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    Π”ΡƒΠΌΠ°Ρ‚ΡŒ ΠΏΠΎ-Π΄Ρ€ΡƒΠ³ΠΎΠΌΡƒ ΠΏΡ€ΠΈ психосоматичСских состояниях Ρƒ рСвматологичСских Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ… (ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ стиля ΠΌΡ‹ΡˆΠ»Π΅Π½ΠΈΡ Π²Ρ€Π°Ρ‡Π°)

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    The concept of a 'health care realm' is introduced. The healthcare realms considered were those patients who have only Physical Health Problems (PH), patients with neither physical nor mental health issues and who are seeking advice to remain healthy (HP), patients only with Mental Health Problems (MH), patients with both Physical Health and Mental Health Problems (PH&MH) and patients with Psychosomatic Health conditions (PS). Described is how patients' minds and bodies interact and its relevance to rheumatology practice. Presented is the culmination of 34 years of the author's experience of rheumatological disorders based in Family Medicine in a United Kingdom General Practice. Also presented are 2 small studies supplementing the main conclusions. The first small study counted the main consultation content of 246 patients, as considered by the principals in the practice. Of these 73.5% were for physical health conditions, 13.3% for health promotion, 11.5% for mental health conditions and 1.8% for psychosomatic conditions. The second small study was a survey of experienced GPs, Physicians and Psychiatrists, asking about their opinions on how well the patients in different health care realms were being managed across the healthcare system. Of the 5 realms, the collective view was that it was the patients in the PH realm who was clearly received the best care. The least good care was being given to patients in the PS realm and only marginally better were patients in the MH Realm. This paper argues that clinicians need a different thinking approach when meeting patients from different healthcare realms. It is known that when doctors treat PH patients, they consider the patient's symptoms against templates of knowledge for the conditions in the differential diagnosis. Furthermore, HP patients are assessed by comparing the patient's bio-measurements against known markers of good health When being consulted by patients in the MH or PS realms, it is advocated, not to follow the approach of PH patients. For patients in the MH realm it is best to address the patient's life as a whole and to consider, how did the person arrive to the situation he is in and what needs to be done to restore the patient's life back on track. For patients in the PS realm, ideally the aim is to help the patient make the link between the physical symptom and its psychological aetiology. A step towards this is to describe how the body physically mediates the symptom.Π’ ΡΡ‚Π°Ρ‚ΡŒΠ΅ рассматриваСтся понятиС «клиничСская Π³Ρ€ΡƒΠΏΠΏΠ°Β». Π’Ρ‹Π΄Π΅Π»Π΅Π½Ρ‹ ΡΠ»Π΅Π΄ΡƒΡŽΡ‰ΠΈΠ΅ клиничСскиС Π³Ρ€ΡƒΠΏΠΏΡ‹: ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Ρ‹, Ρƒ ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… Π΅ΡΡ‚ΡŒ ΠΏΡ€ΠΎΠ±Π»Π΅ΠΌΡ‹ Ρ‚ΠΎΠ»ΡŒΠΊΠΎ с физичСским Π·Π΄ΠΎΡ€ΠΎΠ²ΡŒΠ΅ΠΌ (соматичСскиС расстройства – Π‘Π ); ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Ρ‹ Π±Π΅Π· Π½Π°Ρ€ΡƒΡˆΠ΅Π½ΠΈΠΉ физичСского ΠΈΠ»ΠΈ психичСского Π·Π΄ΠΎΡ€ΠΎΠ²ΡŒΡ, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ ΠΎΠ±Ρ€Π°Ρ‰Π°ΡŽΡ‚ΡΡ ΠΏΠΎ ΠΏΠΎΠ²ΠΎΠ΄Ρƒ сохранСния Π·Π΄ΠΎΡ€ΠΎΠ²ΡŒΡ (Π‘Π—); ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Ρ‹ Ρ‚ΠΎΠ»ΡŒΠΊΠΎ с ΠΏΡ€ΠΎΠ±Π»Π΅ΠΌΠ°ΠΌΠΈ психичСского Π·Π΄ΠΎΡ€ΠΎΠ²ΡŒΡ (психичСскиС расстройства – ПР); ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Ρ‹ с Π½Π°Ρ€ΡƒΡˆΠ΅Π½ΠΈΠ΅ΠΌ физичСского ΠΈ психичСского Π·Π΄ΠΎΡ€ΠΎΠ²ΡŒΡ (соматичСскиС ΠΈ психичСскиС расстройства – Π‘Π  + ПР) ΠΈ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Ρ‹ с психосоматичСскими расстройствами (ПБР). На ΠΏΡ€ΠΈΠΌΠ΅Ρ€Π΅ рСвматичСских Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΠΉ (Π Π—) описано взаимодСйствиС психичСской ΠΈ соматичСской сфСры. Π‘Ρ‚Π°Ρ‚ΡŒΡ являСтся ΠΈΡ‚ΠΎΠ³ΠΎΠΌ 34-Π»Π΅Ρ‚Π½Π΅Π³ΠΎ ΠΎΠΏΡ‹Ρ‚Π° Π°Π²Ρ‚ΠΎΡ€Π° Π² области лСчСния Π Π— Π² условиях сСмСйной ΠΌΠ΅Π΄ΠΈΡ†ΠΈΠ½Ρ‹ ΠΈ ΠΎΠ±Ρ‰Π΅ΠΉ ΠΏΡ€Π°ΠΊΡ‚ΠΈΠΊΠΈ Π’Π΅Π»ΠΈΠΊΠΎΠ±Ρ€ΠΈΡ‚Π°Π½ΠΈΠΈ. ΠžΡΠ½ΠΎΠ²Π½Ρ‹Π΅ полоТСния ΡΡ‚Π°Ρ‚ΡŒΠΈ Π΄ΠΎΠΏΠΎΠ»Π½Π΅Π½Ρ‹ Π΄Π°Π½Π½Ρ‹ΠΌΠΈ Π΄Π²ΡƒΡ… Π½Π΅Π±ΠΎΠ»ΡŒΡˆΠΈΡ… исслСдований. ΠŸΠ΅Ρ€Π²ΠΎΠ΅ исслСдованиС Π²ΠΊΠ»ΡŽΡ‡Π°Π»ΠΎ 246 ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ², срСди ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… 73,5% ΠΏΠΎΠ»ΡƒΡ‡Π°Π»ΠΈ ΠΊΠΎΠ½ΡΡƒΠ»ΡŒΡ‚Π°Ρ†ΠΈΠΈ ΠΏΠΎ ΠΏΠΎΠ²ΠΎΠ΄Ρƒ Π‘Π , 13,3% – Π‘Π—, 11,5% – ПР ΠΈ 1,8% – ПБР. Π’Ρ‚ΠΎΡ€ΠΎΠ΅ исслСдованиС основано Π½Π° Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π°Ρ… анкСтирования ΠΎΠΏΡ‹Ρ‚Π½Ρ‹Ρ… Π²Ρ€Π°Ρ‡Π΅ΠΉ ΠΎΠ±Ρ‰Π΅ΠΉ ΠΏΡ€Π°ΠΊΡ‚ΠΈΠΊΠΈ ΠΈ психиатров, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ ΠΎΡ†Π΅Π½ΠΈΠ²Π°Π»ΠΈ, насколько Ρ…ΠΎΡ€ΠΎΡˆΠΎ, ΠΏΠΎ ΠΈΡ… мнСнию, ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Π°ΠΌ Ρ€Π°Π·Π½Ρ‹Ρ… клиничСских Π³Ρ€ΡƒΠΏΠΏ оказываСтся мСдицинская ΠΏΠΎΠΌΠΎΡ‰ΡŒ Π² Ρ€Π°ΠΌΠΊΠ°Ρ… ΡΡƒΡ‰Π΅ΡΡ‚Π²ΡƒΡŽΡ‰Π΅ΠΉ систСмы здравоохранСния. По ΠΎΡ†Π΅Π½ΠΊΠ°ΠΌ Π²Ρ€Π°Ρ‡Π΅ΠΉ, Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΠΊΠ²Π°Π»ΠΈΡ„ΠΈΡ†ΠΈΡ€ΠΎΠ²Π°Π½Π½ΡƒΡŽ ΠΏΠΎΠΌΠΎΡ‰ΡŒ ΠΏΠΎΠ»ΡƒΡ‡Π°ΡŽΡ‚ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Ρ‹ Π³Ρ€ΡƒΠΏΠΏΡ‹ Π‘Π , Π° Π½Π°ΠΈΠΌΠ΅Π½Π΅Π΅ ΠΊΠ²Π°Π»ΠΈΡ„ΠΈΡ†ΠΈΡ€ΠΎΠ²Π°Π½Π½ΡƒΡŽ – ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Ρ‹ Π³Ρ€ΡƒΠΏΠΏΡ‹ ПБР, Π½Π΅ΠΌΠ½ΠΎΠ³ΠΈΠΌ Π»ΡƒΡ‡ΡˆΠ΅ Π±Ρ‹Π»ΠΈ ΠΏΠΎΠΊΠ°Π·Π°Ρ‚Π΅Π»ΠΈ для ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² Π³Ρ€ΡƒΠΏΠΏΡ‹ ПР. УтвСрТдаСтся, Ρ‡Ρ‚ΠΎ ΠΏΡ€ΠΈ Ρ€Π°Π±ΠΎΡ‚Π΅ с ΠΊΠ°ΠΆΠ΄ΠΎΠΉ клиничСской Π³Ρ€ΡƒΠΏΠΏΠΎΠΉ клиницист Π΄ΠΎΠ»ΠΆΠ΅Π½ ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΠΎΠ²Π°Ρ‚ΡŒ особый ΠΏΠΎΠ΄Ρ…ΠΎΠ΄ Π² ΠΌΡ‹ΡˆΠ»Π΅Π½ΠΈΠΈ. ΠŸΡ€ΠΈ Π»Π΅Ρ‡Π΅Π½ΠΈΠΈ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² с Π‘Π  Π²Ρ€Π°Ρ‡ΠΈ Ρ€Π°ΡΡΠΌΠ°Ρ‚Ρ€ΠΈΠ²Π°ΡŽΡ‚ симптомы, ΠΎΠΏΠΈΡ€Π°ΡΡΡŒ Π½Π° стандарты диагностики этих Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΠΉ. БостояниС ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² Π³Ρ€ΡƒΠΏΠΏΡ‹ Π‘Π— оцСниваСтся ΠΏΡƒΡ‚Π΅ΠΌ сравнСния Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΎΠ² обслСдования с извСстными ΠΌΠ°Ρ€ΠΊΠ΅Ρ€Π°ΠΌΠΈ Ρ…ΠΎΡ€ΠΎΡˆΠ΅Π³ΠΎ Π·Π΄ΠΎΡ€ΠΎΠ²ΡŒΡ. ΠŸΠ°Ρ†ΠΈΠ΅Π½Ρ‚Ρ‹ Π³Ρ€ΡƒΠΏΠΏΡ‹ ПР ΠΈΠ»ΠΈ ПБР Ρ‚Ρ€Π΅Π±ΡƒΡŽΡ‚ ΠΈΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ΄Ρ…ΠΎΠ΄Π°, Ρ‡Π΅ΠΌ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Ρ‹ с Π‘Π . ΠŸΡ€ΠΈ ΠΊΠΎΠ½ΡΡƒΠ»ΡŒΡ‚ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠΈ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² с ПР стоит ΠΎΠ±Ρ€Π°Ρ‚ΠΈΡ‚ΡŒΡΡ ΠΊ истории ΠΈΡ… ΠΆΠΈΠ·Π½ΠΈ ΠΈ ΠΏΡ€ΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡ€ΠΎΠ²Π°Ρ‚ΡŒ, Ρ‡Ρ‚ΠΎ ΠΏΡ€ΠΈΠ²Π΅Π»ΠΎ Ρ‡Π΅Π»ΠΎΠ²Π΅ΠΊΠ° ΠΊ слоТной ситуации ΠΈ Ρ‡Ρ‚ΠΎ Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎ ΡΠ΄Π΅Π»Π°Ρ‚ΡŒ, Ρ‡Ρ‚ΠΎΠ±Ρ‹ Π²Π΅Ρ€Π½ΡƒΡ‚ΡŒ Π΅Π³ΠΎ ΠΊ Π½ΠΎΡ€ΠΌΠ°Π»ΡŒΠ½ΠΎΠΉ ΠΆΠΈΠ·Π½ΠΈ. ΠŸΡ€ΠΈ Π²Π΅Π΄Π΅Π½ΠΈΠΈ ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Π° с ПБР Π²Π°ΠΆΠ½ΠΎ ΠΎΠ±Ρ€Π°Ρ‚ΠΈΡ‚ΡŒ Π΅Π³ΠΎ Π²Π½ΠΈΠΌΠ°Π½ΠΈΠ΅ Π½Π° связь ΠΌΠ΅ΠΆΠ΄Ρƒ соматичСскими Π½Π°Ρ€ΡƒΡˆΠ΅Π½ΠΈΡΠΌΠΈ ΠΈ ΠΈΡ… психичСской ΠΏΡ€ΠΈΡ‡ΠΈΠ½ΠΎΠΉ, Ρ€Π°Π·ΡŠΡΡΠ½ΠΈΠ², ΠΊΠ°ΠΊ ΠΎΡ€Π³Π°Π½ΠΈΠ·ΠΌ Ρ€Π΅Π°Π³ΠΈΡ€ΡƒΠ΅Ρ‚ Π½Π° психичСскоС Π½Π΅Π±Π»Π°Π³ΠΎΠΏΠΎΠ»ΡƒΡ‡ΠΈΠ΅

    Does the Third Law of Thermodynamics hold in the Quantum Regime?

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    The first in a long series of papers by John T. Lewis, G. W. Ford and the present author, considered the problem of the most general coupling of a quantum particle to a linear passive heat bath, in the course of which they derived an exact formula for the free energy of an oscillator coupled to a heat bath in thermal equilibrium at temperature T. This formula, and its later extension to three dimensions to incorporate a magnetic field, has proved to be invaluable in analyzing problems in quantum thermodynamics. Here, we address the question raised in our title viz. Nernst's third law of thermodynamics

    An Introduction to the Source Concept for Antennas

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    Antenna parameters particularly relevant to electrically small antenna design are reviewed in this paper. Source current definitions are accentuated leading to the introduction of the source concept which advantageously utilize only spatially bounded quantities. The framework of the source concept incorporates powerful techniques such as structural and modal decomposition, operator’s inversion and current optimization, thus opening new, challenging possibilities for antenna design, analysis and synthesis

    Upper bounds on absorption and scattering

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    A general framework for determining fundamental bounds in nanophotonics is introduced in this paper. The theory is based on convex optimization of dual problems constructed from operators generated by electromagnetic integral equations. The optimized variable is a contrast current defined within a prescribed region of a given material constitutive relations. Two power conservation constraints analogous to optical theorem are utilized to tighten the bounds and to prescribe either losses or material properties. Thanks to the utilization of matrix rank-1 updates, modal decompositions, and model order reduction techniques, the optimization procedure is computationally efficient even for complicated scenarios. No dual gaps are observed. The method is well-suited to accommodate material anisotropy and inhomogeneity. To demonstrate the validity of the method, bounds on scattering, absorption, and extinction cross sections are derived first and evaluated for several canonical regions. The tightness of the bounds is verified by comparison to optimized spherical nanoparticles and shells. The next metric investigated is bi-directional scattering studied closely on a particular example of an electrically thin slab. Finally, the bounds are established for Purcell's factor and local field enhancement where a dimer is used as a practical example.Comment: 38 pages, 16 figure

    On apparent breaking the second law of thermodynamics in quantum transport studies

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    We consider a model for stationary electronic transport through a one-dimensional chain of two leads attached to a perturbed central region (quantum dot) in the regime where the theory proposed recently by Capek for a similar model of phonon transport predicts the striking phenomenon of a permanent current between the leads. This result based on a rigorous but asymptotic Davies theory is at variance with the zero current yielded by direct transport calculations which can be carried out in the present model. We find the permanent current to be within the error of the asymptotic expansion for finite couplings, and identify cancelling terms of the same order.Comment: 5 pages, 3 figure

    Characteristic modes – progress, overview, and emerging topics

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    Over the past decade, characteristic mode analysis (CMA) research has grown from a niche topic to a mainstream topic, warranting a tutorial-style special issue to survey the significant progress that has been made in this field. In thisintroductory article (PAPER 1), the focus is on providing the big picture. We start with a simple description of characteristic modes. Next, we examine the trends in this field, followed by providing further insights into CMA’s historical development. We will also address common myths surrounding the subject. Then, leaving the detailed coverage of major topics to the following papers, we summarize recent applications of CMA in scattering and other emerging topics. Finally, we conclude with some future perspectives on this field
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