Barn (unit)

A barn (symbol: b) is a metric unit of area equal to (100  fm²). Originally used in nuclear physics for expressing the cross sectional area of nuclei and nuclear reactions, today it is also used in all fields of high-energy physics to express the cross sections of any scattering process, and is best understood as a measure of the probability of interaction between small particles. A barn is approximately the cross-sectional area of a uranium nucleus. The barn is also the unit of area used in nuclear quadrupole resonance and nuclear magnetic resonance to quantify the interaction of a nucleus with an electric field gradient. While the barn never was an SI unit, the SI standards body acknowledged it in the 8th SI Brochure (superseded in 2019) due to its use in particle physics.

Etymology

During Manhattan Project research on the atomic bomb during World War II, American physicists at Purdue University needed a secretive name for a unit with which to quantify the cross-sectional area presented by the typical nucleus (~10⁻²⁸ m²) and decided on "barn". They considered this a large target for particle accelerators that needed to have direct strikes on nuclei, and the proposers, physicists Marshall Holloway and Richard Baker, said that the constant "for nuclear purposes was really as big as a barn". In the American idiom " couldn't hit the broad side of a barn" refers to someone whose aim is very bad. Initially they hoped the name would obscure any reference to the study of nuclear structure; eventually, the word became a standard unit in nuclear and particle physics.

Commonly used prefixed versions

Conversions

Calculated cross sections are often given in terms of gigaelectronvolts ( GeV), via the conversion ''ħ''² ''c''²/ GeV² = = .

In natural units (where ''ħ'' = ''c'' = 1), this simplifies to GeV⁻² = = .

SI units with prefix

In SI, one can use units such as square femtometers (fm²). The most common SI prefixed unit for the barn is the femtobarn, which is equal to a tenth of a square zeptometer. Many scientific papers discussing high-energy physics mention quantities of fractions of femtobarn level.

Inverse femtobarn

The inverse femtobarn (fb⁻¹) is the unit typically used to measure the number of particle collision events per femtobarn of target cross-section, and is the conventional unit for time-integrated luminosity. Thus if a detector has accumulated of integrated luminosity, one expects to find 100 events per femtobarn of cross-section within these data.

Consider a particle accelerator where two streams of particles, with cross-sectional areas measured in femtobarns, are directed to collide over a period of time. The total number of collisions will be directly proportional to the luminosity of the collisions measured over this time. Therefore, the collision count can be calculated by multiplying the integrated luminosity by the sum of the cross-section for those collision processes. This count is then expressed as inverse femtobarns for the time period (e.g., 100 fb⁻¹ in nine months). Inverse femtobarns are often quoted as an indication of particle collider productivity.

Fermilab produced in the first decade of the 21st century. Fermilab's Tevatron took about 4 years to reach in 2005, while two of CERN's LHC experiments, ATLAS and CMS, reached over of proton–proton data in 2011 alone. In April 2012 the LHC achieved the collision energy of with a luminosity peak of 6760 inverse microbarns per second; by May 2012 the LHC delivered 1 inverse femtobarn of data per week to each detector collaboration. A record of over 23 fb⁻¹ was achieved during 2012. As of November 2016, the LHC had achieved over that year, significantly exceeding the stated goal of . In total, the second run of the LHC has delivered around to both ATLAS and CMS in 2015–2018.

Usage example

As a simplified example, if a beamline runs for 8 hours (28 800 seconds) at an instantaneous luminosity of   , then it will gather data totaling an integrated luminosity of  =  = during this period. If this is multiplied by the cross-section, then a dimensionless number is obtained equal to the number of expected scattering events.

See also

* " Shake", a unit of time created by the same people at the same time as the barn
*Orders of magnitude (area)
*List of unusual units of measurement
*List of humorous units of measurement

References

External links

*IUPACbr>citation for this usage of "barn"

{{DEFAULTSORT:Barn (Unit)
Units of area
Non-SI metric units
Particle physics