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Related Concept Videos

Nuclear Fission02:50

Nuclear Fission

Many heavier elements with smaller binding energies per nucleon can decompose into more stable elements that have intermediate mass numbers and larger binding energies per nucleon—that is, mass numbers and binding energies per nucleon that are closer to the “peak” of the binding energy graph near 56. Sometimes neutrons are also produced. This decomposition of a large nucleus into smaller pieces is called fission. The breaking is rather random with the formation of a large number of different...
Nuclear Transmutation03:20

Nuclear Transmutation

Nuclear transmutation is the conversion of one nuclide into another. It can occur by the radioactive decay of a nucleus, or the reaction of a nucleus with another particle. The first manmade nucleus was produced in Ernest Rutherford’s laboratory in 1919 by a transmutation reaction, the bombardment of one type of nuclei with other nuclei or with neutrons. Rutherford bombarded nitrogen-14 atoms with high-speed α particles from a natural radioactive isotope of radium and observed protons being...
Nuclear Stability03:18

Nuclear Stability

Protons and neutrons, collectively called nucleons, are packed together tightly in a nucleus. With a radius of about 10−15 meters, a nucleus is quite small compared to the radius of the entire atom, which is about 10−10 meters. Nuclei are extremely dense compared to bulk matter, averaging 1.8 × 1014 grams per cubic centimeter. If the earth’s density were equal to the average nuclear density, the earth’s radius would be only about 200 meters.
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Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
Radioactivity and Nuclear Equations03:18

Radioactivity and Nuclear Equations

Nuclear chemistry is the study of reactions that involve changes in nuclear structure. The nucleus of an atom is composed of protons and, except for hydrogen, neutrons. The number of protons in the nucleus is called the atomic number (Z) of the element, and the sum of the number of protons and the number of neutrons is the mass number (A). Atoms with the same atomic number but different mass numbers are isotopes of the same element.
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Isotopes and Radioisotopes01:28

Isotopes and Radioisotopes

In the early 1900s, English chemist Frederick Soddy realized that an element could have atoms with different masses that were chemically indistinguishable. These different types are called isotopes — atoms of the same element that differ in mass. Isotopes differ in mass because they have different numbers of neutrons but are chemically identical because they have the same number of protons. Soddy was awarded the Nobel Prize in Chemistry in 1921 for this discovery.
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Related Experiment Video

Updated: Jul 2, 2026

Preparing an Isotopically Pure 229Th Ion Beam for Studies of 229mTh
10:42

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Published on: May 3, 2019

Nuclear susceptibility thermometry using enriched (119)Sn.

J Babcock1, J Kiely, T Manley

  • 1School of Physics and Astronomy, University of Minnesota, Minneapolis, Minnesota 55455.

The Review of Scientific Instruments
|October 1, 1979
PubMed
Summary

Highly enriched 119Sn was used for static nuclear susceptibility thermometry. This new thermometer demonstrates accurate linearity in the 2-15 mK range, offering ease of use and rapid response for low-temperature measurements.

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Area of Science:

  • Low-temperature physics
  • Condensed matter physics
  • Metrology

Background:

  • Accurate thermometry below 10 mK is crucial for fundamental research.
  • Existing methods can be complex or lack precision in this range.
  • Nuclear susceptibility thermometry offers a promising alternative.

Purpose of the Study:

  • To evaluate the performance of enriched 119Sn for static nuclear susceptibility thermometry.
  • To calibrate the 119Sn thermometer in the millikelvin range.
  • To assess its practical usability for low-temperature measurements.

Main Methods:

  • Utilizing 84.5% enriched 119Sn for static nuclear susceptibility measurements.
  • Calibrating the thermometer against known temperature points in the 2-40 mK range.
  • Analyzing the linearity of the thermometer's response with respect to temperature.

Main Results:

  • The 119Sn thermometer exhibits accurate linearity in the 2-15 mK range.
  • The thermometer is characterized by its ease of use.
  • Rapid response times were observed, indicating efficient thermal coupling.

Conclusions:

  • Enriched 119Sn is a viable and effective material for static nuclear susceptibility thermometry.
  • This thermometer provides a reliable and practical tool for measurements in the low millikelvin range.
  • Its performance characteristics make it suitable for various low-temperature experimental applications.