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2 References  





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Isotopes of argon






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From Wikipedia, the free encyclopedia
 

(Redirected from Argon-38)

Isotopesofargon (18Ar)

Main isotopes[1]

Decay

abun­dance

half-life (t1/2)

mode

pro­duct

36Ar

0.334%

stable

37Ar

trace

35 d

ε

37Cl

38Ar

0.0630%

stable

39Ar

trace

268 y

β

39K

40Ar

99.6%

stable

41Ar

trace

109.34 min

β

41K

42Ar

synth

32.9 y

β

42K

Standard atomic weight Ar°(Ar)

  • [39.79239.963][2]
  • 39.95±0.16 (abridged)[3]
  • talk
  • edit
  • Argon (18Ar) has 26 known isotopes, from 29Ar to 54Ar, of which three are stable (36Ar, 38Ar, and 40Ar). On the Earth, 40Ar makes up 99.6% of natural argon. The longest-lived radioactive isotopes are 39Ar with a half-life of 268 years, 42Ar with a half-life of 32.9 years, and 37Ar with a half-life of 35.04 days. All other isotopes have half-lives of less than two hours, and most less than one minute.

    The naturally occurring 40K, with a half-life of 1.248×109 years, decays to stable 40Ar by electron capture (10.72%) and by positron emission (0.001%), and also transforms to stable 40Ca via beta decay (89.28%). These properties and ratios are used to determine the age of rocks through potassium–argon dating.[4]

    Despite the trapping of 40Ar in many rocks, it can be released by melting, grinding, and diffusion. Almost all of the argon in the Earth's atmosphere is the product of 40K decay, since 99.6% of Earth atmospheric argon is 40Ar, whereas in the Sun and presumably in primordial star-forming clouds, argon consists of < 15% 38Ar and mostly (85%) 36Ar. Similarly, the ratio of the three isotopes 36Ar:38Ar:40Ar in the atmospheres of the outer planets is measured to be 8400:1600:1.[5]

    In the Earth's atmosphere, radioactive 39Ar (half-life 268(8) years) is made by cosmic ray activity, primarily from 40Ar. In the subsurface environment, it is also produced through neutron captureby39K or alpha emissionbycalcium. The content of 39Ar in natural argon is measured to be of (8.0±0.6)×10−16 g/g, or (1.01±0.08) Bq/kg of 36, 38, 40Ar.[6] The content of 42Ar (half-life 33 years) in the Earth's atmosphere is lower than 6×10−21 parts per part of 36, 38, 40Ar.[7] Many endeavors require argon depleted in the cosmogenic isotopes, known as depleted argon.[8] Lighter radioactive isotopes can decay to different elements (usually chlorine) while heavier ones decay to potassium.

    36Ar, in the form of argon hydride, was detected in the Crab Nebula supernova remnant during 2013.[9][10] This was the first time a noble molecule was detected in outer space.[9][10]

    37Ar is a synthetic radionuclide that is created via neutron captureof40Ca followed by alpha particle emission, as a result of subsurface nuclear explosions. It has a half-life of 35 days.[4]

    List of isotopes[edit]

    Nuclide
    [n 1]

    Z

    N

    Isotopic mass (Da)[11]
    [n 2][n 3]

    Half-life[1]

    Decay
    mode
    [1]
    [n 4]

    Daughter
    isotope

    [n 5]

    Spin and
    parity[1]
    [n 6][n 7]

    Natural abundance (mole fraction)

    Excitation energy

    Normal proportion[1]

    Range of variation

    29Ar[12]

    18

    11

    29.04076(47)#

    2p

    27S

    5/2+#

    30Ar

    18

    12

    30.02369(19)#

    <10 ps

    2p

    28S

    0+

    31Ar

    18

    13

    31.01216(22)#

    15.0(3ms

    β+, p (68.3%)

    30S

    5/2+

    β+ (22.63%)

    31Cl

    β+, 2p (9.0%)

    29P

    β+, 3p (0.07%)

    28Si

    β+, p, α? (<0.38%)

    26Si

    β+, α? (<0.03%)

    27P

    2p? (<0.03%)

    29S

    32Ar

    18

    14

    31.9976378(19)

    98(2ms

    β+ (64.42%)

    32Cl

    0+

    β+, p (35.58%)

    31S

    33Ar

    18

    15

    32.98992555(43)

    173.0(20ms

    β+ (61.3%)

    33Cl

    1/2+

    β+, p (38.7%)

    32S

    34Ar

    18

    16

    33.980270092(83)

    846.46(35ms

    β+

    34Cl

    0+

    35Ar

    18

    17

    34.97525772(73)

    1.7756(10s

    β+

    35Cl

    3/2+

    36Ar

    18

    18

    35.967545106(28)

    Observationally Stable[n 8]

    0+

    0.003336(210)

    37Ar

    18

    19

    36.96677630(22)

    35.011(19d

    EC

    37Cl

    3/2+

    Trace[n 9]

    38Ar

    18

    20

    37.96273210(21)

    Stable

    0+

    0.000629(70)

    39Ar[n 10]

    18

    21

    38.9643130(54)

    268.2+3.1
    −2.9
     y[13]

    β

    39K

    7/2−

    8×10−16[14][n 9]

    40Ar[n 11]

    18

    22

    39.9623831220(23)

    Stable

    0+

    0.996035(250)[n 12]

    41Ar

    18

    23

    40.96450057(37)

    109.61(4) min

    β

    41K

    7/2−

    Trace[n 9]

    42Ar

    18

    24

    41.9630457(62)

    32.9(11y

    β

    42K

    0+

    43Ar

    18

    25

    42.9656361(57)

    5.37(6) min

    β

    43K

    5/2(−)

    44Ar

    18

    26

    43.9649238(17)

    11.87(5) min

    β

    44K

    0+

    45Ar

    18

    27

    44.96803973(55)

    21.48(15s

    β

    45K

    (5/2−,7/2−)

    46Ar

    18

    28

    45.9680392(25)

    8.4(6s

    β

    46K

    0+

    47Ar

    18

    29

    46.9727671(13)

    1.23(3s

    β (>99.8%)

    47K

    (3/2)−

    β, n? (<0.2%)

    46K

    48Ar

    18

    30

    47.976001(18)

    415(15ms

    β (62%)

    48K

    0+

    β, n (38%)

    47K

    49Ar

    18

    31

    48.98169(43)#

    236(8ms

    β

    49K

    3/2−#

    β, n (29%)

    48K

    β, 2n?

    47K

    50Ar

    18

    32

    49.98580(54)#

    106(6ms

    β (63%)

    50K

    0+

    β, n (37%)

    49K

    β, 2n?

    48K

    51Ar

    18

    33

    50.99303(43)#

    30# ms
    [>200 ns]

    β?

    51K

    1/2−#

    β, n?

    50K

    β, 2n?

    49K

    52Ar

    18

    34

    51.99852(64)#

    40# ms
    [>620 ns]

    β?

    52K

    0+

    β, n?

    51K

    β, 2n?

    50K

    53Ar

    18

    35

    53.00729(75)#

    20# ms
    [>620 ns]

    β?

    53K

    5/2−#

    β, n?

    52K

    β, 2n?

    51K

    54Ar

    18

    36

    54.01348(86)#

    5# ms
    [>400 ns]

    β?

    54K

    0+

    β, n?

    53K

    β, 2n?

    52K

    This table header & footer:
    1. ^ mAr – Excited nuclear isomer.
  • ^ ( ) – Uncertainty (1σ) is given in concise form in parentheses after the corresponding last digits.
  • ^ # – Atomic mass marked #: value and uncertainty derived not from purely experimental data, but at least partly from trends from the Mass Surface (TMS).
  • ^ Modes of decay:

    n:

    Neutron emission

    p:

    Proton emission

  • ^ Bold symbol as daughter – Daughter product is stable.
  • ^ ( ) spin value – Indicates spin with weak assignment arguments.
  • ^ # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
  • ^ Believed to undergo double electron capture to 36S (lightest theoretically unstable nuclide for which no evidence of radioactivity has been observed)
  • ^ a b c Cosmogenic nuclide
  • ^ Used in argon–argon dating
  • ^ Used in argon–argon dating and potassium–argon dating
  • ^ Generated from 40K in rocks. These ratios are terrestrial. Cosmic abundance is far less than 36Ar.
  • References[edit]

    1. ^ a b c d e Kondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S.; Audi, G. (2021). "The NUBASE2020 evaluation of nuclear properties" (PDF). Chinese Physics C. 45 (3): 030001. doi:10.1088/1674-1137/abddae.
  • ^ "Standard Atomic Weights: Argon". CIAAW. 2017.
  • ^ Prohaska, Thomas; Irrgeher, Johanna; Benefield, Jacqueline; Böhlke, John K.; Chesson, Lesley A.; Coplen, Tyler B.; Ding, Tiping; Dunn, Philip J. H.; Gröning, Manfred; Holden, Norman E.; Meijer, Harro A. J. (4 May 2022). "Standard atomic weights of the elements 2021 (IUPAC Technical Report)". Pure and Applied Chemistry. doi:10.1515/pac-2019-0603. ISSN 1365-3075.
  • ^ a b "40Ar/39Ar dating and errors". Archived from the original on 9 May 2007. Retrieved 7 March 2007.
  • ^ Cameron, A.G.W. (1973). "Elemental and isotopic abundances of the volatile elements in the outer planets". Space Science Reviews. 14 (3–4): 392–400. Bibcode:1973SSRv...14..392C. doi:10.1007/BF00214750. S2CID 119861943.
  • ^ P. Benetti; et al. (2007). "Measurement of the specific activity of 39Ar in natural argon". Nuclear Instruments and Methods A. 574 (1): 83–88. arXiv:astro-ph/0603131. Bibcode:2007NIMPA.574...83B. doi:10.1016/j.nima.2007.01.106. S2CID 17073444.
  • ^ V. D. Ashitkov; et al. (1998). "New experimental limit on the 42Ar content in the Earth's atmosphere". Nuclear Instruments and Methods A. 416 (1): 179–181. Bibcode:1998NIMPA.416..179A. doi:10.1016/S0168-9002(98)00740-2.
  • ^ H. O. Back; et al. (2012). "Depleted Argon from Underground Sources". Physics Procedia. 37: 1105–1112. Bibcode:2012PhPro..37.1105B. doi:10.1016/j.phpro.2012.04.099.
  • ^ a b Quenqua, Douglas (13 December 2013). "Noble Molecules Found in Space". The New York Times. Retrieved 13 December 2013.
  • ^ a b Barlow, M. J.; et al. (2013). "Detection of a Noble Gas Molecular Ion, 36ArH+, in the Crab Nebula". Science. 342 (6164): 1343–1345. arXiv:1312.4843. Bibcode:2013Sci...342.1343B. doi:10.1126/science.1243582. PMID 24337290. S2CID 37578581.
  • ^ Wang, Meng; Huang, W.J.; Kondev, F.G.; Audi, G.; Naimi, S. (2021). "The AME 2020 atomic mass evaluation (II). Tables, graphs and references*". Chinese Physics C. 45 (3): 030003. doi:10.1088/1674-1137/abddaf.
  • ^ Mukha, I.; et al. (2018). "Deep excursion beyond the proton dripline. I. Argon and chlorine isotope chains". Physical Review C. 98 (6): 064308–1–064308–13. arXiv:1803.10951. Bibcode:2018PhRvC..98f4308M. doi:10.1103/PhysRevC.98.064308. S2CID 119384311.
  • ^ Golovko, Victor V. (15 October 2023). "Application of the most frequent value method for 39Ar half-life determination". The European Physical Journal C. 83 (10): 930. arXiv:2310.06867. Bibcode:2023EPJC...83..930G. doi:10.1140/epjc/s10052-023-12113-6. ISSN 1434-6052.
  • ^ Lu, Zheng-Tian (1 March 2013). "What trapped atoms reveal about global groundwater". Physics Today. 66 (3): 74–75. Bibcode:2013PhT....66c..74L. doi:10.1063/PT.3.1926.
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