Gregory Breit

Gregory Breit (RussianГригорий Альфредович Брейт-ШнайдерGrigory Alfredovich Breit-Shneider; July 14, 1899, MykolaivKherson Governorate – September 13, 1981, Salem, Oregon) was a Russian-born American physicist and professor at NYU (1929–1934), U. of Wisconsin–Madison (1934–1947), Yale (1947–1968), and Buffalo (1968–1973). In 1921, he was Paul Ehrenfest‘s assistant in Leiden.
https://en.wikipedia.org/wiki/Gregory_Breit

Gregory Breit was last modified: September 9th, 2018 by Jovan Stosic

David Bohm – Wikipedia

David Joseph Bohm FRS (/bm/; December 20, 1917 – October 27, 1992) was an American scientist who has been described as one of the most significant theoretical physicists of the 20th century and who contributed unorthodox ideas to quantum theoryneuropsychology and the philosophy of mind.

David Bohm
David Bohm.jpg
Born December 20, 1917
Wilkes-Barre, Pennsylvania, US
Died October 27, 1992(aged 74)
London, England, UK
Nationality American
Citizenship

  • American
  • Brazilian
  • British
Alma mater

Known for

Awards

Scientific career
Fields Theoretical physics
Institutions

Doctoral advisor Robert Oppenheimer
Doctoral students

Influences Albert Einstein
Jiddu Krishnamurti
Influenced

John Stewart Bell

Peter Senge

Bohm advanced the view that quantum physics meant that the old Cartesian model of reality – that there are two kinds of substance, the mental and the physical, that somehow interact – was too limited. To complement it, he developed a mathematical and physical theory of “implicate” and “explicate” order. He also believed that the brain, at the cellular level, works according to the mathematics of some quantum effects, and postulated that thought is distributed and non-localised just as quantum entities are.

Bohm warned of the dangers of rampant reason and technology, advocating instead the need for genuine supportive dialogue, which he claimed could broaden and unify conflicting and troublesome divisions in the social world. In this, his epistemologymirrored his ontology. Due to his Communist affiliations, Bohm was the subject of a federal government investigation in 1949, prompting him to leave the United States. He pursued his scientific career in several countries, becoming first a Brazilian and then a British citizen. He abandoned Marxism in the wake of the Hungarian Uprising in 1956.

Bohm’s main concern was with understanding the nature of reality in general and of consciousness in particular as a coherent whole, which according to Bohm is never static or complete but rather an unfolding process.

https://en.wikipedia.org/wiki/David_Bohm

David Bohm – Wikipedia was last modified: September 9th, 2018 by Jovan Stosic

Abraham Pais

Abraham Pais (/ps/; May 19, 1918 – July 28, 2000) was a Dutch-born American physicist and science historian. Pais earned his Ph.D. from University of Utrecht just prior to a Nazi ban on Jewish participation in Dutch universities during World War II. When the Nazis began the forced relocation of Dutch Jews, he went into hiding, but was later arrested and saved only by the end of the war.[2] He then served as an assistant to Niels Bohr in Denmark and was later a colleague of Albert Einstein at the Institute for Advanced Study in Princeton, New Jersey. Pais wrote books documenting the lives of these two great physicists and the contributions they and others made to modern physics. He was a physics professor at Rockefeller University until his retirement.
https://en.wikipedia.org/wiki/Abraham_Pais

Abraham Pais was last modified: September 9th, 2018 by Jovan Stosic

Arnold Nordsieck

Arnold Theodore Nordsieck (5 January 1911 – 18 January 1971) was an American theoretical physicist. He is best known for his work with Felix Bloch on the infrared problem in quantum electrodynamics. He developed the inertial electrostatic gyroscope (ESG) used as part of the inertial navigation system of nuclear submarines that allows them to remain underwater without having to surface to ascertain their location.
https://en.wikipedia.org/wiki/Arnold_Nordsieck

Arnold Nordsieck was last modified: September 9th, 2018 by Jovan Stosic

Nuclear magnetic resonance

Nuclear magnetic resonance (NMR) is a physical phenomenon in which nuclei in a strong static magnetic field are perturbed by a weak oscillating magnetic field (in the near field and therefore not involving electromagnetic waves) and respond by producing an electromagnetic signal with a frequency characteristic of the magnetic field at the nucleus. This process occurs near resonance, when the oscillation frequency matches the intrinsic frequency of the nuclei, which depends on the strength of the static magnetic field, the chemical environment, and the magnetic properties of the isotope involved; in practical applications with static magnetic fields up to ca. 20 tesla, the frequency is similar to VHF and UHF television broadcasts (60–1000 MHz). NMR results from specific magnetic properties of certain atomic nuclei. Nuclear magnetic resonance spectroscopy is widely used to determine the structure of organic molecules in solution and study molecular physicscrystals as well as non-crystalline materials. NMR is also routinely used in advanced medical imaging techniques, such as in magnetic resonance imaging (MRI).

All isotopes that contain an odd number of protons and/or neutrons (see Isotope) have an intrinsic nuclear magnetic moment and angular momentum, in other words a nonzero nuclear spin, while all nuclides with even numbers of both have a total spin of zero. The most commonly used nuclei are 1
H
 and 13
C
, although isotopes of many other elements (e.g. 2
H
6
Li
10
B
11
B
14
N
15
N
17
O
19
F
23
Na
29
Si
31
P
35
Cl
113
Cd
129
Xe
195
Pt
) have been studied by high-field NMR spectroscopy as well.

A key feature of NMR is that the resonance frequency of a particular simple substance is usually directly proportional to the strength of the applied magnetic field. It is this feature that is exploited in imaging techniques; if a sample is placed in a non-uniform magnetic field then the resonance frequencies of the sample’s nuclei depend on where in the field they are located. Since the resolution of the imaging technique depends on the magnitude of the magnetic field gradient, many efforts are made to develop increased gradient field strength.

The principle of NMR usually involves three sequential steps:

  • The alignment (polarization) of the magnetic nuclear spins in an applied, constant magnetic field B0.
  • The perturbation of this alignment of the nuclear spins by a weak oscillating magnetic field, usually referred to as a radio-frequency (RF) pulse. The oscillation frequency required for significant perturbation is dependent upon the static magnetic field (B0) and the nuclei of observation.
  • The detection of the NMR signal during or after the RF pulse, due to the voltage induced in a detection coil by precession of the nuclear spins around B0. After a RF pulse, precession usually occurs with the nuclei’s intrinsic Larmor frequency and, in itself, does not involve transitions between spin states or energy levels.

The two magnetic fields are usually chosen to be perpendicular to each other as this maximizes the NMR signal strength. The frequencies of the time-signal response by the total magnetization (M) of the nuclear spins are analyzed in NMR spectroscopy and magnetic resonance imaging. Both use applied magnetic fields (B0) of great strength, often produced by large currents in superconducting coils, in order to achieve dispersion of response frequencies and of very high homogeneity and stability in order to deliver spectral resolution, the details of which are described by chemical shifts, the Zeeman effect, and Knight shifts (in metals). The information provided by NMR can also be increased using hyperpolarization, and/or using two-dimensional, three-dimensional and higher-dimensional techniques.

NMR phenomena are also utilized in low-field NMR, NMR spectroscopy and MRI in the Earth’s magnetic field (referred to as Earth’s field NMR), and in several types of magnetometers.

https://en.wikipedia.org/wiki/Nuclear_magnetic_resonance

Nuclear magnetic resonance was last modified: September 9th, 2018 by Jovan Stosic

Shelter Island Conference

The first Shelter Island Conference on the Foundations of Quantum Mechanics was held from June 2–4, 1947 at the Ram’s Head Inn in Shelter Island, New York. Shelter Island was the first major opportunity since Pearl Harbor and the Manhattan Project for the leaders of the American physics community to gather after the war. As Julian Schwinger would later recall, “It was the first time that people who had all this physics pent up in them for five years could talk to each other without somebody peering over their shoulders and saying, ‘Is this cleared?'”

The conference, which cost $850, was followed by the Pocono Conference of 1948 and the Oldstone Conference of 1949. They were arranged with the assistance of J. Robert Oppenheimer and the National Academy of Sciences (NAS). Later Oppenheimer deemed Shelter Island the most successful scientific meeting he had ever attended; and as Richard Feynman recalled to Jagdish Mehra in April 1970: “There have been many conferences in the world since, but I’ve never felt any to be as important as this…. The Shelter Island Conference was my first conference with the big men…. I had never gone to one like this in peacetime.

https://en.wikipedia.org/wiki/Shelter_Island_Conference

Shelter Island Conference was last modified: September 9th, 2018 by Jovan Stosic