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Standard atomic weight Ar°(N) | |||||||||||||||||||||||||||||||||
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Natural nitrogen (7N) consists of two stable isotopes: the vast majority (99.62%) of naturally occurring nitrogen is nitrogen-14, with the remainder (0.38%) being nitrogen-15. Thirteen radioisotopes are also known, with atomic masses ranging from 9 to 23, along with three nuclear isomers. All of these radioisotopes are short-lived, the longest-lived being 13N with a half-life of 9.965(4) min. All of the others have half-lives shorter than ten seconds. Isotopes lighter than the stable ones generally decay to isotopes of carbon, and those heavier beta decay to isotopes of oxygen.
Nitrogen-13 is a positron emitter and one of the main isotopes used in medical PET scans.
Nuclide [n 1] | Z | N | Isotopic mass (Da) [4] [n 2] [n 3] | Half-life [1] [resonance width] | Decay mode [1] [n 4] | Daughter isotope [n 5] | Spin and parity [1] [n 6] [n 7] | Natural abundance (mole fraction) | |||||||||||
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Excitation energy | Normal proportion [1] | Range of variation | |||||||||||||||||
9 N [5] | 7 | 2 | <1 as [5] | 5p [n 8] | 4 He | ||||||||||||||
10 N | 7 | 3 | 10.04165(43) | 143(36) ys | p ? | 9 C ? | 1−, 2− | ||||||||||||
11 N | 7 | 4 | 11.026158(5) | 585(7) ys [780.0(9.3) keV] | p | 10 C | 1/2+ | ||||||||||||
11m N | 740(60) keV | 690(80) ys | p | 1/2− | |||||||||||||||
12 N | 7 | 5 | 12.0186132(11) | 11.000(16) ms | β+ (98.07(4)%) | 12 C | 1+ | ||||||||||||
β+α (1.93(4)%) | 8 Be [n 9] | ||||||||||||||||||
13 N [n 10] | 7 | 6 | 13.00573861(29) | 9.965(4) min | β+ | 13 C | 1/2− | ||||||||||||
14 N [n 11] | 7 | 7 | 14.003074004251(241) | Stable | 1+ | [0.99578, 0.99663] [6] | |||||||||||||
14m N | 2312.590(10) keV | IT | 14 N | 0+ | |||||||||||||||
15 N | 7 | 8 | 15.000108898266(625) | Stable | 1/2− | [0.00337, 0.00422] [6] | |||||||||||||
16 N | 7 | 9 | 16.0061019(25) | 7.13(2) s | β− (99.99846(5)%) | 16 O | 2− | ||||||||||||
β−α (0.00154(5)%) | 12 C | ||||||||||||||||||
16m N | 120.42(12) keV | 5.25(6) μs | IT (99.999611(25)%) | 16 N | 0− | ||||||||||||||
β− (0.000389(25)%) | 16 O | ||||||||||||||||||
17N | 7 | 10 | 17.008449(16) | 4.173(4) s | β−n (95.1(7)%) | 16 O | 1/2− | ||||||||||||
β− (4.9(7)%) | 17 O | ||||||||||||||||||
β−α (0.0025(4)%) | 13 C | ||||||||||||||||||
18 N | 7 | 11 | 18.014078(20) | 619.2(1.9) ms | β− (80.8(1.6)%) | 18 O | 1− | ||||||||||||
β−α (12.2(6)%) | 14 C | ||||||||||||||||||
β−n (7.0(1.5)%) | 17 O | ||||||||||||||||||
β−2n ? | 16 O ? | ||||||||||||||||||
19 N | 7 | 12 | 19.017022(18) | 336(3) ms | β− (58.2(9)%) | 19 O | 1/2− | ||||||||||||
β−n (41.8(9)%) | 18 O | ||||||||||||||||||
20 N | 7 | 13 | 20.023370(80) | 136(3) ms | β− (57.1(1.4)%) | 20 O | (2−) | ||||||||||||
β−n (42.9(1.4)%) | 19 O | ||||||||||||||||||
β−2n ? | 18 O ? | ||||||||||||||||||
21 N | 7 | 14 | 21.02709(14) | 85(5) ms | β−n (87(3)%) | 20 O | (1/2−) | ||||||||||||
β− (13(3)%) | 21 O | ||||||||||||||||||
β−2n ? | 19 O ? | ||||||||||||||||||
22 N | 7 | 15 | 22.03410(22) | 23(3) ms | β− (54.0(4.2)%) | 22 O | 0−# | ||||||||||||
β−n (34(3)%) | 21 O | ||||||||||||||||||
β−2n (12(3)%) | 20 O | ||||||||||||||||||
23 N [n 12] | 7 | 16 | 23.03942(45) | 13.9(1.4) ms | β− (> 46.6(7.2)%) | 23 O | 1/2−# | ||||||||||||
β−n (42(6)%) | 22 O | ||||||||||||||||||
β−2n (8(4)%) | 21 O | ||||||||||||||||||
β−3n (< 3.4%) | 20 O | ||||||||||||||||||
This table header & footer: |
IT: | Isomeric transition |
n: | Neutron emission |
p: | Proton emission |
Nitrogen-13 and oxygen-15 are produced in the atmosphere when gamma rays (for example from lightning) knock neutrons out of nitrogen-14 and oxygen-16:
The nitrogen-13 produced as a result decays with a half-life of 9.965(4) min to carbon-13, emitting a positron. The positron quickly annihilates with an electron, producing two gamma rays of about 511 keV. After a lightning bolt, this gamma radiation dies down with a half-life of ten minutes, but these low-energy gamma rays go only about 90 metres through the air on average, so they may only be detected for a minute or so as the "cloud" of 13N and 15O floats by, carried by the wind. [7]
Nitrogen-14 makes up the clear majority of natural nitrogen, about 99.62%, and is responsible for the Earth's stable atmosphere.
Nitrogen-14 is one of the very few stable nuclides with both an odd number of protons and of neutrons (seven each) and is the only one to make up a majority of its element. Unpaired protons or neutrons contribute a half-integer nuclear spin, which in this case is a spin 1/2 orbital, giving the nucleus a total magnetic spin of one (as the spins prefer to align).
The original source of nitrogen-14 and nitrogen-15 in the Universe is believed to be stellar nucleosynthesis, where they are produced as part of the CNO cycle.
Nitrogen-14 is the source of naturally occurring, radioactive, carbon-14. Some kinds of cosmic radiation cause a nuclear reaction with nitrogen-14 in the upper atmosphere of the Earth, creating carbon-14, which decays back to nitrogen-14 with a half-life of 5700 years.
Nitrogen-15 is a rare stable isotope of nitrogen, comprising about 0.38%. Nitrogen-15 presents one of the lowest thermal neutron capture cross sections of all isotopes. [8]
Nitrogen-15 is frequently used in NMR (Nitrogen-15 NMR spectroscopy). Unlike the more abundant nitrogen-14, which has an integer nuclear spin and thus a quadrupole moment, 15N has a fractional nuclear spin of one-half, which offers advantages for NMR such as narrower line width. As most nitrogen NMR studies look at a single nitrogen atom in an organic molecule, isotopic labeling is feasible.
Nitrogen-15 tracing is a technique used to study the nitrogen cycle.
The radioisotope 16N is the dominant radioactivity source in the coolant water of nuclear reactors cooled by water during normal operation. It is produced from 16O (in water) via an (n,p) reaction, in which the 16O atom captures a neutron and expels a proton. It has a short half-life of 7.13 seconds, but its decay back to 16O produces high-energy gamma radiation (6.13 MeV principal line [9] ). [10] Because of this, access to the primary coolant piping in a pressurised water reactor must be restricted during reactor power operation. [10] It is a sensitive and immediate indicator of leaks from the primary coolant system to the secondary steam cycle and is the primary means of detection for such leaks. [10]
Daughter products other than nitrogen