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Rudolf Muradyan

Rudolf Muradyan is a physics topic covered in the lgStudy science library. This page brings together a partial reference excerpt, illustrations, worked examples, real-world applications and a short study plan, so you can understand Rudolf Muradyan rather than just read about it. In short: Rudolf Muradovich Muradyan (Armenian: Ռուդոլֆ Մուրադի Մուրադյան; born 19 June 1936, Yerevan, Armenian SSR, USSR) is an Armenian theoretical physicist. Rudolf Muradyan's main research relate to theoretical physics, elementary-particle physics, cosmology and the origin of the Universe.

Rudolf Muradyan — main illustration
Rudolf Muradyan — illustration

Key takeaways

  • Rudolf Muradyan belongs to physics; place it in that map before memorising details.
  • Learn the definition first, then one example that makes the definition concrete.
  • Connect Rudolf Muradyan to a quantity you can measure, compute or draw — that is where exam questions come from.
  • Reproduce the core statement of Rudolf Muradyan from memory before moving on to harder problems.

Reference excerpt

Rudolf Muradovich Muradyan (Armenian: Ռուդոլֆ Մուրադի Մուրադյան; born 19 June 1936, Yerevan, Armenian SSR, USSR) is an Armenian theoretical physicist. Rudolf Muradyan's main research relate to theoretical physics, elementary-particle physics, cosmology and the origin of the Universe. Considering the properties of the interaction of elementary particles, he proposed the possibility of large-scale invariance in high-energy physics, from which the "Matveev-Muradyan-Tavkhelidze quark counting rule" is derived especially. He also researched the connection between the appearance of the Universe's rotation and magnetic fields and the cosmological constant. He is the recipient of the 1988 Lenin Prize, along with Albert Tavkhelidze and Viktor Matveev, for the discovery of dimensional quark counting rules.

Biography Rudolf Muradyan was born on June 19, 1936, in Yerevan, Armenia. After graduating from the Yerevan Secondary School № 25 in 1953, Muradyan entered the Faculty of Physics at Moscow State University in Moscow, graduating in 1959. In 1962 he finished his postgraduate study in the Faculty of Physics of Moscow State University and defended his thesis for a PhD in Physics and Mathematics. He then worked at the Laboratory of Theoretical Physics of the Joint Institute of Nuclear Research (OIJI) in Dubna near Moscow between 1962-1979 (from 1966 as a senior research fellow). In 1970 he was awarded a doctorate in physical-mathematical sciences and appointed professor. In 1972 he joined the Communist Party of the Soviet Union. His scientific papers appeared in Theoretical and Mathematical Physics. In 1970 at JINR he defended his thesis for the degree of Doctor of physical and mathematical sciences, and received the academic rank of professor.

In 1979 Rudolf Muradyan moved to Yerevan, he headed the Department of Radiation Studies of the Yerevan Physics Institute in 1979-1984. At the same time he gave special lectures on quantum theory of solids at the Faculty of Physics of Yerevan State University. In 1986 Muradyan was elected a corresponding member of the Academy of Sciences of the Armenian SSR.From 1984 to 1994 he worked at Byurakan Astrophysical Observatory of Armenian SSR Academy of Sciences (NAS RA) as a Leading Researcher and since 1985 he worked as a Team Leader. On October 16, 1994, he was elected an academician of the Pontifical Academy of Sciences. In the same year he moved again to Dubna and worked in the laboratory of theoretical physics of JINR until 1996. Since 1996 he was professor of the Institute of Physics of the Federal University of Bahia, Salvador, Brazil. In the same year he was elected an academician of the National Academy of Sciences of Armenia.

Scientific Work Rudolf Muradyan's main research is in theoretical physics, elementary particle physics, high-energy physics, cosmology and mathematical physics. In 1969, based on the quasi-free quark model, Rudolf Muradyan, together with Albert Tavkhelidze and Victor Matveev, proposed that the scaling properties of high-energy electron-nucleon interaction processes found in experiments are common to all deep inelastic lepton-hadron processes. Muradyan, Tavkhelidze and Matveev have developed an automodelicity (self-similarity) principle on the basis of which these properties may be derived directly. According to this principle, many characteristics of processes in the field of high energies and high momentum transfer, including particle form factors, do not depend on characteristic length and momentum scaling of dimensional parameters. They are homogeneous functions of relativistically invariant kinematical variables and a degree of homogeneity of these functions is determined by their physical dimensionality. A scale law describing the mass spectrum of muon pairs produced at high energies in proton ρ + ρ = μ + + μ − + {\displaystyle \rho +\rho =\mu ^{+}+\mu ^{-}+} hadrons collisions was first established using the principle of automodelicity:

d σ d M 2 ≈ 1 M 4 f ( M E ) {\displaystyle {\frac {d\sigma }{dM^{2}}}\approx {\frac {1}{M^{4}}}f\left({\frac {M}{E}}\right)}

Where M {\displaystyle M} is the effective mass of the muon pair and E {\displaystyle E} is the energy of the colliding particles. This sweeping law was confirmed in experimental studies begun in 1970 by Leon Lederman's group at Brookhaven. Subsequently, it was in these processes that a new class of hadrons - J / Ψ {\displaystyle J/\Psi } particles - were discovered. In 1973, based on the principle of self-similarity, the so-called "Matveev-Muradyan-Tavkhelidze quark counting rules" were established. They define the asymptotics of the form factors at large momentum transfer Q = − t {\displaystyle Q={\sqrt {-t}}} as well as the nature of the energy dependence of the differential cross section of an arbitrary binary scattering reaction at large angles at high energies E = s {\displaystyle E={\sqrt {s}}} :

… excerpt ends here. Continue reading the full article.

Illustrations

Rudolf Muradyan: Moscow State University
Moscow State University

Worked examples

Example 1 — a first encounter with Rudolf Muradyan

Start with the simplest possible case. Write down what Rudolf Muradyan claims or describes in one sentence, then invent the smallest concrete situation in which that sentence is true. In physics, the smallest case is usually a single object, a single equation or a single measurement. Check that every symbol or term in your sentence has a meaning in that case.

Example 2 — changing one variable

Take the situation from Example 1 and change exactly one quantity: double it, halve it, or set it to zero. Predict what should happen to Rudolf Muradyan before you calculate. Comparing your prediction with the result is the fastest way to find out whether you understand the idea or only the words.

Example 3 — an exam-style question

Typical questions about Rudolf Muradyan ask you to (a) state it precisely, (b) apply it to given data, and (c) explain a limitation. Practise writing all three answers in under five minutes; the third part is what separates a full-mark answer from an average one.

Applications of Rudolf Muradyan

In research
Rudolf Muradyan appears in physics research whenever the underlying quantities have to be modelled precisely. Papers usually cite it as a starting assumption and then explore where it breaks down.
In technology and industry
Engineering practice reuses Rudolf Muradyan in design rules, simulations and safety margins. Knowing the idea lets you read a specification sheet and understand why the numbers look the way they do.
In the classroom
Rudolf Muradyan is common in secondary-school and first-year university syllabi. It links to neighbouring topics 1936 births, Academic staff of the Federal University of Bahia, Armenian physicists, so understanding it makes those chapters shorter.
In everyday life
Look for Rudolf Muradyan outside the textbook — in sport, cooking, traffic, electronics or the sky above you. An example you found yourself is remembered far longer than one you were given.
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How to study Rudolf Muradyan in 20 minutes

  1. Read the reference excerpt below once, without taking notes.
  2. Close the page and write down what Rudolf Muradyan means in your own words.
  3. Compare your version with the excerpt and mark what you missed.
  4. Work through the three examples above with pen and paper.
  5. Explain Rudolf Muradyan out loud to somebody else — or to Teacher Smith in the lgStudy chat.

Frequently asked questions

What is Rudolf Muradyan in simple terms?

Rudolf Muradovich Muradyan (Armenian: Ռուդոլֆ Մուրադի Մուրադյան; born 19 June 1936, Yerevan, Armenian SSR, USSR) is an Armenian theoretical physicist. Rudolf Muradyan's main research relate to theoretical physics, elementary-particle physics, cosmology and the origin of the Universe.

Why does Rudolf Muradyan matter?

Because it connects several physics ideas at once: it gives you a definition you can apply, a quantity you can calculate, and a way to check whether a result is plausible.

How should I study Rudolf Muradyan?

Read the excerpt, restate it from memory, then work through the examples and applications listed on this page. The five-step study plan above takes about twenty minutes.

What does this page cover?

It gives you a compact reference excerpt plus original lgStudy explanations, examples, applications and study material on Rudolf Muradyan.

Tags

  • 1936 births
  • Academic staff of the Federal University of Bahia
  • Armenian physicists
  • Living people
  • Soviet emigrants to Brazil
  • Soviet physicists
  • Theoretical physicists

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