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Marvin L. Cohen

Marvin L. Cohen 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 Marvin L. Cohen rather than just read about it. In short: Marvin Lou Cohen (born March 3, 1935) is an American–Canadian theoretical physicist. He is a physics professor at the University of California, Berkeley.

Marvin L. Cohen — main illustration
Marvin L. Cohen — illustration

Key takeaways

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

Reference excerpt

Marvin Lou Cohen (born March 3, 1935) is an American–Canadian theoretical physicist. He is a physics professor at the University of California, Berkeley. Cohen is an expert in the field of condensed matter physics. He is widely known for his seminal work on the electronic structure of solids.

Biography

Early life and education Cohen was born in Montreal, Quebec, Canada. His parents Elmo and Molly (Zaritsky) Cohen were both born in Montreal and his grandparents, all of Jewish descent, emigrated to Canada from the Baltic states and Russia. He, together with his parents and younger brother, Gordon, moved to San Francisco, California, in 1947, where he attended Roosevelt Junior High School and George Washington High School. He was naturalized a U.S. citizen, November 1953. He attended the University of California, Berkeley, for an A.B. in physics in 1957 and the University of Chicago with a M.S. in physics in 1958 and a Ph.D. in physics completed 1963, conferred 1964. His Ph.D. thesis advisor was James C. Phillips.

Career

From 1963 to 1964, Cohen was a member of the technical staff with a postdoctoral position in the theoretical physics group at Bell Laboratories, Murray Hill, New Jersey, where his mentors were primarily Philip W. Anderson and Conyers Herring. He joined the faculty of the University of California, Berkeley in 1964 (assistant professor of physics 1964–66; associate professor 1966–69; professor 1969–1995; university professor 1995–present; professor of the graduate school, 2010–present.) He supervised approximately fifty graduate students and fifty postdoctoral researchers since 1964. He was president of the American Physical Society in 2005.

Personal life Marvin Cohen is married to Suzy Locke Cohen who is an Art Advisor. Cohen and his late wife Merrill Leigh Gardner Cohen (deceased 1994) had a son and a daughter. He has three grandchildren. Cohen has played the clarinet since age 13.

Research One of the most influential and broadest advances in the study of the physics of materials in the last fifty years is the use of computational tools to explain and predict properties of materials. Marvin Cohen has been honored for his creation of physical models and computational methods and applications that made a large fraction of these advances possible. This approach is often referred to as the "Standard Model" for computing properties of solids, and this work played an important part in the creation and development of the field of computational physics. The successful predictions of new materials and material properties have led to new insights in fundamental science, the production of useful materials, and the creative manipulations of known materials. An essential and standard tool is the availability of accurate electronic band structures for materials ranging from ceramics to metals, and the models and method mentioned above have made the use of electronic band structures and related calculations ubiquitous in pure and applied condensed matter physics. For electronic structure, in the mid 1960's it became possible to use pseudopotentials for accurately computing band structures for 14 semiconductors at a time when little was known about their electronic structure. This advance was revolutionary as it explained optical properties of semiconductors in the visible and UV range and led to the first pictures of electron density and bonds in semiconductors. These results were later confirmed experimentally. This work also led to the creation of the field of surface calculations of electronic structure using the invention of the supercell. This was followed by the development of a total energy scheme which initiated a new era of first principles predictions of structural, vibrational, and high-pressure properties of solids using only atomic numbers and atomic masses as input. For superconductivity, there were successes in the prediction of superconductivity in doped semiconductors, the prediction of the first superconducting oxide, and the confirmation of the ab initio proposed existence of two new high-pressure phases of silicon and their properties including the successful prediction of their superconducting properties. In the area of nanostructures, it was shown that the methods used for calculating bulk and surfaces properties were applicable for studies of nanoscale materials such as the C60, carbon nanotubes, and other low dimensional structures. These studies led to the successful prediction of the existence the boron nitride nanotube and its properties. Seminal studies were done explaining and predicting properties of graphene nanoribbons and their energy gaps, and the properties of layered systems of graphene and BN sheets were calculated suggesting a path for fabrication of useful electronic materials. The first theoretical and experimental studies of the electronic and vibrational properties of one-dimensional isolated chains were done, and the underlying physics was determined for controlling the size and shape of 2D nanopores with applications for DNA sequencing, sieving, and quantum emission. Another nanoscience contribution was an important study of the physics of metallic clusters using electronic energies to explain their size abundances, referred to as "magic numbers". The methods developed for the above studies are numerous. Some examples include the empirical pseudopotential method, ab initio pseudopotentials, supercells for surfaces and localized configurations, a method for calculating the total energy of solids, the creation of an empirical formula used to obtain the bulk moduli of many semiconductors and insulators, and the development of a method for calculating electron-phonon interactions using Wannier functions. These approaches and others first developed for this research are now used worldwide.

… excerpt ends here. Continue reading the full article.

Illustrations

Marvin L. Cohen illustration

Worked examples

Example 1 — a first encounter with Marvin L. Cohen

Start with the simplest possible case. Write down what Marvin L. Cohen 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 Marvin L. Cohen 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 Marvin L. Cohen 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 Marvin L. Cohen

In research
Marvin L. Cohen 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 Marvin L. Cohen 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
Marvin L. Cohen is common in secondary-school and first-year university syllabi. It links to neighbouring topics 1935 births, 20th-century American physicists, 21st-century American physicists, so understanding it makes those chapters shorter.
In everyday life
Look for Marvin L. Cohen 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 Marvin L. Cohen in 20 minutes

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

Frequently asked questions

What is Marvin L. Cohen in simple terms?

Marvin Lou Cohen (born March 3, 1935) is an American–Canadian theoretical physicist. He is a physics professor at the University of California, Berkeley.

Why does Marvin L. Cohen 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 Marvin L. Cohen?

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 Marvin L. Cohen.

Tags

  • 1935 births
  • 20th-century American physicists
  • 21st-century American physicists
  • Academics from Montreal
  • Benjamin Franklin Medal (Franklin Institute) laureates
  • Canadian expatriate academics in the United States
  • Fellows of the American Association for the Advancement of Science
  • Fellows of the American Physical Society
  • Living people
  • Members of the American Philosophical Society
  • Members of the United States National Academy of Sciences
  • National Medal of Science laureates

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