Results for 'interacting bosons'

959 found
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  1. Interacting Bosons at Finite Temperature: How Bogolubov Visited a Black Hole and Came Home Again. [REVIEW]S. A. Fulling, B.-G. Englert & M. D. Pilloff - 2003 - Foundations of Physics 33 (1):87-110.
    The structure of the thermal equilibrium state of a weakly interacting Bose gas is of current interest. We calculate the density matrix of that state in two ways. The most effective method, in terms of yielding a simple, explicit answer, is to construct a generating function within the traditional framework of quantum statistical mechanics. The alternative method, arguably more interesting, is to construct the thermal state as a vector state in an artificial system with twice as many degrees of (...)
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  2.  78
    Slave-Boson Mean-Field Theory of Spin- and Orbital- Ordered States in the Degenerate Hubbard Model.Hideo Hasegawa - 2000 - Foundations of Physics 30 (12):2061-2078.
    The mean-field theory with the use of the slave-boson functional method has been generalized to take account of the spin- and/or orbital-ordered state in the doubly degenerate Hubbard model. Numerical calculations are presented of the antiferromagnetic orbital-ordered state in the half-filled simple-cubic model. The orbital order in the present theory is much reduced compared with that in the Hartree–Fock approximation because of the large orbital fluctuations. From a comparison of the ground-state energy, the antiferromagnetic orbital state is shown to be (...)
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  3. On the nature of the Higgs boson.Damiano Anselmi - 2019 - Mod. Phys. Lett. A 34.
    Several particles are not observed directly, but only through their decay products. We consider the possibility that they might be fakeons, i.e. fake particles, which mediate interactions but are not asymptotic states. A crucial role to determine the true nature of a particle is played by the imaginary parts of the one-loop radiative corrections, which are affected in nontrivial ways by the presence of fakeons in the loop. The knowledge we have today is sufficient to prove that most non directly (...)
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  4.  40
    Phonon Superfluids in Sets of Trapped Ions.D. Porras & J. I. Cirac - 2006 - Foundations of Physics 36 (4):465-476.
    We show that transverse phonons in a set of trapped ions under the action of lasers are described by an interacting boson model whose parameters can be externally adjusted. If the radial trapping frequency is large enough, the system is described by a Bose–Hubbard model, in which hopping of the phonons between different ions is provided by the Coulomb interaction. On the other hand, the non-linear terms in the interaction of the ions with a standing-wave provide us with the (...)
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  5.  99
    The superfluid as a source of all interactions.K. P. Sinha & E. C. G. Sudarshan - 1978 - Foundations of Physics 8 (11-12):823-831.
    The superfluid state of fermion-antifermion fields developed in our previous papers is generalized to include higher orbital and spin states. In addition to single-particle excitations, the system is capable of having real and virtual bound or quasibound composite excitations which are akin to bosons of spinJ P equal to0 −, 1−, 2+, etc. These pseudoscalar, vector, and tensor bosons can be massive or massless and provide the vehicles for strong, electromagnetic, weak, and gravitational interactions. The concept that the (...)
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  6.  50
    Bose Condensation Without Broken Symmetries.Andrei E. Ruckenstein - 2000 - Foundations of Physics 30 (12):2113-2124.
    This paper considers the issue of Bose–Einstein condensation in a weakly interacting Bose gas with a fixed total number of particles. We use an old current algebra formulation of non-relativistic many body systems due to Dashen and Sharp to show that, at sufficiently low temperatures, a gas of weakly interacting Bosons displays Off-diagonal Long Range Order in the sense introduced by Penrose and Onsager. Even though this formulation is somewhat cumbersome it may demystify many of the standard (...)
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  7.  15
    The Standard Model's Form Derived From Operator Logic, Superluminal Transformations and Gl(16).Stephen Blaha - 2010 - Pingree-Hill.
    This new edition of work that has evolved over the past seven years completes the derivation of the form of The Standard Model from quantum theory and the extension of the Theory of Relativity to superluminal transformations. The much derided form of The Standard Model is established from a consideration of Lorentz and superluminal relativistic space-time transformations. So much so that other approaches to elementary particle theory pale in comparison. In previous work color SU(3) was derived from space-time considerations. This (...)
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  8.  45
    Is the Luttinger Liquid a New State of Matter?V. V. Afonin & V. Y. Petrov - 2010 - Foundations of Physics 40 (2):190-204.
    We are demonstrating that the Luttinger model with short range interaction can be treated as a type of Fermi liquid. In line with the main dogma of Landau’s theory one can define a fermion excitation renormalized by interaction and show that in terms of these fermions any excited state of the system is described by free particles. The fermions are a mixture of renormalized right and left electrons. The electric charge and chirality of the Landau quasi-particle is discussed.
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  9.  49
    Materialism and mentality.G. D. Wassermann - 1982 - Review of Metaphysics 35 (4):715-30.
    MATERIALISTS claim that in principle mentality could be accounted for entirely by properties of matter. They must, of course, clarify, as far as possible, the precise scope of the concept "properties of matter." According to materialists there exists only one type of "substance" in the universe, namely matter. Sophisticated experimental and theoretical analyses have led contemporary physicists to interpret known material entities as being composed of two classes of elementary particles, namely quarks and leptons and constituents of interaction fields that (...)
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  10.  38
    Bose–Einstein Condensation of Nonideal Cooper Pairs in the Hartree–Fock–Popov Theory.Ze Cheng - 2016 - Foundations of Physics 46 (8):915-942.
    The Hartree–Fock–Popov theory of interacting Bose particles is generalized to the Cooper-pair system with a screened Coulomb repulsive interaction in high-temperature superconductors. At zero temperature, it is found that the condensate density \\) of Cooper pairs is of the order \\simeq 10^{18}\) cm\, consistently with the fact that a small fraction of the total p holes participate in pairing. We find that the phonon velocity c at zero temperature is of the order \\simeq 10\) km s\. The computation shows (...)
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  11. Unified spin gauge model and the top quark mass.J. S. R. Chisholm & R. S. Farwell - 1995 - Foundations of Physics 25 (10):1511-1522.
    Spin gauge models use a real Clifford algebraic structure Rp,q associated with a real manifold of dimension p + q to describe the fundamental interactions of elementary particles. This review provides a comparison between those models and the standard model, indicating their similarities and differences. By contrast with the standard model, the spin gauge model based on R3,8 generates intermediate boson mass terms without the need to use the Higgs-Kibble mechanism and produces a precise prediction for the mass of the (...)
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  12. The arbitrariness of local gauge symmetry.Alexandre Guay - 2004
    This paper shows how the study of surpluses of structure is an interesting philosophical task. In particular I explore how local gauge symmetry in quantized Yang-Mills theories is the by-product of the specific dynamical structure of interaction. It is shown how in non relativistic quantum mechanics gauge symmetry corresponds to the freedom to locally define global features of gauge potentials. Also discussed is how in quantum field theory local gauge symmetry is replaced by BRST symmetry. This last symmetry is apparently (...)
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  13.  40
    On the indistinguishability of classical particles.S. Fujita - 1991 - Foundations of Physics 21 (4):439-457.
    If no property of a system of many particles discriminates among the particles, they are said to be indistinguishable. This indistinguishability is equivalent to the requirement that the many-particle distribution function and all of the dynamic functions for the system be symmetric. The indistinguishability defined in terms of the discrete symmetry of many-particle functions cannot change in the continuous classical statistical limit in which the number density n and the reciprocal temperature β become small. Thus, microscopic particles like electrons must (...)
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  14. The mechanics of individuality in nature. II. Barriers, cells, and individuality.Stanford Goldman - 1973 - Foundations of Physics 3 (2):203-228.
    The cell theory of Schleiden and Schwann is generalized to the effect that throughout the natural world, in physics, biology, and sociopsychology, there is a widespread phenomenon of the existence of organized cells, whose organization is usually protected by barriers. These barriers exist not only in space, but in time and even in other domains. These barriers typically not only protect the organization within the cell from external disturbance, but they actively participate in reducing the internal disorganization. It appears that (...)
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  15.  29
    Unobservable entities in modern physics.Elena Mamchur - 2017 - Epistemology and Philosophy of Science 51 (1):106-123.
    The paper deals with the problem of ontological status of unobservable entities of modern physics. Author considers the question whether they are real objects or social constructs? The first point is being supported by constructive realists; the second one is backed by those who stand by a very influential strategy of the so-called social constructionism. Realists assume that intermediate vector bosons (as well as Higgs boson recently discovered by the experiments at the Large Hadron Collider) do exist in reality (...)
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  16.  39
    Matrix models as non-local hidden variables theories.Lee Smolin - unknown
    It is shown that the matrix models which give non-perturbative definitions of string and M theory may be interpreted as non-local hidden variables theories in which the quantum observables are the eigenvalues of the matrices while their entries are the non-local hidden variables. This is shown by studying the bosonic matrix model at finite temperature, with T taken to scale as 1/N, with N the rank of the matrices. For large N the eigenvalues of the matrices undergo Brownian motion due (...)
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  17.  32
    Nova fizika na LHC-u i nova filozofska istraživanja.Tomislav Petković - 2010 - Filozofska Istrazivanja 30 (1-2):193-209.
    Članak je usmjeren ususret paradigmi nove fizike koju treba iznijeti LHC, ali s kritičkim prosuđivanjem toga razvoja pomoću Kuhnovih teza i epistemologije povezanih s modernom fizikom. Promišljanja i prosudbe nove filozofije niču iz LHC-fizike, koja se tumači kao »science universelle« . LHC, kao najveći sudarivač čestica u svijetu do sada, nije motiviran time da uništi Boga niti bilo koju vjeru u svijetu, već za otkrivanje novih čestica s njihovim interakcijama i kozmologijom u Prirodi, baš onoliko koliko pružaju LHC-scenariji na Tera-elektron-volt (...)
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  18.  70
    Composite structure of the nucleon.M. M. Islam - 1994 - Foundations of Physics 24 (3):419-425.
    The nonlinear σ-model with vector mesons introduced as gauge bosons and an interacting chiral quark sector depicts the nucleon as a topological soliton embedded in a chiral condensate. High-energy elastic pp and ¯pp scattering data from CERN ISR and SPS Collider appear to provide strong evidence in favor of this nucleon structure.
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  19.  49
    Momentum projection of solitons including quantum corrections.Lawrence Wilets - 1986 - Foundations of Physics 16 (2):171-185.
    The method of projection is applied to a relativistic field theory of fermions interacting with a nonlinear scalar field, specifically the Friedberg-Lee soliton model. Projection is effected by operating on a localized “bag” state with the translation operator exp (iP·Z), and integrating overZ. The resulting state is an eigenstate of zero momentum. The energy and the expectation value of other physical operators can be expressed as Gaussian moments of the Hamiltonian or the physical operator times powers of the momentum (...)
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  20.  62
    Random matrices, fermions, collective fields, and universality.B. Sakita - 1997 - Foundations of Physics 27 (11):1519-1525.
    We first relate the random matrix model to a Fokker-Planck Hamiltonian system, such that the correlation functions of the model are expressed as the vacuum expectation values of equal-time products of density operators. We then analyze the universality of the random matrix model by solving the Focker-Planck Hamiltonian system for large N. We use two equivalent methods to do this, namely the method of relating it to a system of interacting fermions in one space dimension and the method of (...)
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  21.  33
    Generalized Stefan–Boltzmann Law.Gilles Montambaux - 2018 - Foundations of Physics 48 (4):395-410.
    We reconsider the thermodynamic derivation by L. Boltzmann of the Stefan law and we generalize it for various different physical systems whose chemical potential vanishes. Being only based on classical arguments, therefore independent of the quantum statistics, this derivation applies as well to the saturated Bose gas in various geometries as to “compensated” Fermi gas near a neutrality point, such as a gas of Weyl Fermions. It unifies in the same framework the thermodynamics of many different bosonic or fermionic non- (...) gases which were until now described in completely different contexts. (shrink)
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  22. Towards unified field theory: Quantitative differences and qualitative sameness.Mael A. Melvin - 1982 - Synthese 50 (3):359 - 397.
    A survey is given of the concepts of interaction (force) and matter, i.e., of process and substance. The development of these concepts, first in antiquity, then in early modern times, and finally in the contemporary system of quantum field theory is described. After a summary of the basic phenomenological attributes (coupling strengths, symmetry quantities, charges), the common ground of concepts of quantum field theory for both interactions and matter entities is discussed. Then attention is focused on the gauge principle which (...)
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  23.  35
    The CERN LHC: A Black Hole Factory?John Cramer - unknown
    The Large Hadronic Collider (LHC), which is to be the world’s highest energy particle accelerator, is currently being constructed at the CERN laboratory in Geneva, Switzerland. The machine was designed to be high enough in energy to produce a completely new type of particle, the Higgs boson, which is considered to be the missing puzzle-piece in the Standard Model of particle interactions. According to current theoretical thinking, it is the Higgs particle that gives mass to all the other particles, quarks, (...)
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  24.  85
    The Higgs mechanism and superconductivity: A case study of formal analogies.Doreen Fraser & Adam Koberinski - 2016 - Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics 55:72-91.
    Following the experimental discovery of the Higgs boson, physicists explained the discovery to the public by appealing to analogies with condensed matter physics. The historical root of these analogies is the analogies to models of superconductivity that inspired the introduction of spontaneous symmetry breaking into particle physics in the early 1960s. We offer a historical and philosophical analysis of the analogies between the Higgs model of the electroweak interaction and the Ginsburg-Landau and Bardeen-Cooper-Schrieffer models of superconductivity, respectively. The conclusion of (...)
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  25.  71
    Guest Editor’s Introduction: An Overview of the Epistemological Perspectives on the Higgs Mechanism.Koray Karaca - 2014 - Journal for General Philosophy of Science / Zeitschrift für Allgemeine Wissenschaftstheorie 45 (2):329-333.
    The present special section brings together three articles that seek to elucidate the epistemological and ontological foundations of the Higgs mechanism, as well as the epistemic dynamics of the development of the models beyond the “standard model” of elementary particle physics.The standard model of elementary particle physics consists of two gauge theories; namely, the electroweak theory of the weak and electromagnetic interactions, and the theory of quantum chromo-dynamics which describes the strong interaction. This introduction will provide a brief overview of (...)
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  26.  47
    Particles vs. events: The concatenated structure of world lines in relativistic quantum mechanics. [REVIEW]R. Arshansky, L. P. Horwitz & Y. Lavie - 1983 - Foundations of Physics 13 (12):1167-1194.
    The dynamical equations of relativistic quantum mechanics prescribe the motion of wave packets for sets of events which trace out the world lines of the interacting particles. Electromagnetic theory suggests thatparticle world line densities be constructed from concatenation of event wave packets. These sequences are realized in terms of conserved probability currents. We show that these conserved currents provide a consistent particle and antiparticle interpretation for the asymptotic states in scattering processes. The relation between current conservation and unitarity is (...)
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  27.  22
    Statistical Properties of Strongly Correlated Quantum Liquids.M. L. Ristig & K. A. Gernoth - 2010 - Foundations of Physics 40 (9-10):1253-1262.
    Modern microscopic theory is employed to construct a powerful analytical algorithm that permits a clear description of characteristic features of strongly correlated quantum fluids in thermodynamic equilibrium. Using recently developed formal results we uncover an intricate relationship between strongly correlated systems and free quantum gases of appropriately defined constituents. The latter entities are precisely defined renormalized bosons or fermions. They carry all the information contained in the statistical correlations of the strongly interacting many-particle system by virtue of their (...)
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  28.  16
    Consistent or inconsistent? The effects of inducing cognitive dissonance vs. cognitive consonance on the intention to engage in pro-environmental behaviors.Lucia Bosone, Marie Chevrier & Franck Zenasni - 2022 - Frontiers in Psychology 13.
    How do individuals rationalize the cognitive dissonance between their environmental awareness and the maintenance of environmentally unfriendly behaviors? The main goal is to explore the rationalization strategies used by individuals in order to maintain their current behaviors. The secondary goal is to understand if it is possible to induce cognitive consonance, and how this influences intention to change. We present a study with three experimental conditions: inconsistency, control, and consistency. The method to induce inconsistency and consistency was inspired by the (...)
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  29. Hitman: Blood Money.[XBOX360].I. O. Interactive - forthcoming - Eidos: Revista de Filosofía de la Universidad Del Norte.
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  30. George L. Gerstein.Interactions Within Neuronal - 1990 - In J. McGaugh, Jerry Weinberger & G. Lynch (eds.), Brain Organization and Memory: Cells, Systems, and Circuits. Guilford Press.
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  31. Optimally interacting minds.Bahador Bahrami, Karsten Olsen, Peter Latham, Andreas Roepstorff, Geraint Rees & Chris Frith - 2010 - Science 329 (5995):1081–5.
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  32.  92
    Interacting with Emotions: Imagination and Supposition.Margherita Arcangeli - 2017 - Philosophical Quarterly 67 (269):730-750.
    A widespread claim, which I call ‘the Emotionality Claim’, is that imagination but not supposition is intimately linked to emotion. In more cognitive jargon, imagination is connected to the affect system, whereas supposition is not. EC is open to several interpretations which yield very different views about the nature of supposition. The literature lacks an in-depth analysis of EC which sorts out these different readings and ways to carve supposition and imagination at their joints. The aim of this paper is (...)
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  33.  16
    Journal of the International Association for Semiotic Studies/Revue de l'Association Internationale de Sémiotique.Meaning In Motion & Interaction In Cars - 2012 - Semiotica 2012 (191).
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  34.  17
    Interacting Plans.Bertram Bruce & Denis Newman - 1978 - Cognitive Science 2 (3):195-233.
    The paper explores certain phenomena which arise in stories, conversations, and human activity in general when the plans of two individuals are formed and carried out in an interactive situation. A notation system for representing interacting plans is introduced and applied in the analysis of a small portion of “Hansel and Gretel.” The analysis illustrates how a single actor plan can be modified by the needs of cooperative interaction with others and how cooperative interactive episodes can be transformed and (...)
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  35.  19
    Interacting With Multiple Partners Improves Communication Skills.Shiri Lev-Ari & Natalie Sebanz - 2020 - Cognitive Science 44 (4):e12836.
    Successful communication is important for both society and people’s personal life. Here we show that people can improve their communication skills by interacting with multiple others, and that this improvement seems to come about by a greater tendency to take the addressee’s perspective when there are multiple partners. In Experiment 1, during a training phase, participants described figures to a new partner in each round or to the same partner in all rounds. Then all participants interacted with a new (...)
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  36.  14
    From interacting systems to a system of divisions: The concept of society and the ‘mutual constitution’ of intersecting social divisions.Marcel Stoetzler - 2017 - European Journal of Social Theory 20 (4):455-472.
    This article examines a fundamental theoretical aspect of the discourse on ‘intersectionality’ in feminist and anti-racist social theory, namely, the question whether intersecting social divisions including those of sex, gender, race, class and sexuality are interacting but independent entities with autonomous ontological bases or whether they are different dimensions of the same social system that lack separate social ontologies and constitute each other. Based on a historical reconstruction of its genesis, the article frames this as a dispute between system-theoretical (...)
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  37.  26
    Room temperature ionic liquids interacting with bio-molecules: an overview of experimental and computational studies.Antonio Benedetto & Pietro Ballone - 2016 - Philosophical Magazine 96 (7-9):870-894.
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  38.  34
    Stochastic processes for indirectly interacting particles and stochastic quantum mechanics.V. Buonomano & A. F. Prado de Andrade - 1988 - Foundations of Physics 18 (4):401-426.
    This work has two objectives. The first is to begin a mathematical formalism appropriate to treating particles which only interact with each otherindirectly due to hypothesized memory effects in a stochastic medium. More specifically we treat a situation in which a sequence of particles consecutively passes through a region (e.g., a measuring apparatus) in such a way that one particle leaves the region before the next one enters. We want to study a situation in which a particle may interact with (...)
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  39.  10
    System Green functions for interacting quantum particles.A. Gonis - 2006 - Philosophical Magazine 86 (17-18):2537-2552.
  40.  5
    Reaching Agreement Among Randomly Interacting Agents: Brain Models, Schemas, and Unitary Responses.William Kilmer - 1999 - Journal of Intelligent Systems 9 (3-4):203-218.
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  41. Interacting with fiction?Luca Baptista - 2009 - Proceedings of the Philosophy of Computer Games Conference.
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  42.  52
    The PIWI-Interacting RNA Molecular Pathway: Insights From Cultured Silkworm Germline Cells.Kazuhiro Sakakibara & Mikiko C. Siomi - 2018 - Bioessays 40 (1):1700068.
    The PIWI-interacting RNA pathway, one of the major eukaryotic small RNA silencing pathways, is a genome surveillance system that silences selfish genes in animal gonads. piRNAs guide PIWI protein to target genes through Watson–Crick RNA–RNA base-parings. Loss of piRNA function causes genome instability, inducing failure in gametogenesis and infertility. Studies using fruit flies and mice as key experimental models have resulted in tremendous progress in understanding the mechanism underlying the piRNA pathway. Recent work using cultured silkworm germline cells has (...)
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  43.  54
    Do people with social anxiety feel anxious about interacting with a robot?Tatsuya Nomura, Takayuki Kanda, Tomohiro Suzuki & Sachie Yamada - 2020 - AI and Society 35 (2):381-390.
    To investigate whether people with social anxiety have less actual and “anticipatory” anxiety when interacting with a robot compared to interacting with a person, we conducted a 2 × 2 psychological experiment with two factors: social anxiety and interaction partner. The experiment was conducted in a counseling setting where a participant played the role of a client and the robot or the confederate played the role of a counselor. First, we measured the participants’ social anxiety using the Social (...)
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  44. Decision-making with interacting goals.R. Felix - 1998 - In Enrique H. Ruspini, Piero Patrone Bonissone & Witold Pedrycz (eds.), Handbook of fuzzy computation. Philadelphia: Institute of Physics.
     
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  45.  28
    Assumption-based argumentation with preferences and goals for patient-centric reasoning with interacting clinical guidelines.Kristijonas Čyras, Tiago Oliveira, Amin Karamlou & Francesca Toni - 2021 - Argument and Computation 12 (2):149-189.
    A paramount, yet unresolved issue in personalised medicine is that of automated reasoning with clinical guidelines in multimorbidity settings. This entails enabling machines to use computerised generic clinical guideline recommendations and patient-specific information to yield patient-tailored recommendations where interactions arising due to multimorbidities are resolved. This problem is further complicated by patient management desiderata, in particular the need to account for patient-centric goals as well as preferences of various parties involved. We propose to solve this problem of automated reasoning with (...)
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  46.  24
    Beyond the merely visual: interacting with digital objects in interdisciplinary scientific practice.Marko Monteiro - 2010 - Semiotica 2010 (181):127-147.
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  47.  14
    Eigenstates in the Many Interacting Worlds Approach: Focus on 2D Ground States.Hannes Herrmann, Michael J. W. Hall, Howard M. Wiseman & Dirk-André Deckert - 2024 - In Angelo Bassi, Sheldon Goldstein, Roderich Tumulka & Nino Zanghi (eds.), Physics and the Nature of Reality: Essays in Memory of Detlef Dürr. Springer. pp. 125-140.
    The Many-Interacting-Worlds (MIW) approach to a quantum theory without wave functions proposed in [8] leads naturally to numerical integrators of the Schrödinger equation on comoving grids. As yet, little is known about concrete MIW models for more than one spatial dimension and/or more than one particle. In honour of Detlef Dürr, we report on a further development of the MIW approach to treat arbitrary degrees of freedom and provide a numerical proof of concept for ground states in 2d. The (...)
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  48.  3
    On knowledge representing interacting systems.A. Müller - 1993 - In René J. Jorna, Barend van Heusden & Roland Posner (eds.), Signs, Search and Communication: Semiotic Aspects of Artificial Intelligence. De Gruyter. pp. 271-305.
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  49. Interacting with captive dolphins.Toni Frohoff - forthcoming - Between Species: Celebrating the Dolphin–Human Bond. Sierra Club Books, San Francisco.
     
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  50. The Common Basis of Memory and Consciousness: Understanding the Brain as a Write–Read Head Interacting With an Omnipresent Background Field.Joachim Keppler - 2020 - Frontiers in Psychology 10 (Article 2968):1-13.
    The main goal of this article consists in addressing two fundamental issues of consciousness research and cognitive science, namely, the question of why declarative memory functions are inextricably linked with phenomenal awareness and the question of the physical basis of memory traces. The presented approach proposes that high-level cognitive processes involving consciousness employ a universal mechanism by means of which they access and modulate an omnipresent background field that is identified with the zero-point field (ZPF) specified by stochastic electrodynamics, a (...)
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