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Mihai Gavrilă

Mihai Gavrilă 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 Mihai Gavrilă rather than just read about it. In short: Mihai Gavrilă (Romanian pronunciation: [miˈhaj ɡaˈvrilə]; b. October 16, 1929, Cluj) is a Romanian quantum physicist and a corresponding member of the Romanian Academy since 1974.

Mihai Gavrilă — main illustration
Mihai Gavrilă — illustration

Key takeaways

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  • Reproduce the core statement of Mihai Gavrilă from memory before moving on to harder problems.

Reference excerpt

Mihai Gavrilă (Romanian pronunciation: [miˈhaj ɡaˈvrilə]; b. October 16, 1929, Cluj) is a Romanian quantum physicist and a corresponding member of the Romanian Academy since 1974. He made fundamental contributions to the quantum theories of electromagnetic interactions with atoms.

Education His parents were Ion and Florica Gavrilă (née Vișoiu). His father taught medicine and his mother taught English at the University of Cluj. He began his higher education at the Gheorghe Lazăr High School in Sibiu, and completed his studies at the Seminarul Pedagogic Universitar of the University of Cluj. Then, in 1948, he enrolled in the School of Mathematics and Physics at the University of Bucharest, from which he graduated in 1953 with a major in physics, and a minor in radiotechnology. While still a student, between 1951 and 1953, he became a teaching assistant to Professor Eugen Bădărău in the Optics Laboratory of the School of Physics.

Doctoral studies In 1953, Gavrilă was accepted for doctoral studies in theoretical physics by Professor Șerban Țițeica in the School of Physics at the University of Bucharest. He completed successfully his doctoral studies with a Ph.D. thesis entitled The Relativistic Theory of the Photoelectric Effect, building on work of Albert Einstein and Alexandru Proca. He published in 1959 the main results of his Ph.D. thesis in a peer-reviewed paper in Physical Review.

Academic career In 1956, Gavrilă was appointed Assistant Professor in the Department of Thermodynamics, Statistical Physics and Quantum Mechanics of the School of Physics of the University of Bucharest, where he was subsequently promoted to Associate Professorsh in 1962, and to full Professor in 1968. He also studied as a visiting scholar at several major physics centers around the world: the Joint Institute for Nuclear Research in Dubna, Soviet Union, the Joint Institute for Laboratory Astrophysics in Boulder, Colorado, the International Centre for Theoretical Physics in Trieste, Italy, and the University of Pittsburgh, in Pittsburgh, Pennsylvania. He taught courses on Quantum mechanics, Group representations, and Lorentz group transformations. He was elected a corresponding Member of the Romanian Academy in 1974. However, in spite of his election to the Academy, he refused to become entangled in any political affairs under the increasingly dictatorial communist regime, and finally he had to leave his country for Norway in the autumn of 1974. At first, Gavrilă worked at the Norwegian University of Science and Technology in Trondheim) and at the Royal Institute of Technology (KTH), in Stockholm, Sweden. In 1975 he settled in Amsterdam at the FOM Institute for Atomic and Molecular Physics (AMOLF), where he became the theoretical physics group leader. Since 1992 he has worked as a Senior Scientist at the Institute for Theoretical Atomic, Molecular and Optical Physics (ITAMP) based at the Harvard–Smithsonian Center for Astrophysics, in Cambridge, Massachusetts. After 1990 he was able to visit Romania several times and continued to contribute also to the development of theoretical physics research in Romania.

Scientific achievements

Radiative transitions between the inner atomic shells Gavrilă completed in 1977 his previous work on the relativistic theory of the photoelectric effect in the inner atomic orbitals that he had begun in his Ph.D. thesis in 1958; thus, he applied radiative corrections to his previous calculations He also investigated two-photon excitations and the elastic photon scattering amplitude in the hydrogen ground state. He completed also the non-relativistic Compton scattering calculation for an electron in the K-shell These calculations were then extended in the dipolar approximation to the study of Compton scattering in the L- shell. The results of his investigations confirmed the presence of the infrared divergence—as predicted in quantum electrodynamics, and also predicted the presence of a resonance in the spectrum of the scattered photons.

Interactions of laser beams with atoms He began this research in 1976 in connection with experimental studies carried out at AMOLF by the group of Marnix van der Wiel. Initially, his interest was focused on multi-photon transitions treated by non-perturbation quantum theory. However, he switched to perturbation methods in quantum theory when it became possible experimentally to attain ultra-high laser intensities at very high frequencies based on the High-Intensity High-Frequency Floquet Theory (HI-HFFT). His investigations lead to very surprising results—the phenomenon of ``atomic dichotomy" in which the hydrogen atom when it is placed in a linearly polarized field exhibits a splitting of its spherical charge distribution into two lobes that oscillate in the laser field. On the other hand, in a circularly polarized laser field, the hydrogen atom's charge distribution takes on a toroidal shape with its symmetry axis oriented along the propagation vector of the field and passing through the center of the atom. His theory also predicts for two-electron atoms the appearance of a new bound state which is induced by the ultra-intense laser field; these are 'light-induced excited states'. Apparently paradoxical events do occur in the presence of the extremely intense laser field: a proton can bind more than two electrons thus leading to the formation of hydrogen negative ions with multiple negative charges that are relatively stable. Other novel and unexpected properties of molecules were also predicted in the presence of such ultra-intense laser fields.

Scientific leadership Gavrilă organized several international physics conferences, such as International Conference on Atomic Physics, International Conference on Photonic, Electronic, and Atomic Collisions, and International Conference on Multiphoton Processes. He was also a peer-reviewer for Physical Review A (1991–1993), Journal of Physics B and several other international physics journals. He also managed several projects financed by the European Union and Stichting FOM. He coordinated successfully the project Atoms in Super-intense, Femtosecond Pulses involving four experimental laboratories and theoretical groups from France, Belgium and the Netherlands, to build an ultra high-power laser at the Laboratoire d'Optique Appliquée in Palaiseau, France.

… excerpt ends here. Continue reading the full article.

Illustrations

Mihai Gavrilă illustration
Mihai Gavrilă: Atomic Dichotomy. The wave function of atomic hydrogen in a high frequency, ultra-high intensity laser field, represented in a plane passing through the symmetry axis of the laser field. 
  
    
      
        
          α
          
            0
          
        
        =
        
          I
          
            1
            
              /
            
            2
          
        
        
          ω
          
            −
            2
          
        
      
    
    {\displaystyle \alpha _{0}=I^{1/2}\omega ^{-2}}
  
, where 
  
    
      
        I
      
    
    {\displaystyle I}
  
 is the laser field intensity, and 
  
    
      
        ω
      
    
    {\displaystyle \omega }
  
 is its frequency in atomic units.
Atomic Dichotomy. The wave function of atomic hydrogen in a high frequency, ultra-high intensity laser field, represented in a plane passing through the symmetry axis of the laser field. α 0 = I 1 / 2 ω − 2 {\displaystyle \alpha _{0}=I^{1/2}\omega ^{-2}} , where I {\displaystyle I} is the laser field intensity, and ω {\displaystyle \omega } is its frequency in atomic units.

Worked examples

Example 1 — a first encounter with Mihai Gavrilă

Start with the simplest possible case. Write down what Mihai Gavrilă 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 Mihai Gavrilă 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 Mihai Gavrilă 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 Mihai Gavrilă

In research
Mihai Gavrilă 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 Mihai Gavrilă 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
Mihai Gavrilă is common in secondary-school and first-year university syllabi. It links to neighbouring topics 1929 births, Academic staff of the University of Bucharest, Corresponding members of the Romanian Academy, so understanding it makes those chapters shorter.
In everyday life
Look for Mihai Gavrilă 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 Mihai Gavrilă in 20 minutes

  1. Read the reference excerpt below once, without taking notes.
  2. Close the page and write down what Mihai Gavrilă 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 Mihai Gavrilă out loud to somebody else — or to Teacher Smith in the lgStudy chat.

Frequently asked questions

What is Mihai Gavrilă in simple terms?

Mihai Gavrilă (Romanian pronunciation: [miˈhaj ɡaˈvrilə]; b. October 16, 1929, Cluj) is a Romanian quantum physicist and a corresponding member of the Romanian Academy since 1974.

Why does Mihai Gavrilă 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 Mihai Gavrilă?

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 Mihai Gavrilă.

Tags

  • 1929 births
  • Academic staff of the University of Bucharest
  • Corresponding members of the Romanian Academy
  • Living people
  • Quantum physicists
  • Romanian emigrants to the Netherlands
  • Romanian nuclear physicists
  • Scientists from Cluj-Napoca
  • University of Bucharest alumni

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