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Joel M. Moss

Joel M. Moss 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 Joel M. Moss rather than just read about it. In short: Joel Marshall Moss (born November 29, 1942) is an American experimental nuclear physicist. Education and career Moss received his bachelor's degree from Fort Hays State University in 1964 and his doctorate in physics from the University of California, Berkeley in 1969.

Key takeaways

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

Reference excerpt

Joel Marshall Moss (born November 29, 1942) is an American experimental nuclear physicist.

Education and career Moss received his bachelor's degree from Fort Hays State University in 1964 and his doctorate in physics from the University of California, Berkeley in 1969. As a postdoc he was from 1969 to 1971 a research associate at the Saclay Nuclear Research Centre and from 1971 to 1973 an instructor in physics at the University of Minnesota. He was from 1973 to 1978 an assistant professor and from 1978 to 1980 associate professor at Texas A&M University. There he studied giant resonances of atomic nuclei with Texas A&M's cyclotron and introduced a new technique of focal plane polarimetry using a high-efficiency, high-resolution polarimeter in conjunction with an Enge split-pole spectrograph. In 1979 he became a researcher in the physics division of Los Alamos National Laboratory (LANL), where he developed and applied his technique of focal plane polarimetry at Los Alamos Meson Physics Facility (LAMPF) and also at the cyclotron of Indiana University. For example, he used his polarimetry technique to search (unsuccessfully) for collective pion excitations in nuclei in spin-sensitive experiments. At LANL he was steadily promoted: Leader of the Nuclear Physics Group from 1982 to 1984, Leader from of the Medium Energy Physics Group from 1984 to 1987, Deputy Division Leader of the Medium Energy Physics Group from 1987 to 1993, and Program Director of Nuclear and Particle Physics from 1988 to 1990. In 1986 Moss became the spokesperson for the E772 experiment at Fermilab, which involved dimuon production (i.e. of muon pairs via a Drell–Yan process and from charmonium decays) in high-energy proton-nucleus collisions with 800 GeV protons at the Tevatron. In particular, they obtained information about the antiquark distribution of sea quarks in the nucleons in the nuclei of hydrogen and deuterium targets and were able to study their dependence on the mass number of the nucleus. There was no mass-number-dependent modification (i.e. a different behavior of nucleons in nuclei than in free nucleons), as was observed in 1983 in the EMC effect found in the European Muon Collaboration experiments on deep inelastic lepton scattering on nuclear targets. This was contrary to what was expected from the explanation of the EMC effect from pion effects (increased occurrence of antiquarks) in nuclei. E772 could not detect any such antiquark enhancement. In addition, the E772 science team gained evidence of charmonium and charm formation in nuclei from dimuon generation. He was also involved in experiments on deep inelastic scattering from nuclei and nucleons at Fermilab. He participated in experiments at the PHENIX detector of the RHIC heavy ion accelerator to study high-energy nuclear collisions and the spin structure of the nucleon. In 1983 Moss was elected a Fellow of the American Physical Society. In 1998 he received the Tom W. Bonner Prize in Nuclear Physics with citation:

"For his pioneering experiments using dimuon production in proton-nucleus interactions which demonstrate that there is no antiquark enhancement in nuclei, and which delineate the characteristics of charmonium and open charm production in nuclear systems.

References

Worked examples

Example 1 — a first encounter with Joel M. Moss

Start with the simplest possible case. Write down what Joel M. Moss 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 Joel M. Moss 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 Joel M. Moss 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 Joel M. Moss

In research
Joel M. Moss 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 Joel M. Moss 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
Joel M. Moss is common in secondary-school and first-year university syllabi. It links to neighbouring topics 1943 births, 20th-century American physicists, 21st-century American physicists, so understanding it makes those chapters shorter.
In everyday life
Look for Joel M. Moss 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 Joel M. Moss in 20 minutes

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

Frequently asked questions

What is Joel M. Moss in simple terms?

Joel Marshall Moss (born November 29, 1942) is an American experimental nuclear physicist. Education and career Moss received his bachelor's degree from Fort Hays State University in 1964 and his doctorate in physics from the University of California, Berkeley in 1969.

Why does Joel M. Moss 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 Joel M. Moss?

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 Joel M. Moss.

Tags

  • 1943 births
  • 20th-century American physicists
  • 21st-century American physicists
  • American experimental physicists
  • American nuclear physicists
  • Fellows of the American Physical Society
  • Fort Hays State University alumni
  • Living people
  • Los Alamos National Laboratory personnel
  • People associated with Fermilab
  • Texas A&M University faculty
  • University of California, Berkeley alumni

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