive . 1.5 stop 1 Not all electrons will leave with the maximum V f0 kinetic energy (due to losses). 0.5 0 0 5 10 15 Conclusions: f (x10 14 Hz) • Light arrives in “packets” of energy (photons ). • Ephoton = hf • Increasing the intensity increases # photons, not the photon energy. Each photon ejects (at most) one electron from the metal. Recall: For EM waves, frequency and wavelength are related by f = c/ λ. Therefore: Ephoton = hc/ λ = 1240 eV-nm/ λ Lecture 9, p 3 Photoelectric Effect Example 1. When light of wavelength λ = 400 nm shines on lithium, the stopping voltage of the electrons is Vstop = 0.21 V . What is the work function of lithium? Lecture 9, p 4 Photoelectric Effect: Solution 1. When light of wavelength λ = 400 nm shines on lithium, the stopping voltage of the electrons is Vstop = 0.21 V . What is the work function of lithium? Φ = hf - eV stop Instead of hf, use hc/ λ: 1240/400 = 3.1 eV = 3.1eV - 0.21eV For Vstop = 0.21 V, eV stop = 0.21 eV = 2.89 eV Lecture 9, p 5 Act 1 3 1. If the workfunction of the material increased, (v) 2 how would the graph change? stop a. -
Waves: Interference Instructions: Read Through the Information Below
Pre-AP Physics Week 2: Day 1 Notes Waves: Interference Instructions: Read through the information below. Then answer the questions below. When two or more waves meet, they interact with each other. The interaction of waves with other waves is called wave interference. Wave interference may occur when two waves that are traveling in opposite directions meet. The two waves pass through each other, and this affects their amplitude. Amplitude is the maximum distance the particles of the medium move from their resting positions when a wave passes through. How amplitude is affected by wave interference depends on the type of interference. Interference can be constructive or destructive. Constructive Interference Destructive Interference Constructive interference occurs when crests of one Destructive interference occurs when the crests of one wave overlap the crests of the other wave. The figure wave overlap the troughs, or lowest points, of another above shows what happens. As the waves pass through wave. The figure above shows what happens. As the each other, the crests combine to produce a wave with waves pass through each other, the crests and troughs greater amplitude. The same can happen with two cancel each other out to produce a wave with zero troughs interacting. amplitude. (NOTE: They don’t always have to fully cancel out. Destructive interference can be partial cancellation.) TRUE or FALSE: Identify the following statements as being either true (T) or false (F). 1. When two pulses meet up with each other while moving through the same medium, they tend to bounce off each other and return back to their origin. -
Time-Domain Grating with a Periodically Driven Qutrit
PHYSICAL REVIEW APPLIED 11, 014053 (2019) Time-Domain Grating with a Periodically Driven Qutrit Yingying Han,1,2,3,§ Xiao-Qing Luo,2,3,§ Tie-Fu Li,4,2,* Wenxian Zhang,1,† Shuai-Peng Wang,2 J.S. Tsai,5,6 Franco Nori,5,7 and J.Q. You3,2,‡ 1 School of Physics and Technology, Wuhan University, Wuhan, Hubei 430072, China 2 Quantum Physics and Quantum Information Division, Beijing Computational Science Research Center, Beijing 100193, China 3 Interdisciplinary Center of Quantum Information and Zhejiang Province Key Laboratory of Quantum Technology and Device, Department of Physics and State Key Laboratory of Modern Optical Instrumentation, Zhejiang University, Hangzhou 310027, China 4 Institute of Microelectronics, Department of Microelectronics and Nanoelectronics, and Tsinghua National Laboratory of Information Science and Technology, Tsinghua University, Beijing 100084, China 5 Theoretical Quantum Physics Laboratory, RIKEN Cluster for Pioneering Research, Wako-shi, Saitama 351-0198, Japan 6 Department of Physic, Tokyo University of Science, Kagurazaka, Shinjuku-ku, Tokyo 162-8601, Japan 7 Department of Physics, The University of Michigan, Ann Arbor, Michigan 48109-1040, USA (Received 23 October 2018; revised manuscript received 3 December 2018; published 28 January 2019) Physical systems in the time domain may exhibit analogous phenomena in real space, such as time crystals, time-domain Fresnel lenses, and modulational interference in a qubit. Here, we report the experi- mental realization of time-domain grating using a superconducting qutrit in periodically modulated probe and control fields via two schemes: simultaneous modulation and complementary modulation. Both exper- imental and numerical results exhibit modulated Autler-Townes (AT) and modulation-induced diffraction (MID) effects. -
Physical Quantum States and the Meaning of Probability Michel Paty
Physical quantum states and the meaning of probability Michel Paty To cite this version: Michel Paty. Physical quantum states and the meaning of probability. Galavotti, Maria Carla, Suppes, Patrick and Costantini, Domenico. Stochastic Causality, CSLI Publications (Center for Studies on Language and Information), Stanford (Ca, USA), p. 235-255, 2001. halshs-00187887 HAL Id: halshs-00187887 https://halshs.archives-ouvertes.fr/halshs-00187887 Submitted on 15 Nov 2007 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. as Chapter 14, in Galavotti, Maria Carla, Suppes, Patrick and Costantini, Domenico, (eds.), Stochastic Causality, CSLI Publications (Center for Studies on Language and Information), Stanford (Ca, USA), 2001, p. 235-255. Physical quantum states and the meaning of probability* Michel Paty Ëquipe REHSEIS (UMR 7596), CNRS & Université Paris 7-Denis Diderot, 37 rue Jacob, F-75006 Paris, France. E-mail : [email protected] Abstract. We investigate epistemologically the meaning of probability as implied in quantum physics in connection with a proposed direct interpretation of the state function and of the related quantum theoretical quantities in terms of physical systems having physical properties, through an extension of meaning of the notion of physical quantity to complex mathematical expressions not reductible to simple numerical values. -
Abstract for Non Ideal Measurements by David Albert (Philosophy, Columbia) and Barry Loewer (Philosophy, Rutgers)
Abstract for Non Ideal Measurements by David Albert (Philosophy, Columbia) and Barry Loewer (Philosophy, Rutgers) We have previously objected to "modal interpretations" of quantum theory by showing that these interpretations do not solve the measurement problem since they do not assign outcomes to non_ideal measurements. Bub and Healey replied to our objection by offering alternative accounts of non_ideal measurements. In this paper we argue first, that our account of non_ideal measurements is correct and second, that even if it is not it is very likely that interactions which we called non_ideal measurements actually occur and that such interactions possess outcomes. A defense of of the modal interpretation would either have to assign outcomes to these interactions, show that they don't have outcomes, or show that in fact they do not occur in nature. Bub and Healey show none of these. Key words: Foundations of Quantum Theory, The Measurement Problem, The Modal Interpretation, Non_ideal measurements. Non_Ideal Measurements Some time ago, we raised a number of rather serious objections to certain so_called "modal" interpretations of quantum theory (Albert and Loewer, 1990, 1991).1 Andrew Elby (1993) recently developed one of these objections (and added some of his own), and Richard Healey (1993) and Jeffrey Bub (1993) have recently published responses to us and Elby. It is the purpose of this note to explain why we think that their responses miss the point of our original objection. Since Elby's, Bub's, and Healey's papers contain excellent descriptions both of modal theories and of our objection to them, only the briefest review of these matters will be necessary here. -
When the Uncertainty Principle Goes to 11... Or How to Explain Quantum Physics with Heavy Metal
Ronald E. Hatcher Science on Saturday Lecture Series 12 January 2019 When The Uncertainty Principle goes to 11... or How to Explain Quantum Physics with Heavy Metal Philip Moriarty Professor, University of Nottingham, United Kingdom ABSTRACT: There are deep and fundamental linKs between quantum physics and heavy metal. No, really. There are. Far from being music for Neanderthals, as it’s too often construed, metal can be harmonically and rhythmically complex. That complexity is the source of many connections to the quantum world. You’ll discover how the Heisenberg uncertainty principle comes into play with every chugging guitar riff, what wave interference has to do with Iron Maiden, and why metalheads in mosh pits behave just liKe molecules in a gas. BIOGRAPHY: Philip Moriarty is a professor of physics, a heavy metal fan, a Keen air-drummer, and author of “When The Uncertainty Principle Goes To 11 (or How To Explain Quantum Physics With Heavy Metal” (Ben Bella 2018). His research at the University of Nottingham focuses on prodding, pushing, and poKing single atoms and molecules; in this nanoscopic world, quantum physics is all. Moriarty has taught physics for twenty years and has always been strucK by the number of students in his classes who profess a love of metal music, and by the deep connections between heavy metal and quantum mechanics. A frequent contributor to the Sixty Symbols YouTube channel, which won the Institute of Physics’ Kelvin Award in 2016 for “for innovative and effective promotion of the public understanding of physics”, he has a Keen interest in public engagement, outreach, and bridging the arts-science divide. -
1 Does Consciousness Really Collapse the Wave Function?
Does consciousness really collapse the wave function?: A possible objective biophysical resolution of the measurement problem Fred H. Thaheld* 99 Cable Circle #20 Folsom, Calif. 95630 USA Abstract An analysis has been performed of the theories and postulates advanced by von Neumann, London and Bauer, and Wigner, concerning the role that consciousness might play in the collapse of the wave function, which has become known as the measurement problem. This reveals that an error may have been made by them in the area of biology and its interface with quantum mechanics when they called for the reduction of any superposition states in the brain through the mind or consciousness. Many years later Wigner changed his mind to reflect a simpler and more realistic objective position, expanded upon by Shimony, which appears to offer a way to resolve this issue. The argument is therefore made that the wave function of any superposed photon state or states is always objectively changed within the complex architecture of the eye in a continuous linear process initially for most of the superposed photons, followed by a discontinuous nonlinear collapse process later for any remaining superposed photons, thereby guaranteeing that only final, measured information is presented to the brain, mind or consciousness. An experiment to be conducted in the near future may enable us to simultaneously resolve the measurement problem and also determine if the linear nature of quantum mechanics is violated by the perceptual process. Keywords: Consciousness; Euglena; Linear; Measurement problem; Nonlinear; Objective; Retina; Rhodopsin molecule; Subjective; Wave function collapse. * e-mail address: [email protected] 1 1. -
Rethinking a Delayed Choice Quantum Eraser Experiment: a Simple Baseball Model Jeffrey H
PHYSICS ESSAYS 26, 1 (2013) Rethinking a delayed choice quantum eraser experiment: A simple baseball model Jeffrey H. Boyda) 57 Woods Road, Bethany, Connecticut 06524, USA (Received 10 June 2012; accepted 26 December 2012; published online 26 February 2013) Abstract: In a double slit experiment, you can see an interference fringe pattern or you can know which slit the photon came through, but not both. There are two diametrically opposite theories about why this happens. One is complementarity. The other is the proposal made in this article. An experiment, published in 2000 [Y.-H. Kim et al., Phys. Rev. Lett. 8, 1 (2000)] allegedly supports the idea of complementarity. With different starting assumptions, we arrive at opposite conclusions: complementarity is irrelevant to this experiment. Our assumptions come from the Theory of Elementary Waves. Waves are assumed to travel in the opposite direction: from the detector to the laser. All wave interference is located at the laser. All decisions of importance are located at the laser, not at the detectors. The “decisions” concern which of several elementary rays a photon chooses to follow (this is a probabilistic decision). If a photon is emitted in response to one such impinging ray, all wave interference is then complete. The photon will follow backwards that ray alone, with a probability of one, back to the pair of detectors from which that ray originated. Based on these assumptions, the experiment has nothing to do with complementarity. There is also no delayed choice and no quantum eraser. Conclusion: complementarity is not the only way to understand this experiment.