Age, Biography and Wiki
Solomon Pekar was born on 16 March, 1917 in Kyiv, Ukraine. Discover Solomon Pekar's Biography, Age, Height, Physical Stats, Dating/Affairs, Family and career updates. Learn How rich is He in this year and how He spends money? Also learn how He earned most of networth at the age of 68 years old?
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Age |
68 years old |
Zodiac Sign |
Pisces |
Born |
16 March, 1917 |
Birthday |
16 March |
Birthplace |
Kyiv, Ukraine |
Date of death |
(1985-07-08) Kyiv, Ukraine |
Died Place |
Kyiv, Ukraine |
Nationality |
Ukraine |
We recommend you to check the complete list of Famous People born on 16 March.
He is a member of famous with the age 68 years old group.
Solomon Pekar Height, Weight & Measurements
At 68 years old, Solomon Pekar height not available right now. We will update Solomon Pekar's Height, weight, Body Measurements, Eye Color, Hair Color, Shoe & Dress size soon as possible.
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Dating & Relationship status
He is currently single. He is not dating anyone. We don't have much information about He's past relationship and any previous engaged. According to our Database, He has no children.
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Solomon Pekar Net Worth
His net worth has been growing significantly in 2022-2023. So, how much is Solomon Pekar worth at the age of 68 years old? Solomon Pekar’s income source is mostly from being a successful . He is from Ukraine. We have estimated
Solomon Pekar's net worth
, money, salary, income, and assets.
Net Worth in 2023 |
$1 Million - $5 Million |
Salary in 2023 |
Under Review |
Net Worth in 2022 |
Pending |
Salary in 2022 |
Under Review |
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Not Available |
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Timeline
After WWII Pekar established a Chair in theoretical physics in the T. G. Shevchenko Kiev University and undergraduate and graduate programs in this field. In 1960, together with V. E. Lashkaryov, Pekar established in Kiev the Institute of Semiconductor Physics of the Ukrainian Academy of Sciences. This Academy awards the Pekar Prize in theoretical physics.
In his 1957 paper, Pekar advanced a theory of electromagnetic waves near exciton resonances currently known as polaritons. He predicted existence of new (additional, or Pekar) light waves due to a small effective mass of electronic excitons. Small mass translates into a large curvature of the polariton spectrum and additional roots for the momentum at a given wave frequency. Inclusion of the additional waves into the classical crystal optics requires additional boundary conditions onto the mechanical and electromagnetic components of polaritons. These waves were observed experimentally and certified as a discovery. An important prediction of Pekar’ theory is violation of the Kramers-Kronig relation in polariton resonances because the real part of dielectric function is controlled by the oscillator strength of polariton transition (or the splitting between the upper and lower polariton branches) while the imaginary part of it by the decay of polaritons. This prediction of the theory is supported by the low-temperature spectrum of the first exciton-polariton band of naphthalene crystals. A phenomenological theory of additional waves has been developed in the framework of the crystal optics with spatial dispersion.
In 1941 Pekar submitted his Candidate of Science thesis on nonlinear theory of semiconductor rectifiers for which he was awarded Doctor of Science Degree, this work was strongly approved by Lev Landau. In 1946, Pekar developed a concept of a polaron and coined this term. The model developed in this paper is macroscopic and based on electrostatic coupling of an electron to polar optical phonons. This coupling results in dressing of the electron by a cloud of virtual phonons and renormalization of its energy spectrum. In the strong coupling limit, polaron binding energy was found by Pekar, and its effective mass is described by the Landau-Pekar formula. While polaron moves freely across the crystal, a term self-trapping is sometimes used for forming polarons. Landau's original idea of trapping electrons by crystal lattice was based on producing by them color centers (F-centers) which consist of an electron tightly bound to a lattice defect rather than polarons as quasiparticles freely moving across the crystal and consisting of an electron dressed by a phonon cloud. Pekar’s macroscopic model of polarons became a field theory without singularities, and was afterwards applied to weak and intermediate electron-phonon coupling. Further generalizations included coupling of electrons to acoustic phonons and magnons, excitonic polarons, polarons in low-dimensional systems, and bipolarons. Methods of polaron theory were applied to the theory of optical spectra of impurity centers where the distribution of the intensities of phonon satellites is known as Pekarian. Concept of polarons and bipolarons penetrated also into the field of superconductivity, especially as applied to the phase transition between the BCS (Bardeen, Cooper, Schrieffer) and Bose-Einstein phases.
Solomon Isaakovich Pekar (Ukrainian: Соломон Ісаакович Пекар; Russian: Соломон Исаакович Пекар; 16 March 1917 – 8 July 1985) was a Soviet theoretical physicist, born in Kyiv, Ukraine. He was a full Member of the Ukrainian Academy of Sciences and is known for his fundamental contributions to condensed matter physics, especially for introducing and advancing the concept of polaron as a charge carrier in solids.