Conserved quantities (IFCS), Darvas lectures

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Kötelezően választható társadalomtudományi tárgyak

MEGMARADÓ MENNYISÉGEK A MODERN FIZIKA TÖRTÉNETÉBEN
Ajánlott szakok:	fizikus, fizika, csillagász, geofizikus, vegyész, matematikus szak számára, MS
Kód:	xxxn9058/1
Heti óraszám	2+0
Ajánlás szintje:	választható tárgy
Előadó	Darvas György , megbízott előadó, Symmetrion

Előismeretek	Tematika Conserved Quantities: in English	Számonkérés módja
Hírek, információk		Irodalom

Vissza

A Tantárgy Részletes Leírásához

MEGMARADÓ MENNYISÉGEK
A MODERN FIZIKA TÖRTÉNETÉBEN
Az izotóp tértöltés megmaradásához vezetõ út

Heti 2 órás előadás, amely SPECIÁLIS előadásként vehető fel.

Előadó:

Darvas György, megbízott külső előadó

Helye:

Ideje: szerda 17.45-19.15

Kezdés: 2014. február 12. szerda

Ajánlás:

Elsõsorban fizikus, vagy fizikához kapcsolódó szakos hallgatóknak ajánlom, akik érdeklődést mutatnak részecskefizika, vagy térelméletek és ezekhez kapcsolódó témáknak a fizikán túlmutató háttere, története iránt. Felveheti bármely felsõbb évfolyamos, MS hallgató.

Előismeretek:

A téma feltételezi a tematikához kapcsolódó fizikai alapkurzusok elvégzését, és a XX. századi fizika története iránti érdeklõdést.

Számonkérés:

Szóbeli kollokvium.

Tematika:

BEVEZETÉS: FIZIKAI SZIMMETRIÁK, SZUPERSZIMMETRIÁK ÉS MEGMARADÁSI TÉTELEK

1. AZ IZOTÓP TÉRTÖLTÉS SPIN (IFCS) MODELL

1.1 Az izotóp tértöltés spin (isotopic field-charge spin: IFCS) modell elõtörténete

1.2 Szimmetriaelvek szerepe a tudományos gondolkodás történetében
- a XVIII-XIX. sz. fizika princípiumai (elvei),
- megmaradási törvények és szimmetriaelvek,
- F. Klein, S. Lie, E. Noether, H. Weyl, Utiyama, Pauli, Heisenberg, Wigner, C.N. Yang, ‘t Hooft, Nambu, Gell-mann és Ne’eman, S. Weinberg, Higgs, és … hozzájárulása

1.3 A spin megmaradás története

1.4 Analóg jelenségek: spin-szerû mennyiségek

1.5 Az izotóp spin fogalma és megmaradása történeti összefüggésében (az 1930-as évektõl a Yang-Mills modellig és tovább)

1.6 Szimmetria és szimmetria-sértés az elektromos töltések közti kölcsönhatás leírásának történetében

1.7 Izotóp tértöltések (IFC) megkülönböztetése

1.7.1 A súlyos és a tehetetlen tömeg megkülönbözetése a fizika történetében

1.7.2 Izotóp elektromos töltések megkülönböztetése

1.8 Az izotóp tértöltések kicserélodésének fenomenológkus modellje

1.9 Egy szimmetria sérülése és a harmónia helyreállítása egy másik szimmetriával kombinálva

1.10 Az izotóp tértöltés spin (IFCS) fizikai fogalma

1.11 Az IFCS megmaradása

1.12 Hogyan változtatta meg az izotóp tértöltés spin invarianciája fizikai világképünket

2. AZ ELEKTROMÁGNESES KÖLCSÖNHATÁS IFCS MODELLJE

2.1 A kvantumelektrodinamika (QED) korai története (1929-1932)

2.2 C. Moeller elektromágnese kölcsönhatás modelljének aszimmetriája és annak “szimmetrizálása” (H. Bethe and E. Fermi, 1932)

2.3 Dirac kiegészítései a QED-hoz (1951, 1962)

2.4 Dirac QED egyenletének kibõvítése az izotóp tértöltéssel

2.5 A kibõvített Dirac egyenlet elemzése

2.6 A kibõvített Dirac egyenlet következményei

3. A GRAVITÁCIÓS KÖLCSÖNHATÁS IFCS MODELLJE

3.1 A gravitáció elmélete és az általános relativitáselmélet

3.2 Az általános relativitáselmélet geometriái (Riemann, Finsler)

3.3 Ekvivalencia és azonosság különbözõségérõl filozófiai megközelítésben. Mit nem jelent az ekvivalencia elve?

3.4 A gravitációs egyenlet a(z izotóp) súlyos és tehetetlen tömeg megkülönböztetésével

3.5 A módosított gravitációs egyenlet megoldásának várható változásai

4. AZ IFCS MODELL PERSPEKTÍVÁI

4.1 Kalandozás a Standard Modellen túl

4.2 A szuperszimmetrikus modell egy alternatívája

4.3 Lehetséges új közvetítõ bozonok elõrejelzése

Tankönyv: G. Darvas (2014) Another Version of Facts. On Physical Interactions, 134 p.

Ajánlott olvasnivaló:
http://arxiv.org/abs/0811.3189v1
http://www.springerlink.com/content/g28q43v2112721r1/
http://link.springer.com/article/10.1007/s10773-013-1693-1
http://link.springer.com/article/10.1007%2Fs10773-013-1781-2

Conserved Quantities in the History of Modern Physics:
The road to the conservation of the isotopic field-charge spin (IFCS)

Lecture themes

Motto:
The physicist Leo Szilard once announced to his friend Hans Bethe that he was thinking of keeping a diary:
“ I don't intend to publish. I am merely going to record the facts for the information of God.”
“ Don't you think God knows the facts?” - Bethe asked.
“ Yes,” said Szilard,
“ He knows the facts, but He does not know this version of the facts.”

INTRODUCTION: PHYSICAL SYMMETRIES, SUPERSYMMETRIES AND CONSERVATION LAWS

1. THE ISOTOPIC FIELD-CHARGE SPIN MODEL

1.1 Prehistory of the isotopic field-charge spin (IFCS) model

1.2 The role of symmetry principles in the history of sientific thinking
- “principles” of the 18-19th c. physics,
- conservation laws and symmetry principles,
- contributions by F. Klein, S. Lie, E. Noether, H. Weyl, Utiyama, Pauli, Heisenberg, Wigner, C.N. Yang, ‘t Hooft, Nambu, Gell-mann and Ne’eman, S. Weinberg, Higgs, and …

1.3 History of the spin conservation

1.4 Analogue phenomena: Spin-like quantities

1.5 The concept of the isotopic spin and its conservation in historical context (from the 1930-ies to the Yang-Mills model and further)

1.6 Symmetry and symmetry violation in the history of the description of interaction between electric charges

1.7 Distinction between isotopic field-charges (IFC)

1.7.1 Distinction between the masses of gravity and inertia in the history of physics

1.7.2 Distinction between isotopic electric charges

1.8 Phenomenological model of the commutation between the isotopic field-charges

1.9 Loss of a symmetry and recovery of the harmony by another

1.10 The physical concept of the isotopic field-charge spin (IFCS)

1.11 Conservation of the IFCS

1.12 How did our physical world view change as a result of the isotopic field-charge spin invariance

2. THE IFCS MODEL OF THE ELECTROMAGNETIC INTERACTION

2.1 History of QED (1929-1932)

2.2 Asymmetry in the electromagnetic interaction model by C. Moeller and its “symmetrisation” by H. Bethe and E. Fermi (1932)

2.3 Extensions of QED by Dirac (1951, 1962)

2.4 IFC extension of the Dirac equation of QED

2.5 Discussion of the extended Dirac equation

2.6 Consequences of the extended Dirac equation

3. THE IFCS MODEL OF THE GRAVITATIONAL INTERACTION

3.1 The theory of gravitation and the General Theory of Relativity

3.2 Geometries of the GTR (Riemann, Finsler)

3.3 Philosophical considerations on the difference between equivalence and identity. What does not mean the equivalence principle?

3.4 The gravitational equation with the distinction between the (isotopic) gravitational and inertial masses

3.5 Expected changes in the solutions of the modified gravitational equation

4. PERSPECTIVES OF THE IFCS MODEL

4.1 Adventures beyond the Standard Model

4.2 An alternative to the supersymmetric model

4.3 Prediction of possible new mediating bosons

Textbook: G. Darvas (2014) Another Version of Facts. On Physical Interactions, 134 p.

Proposed reading:
http://arxiv.org/abs/0811.3189v1
http://www.springerlink.com/content/g28q43v2112721r1/
http://link.springer.com/article/10.1007/s10773-013-1693-1
http://link.springer.com/article/10.1007%2Fs10773-013-1781-2

______________________________

INTRODUCTION to the Textbook

This book treats fundamental physical interactions starting from two preliminary assumptions.

(a) Although mass of gravity and mass of inertia are equivalent quantities in their measured values, they are qualitatively not identical physical entities. We will take into consideration this difference in our equations.
Later we will extend this ‘equivalence is not identity’ principle to sources of further fundamental interaction fields, other than gravity.

(b) Physical interactions occur between these qualitatively different entities.

These two assumptions do not contradict to any known physical theory, however, they allow another interpretation of facts built in our explanations of physical experience.

First we interpret the mentioned preliminary assumptions. Then we will sketch in main lines a picture of fundamental physical fields influenced by the distinction between the two qualitative forms of the individual field-charges and interaction between them. A next part will demonstrate the existence of an invariance between the two isotopic forms of the field charges, and will formulate certain consequences in our view on the physical structure of matter. Finally we will discuss how can these results potentially change our approach to a few open questions of physics, including the effects of a family of intermediate bosons to be predicted by the proven invariance between the assumed isotopic states of the individual field charges.

The proposed conceptual framework and assumption on the interaction mechanism goes beyond the Standard Model (SM). Many physicists are convinced that SM does not hold eternally alone and is not untranscendable; there will appear new, more precise theories that will partially include the SM, and answer those questions that are left open by the SM. However we do not certainly know how, at least at present.

CERN organised three workshops to discuss possible theoretical candidate models beyond the SM to base a “new physics” in accordance with fine scale anomalies and symmetry breakings in high energy experiments, in 2005-2007 (CERN workshop, 2008a; CERN workshop, 2008b; CERN workshop, 2008c). They agreed that SM holds, it needs only some extensions. So do we as well. Section IV of the present work provides an alternative extension theory, still not discussed in those three working group reports.

This work (started in January 2001) is an attempt to exceed a couple of the limits of the Standard Model. Gerard ‘t Hooft expressed his view on the physics after the SM: “What is generally expected is either a new symmetry principle or possibly a new regime with an altogether different set of physical fields.” ( See in: Hooft, 2005, Sec. 12). The isotopic field charge spin conservation and the D field, being introduced in this book, are candidates (Darvas, 2011).

The presented idea is based on the same facts like those considered in the SM, only on “another version” of them. It clusters the observations in another way. Unlike existing alternative theories, e.g., the SUSY, which renders a new (“supersymmetric”) brother to each particle, this model clusters the observed sources of fields in two-eggs twin pairs, regarding them as isotopic states of each other, and there is left “only” the twin brothers of the bosons mediating their interactions to be observed. It covers gravitational, electroweak and strong interactions. In contrast to the SUSY, which renders fermion-boson pairs as new-born brothers to each other, the Isotopic Field Charge Spin (IFCS) assumption, proposed in the present work, renders fermion-fermion and boson-boson twins to each other.

This assumption does not assume new fermions; the twin brothers of fermions originate in splitting the existing ones. Fermions split as a result of a newly interpreted property. The assumption is mathematically based (Darvas, 2009) on an invariance of interactions under rotation of the isotopic field charges’ spin (a property that distinguishes the field charge twins from each other) in a still hypothetical gauge field, that means, on the conservation of the isotopic field charge spin.

The bosonic twin brothers should appear as the quanta of the D field (cf., Section IV.3.2) that mediate between the split fermion states, that means, between isotopic states of field charges. The prediction of bosonic twin brothers will be discussed in Section IV.3.5.

The IFCS assumption theory does not give a clue to everything, (e.g., mass). It is a modest attempt to answer a few open questions of contemporary physics (Darvas, 2011).

Section I provides a conceptual introduction to the theme, Section II treats the introduced concepts in classical approaches and conjectures interaction between isotopic states of field charges, while the next one (III) discusses historical roots of the topic and their approaches from classical through quantum physics to field theories. Appearance of two different variants of the individual field charges in our physical equations would cause so far not experienced distortion in symmetries, unless another invariance does not counterbalance the apparently lost symmetries in our laws of nature. Section IV demonstrates the existence of this invariance, presents its exact mathematical proof and the physical consequences in field theory, then Section V derives conclusions.

Irodalom:

Kötelező:

G. Darvas (2014) Another Version of Facts. On Physical Interactions, 134 p.

Ajánlott:

http://arxiv.org/abs/0811.3189v1
http://www.springerlink.com/content/g28q43v2112721r1/
http://link.springer.com/article/10.1007/s10773-013-1693-1
http://link.springer.com/article/10.1007%2Fs10773-013-1781-2
+ A tanköny végén található irodalomjegyzék

Hirek, információk:

Utolsó frissítés: 2013.november 21.

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